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crackrn


Dec 30, 2004, 7:31 AM
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pendulum fall...
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What's the best way to take that kind of fall? I just sprained the bejesus out of my ankle taking a pendulum fall. I don't remember exactly the specifics but I'm guessing I tried to absorb some of the shock with my legs and did it wrong. Any suggestions?


overlord


Dec 30, 2004, 8:05 AM
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dont take such a fall.

but if you do, its better to have some more slack in the system (if the impact wall is overhanging or vertical, less slack if its a slab, in wich case youre proper f***ed) to kinda lessen the pendulum effect. apart from that, its better to absorb the shock with your arms/legs than your torso/head.


thegreytradster


Dec 30, 2004, 8:51 PM
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What's the best way to take that kind of fall? I just sprained the bejesus out of my ankle taking a pendulum fall. I don't remember exactly the specifics but I'm guessing I tried to absorb some of the shock with my legs and did it wrong. Any suggestions?

What is not intuitively obvious is that the force involved is exactly the same as a vertical fall. Only the direction of impact is changed. That's why intentional payout of slack may sometimes be a good idea. Changes the directon of fall to a more conventional angle.

In other words consider a fall where you traverse 15 ft from a vertical dihedral with your last pro. You then fall. Your total fall verticaly is 15 ft but now your direction of movement is sideways into the dihedral, BUT, AT THE SAME VELOCITY AS A VERTICAL FALL!. Ouch :shock:

Just do what you can to make sure the parts that heal fastest hit first. A sprained ankle, consider you got off light.


grayhghost


Dec 30, 2004, 9:13 PM
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Yeah, I broke my foot in
a 60 ft. pengi-swing during
a rappel, sucks when your
in the middle of it and know
how hard you are going to hit,
just make sure you go in feet-
first, kind of like a shallow pool.


jt512


Dec 31, 2004, 1:03 AM
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What's the best way to take that kind of fall? I just sprained the bejesus out of my ankle taking a pendulum fall. I don't remember exactly the specifics but I'm guessing I tried to absorb some of the shock with my legs and did it wrong. Any suggestions?

What is not intuitively obvious is that the force involved is exactly the same as a vertical fall.

What force, the impact force? The impact force is much higher for a pendulum fall into a wall than it is for a vertical fall onto a rope.

In reply to:
That's why intentional payout of slack may sometimes be a good idea. Changes the directon of fall to a more conventional angle.

Slack reduces the impact force into the wall because it increases the radius of the arc and hence reduces the angular velocity.

-Jay


dirtineye


Dec 31, 2004, 2:10 AM
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How exactly did you fall? Did you know it was coming or was it sudden? Did your hands come off first or was it your feet? How much rope was in the system? Were you spinning? did you swing along the wall or swing against it?

You are going to have to give a detailed description of the distances, the angles, your body position, how you approached the wall, what the wall was like where you hit and more to get specific advice.

Since you are having to guess at how you hit the wall, it doesn't sound like you know what happened, and that will make it hard to tell you what you should have done other than in a generic sense.\


swinging into a wall. perpendicular to the wall:

Basically you have to react immediately and get in a good position to meet the wall with your feet. You have to use your eyes to guide your feet. you want both feet to hit at the same time (probably you hit with one foot a lot more than the other) with your knees bent. keep your center of gravity between your feet. Keep your hands up (elbows bent) to protect your head from the wall and also absorb some impact, don't grab the rope.

Along the wall, paralel:

Try to keep from skittering over the wall in a spin. You might need to 'pat ' your way along-- if your feet or hands touch, get em off fast-- and ready to touh down again. If you keep contact with the wall for more than a split second at a time, you may start to spin. Do most of the work with your feet, keep em moving, and use your hands to protect your head (hands up in front of you, not grabbing the rope). IF you scrape your hands or other body parts along the wall you will probably be sorry.

That's only two cases, and they assume you are already or are able to quickly get into the good position to make contact.

IF you fall at some other angle to the wall or out of a double heel hook and get sideways or maybe upside down, things are a little different, but hte big thing is still , look where you are going, and protect your head with your hands.

IF the situation is dicey, you should already have a plan for how you would deal with the fall-- in other words, know the fall consequences before you get into the falling situation and be ready to act in your best interests should you fall.

And last, but truly not least, sometimes your pro will determine the kind of fall you take. For example, if you are exiting a horizontal roof, with a possible perpendicular (Or similar) to the wall fall, and you can get pro away from the wall, GET IT IN. (If you can get pro toward the roof edge in the direction yo uare climbing so much the better. Swinging out into space is so much better than swinging back into the wall) In a clean pendulum fall, your greatest horizontal velocity is when the rope is stright down-- as you start to swing back up, you lose some horizontal velocity.


thegreytradster


Dec 31, 2004, 5:20 AM
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[
What force, the impact force? The impact force is much higher for a pendulum fall into a wall than it is for a vertical fall onto a rope.

-Jay

Correctomundo; a cat named Galleo figured that one out. The TIME to fall is the same and since you must sweep out a longer path (arc) the final velocity and energy is higher than falling vertically. The bigest contributor to injury though is that parts a lot more fragile than the legs are more likely to hit first.

Dirtineyes' point about placing some pro as soon as possible horizontally after the start of a traverse is important. You really need to treat it the same as placing gear soon at the start of a pitch. It's just as important, but not obvious to the noob and not often emphasized.


crackrn


Jan 1, 2005, 1:53 AM
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I'm getting a refresher course in physics!

Curt, I fell parallel to the wall, was just starting to move vertically (but at an angle) off the traverse when my feet slipped. I remember trying to bring my body around so I could absorb some of the shock with my legs but hit the wall too soon. I definitely spun once or twice. I must have braced with my (now) injured ankle but not in ANY kind of controlled fashion Those are good tips. I think my biggest mistake was not planning for the possibility of that fall. Like the graytradster said, I think I got off lightly.


esallen


Jan 1, 2005, 2:14 AM
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Grip rope tightly, then cose your eyes and cry.


chiranjeeb


Jan 1, 2005, 2:21 AM
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Thegreytradster : I think a correction is due. The impact force is higher not because you are tracing a longer trajectory.
The kinetic energy generated in a 30 foot fall is same whether you fall that 30 foot straight down or fall that 30 foot in an arc (conservation of energy). The pendulum fall is worse only because in the pendulum the rope is not able to absorb that kinetic energy and your body is left to absorb that energy. Actually, the rope does absorb some enrgy in a pendulum fall, but it is not the same as falling onto the rope vertically. So if you fall 30 foot and smack into a dihedral, it is pretty similar to falling 30 foot vertically onto a ledge with the rope not absorbing much energy.


dirtineye


Jan 1, 2005, 2:45 AM
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I'm getting a refresher course in physics!

Curt, I fell parallel to the wall, was just starting to move vertically (but at an angle) off the traverse when my feet slipped. I remember trying to bring my body around so I could absorb some of the shock with my legs but hit the wall too soon. I definitely spun once or twice. I must have braced with my (now) injured ankle but not in ANY kind of controlled fashion Those are good tips. I think my biggest mistake was not planning for the possibility of that fall. Like the graytradster said, I think I got off lightly.

Ok, starting to get a picture.

Were you leading or following, or top roping? If you were on pro, did you go back toward the last piece (as in leading) or forward toward the next pice as in following)?

Glad those tips help.

Edit:
And since it was sa parallel fall, Scraping along the wall, now you can see how NOT trying to brace but instead trying to 'pat ' your way along with quick light touches and go with the flow might have helped you avoid your sprain. You would swing back and forth a little, but this is fine.

Arno covers some of this swinging over the rock foot work at the start of his falling clinic, which I highly recommend to anyone.


crackrn


Jan 1, 2005, 3:47 AM
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Curt, I was leading (woohoo! Sorry, still new, obviously, and excited about it!) and fell back towards the last bolt. I have a nice (rope?) burn on my arm from it too. I think I was so focused on trying to control the fall I didn't "go with it" and thus was more injured. Patting along the wall might have been more scary but might have ended up better. It's better now though...I can actually bear weight now!

I've seen several references to Arno and his clinics. If I do a search will I get numerous threads with relevant info?


jcshaggy


Jan 3, 2005, 11:16 AM
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I was above my clipped bolt to the left when i bailed on a 5.11c this last December. I swung and clipped the rope which flipped me upside down.

Nothing beats knocking your head against rock while you are looking at the ground(I put it down to my own stupidity).
Going to write a big THANK YOU letter to my harness manufacturer.


nicklikesfire


Jan 3, 2005, 11:53 AM
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Instead of getting into a lot of pysics, jt512 is (for all practical and simple purposes, especially this one) correct.


dutyje


Jan 3, 2005, 12:17 PM
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In reply to:
Slack reduces the impact force into the wall because it increases the radius of the arc and hence reduces the angular velocity.

:roll:

Technically, Jay, it wasn't the angular velocity that hurt his ankles. It was the tangential linear velocity. Or, to be more precise, it was the sudden, rapid deceleration from that linear velocity that caused his pain. :wink:

Responses composed with the intent to project maximum apparent intellect always sound so patronizing.

(side note to crackrn -- he's right, though)


dirtineye


Jan 3, 2005, 3:44 PM
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Curt, I was leading (woohoo! Sorry, still new, obviously, and excited about it!) and fell back towards the last bolt. I have a nice (rope?) burn on my arm from it too. I think I was so focused on trying to control the fall I didn't "go with it" and thus was more injured. Patting along the wall might have been more scary but might have ended up better. It's better now though...I can actually bear weight now!

I've seen several references to Arno and his clinics. If I do a search will I get numerous threads with relevant info?

That "patting along" idea is how I describe it, cause I patted my way down (mostly vertical fall) a high angle slab once and didn't get a scratch. It was like playing high speed patty cake with your hands and feet, sort of, and it worked.

I think most of the time a better way to describe what to do in a pendulum along the wall is "dancing along the wall", if that helps. Be light on your feet with quick touches, using your eyes to guide your feet.

You could just go to Arno's website for clinic info, put Warrior's Way or rock warrior's way in a search engine like google. I think his site is the desiderata institute or something like that.

I think the most important thing you have learned the hard way is that if your feet hit wrong or stay on too long during a fall, you won't like the result.


jt512


Jan 3, 2005, 7:24 PM
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In reply to:
Slack reduces the impact force into the wall because it increases the radius of the arc and hence reduces the angular velocity.

:roll:

Technically, Jay, it wasn't the angular velocity that hurt his ankles. It was the tangential linear velocity. Or, to be more precise, it was the sudden, rapid deceleration from that linear velocity that caused his pain. :wink:

Responses composed with the intent to project maximum apparent intellect always sound so patronizing.

As your post clearly demonstrated.

In reply to:
(side note to crackrn -- he's right, though)

And therefore the point of your post was, what, then?

-Jay


dutyje


Jan 3, 2005, 11:48 PM
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In reply to:
In reply to:
Slack reduces the impact force into the wall because it increases the radius of the arc and hence reduces the angular velocity.

:roll:

Technically, Jay, it wasn't the angular velocity that hurt his ankles. It was the tangential linear velocity. Or, to be more precise, it was the sudden, rapid deceleration from that linear velocity that caused his pain. :wink:

Responses composed with the intent to project maximum apparent intellect always sound so patronizing.

As your post clearly demonstrated.

In reply to:
(side note to crackrn -- he's right, though)

And therefore the point of your post was, what, then?

-Jay

to get you riled up.


rockrat_co


Jan 13, 2005, 2:44 AM
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IF you can tell when you may launch off, jump off in the direction of your last pro, this will minimize the fall's impact. Just to inform; a fifteen foot pendulum fall (spelling??) can exert forces similar to getting hit by a car going 30 miles per hour on your body! Awesome isn't it??! :shock: :wink:


4togo


Jan 17, 2006, 3:52 AM
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That "patting along" idea is how I describe it, cause I patted my way down (mostly vertical fall) a high angle slab once and didn't get a scratch. It was like playing high speed patty cake with your hands and feet, sort of, and it worked.

As part of learning to place gear this summer I took "lead falls" with a toprope back-up. The climb was mostly slab and I was told to basically run backwards as fast as I could. Give in to the fall, in particular no knees / crouching on the rock. Worked really well. Is this "patting along" concept basically the same thing? Or a version for use on higher-angle slab?

Trying to get a mental picture since I have yet to read Arno's book.

(side note -- falling like that, with a good dynamic belay (and of course the mental training wheels of the top-rope backup) was FUN! I'm running backwards down the rock... I'm running backwards down the rock... I'm running backwa.. hey, I stopped running?)


majid_sabet


Jan 17, 2006, 4:20 AM
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I remember one case of Peng 10-15 feet fall + short swing 2-3 feet, climber hide the side of the rock with his climbing rack, broke 2-3 ribs 21 pitches up .


Partner robdotcalm


Jan 17, 2006, 4:34 AM
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Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)


jt512


Jan 17, 2006, 5:07 AM
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fucking website


jt512


Jan 17, 2006, 5:09 AM
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In reply to:
Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)

Pnedulum fall: give slack. It really is that simple, though I'm sure the collective internet community will have no trouble coming up with several pathological counter-examples.

Jay


curt


Jan 17, 2006, 5:20 AM
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In reply to:
In reply to:
Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)

Pnedulum fall: give slack. It really is that simple, though I'm sure the collective internet community will have no trouble coming up with several pathological counter-examples.

Jay

No, it's not that simple--it's situational. Feed out slack and mgh increases.

Curt


jt512


Jan 17, 2006, 5:38 AM
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In reply to:
In reply to:
In reply to:
Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)

Pnedulum fall: give slack. It really is that simple, though I'm sure the collective internet community will have no trouble coming up with several pathological counter-examples.

Jay

No, it's not that simple--it's situational. Feed out slack and mgh increases.

Curt

But so does the amount of rope out to absorb the additional energy. The result is that letting rope out slightly increases the fall factor, but greatly decreases the horizontal velocity. It is pretty simple: you have a rope to limit the impact force with the rope, and a rock face to limit the impact force with the wall. If y'all put your heads together, I'm sure you can proudly name many exceptions, but in general, it should be clear that the rock wall presents the greater danger, and is the impact you want to take steps to minimize.

Jay


curt


Jan 17, 2006, 5:58 AM
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In reply to:
In reply to:
In reply to:
In reply to:
Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)

Pnedulum fall: give slack. It really is that simple, though I'm sure the collective internet community will have no trouble coming up with several pathological counter-examples.

Jay

No, it's not that simple--it's situational. Feed out slack and mgh increases.

Curt

But so does the amount of rope out to absorb the additional energy. The result is that letting rope out slightly increases the fall factor, but greatly decreases the horizontal velocity. It is pretty simple: you have a rope to limit the impact force with the rope, and a rock face to limit the impact force with the wall. If y'all put your heads together, I'm sure you can proudly name many exceptions, but in general, it should be clear that the rock wall presents the greater danger, and is the impact you want to take steps to minimize.

Jay

Right. Then, by that logic, the amount of rope you should feed out (to improve the situation) should be infinite.

Curt


cintune


Jan 18, 2006, 7:48 PM
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But only if you have infinite space to fall in.

Fallllllliiiiinnggggggggggggggggggggggggggggggggg................


billl7


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There are two aspects in this slack-or-not-to-slack for a pendulum fall:

more slack -> more potential energy
more slack -> smaller percentage of energy is converted into horizontal motion

Anyone care to whip out the pencil and see which one dominates (edit: in terms of total horizontal energy)?

Bill


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Jan 18, 2006, 8:39 PM
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[quote="billl7"

more slack -> more potential energy
more slack -> smaller percentage of energy is converted into horizontal motion

Bill
How did you arrive at the 2nd conclusion?

Cheers,
Rob.calm


billl7


Jan 18, 2006, 8:52 PM
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In reply to:
In reply to:

more slack -> more potential energy
more slack -> smaller percentage of energy is converted into horizontal motion

Bill

How did you arrive at the 2nd conclusion?

Cheers,
Rob.calm
Without slack, the actual pendulum starts with the rope horizontal (assume horizontal traverse). With slack the pendulum actually starts when the rope becomes taught with the rope (editted typo) at some angle from horizontal.

The varying angle makes a difference in how much of the total energy is transferred into horizontal energy. But also total energy is higher when there is slack. And so was wondering which one made more difference in terms of the final horizontal energy.


pastprime


Jan 18, 2006, 9:33 PM
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Good info, thanks. It occurs to me that in an alpine/trad situation where it is hard to communicate with your belayer, if you were leading and in danger of a pendulum into a wall, it would be wise to be pulling slack as you went, and the amount of slack you would want to keep in the rope would be enough that your vertical drop before hitting the end of the rope would be somewhat more than the distance of the swing horizontally that would follow.
Example: your last piece is at the top of an open book, and you have led 10 feet horizontally to the right without yet being able to get anything in. you would be wise to have pulled enough rope so that there is at least 15 feet of rope between you and the last piece, and better more than that than less.

Do you physicists agree, or am I seeing it wrong?


talons05


Jan 18, 2006, 9:57 PM
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In reply to:
Good info, thanks. It occurs to me that in an alpine/trad situation where it is hard to communicate with your belayer, if you were leading and in danger of a pendulum into a wall, it would be wise to be pulling slack as you went, and the amount of slack you would want to keep in the rope would be enough that your vertical drop before hitting the end of the rope would be somewhat more than the distance of the swing horizontally that would follow.
Example: your last piece is at the top of an open book, and you have led 10 feet horizontally to the right without yet being able to get anything in. you would be wise to have pulled enough rope so that there is at least 15 feet of rope between you and the last piece, and better more than that than less.

Do you physicists agree, or am I seeing it wrong?

I am not a physicist, but have studied a lot of physics for my major. IMHO, what you say does have a basis in classical physics. But you have to find a compromise. As the length of rope increases relative to your horizontal distance from the piece, the angle of your fall increases (steepens) and approaches (but does not reach) vertical. Of course at some point, this fails to help and begins to increase the force again. Probably somewhere around 1.5x the horizontal distance.

Basically, you are trying to increase the y (vertical) component of your trajectory since that is the vector in which the rope is able to absorb force.

Cheers,

A.W.


billl7


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In reply to:
Good info, thanks. It occurs to me that in an alpine/trad situation where it is hard to communicate with your belayer, if you were leading and in danger of a pendulum into a wall, it would be wise to be pulling slack as you went, and the amount of slack you would want to keep in the rope would be enough that your vertical drop before hitting the end of the rope would be somewhat more than the distance of the swing horizontally that would follow.
Example: your last piece is at the top of an open book, and you have led 10 feet horizontally to the right without yet being able to get anything in. you would be wise to have pulled enough rope so that there is at least 15 feet of rope between you and the last piece, and better more than that than less.

Do you physicists agree, or am I seeing it wrong?
You would be right if the smaller percent of total energy transferred horizontally more than negates the potential energy added by having more slack.

I'm no physicist but the interplay isn't hard to calculate when assuming a very simple system (e.g., not addressing how friction and/or stretch come into play differently). I'll try to do it tonight if someone doesn't beat me to it; either way it would be good for us to have more than one person weigh in on the issue.

Bill


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None of the arguments so far, except mine, have taken into account that even though you produce more energy with more slack out, you also have more rope out to absorb that energy. The net result, in practical situations, is a only a small increase in the vertical component of impact force, so small that you probably wouldn't notice it. I haven't done the math, but the small increase in impact force is a small price to pay for the reduction in horizontal swing.

Jay


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Jan 18, 2006, 10:20 PM
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What's the best way to take that kind of fall? I just sprained the bejesus out of my ankle taking a pendulum fall. I don't remember exactly the specifics but I'm guessing I tried to absorb some of the shock with my legs and did it wrong. Any suggestions?

What is not intuitively obvious is that the force involved is exactly the same as a vertical fall.

What force, the impact force? The impact force is much higher for a pendulum fall into a wall than it is for a vertical fall onto a rope.

In reply to:
That's why intentional payout of slack may sometimes be a good idea. Changes the directon of fall to a more conventional angle.

Slack reduces the impact force into the wall because it increases the radius of the arc and hence reduces the angular velocity.

-Jay

Jay, you have a lot of things wrong here with what actually happens.
First, the impact of swinging into a wall is exactly the same as hitting the ground if you were to be fallign vertical the same distance as that of the rope that has been paid out to allow for the swing.
Second, the payout of slack does help but keeping slack in the system would not help. If you think about the translation of vertical fall velocity into a horizontal velocity, initial slack in the system would act like the climber taking a larger swing. The tricky, dangerous, and highly skilled payout of slack during a fall would, in fact, lessen the inpact on the slab you would be swinging into.

To experience this hang a weight by a string, give it some inches slack and drop it at the top of a pendulum. By the time it crosses a plum line from your hand to the ground, it is moving faster than no slack. (make sure yo take the slack from your hand and not just move the climber closer to the swing point.) Then try, as your 'climber' starts to swing in, drop your hand and notice how much slower he climber crosses that plum line.

That's the physics of the pendulum, well not really why, just what happens (form a mech. eng. major), but that gradual payout is difficult, and sometimes painfull, for the belay. My advice would be...

Wear a helmet, don't close your eyes, keep your head over your heels, hold on for the ride, and don't poop yourself...or cry, and at least you'll have your dignity.


billl7


Jan 18, 2006, 10:20 PM
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In reply to:
None of the arguments so far, except mine, have taken into account that even though you produce more energy with more slack out, you also have more rope out to absorb that energy. The net result, in practical situations, is a only a small increase in the vertical component of impact force, so small that you probably wouldn't notice it. I haven't done the math, but the small increase in impact force is a small price to pay for the reduction in horizontal swing.

Jay
Right. Your point is relevant: there's more rope to stretch but also the fall factor goes up as slack is paid out. But I was thinking of starting with a simple system - maybe fall factor could be brought in later or maybe not if the pay-off for slack is clear enough (assuming it doesn't cause a collision with something else).

Bill

Edit: curtis_g - I don't see anything wrong with your quotes of Jay, allowing for some interpretation on my part. Maybe we can hold off with the debate until someone produces some numbers? (no abuse intended)


pastprime


Jan 18, 2006, 10:27 PM
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It also occurs to me, which thing I had never before considered, that if you are faced with a traversing exit from a corner, you would be better off not placing that last piece high in the corner before leaving, which is a pretty common habit. It seems it would be better to get a good piece into the corner a ways below the exit so your progress is more decidedly above the piece than sideways from it.
Never thought of that before. Good to know.


Partner cracklover


Jan 18, 2006, 10:33 PM
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In reply to:
None of the arguments so far, except mine, have taken into account that even though you produce more energy with more slack out, you also have more rope out to absorb that energy. The net result, in practical situations, is a only a small increase in the vertical component of impact force, so small that you probably wouldn't notice it. I haven't done the math, but the small increase in impact force is a small price to pay for the reduction in horizontal swing.

Jay

Another point:

If you give the classic version of a soft catch* you can "absorb" a fair bit of energy through the friction in the rope around the bends over the top biner, belay biner, and belay device.

GO

*Do people know what a soft catch even means? It doesn't mean just feeding out slack before the rope goes tight. It means allowing some rope to slip through the belay device as it comes tight. Practice.


pastprime


Jan 18, 2006, 10:39 PM
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OK, I did the weight on a string, holding one end against the wall, and letting it drop from a point horizontally away from the anchor. With no slack, it really smacks the wall, just as expected. With even a bit of slack in the line before dropping, the impact is quite dramatically reduced.
Try it you own self. You'll see.


pastprime


Jan 18, 2006, 11:21 PM
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I shouldn't have said "even a bit of slack", that's an exaggeration; the crossover point where an improvement is pretty apparent seems to be where the dropping object falls a distance of half or more of the horizontal distance it was from the anchor before it comes tight on the string. I would expect on a dynamic rope where much of the energy is dissipated before being translated to horizontal motion, the difference would be even greater.
I hate trying to write coherently here at work, where there's not time to think out the proper way to say things before consigning them to all the world/


curtis_g


Jan 18, 2006, 11:28 PM
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In reply to:
In reply to:
None of the arguments so far, except mine, have taken into account that even though you produce more energy with more slack out, you also have more rope out to absorb that energy. The net result, in practical situations, is a only a small increase in the vertical component of impact force, so small that you probably wouldn't notice it. I haven't done the math, but the small increase in impact force is a small price to pay for the reduction in horizontal swing.

Jay

Another point:

If you give the classic version of a soft catch* you can "absorb" a fair bit of energy through the friction in the rope around the bends over the top biner, belay biner, and belay device.

GO

*Do people know what a soft catch even means? It doesn't mean just feeding out slack before the rope goes tight. It means allowing some rope to slip through the belay device as it comes tight. Practice.


This is what I was talking about as the gradual feed of slack during the fall. It does need to be practiced esp. by new climbers that tend to get fingers all up in the friction and ouch, bad news and possibly a drop. It pretty much came naturally to me, no one ever taught me it so I didn't know what to call it but I have always done out of personal comfort mostly.

To the reply after the one i quote: I know what you are talking about when you are seeing less of a horizontal velocity with initial slack, but make sure your 'anchor' hand that the 'rope' is swinging from is fixed and you will also notice a 'jarring' from a change in direction. Climbing ropes, being dynamic, will transfer the direction of the force much smoother and eliminate this jarring, but with the smoother transfer in this direction of force, comes a smoother transfer in the direction of velocity. The fall won't hurt as much in your transfer to horizontal motion because of the rope dynamics, but it will hurt more in the acceleration retained by a smooth motion transfer...an equal payoff.

Think about the scenario of initial slack in the rope/system in this mindest. For the first few feet of the pendulum, you are in a freefall until the slack is picked up. Now that you have fallen you have gained vertical speed which will translate into higher horizontal speed when you hit the wall on your swing.
Or...after the slack has been taken up by a fall, picture yourself still on the rock, but only with your anchor point 'magically' moved above its original position by a few feet. You will be lower in relation to your anchor but will have more rope paid out to allow you to swing during the fall....yet another equal payoff.

Again, the best idea: forethought...have your belay practice soft catches with youand you practice too...out of courtesey. Haha.


curtis_g


Jan 18, 2006, 11:39 PM
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I shouldn't have said "even a bit of slack", that's an exaggeration; the crossover point where an improvement is pretty apparent seems to be where the dropping object falls a distance of half or more of the horizontal distance it was from the anchor before it comes tight on the string. I would expect on a dynamic rope where much of the energy is dissipated before being translated to horizontal motion, the difference would be even greater.
/

After reading some more I found this.
yes, a 'great amount' of slack will allow the stretch of the rope to perform just like the 'soft catch' method that I described. It wold just be the amazing amount of rope and its porportional amount of stretch that would be providing the 'soft' part. The only problem or more like the only possibly problematic factor would be the affordable amount of rope available on each spicific climb.


cintune


Jan 19, 2006, 1:37 PM
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It pretty much came naturally to me, no one ever taught me it so I didn't know what to call it but I have always done out of personal comfort mostly.

That's a good point. It's definitely something you have to have a feel for, whether or not you want to talk about forces and vectors and calculations. It's a matter of the belayer deliberately manipulating the rope to create an elastic moment between the initial fall and the swing. In the end, though, smacking into a wall is smacking into a wall. How it turns out is more up to the faller than the belayer, if it's up to anyone. Having a soft catch provides an extra second or two to get your reflexes primed for what's about to happen, while a tight pendulum might be over before you know it.


billl7


Jan 19, 2006, 3:27 PM
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Did get through some numbers last night but not ready to post. Was using the model equivalent to a steel cable, no soft catch, and the only slack is past the last piece. Either I have something wrong or it does not pay in practice to have additional slack for that unrealistic model. Hope to look at it more tonight.

Anyone else look at the numbers or have ideas about modeling the rope stretch and/or soft catch?


jt512


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None of the arguments so far, except mine, have taken into account that even though you produce more energy with more slack out, you also have more rope out to absorb that energy. The net result, in practical situations, is a only a small increase in the vertical component of impact force, so small that you probably wouldn't notice it. I haven't done the math, but the small increase in impact force is a small price to pay for the reduction in horizontal swing.

Jay
Right. Your point is relevant: there's more rope to stretch but also the fall factor goes up as slack is paid out. But I was thinking of starting with a simple system - maybe fall factor could be brought in later or maybe not if the pay-off for slack is clear enough (assuming it doesn't cause a collision with something else).

Bill

If you ignore the additonal rope in the system to absorb energy, then you've ignored a major factor, and might as well not do the problem. If you want to ignore something to simplify the problem, ignore the increase in the fall factor due to letting slack out, because it is minimal anyway.

Jay


billl7


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If you ignore the additonal rope in the system to absorb energy, then you've ignored a major factor, and might as well not do the problem. If you want to ignore something to simplify the problem, ignore the increase in the fall factor due to letting slack out, because it is minimal anyway.

You probably know, the concept of fall factor does include additional rope stretch. But accounting for this in a model is hard.

A conservative approach either takes into account or captures the things that help in terms of not smashing into the wall. Ignoring the increase in fall factor isn't conservative. Showing why it is negligible would be helpful.

What I mean by "capture" would be to have an outcome that says, the model shows X benefit in slack and things like rope stretch and soft catch will only make it better. By the way, for those promoting the soft catch, how much rope is typically let out in a "soft catch"?

Bill


daithi


Jan 19, 2006, 5:09 PM
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In reply to:
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Jay:

The problem I have with just giving slack is that the system isn’t analogous to the figure skater who increases her angular velocity while twirling by bringing her arms closer to her body. In other words, she’s in a situation in which angular momentum is conserved. Not so for the climber. Giving slack causes the climber to fall further down the cliff before hitting wall. As an example, it there’s a meter of rope out, which is held tight, then when the climber bangs into the wall, his body needs to dissipate the potential energy from falling vertically 1 meter. If slack is provided so that 2 meters of rope is out, his body needs to dissipate the energy from falling 2 meters. (Obvious simplification in ignoring such items as energy absorption by rope, etc. Just trying to make point that energy is being put into the system so that angular momentum is not conserved.)

I’m not saying one shouldn’t give out slack, but rather it’s a complicated problem, which most likely would call for different actions in different situations.

Cheers,

RobKelman.calm
16-Jan-06 21:24:00 MST (-6 UMT)

Pnedulum fall: give slack. It really is that simple, though I'm sure the collective internet community will have no trouble coming up with several pathological counter-examples.

Jay

No, it's not that simple--it's situational. Feed out slack and mgh increases.

Curt

But so does the amount of rope out to absorb the additional energy. The result is that letting rope out slightly increases the fall factor, but greatly decreases the horizontal velocity. It is pretty simple: you have a rope to limit the impact force with the rope, and a rock face to limit the impact force with the wall. If y'all put your heads together, I'm sure you can proudly name many exceptions, but in general, it should be clear that the rock wall presents the greater danger, and is the impact you want to take steps to minimize.

Jay

Right. Then, by that logic, the amount of rope you should feed out (to improve the situation) should be infinite.

Curt

Absolutely. As the rope length goes to infinity the horizontal component of velocity goes to zero (presuming you had an infinite space to fall in!) :)

In general I would agree though and say more slack would reduce the horizontal component of velocity.


daithi


Jan 19, 2006, 5:21 PM
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In reply to:
Right. Your point is relevant: there's more rope to stretch but also the fall factor goes up as slack is paid out. But I was thinking of starting with a simple system - maybe fall factor could be brought in later or maybe not if the pay-off for slack is clear enough (assuming it doesn't cause a collision with something else).

The closer the rope angle is to vertical when it is weighted in a pendulum fall the more kinetic energy it absorbs and the horizontal velocity is less. Therefore the energy absorption of the system is a crucial component.

Describe the fall you are trying to model and I will put some numbers on it.


billl7


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Right. Your point is relevant: there's more rope to stretch but also the fall factor goes up as slack is paid out. But I was thinking of starting with a simple system - maybe fall factor could be brought in later or maybe not if the pay-off for slack is clear enough (assuming it doesn't cause a collision with something else).

The closer the rope angle is to vertical when it is weighted in a pendulum fall the more kinetic energy it absorbs and the horizontal velocity is less. Therefore the energy absorption of the system is a crucial component.

Describe the fall you are trying to model and I will put some numbers on it.
Constants:
* climber is 10 feet into horizontal traverse from last piece of pro;
* the point at impact is vertically below the last piece of pro;
variable:
* the amount of slack on the climber's side of last piece of pro;
my model constraints:
* no rope stretch (albeit a significant omission);
* kinetic energy from vertical fall translates to KE in pendulum motion through unsophisticated trig properties at the point where the rope goes taught;
* from pendulum begin (rope taught) to pendulum end, total KE is increased by the vertical height change through the actual pendulum (not including any initial vertical fall)
So, the leader's horizontal KE is the component derived from the KE of the vertical drop plus the KE from the vertical change during the pendulum.


jt512


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If you ignore the additonal rope in the system to absorb energy, then you've ignored a major factor, and might as well not do the problem. If you want to ignore something to simplify the problem, ignore the increase in the fall factor due to letting slack out, because it is minimal anyway.

You probably know, the concept of fall factor does include additional rope stretch. But accounting for this in a model is hard.

A conservative approach either takes into account or captures the things that help in terms of not smashing into the wall. Ignoring the increase in fall factor isn't conservative. Showing why it is negligible would be helpful.

Bill

A model has to take into account all the salient factors. I don't see how you can ignore rope stretch.

Showing that the increase in fall factor resulting from slack is ignorable -- at least compared with assuming the rope doesn't stretch -- is simple. Assume you have 80 feet of rope out and the climber falls from 5 feet above top pro. With no slack, ff = 10/80 = .125. With 3 feet of slack, a realistic amount, ff = 13/83 = .157. In practice, the climber will not notice the difference beteen these fall factors, whereas the difference between assuming no stretch in the rope and using a realistic dynamic rope is the difference between life and death. So, if you've got to ignore something, ignore the increase in fall factor, rather than assume that the rope doesn't stretch.

Jay


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Jan 19, 2006, 6:12 PM
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Sort of like a fall on a zipline, even though it's static. There's the initial drop, which shortens the distance of the...zipping...part. Feeding slack on a dynamic rope lengthens the radius of the pendulum, but it shortens the arc traveled. Win-win situation.


billl7


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how much rope is typically let out in a "soft catch"?

Reason I ask is, if the amount of rope let out is as negligible as some say for the effect of purposefully added slack on fall factor then I will defend that a soft catch makes (editted for clarity here) little difference in the pendulum impact. Reasoning is that the soft catch lessons the jarring at the point where the rope goes taught but this effects only the force in-line with the rope and not the force associated with the climber's acceleration into the beginning of the pendulum.

Bill


billl7


Jan 19, 2006, 6:32 PM
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A model has to take into account all the salient factors. I don't see how you can ignore rope stretch.

This is only because you have prejudged that rope stretch is necessary and significant in terms of answering the question. "prejudged" is probably too strong of a word; maybe its just an issue of whether you have sufficiently justified that.

I'm ready to concede that fall factor does not change significantly. :)

Bill


jt512


Jan 19, 2006, 6:52 PM
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A model has to take into account all the salient factors. I don't see how you can ignore rope stretch.

This is only because you have prejudged that rope stretch is necessary and significant in terms of answering the question. "prejudged" is probably too strong of a word; maybe its just an issue of whether you have sufficiently justified that.

I'm ready to concede that fall factor does not change significantly. :)

Bill

Maybe I haven't read the posts in the thread clearly enough to understand the question. But it seems to me that the rope stretch changes everything, a lot. If it didn't, we would use static ropes.

Jay


billl7


Jan 19, 2006, 6:54 PM
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I need to go back on what I said about the soft catch. The soft catch is going to contribute in the same way that rope stretch will. It delays the transfer of KE from the vertical fall into the KE that the climber will have going into the pendulum (when the rope goes taught). By delaying the transfer of the force the angle between vertical and the taught rope is allowed to decrease a bit more and so less KE from the vertical fall is transferred into the pendulum swing.

Sorry.

All this still doesn't answer the question of which one dominates:

more slack -> overall greater energy (regardless of what absorbs it);
more slack -> less percentage of energy from the vertical fall is transfered to horizontal;


cintune


Jan 19, 2006, 6:56 PM
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the soft catch lessons the jarring at the point where the rope goes taught but this effects only the force in-line with the rope and not the force associated with the climber's acceleration into the beginning of the pendulum.Bill

- That's it, and the pendulum itself describes a shorter arc, therefore less acceleration before impact. It's all good.
If the rope did stretch enough, you'd leave an upward-pointing red smear on the rock when it lifted what was left of you, under reduced load. :)


billcoe_


Jan 19, 2006, 7:01 PM
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Maybe I haven't read the posts in the thread clearly enough to understand the question. But it seems to me that the rope stretch changes everything, a lot. If it didn't, we would use static ropes.

Jay

You could always try reading them J :wink: .

Sure it matters, point is, the farther you fall, the faster you go. (talking slow here). Even if it is sideways.

Then, if you happen to smack a wall at the end of you penji, the physics change even faster the other direction.

Better not to fall.
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cintune


Jan 19, 2006, 7:02 PM
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the soft catch lessons the jarring at the point where the rope goes taught but this effects only the force in-line with the rope and not the force associated with the climber's acceleration into the beginning of the pendulum.Bill

- That's it, plus the pendulum itself describes a shorter arc, therefore less overall acceleration before impact. It's all good.
If the swing was long enough and the rope did stretch enough, you'd leave a nice upward-pointing red smear on the rock. :)


billl7


Jan 19, 2006, 7:19 PM
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Wear a helmet, don't close your eyes, keep your head over your heels, hold on for the ride, and don't poop yourself...or cry, and at least you'll have your dignity.

... just thought it was worthy of repeating ...


curtis_g


Jan 19, 2006, 8:11 PM
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that's crazy that you did put numbers/a model to it in an experiment. Just like I explained, slack in the system after the the last piece of pro wouldn't help because while you start the swing farther along in the fall, you are also falling farther.

the dynamic rope and a dynamic belay catch (soft catch) would make the difference. the original person that suggested slack in the system revised his suggestion to say something like "i meant lots of slack" and I already commented on that practicality and how the rope would onyl help then in providing the "soft catch" instead of the experienced belay.

like you said, it really comes down to a) an experienced belay but more inportantly b) knowing how you are going to fall and keeping your head straight during the fall enough to control yourself

to model a soft catch i would say to have the rope run from the climber over a pulley and the other end of the rope attached to a weight maybe 1/4 the weight of your climber sitting on a ledge so that the 1/4 weight will be lifted off of it's ledge maybe halfway through the climber's fall.
or i would just use some shock cord like from the inside of a tent pole.


jt512


Jan 19, 2006, 8:14 PM
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Maybe I haven't read the posts in the thread clearly enough to understand the question. But it seems to me that the rope stretch changes everything, a lot. If it didn't, we would use static ropes.

Jay

You could always try reading them J :wink: .

Sure it matters, point is, the farther you fall, the faster you go. (talking slow here). Even if it is sideways.

Bill, the whole point is that even though you build up more speed/energy the further you fall, YOU HAVE A FUCKING DYNAMIC ROPE THAT ABSORBS MOST OF THE ADDITIONAL ENERGY, and thus negating it. Therefore, how can you dream of ignoring the rope? If you have to ignore something, ignore the additional energy, because the rope takes care of most of that.

Jay


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Jan 19, 2006, 8:27 PM
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Maybe I haven't read the posts in the thread clearly enough to understand the question. But it seems to me that the rope stretch changes everything, a lot. If it didn't, we would use static ropes.

Jay

You could always try reading them J :wink: .

Sure it matters, point is, the farther you fall, the faster you go. (talking slow here). Even if it is sideways.

Bill, the whole point is that even though you build up more speed/energy the further you fall, YOU HAVE A f---ing DYNAMIC ROPE THAT ABSORBS MOST OF THE ADDITIONAL ENERGY, and thus negating it. Therefore, how can you dream of ignoring the rope? If you have to ignore something, ignore the additional energy, because the rope takes care of most of that.

Jay

The rope absorbs some additional energy. The real problem is to quantify if this is signficant or not.

rob.calm


curtis_g


Jan 19, 2006, 8:28 PM
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that's crazy that you did put numbers/a model to it in an experiment. Just like I explained, slack in the system after the the last piece of pro wouldn't help because while you start the swing farther along in the fall, you are also falling farther.

the dynamic rope and a dynamic belay catch (soft catch) would make the difference. the original person that suggested slack in the system revised his suggestion to say something like "i meant lots of slack" and I already commented on that practicality and how the rope would onyl help then in providing the "soft catch" instead of the experienced belay.

like you said, it really comes down to a) an experienced belay but more inportantly b) knowing how you are going to fall and keeping your head straight during the fall enough to control yourself

to model a soft catch i would say to have the rope run from the climber over a pulley and the other end of the rope attached to a weight maybe 1/4 the weight of your climber sitting on a ledge so that the 1/4 weight will be lifted off of it's ledge maybe halfway through the climber's fall.
or i would just use some shock cord like from the inside of a tent pole.

...but there was some ongoing discussion started by someone who probably sounded to many like they were correct in their reasoning while reall they weren't. the comment was made that a soft catch, either by rope or the belay, will simply delay the transfer of Kinetic Energy of the vertical fall into the KE of th swing. First, the energy of the fall would be porportionate to the height of the fall, so if the climber is let fall a greater distance vertically by means of a soft catch then wouldn't less potential energy remain to translate into horizontal KE? Fact is, as more slack is paid out during the fall, the lesser the angle (vertex on the last piece of pro) of the rope. Now consider vectors and it should be clear to see that, with this lessened angle during the fall, more of the force of the fall will be felt vertically (how we are used to) and less will be translated into horizontal KE.


jt512


Jan 19, 2006, 8:33 PM
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Maybe I haven't read the posts in the thread clearly enough to understand the question. But it seems to me that the rope stretch changes everything, a lot. If it didn't, we would use static ropes.

Jay

You could always try reading them J :wink: .

Sure it matters, point is, the farther you fall, the faster you go. (talking slow here). Even if it is sideways.

Bill, the whole point is that even though you build up more speed/energy the further you fall, YOU HAVE A f---ing DYNAMIC ROPE THAT ABSORBS MOST OF THE ADDITIONAL ENERGY, and thus negating it. Therefore, how can you dream of ignoring the rope? If you have to ignore something, ignore the additional energy, because the rope takes care of most of that.

Jay

The rope absorbs some additional energy. The real problem is to quantify if this is signficant or not.

rob.calm

You don't need to quantify it at all. You need only take a 10-foot fall onto a static rope.

Jay


jt512


Jan 19, 2006, 8:36 PM
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that's crazy that you did put numbers/a model to it in an experiment. Just like I explained, slack in the system after the the last piece of pro wouldn't help because while you start the swing farther along in the fall, you are also falling farther.

*broken record* You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases. You have more rope out to absorb the additional energy. The fall-factor hardly increases.

Jay


billl7


Jan 19, 2006, 8:38 PM
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that's crazy that you did put numbers/a model to it in an experiment.
Just to be clear, there was no experiment on my end. Just trying to work it out with math on paper. But I'm starting to give more and more credit to using a weight and a string - that you and others have talked about - and listening to how hard it smacks the wall. :-)


billl7


Jan 19, 2006, 8:46 PM
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You don't need to quantify it at all. You need only take a 10-foot fall onto a static rope.
Jay, you may be correct about everything you've said but your powers of persuasion have room for improvement. Remember, a vertical fall as you suggest here is not the same as a pendulum because in a pendulum the rope simply cannot absorb all the energy. And mimicing a broken record has zero merit - indeed, negative merit.

Bill
Editted to get the quote right.


cchildre


Jan 19, 2006, 8:59 PM
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My single point. The angle of the pendlum can be decreased by paying out some extra slack. So if a climber falls on a tensioned rope at the same height of his last piece of pro and is ten feet out. His starting angle is 90 degrees and the fall would immediately pull him back towards his last pro. If he has say 5 feet of slack then he falls down 3-5 feet before he starts to load the rope and start the swing thus the starting angle would be more like 50 or 60 degrees. Their still swinging just not as violently and perhaps in a more controlled manner. Get some physics guys to explain it...but then we would probably still be scratching our heads.


curtis_g


Jan 19, 2006, 9:21 PM
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by cchildre My single point. The angle of the pendlum can be decreased by paying out some extra slack. So if a climber falls on a tensioned rope at the same height of his last piece of pro and is ten feet out. His starting angle is 90 degrees and the fall would immediately pull him back towards his last pro. If he has say 5 feet of slack then he falls down 3-5 feet before he starts to load the rope and start the swing thus the starting angle would be more like 50 or 60 degrees. Their still swinging just not as violently and perhaps in a more controlled manner. Get some physics guys to explain it...but then we would probably still be scratching our heads.

my point, however hidden it was, was that while this angle between the sections of rope on either side of the last piece of pro will be reduced, with slack in the system (but no soft catch), the advantage of the decreased angle will be negated by the increase of energy produced by that extra five feet of slack that will be 'used up' entirely in freefall. so...the speed of the swing would only be reduced by the release of slack during the fall. I think I worded this explination best in my reply one earlier.

even if you cant exactly undertand my explination, try my 'weight on a string' example in my first post so that you can see what works...initial slack doesn't. visually measure the speed by the height of the pendulum after it has past where the climber would normally go smack.

IN CONCLUSION...
- we all use dynamic ropes so end that argument already
- initial slack makes negligable (in theory, if not zero) difference
- practice your soft catches
- keep your head straight during the fall and don't poop yourself
- the outcome is most essentially a result of the climber's actions during the fall


curtis_g


Jan 19, 2006, 9:23 PM
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by cchildre My single point. The angle of the pendlum can be decreased by paying out some extra slack. So if a climber falls on a tensioned rope at the same height of his last piece of pro and is ten feet out. His starting angle is 90 degrees and the fall would immediately pull him back towards his last pro. If he has say 5 feet of slack then he falls down 3-5 feet before he starts to load the rope and start the swing thus the starting angle would be more like 50 or 60 degrees. Their still swinging just not as violently and perhaps in a more controlled manner. Get some physics guys to explain it...but then we would probably still be scratching our heads.

my point, however hidden it was, was that while this angle between the sections of rope on either side of the last piece of pro will be reduced, with slack in the system (but no soft catch), the advantage of the decreased angle will be negated by the increase of energy produced by that extra five feet of slack that will be 'used up' entirely in freefall. so...the speed of the swing would only be reduced by the release of slack during the fall. I think I worded this explination best in my reply one earlier.

even if you cant exactly undertand my explination, try my 'weight on a string' example in my first post so that you can see what works...initial slack doesn't. visually measure the speed by the height of the pendulum after it has past where the climber would normally go smack.

IN CONCLUSION...
- we all use dynamic ropes so end that argument already
- initial slack makes negligable (in theory, if not zero) difference
- practice your soft catches
- a WHOLE LOT of rope will act like a soft catch
- keep your head straight during the fall and don't poop yourself
- the outcome is most essentially a result of the climber's actions during the fall


jt512


Jan 19, 2006, 9:44 PM
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You don't need to quantify it at all. You need only take a 10-foot fall onto a static rope.
Jay, you may be correct about everything you've said but your powers of persuasion have room for improvement. Remember, a vertical fall as you suggest here is not the same as a pendulum because in a pendulum the rope simply cannot absorb all the energy. And mimicing a broken record has zero merit - indeed, negative merit.

Bill
Editted to get the quote right.

I'm not trying to pursuade anyone. Do what you want with your model, just don't use it to belay me, if your results are based on a static rope.

Jay


jt512


Jan 19, 2006, 9:47 PM
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- initial slack makes negligable (in theory, if not zero) difference

If it makes no difference ito you in theory, you need to find another theory.

Jay


billl7


Jan 19, 2006, 10:32 PM
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You don't need to quantify it at all. You need only take a 10-foot fall onto a static rope.
Jay, you may be correct about everything you've said but your powers of persuasion have room for improvement. Remember, a vertical fall as you suggest here is not the same as a pendulum because in a pendulum the rope simply cannot absorb all the energy. And mimicing a broken record has zero merit - indeed, negative merit.

Bill
Editted to get the quote right.

I'm not trying to pursuade anyone. Do what you want with your model, just don't use it to belay me, if your results are based on a static rope.

Jay
My mistake. I thought you were trying to convince of us something relevant.

Bill


cchildre


Jan 19, 2006, 10:46 PM
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I still question some of the conclusions made for not leaving slack. Only because my basic logic says differently, and I lack the working knowledge to challenge any of it. So, unless I go study up, do the math, and conclude otherwise, I shall stand down. This all comes back to the individuals choice. I belay everyone according to their wishes. You want it tight, loose, hell you want a hip belay....I am the slave!


billl7


Jan 19, 2006, 11:09 PM
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I still question some of the conclusions made for not leaving slack. Only because my basic logic says differently, ....
Again, to be clear, I'm not arguing that one should or shouldn't leave slack; at least not yet. Just trying to find something stronger than has been discussed. Feel free to come back if for nothing else than to calibrate me. I've actually learned quite a lot from others here, including Jay.

Bill


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Jan 19, 2006, 11:32 PM
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- initial slack makes negligable (in theory, if not zero) difference

If it makes no difference ito you in theory, you need to find another theory.

Jay

Dear Jay, I will restate...with initial slack in the system (your rope), you will only increase your vertical fall velocity and THEN translate it into the SAME AMOUNT of horizontal velocity once the swing starts instead of doing it all over the same radius. It would be like falling in the path of a circle or the path of a 'J' a soft catch would prouce a parabolic fall path. Initial slack does not decrease the amount of total potential energy that will all eventually end up as your horizontal slam. A soft catch is your best bet, not giving out more rope to fall farther. But I wouldn't say keep an uber tight belay, that wouldn't help the climber catch his bearings before he starts to scrape across the rock...but that's headsense, not physics.

again, my conclusion about slack on a traverse...if I was the belay I would give just enough to make sure the first very few feet weren't awkward so that the climber isn't being dragged across the rock before he knows he's falling.


whoa


Jan 20, 2006, 12:33 AM
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Here's a try. Let me know what you think.

If no slack is let out for a rigid rope L meters long, the potential energy is entirely turned into horizontal kinetic energy at the wall:

e_no-slack = mGL

So, suppose we let out enough slack to generate a free-fall of h meters before finishing with a partial pendulum arc to the wall. When the rope is first taut, the velocity that is in the direction of possible motion (tangent to the arc, perpindicular to the rope) is preserved. But there is no way that the component of motion parallel to the rope can be translated into motion perpindicular to the rope. So maybe the rope absorbs it, maybe the climber absorbs it, maybe the earth gets accelerated ... whatever!

(crude sketch added in edit)
http://groups.msn.com/...=4675556766064520295

The velocity downwards (when the rope is first taut) is:

v = sqrt(2Gh)

The component of v tangent to the pendulum arc would be v * sin(angle), where "angle" is the angle of the rope against the wall.

v_tangent = [sqrt(2Gh)] * [L/(sqrt(h^2 + L^2)]

The energy due to v_tangent is preserved and becomes horizontal energy at the wall:

e_tangent = 1/2 * m * v_tangent^2 = mGh * [L^2 / (h^2 + L^2)] =
= mGL * Lh/(h^2 + L^2) = mGL / (h/L + L/h)

Let R be h/L --- the ratio of the slack-fall to the initial length of the rope. Then,

e_tangent = e_no-slack * (1/(R + 1/R))

but there is also additional horizontal energy due to the partial pendulum, equal to the potential energy of the remaining vertical drop, or:

e_pendulum = mG(sqrt(h^2 + L^2) - h) = mgL * (sqrt(1 +h^2/L^2) - h/L)
= e_no-slack * [sqrt(1 + R^2) - R]

Adding:

e = mGL * [ 1/(R+1/R) + sqrt(1 + (1/R)^2) - R ]

See the graph below. Looks like letting out rope right at the start is a win if you can let out enough rope such that R = 1. That would be sqrt(2) - 1, or about 41% of the (run-out) rope's length.

http://groups.msn.com/...=4675556743304009216

But then I probably goofed somewhere.


whoa


Jan 20, 2006, 2:57 AM
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Maybe, but I think you can accommodate the only important effect of the rope's springiness (namely, the change in the rope's final length) by including the added length as "slack" in the model. No particular trajectory after tautness was assumed--all we need are conservation of energy assumptions--so it doesn't really matter what the precise trajectory is.

As for the assumption that a tugging on a rope doesn't alter the climber's velocity perpindicular to it, I'm still pretty comfortable with that one. :)


daithi


Jan 20, 2006, 3:07 AM
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Edit: I have edited the numbers and figures in this post as the original contained a rather large (and embarrassingly basic) error! :oops: Like a certain South Korean human stem cell researcher my reputation is forever tarnished! Thankfully this has nothing to do with my real research! :)

In reply to:
v_tangent = [sqrt(2Gh)] * [L/(sqrt(h^2 + L^2)]

I think this is wrong or else I am not visualising your definition of L, h and angle correct (also likely!).

Edit: I had misunderstood your definitions. I see you redid yours using the same definition that I used for R.

I did some numbers too. Here is the setup that I am attempting to model.

http://www.rockclimbing.com/...p.cgi?Detailed=68012

R is the length of slack rope that has been normalised wrt the horizontal distance from the climber to his last runner. The minimum value is unity obviously (no slack - pure pendulum). h is the vertical distance the climber falls before the rope gets taut and the pendulum into the wall begins and theta is the angle between the rope and the vertical fall.

I used a similar method to whoa I think. A combination of the conservation of energy and the equations of motion of a pendulum to calculate the impact velocity at the wall (which was normalised wrt to the impact velocity of a pure pendulum swing 4.429 m/s).

Edit: Similarly, energy has been normalised.

The huge assumption of this is, at the moment the rope gets taut at the start of the pendulum the radial component (in my polar coordinate system) of linear momentum is instantly absorbed by the dynamic rope (this assumes the rope performs a lot better than it does in reality). In reality this will also be a function of time and would need to be incorporated into the model. I have no data on the dynamic mechanical response of climbing ropes so nothing on this is included. This assumption becomes more reasonable as the fall factor goes to zero (lots and lots of rope and small falls). Here is the result.

http://www.rockclimbing.com/...p.cgi?Detailed=68011

Some comments:

1. Initial pay out of slack does not reduce the impact velocity at the wall (compared to a pure pendulum) in this model, it actually increases it. The slack needs to be 1.2 times greater than the horizontal distance before any favourable reduction is achieved. Those who conjectured that the initial increase of kinetic energy due to the longer fall results in a higher impact velocity seem to be on to something. This is not what I expected when I first thought about it.

Edit: The actual increase at the worst possible case, which is a 7% increase of slack, is only 2% in energy or approximately 1% in impact velocity at the wall. This is not significant enough to warrant ever refusing to give slack to a falling climber, since in a real system slack will always be favourable when we take into account rope stretch that takes place over a finite time, as opposed to instantaneously! At 20% slack and above the impact force dramatically reduces with increasing slack.

2. However, as further and further slack is paid out, the impact velocity does get smaller. The rope gets a chance to absorb more of the linear momentum of the falling body.

3. The limits of the model are as R -> 1 (no slack) impact velocity is that of a pure pendulum (4.429 m/s). As R -> OO the impact velocity goes to zero (becomes a vertical fall with the rope absorbing everything). Anyone else doing a model make sure it obeys those physical limits.

4. The highest impact velocity is at a 7% let out of slack, which corresponds to an angle of 60°, with a 1% increase in impact velocity (2% in energy).

5. The rope in this model performs better than it could ever do in reality. It absorbs all the linear momentum in the direction of rope instantaneously before the pendulum trajectory.

6. Although this is a very simple model at least it gives us some physics to discuss as opposed to some pure conjecture and mis-applied physical principles, which the majority of this thread has been thus far!


The final equation plotted is

V = sqrt(2gRcosq)sin q + sqrt(2gR (1-cosq))

Edit:
V = sqrt(2gRcosq)sin^2q + 2gR (1-cosq))


daithi


Jan 20, 2006, 3:25 AM
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But so does the amount of rope out to absorb the additional energy.

The point is only the component of linear momentum that is absorbed by the rope is the component that is parallel to the rope (it would be the dot product of the momentum vector and the elsatic deformation vector of the rope). The rope has no mechanical means (or almost none) to absorb energy in any direction other than along it.


whoa


Jan 20, 2006, 3:42 AM
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[I see that the delcross post I was replying to has been deleted, so I've deleted my response.]

Daithi, nice pics!!! As for my trig, I've added a pic to make it clearer. (Though I am bowing my head in shame to post it near yours.)


curtis_g


Jan 20, 2006, 4:09 AM
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First, nicely done daithi. And a convincing explination to the practical conclusion.

In reply to:
In reply to:
But so does the amount of rope out to absorb the additional energy.

The point is only the component of linear momentum that is absorbed by the rope is the component that is parallel to the rope (it would be the dot product of the momentum vector and the vector that describes the rope direction). The rope has no mechanical means (or almost none) to absorb energy in any direction other than along it.

daithi is correct once again. I guess I didn't explain myself fully, or maybe I wasn't read, but (and this is what I believe daithi is getting at), is that the rope does nothing to weaken a force or absorb some force or absorb some velocity. What the dynamics of the rope does is decrease the change in acceleration more spicifically (slang and scientifically) known as jerk. The dynamic rope only elongates the time over which the force is applied and lessens the impulse of the preassure on you from the force.

All the energy is still there! It can't just go away or 'be absorbed' like so many people have claimed. That's day one stuff. Actually its the law of conservation of evergy. IT'S a LAW...you all should go to jail...or at least pay me a hefty fine.


colkurtz


Jan 20, 2006, 5:21 AM
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All the energy is still there! It can't just go away or 'be absorbed' like so many people have claimed. That's day one stuff. Actually its the law of conservation of energy. IT'S a LAW...you all should go to jail...or at least pay me a hefty fine.

you couldn't be more wrong. energy will escape the system.

but

this problem is fascinating. my intuition is that the rope should not absorb the energy instantaneously. and right now i think this is a big factor. as are the properties of the rope.

i would rather see some empirical data if someone is motivated enough.

i am more concerned with the ability to use my feet to control the swing. adding a layer of complexity


billl7


Jan 20, 2006, 7:16 AM
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In reply to:
In reply to:
All the energy is still there! It can't just go away or 'be absorbed' like so many people have claimed. That's day one stuff. Actually its the law of conservation of energy. IT'S a LAW...you all should go to jail...or at least pay me a hefty fine.
you couldn't be more wrong. energy will escape the system.
Right. It starts to leak out as soon as the rope starts to stretch. Might be safe to say that any energy sent through the rope when it goes taught is lost ("instantly" as daithi said) as it seems the only way to reintroduce it to the climber's tangential velocity is if the rope significantly springs back well before the climber hits the wall.

Paying out slack to the tune of 250% of the traverse just to break even seems dicey; understanding the model is limited, maybe in reality not so much is needed. However, I do appreciate curtis_g's early remark about having time to get yourself oriented.

Very nice efforts by whoa and daithi. I'm simply outdone here: I degenerated into chasing my tail when trying to find the angle based on dynamic stretch and the dynamic stretch needed the force parallel to the rope which depended on that very same angle; obviously, I'm not looking at it properly.

Hmm, anyone work for one of those car crash test organizations? We could "borrow" a crash dummy with internal accelerometers and probably return it maybe only a little worse for the wear. I'm sure we've got enough of the other needed gear between us. ;-) (Good idea colkurtz.)

Thanks again for sticking with this!

Bill


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Jan 20, 2006, 7:50 AM
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for some reason i find it hard to accept when you say that the rope absorbs energy. it could gain a certain potential engery stored in its stretch and its stretch could slightly warm up the rope as energy will always escape into dissepated heat (negligable), and in a direct vertical fall many things (rope, belay, anything in the system including the two harnesses) are moved and tensioned as well as the climber springing back up as he bounces on the rope.

ok so i read on and you comment that
In reply to:
as it seems the only way to reintroduce it to the climber's tangential velocity is if the rope significantly springs back well before the climber hits the wall.
I would readily believe that this does happen. as the climber nears a total horizontal vector of velocity, wouldn't the rope regain some of it's pull and toss the climber a bit harder...or possibly the climber would oscillate during his swing that would loot something like the function of y = x sinx (with any number of phase shifts or stretches determined by extraneous factors of the fall) as the climber falls from x = 2 pi in the negative direction towards x=0. just an example/thought.


billl7


Jan 20, 2006, 2:32 PM
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In reply to:
for some reason i find it hard to accept when you say that the rope absorbs energy. it could gain a certain potential engery stored in its stretch and its stretch could slightly warm up the rope as energy will always escape into dissepated heat (negligable), and in a direct vertical fall many things (rope, belay, anything in the system including the two harnesses) are moved and tensioned as well as the climber springing back up as he bounces on the rope.
Recall too how much a biner heats up during a rap. Probably similar thing with at least the rope/biner where it hangs from the top piece of pro.

In reply to:
ok so i read on and you comment that
In reply to:
as it seems the only way to reintroduce it to the climber's tangential velocity is if the rope significantly springs back well before the climber hits the wall.
I would readily believe that this does happen. as the climber nears a total horizontal vector of velocity, wouldn't the rope regain some of it's pull and toss the climber a bit harder...or possibly the climber would oscillate during his swing that would loot something like the function of y = x sinx (with any number of phase shifts or stretches determined by extraneous factors of the fall) as the climber falls from x = 2 pi in the negative direction towards x=0. just an example/thought.
I agree that there probably are some oscillations and so some energy returns to the leader's horizontal energy.

However, the most efficient way for that shrink of the rope to speed up the arcing leader is if the shrink(s) occur fairly far away from impact where the angles are more favorable for that kind of energy transfer (i.e., if say the first shrink instantly follows the first tension period). As the leader gets closer to impact, more and more of the shrink action only lifts the leader up instead of propelling her towards the wall.

Practically speaking, a shrink just isn't going to happen under conditions as favorable as the last tensioning for transferring energy back to horizontal movement because some of the pendulum arc will have passed and so the angles aren't as favorable.

My guess (don't know) is that the delay in time for the oscillation to reverse plus the energy loss due to friction keep the initial shrink episode relatively weak and relatively ineffective. Throw in a soft catch and there would be even less and weaker oscillations as well (where's Jay! he's probably going to miss another opportunity to crow!! :) ).

Bill


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Jan 20, 2006, 3:33 PM
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Throw in a soft catch and there would be even less and weaker oscillations as well (where's Jay! he's probably going to miss another opportunity to crow!! :) ).

Bill

Actually, I introduced the soft catch way back on page 3. Unfortunately, curtis_g agreed with me, causing me to lose all credibility. :)

Nevertheless, I'm quite convinced that the dampening effect of the soft catch is quite significant. Unfortunately, I haven't studied enough physics to plot out any more than the simple models that have already been done here online (much more gracefully than the scratches I'd worked out on my own, I must say!) But while I *think* I do understand the more complex principles that come into play with the soft catch, I don't know how to plot them out, and of course I wouldn't have the means to test my theories either.

It *is* an interesting problem though. I'd like to see a good physical modelling of it. Anyone know an under-employed physicist climber with some time on his/her hands?

GO


daithi


Jan 20, 2006, 4:02 PM
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But while I *think* I do understand the more complex principles that come into play with the soft catch, I don't know how to plot them out, and of course I wouldn't have the means to test my theories either.

Describe how you think it works in the form of a differential equation, or failing that even the principle and I will do the maths and the numerical modeling part (at some stage!).


billl7


Jan 20, 2006, 4:27 PM
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In reply to:
In reply to:
Throw in a soft catch and there would be even less and weaker oscillations as well (where's Jay! he's probably going to miss another opportunity to crow!! :) ).
Actually, I introduced the soft catch way back on page 3. Unfortunately, curtis_g agreed with me, causing me to lose all credibility. :)
My bad. :)

Which do you think typically causes more pendulum elongation: belay slippage or plain rope stretch? That probably needs some qualification but I'm too lazy right now.

It's tempting to make an effort to take daithi up on the offer to crunch more numbers.

Bill


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In reply to:
In reply to:
But while I *think* I do understand the more complex principles that come into play with the soft catch, I don't know how to plot them out, and of course I wouldn't have the means to test my theories either.

Describe how you think it works in the form of a differential equation, or failing that even the principle and I will do the maths and the numerical modeling part (at some stage!).

I'm just running out to lunch now, and when I get back I need to get some work done.

I'll write back as soon as I can, sorry! :(

GO


pastprime


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It comes down to this:
In a fall into a corner from a piece horizontal to the climbers position with no slack in the rope, virtually none of the energy is transferred to the rope or absorbed by it; almost all of the energy is absorbed by the climber's body smacking into the wall.

With a small amount of slack out, the climber falls further, generating more energy, and the faller's motion is transfered into swinging motion while still quite a bit sideways from the last piece, so the pull is not parallel to the rope, and the increased energy is still mostly absorbed by the climbers body smacking the wall.

With a whole lot of slack out at the time of the fall, even more energy is generated that is going to need to be absorbed at some time, but by the time the faller hits the end of the rope, the rope is much closer to being lined up with the direction the faller is moving, so much more of the energy is absorbed by the rope before or as translation to horizontal movement occurs.

In the case of little slack, less energy is generated, but it is all absorbed by the climber at the moment of impact. In the case of lots of slack, much more energy is generated, but much more of the total energy is absorbed by the rope. At it's most extreme, in an ideal situation with lots of rope and nothing below to hit, it is like the difference between hitting a solid wall in your car at 30 mph or braking hard from 90 mph.
In real situations, I expect its more like a question of driving into a wall at 30 mph or going into a grove of trees at 60.


dirtineye


Jan 20, 2006, 6:03 PM
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I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ?


cause from the way you are writing it sounds like you have not done it very much.


curtis_g


Jan 20, 2006, 6:12 PM
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In reply to:
With a small amount of slack out, the climber falls further, generating more energy, and the faller's motion is transfered into swinging motion while still quite a bit sideways from the last piece, so the pull is not parallel to the rope, and the increased energy is still mostly absorbed by the climbers body smacking the wall.

With a whole lot of slack out at the time of the fall, even more energy is generated that is going to need to be absorbed at some time, but by the time the faller hits the end of the rope, the rope is much closer to being lined up with the direction the faller is moving, so much more of the energy is absorbed by the rope before or as translation to horizontal movement occurs.

Yes, that was the situation founded by daithi with his explination and I believe the line was drawn at something like a slack payout 250% larger than the horizontal distance of the swing to break even and cause the climber to hit with less speed. That's one hell of a free fall and one I'm not interested in just to 'break even' in terms of final horizontal velocity.

My comment that someone appreciated was that I would enjoy only enough slack so that I can realize that I have fallen before I'm being thrown sideways followed by a soft catch with a gradual slack payout of 5 to 10 ft, and, while more complicated models and introducing a higher level of variables shouldn't be discontinued, I would probably still ask for the scenario I just outlined. A soft catch would do wonders, but the climber will ultimately make the difference.

"I would enjoy only enough slack so that I can realize that I have fallen before I'm being thrown sideways followed by a soft catch with a total gradual slack payout of 5 to 10 ft."

I am starting a physics course on Tuesday with one of my favorite professors who is a big big climber, rock and ice. Denali and a bunch of others. The entire semester is an independant study project presented at the end of the year. Mine will definitely be on tests of climbing gear, dynamics of a fall, friction, something like that, so I'm looking ofrward to making my presentation readable on RC.com and owning my first gold trophy, haha.


billl7


Jan 20, 2006, 6:23 PM
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I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ? cause from the way you are writing it sounds like you have not done it very much.
I don't know how many. Why wait for a response? Tell us what you think from experience.

Since the approach to mathematical modeling generally starts out fairly conservative, because most of us try the easiest things first, the approach could be confused with lack of experience. However, in my case you can accurately chalk it up to inexperience if you like. :)

Bill


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Jan 20, 2006, 7:05 PM
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In reply to:
In reply to:
In reply to:
- initial slack makes negligable (in theory, if not zero) difference

If it makes no difference ito you in theory, you need to find another theory.

Jay

Dear Jay, I will restate...with initial slack in the system (your rope), you will only increase your vertical fall velocity and THEN translate it into the SAME AMOUNT of horizontal velocity


By looking at the extreme case suggested by Curt, an infinitie amount of slack, it can be seen that you are wrong. The horizontal velocity would be 0 (and, incidentally, the fall factor would only be 1). So, assuming, as we should, until someone proves otherwise (using real equations), that the relationship between slack and horizontal velocity is monotonic, then the more slack in the rope, the less the horizontal velocity.

Edit: Actually, in daithi's model the realtionship is not monotonic.

Jay


dirtineye


Jan 20, 2006, 7:08 PM
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In reply to:
I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ? cause from the way you are writing it sounds like you have not done it very much.
I don't know how many. Why wait for a response? Tell us what you think from experience.

Since the approach to mathematical modeling generally starts out fairly conservative, because most of us try the easiest things first, the approach could be confused with lack of experience. However, in my case you can accurately chalk it up to inexperience if you like. :)

Bill

I hate to say this, and I have a degree in math (lots of modeling with PDE) with minor in physics plus grad school math (all behind me now and obviously fading LOL), but I don't give a crap about a mathematical model for this pendulum falling stuff, because one, I know the general principle that as long as the wall is overhanging then you are actually slowing down after you swing past vertical, and two, from actual pendulum falls I have taken, I know that if you do it right you can hit the wall with both feet , with your weight centered between your feet, and absorb the impact with your legs and suffer no ill consequences, period.

I don't blame you for wanting to model, and it woud be interesting, but in the end, when you take the fall two things will matter:

Are you in a good falling position and have you got a plan for meeting the wall?

Keep in mind that you are not a point mass in a theoretical pen and paper model. You can react. You can take action for better or for worse. Pity the poor inanimate dumb as a rock point mass, for he is doomed to smack the wall in a simple collision at whatever velocity the math dictates.

You are not an unyeilding point mass, you are a complicated organism with excellent built in damping devices and intelligence, and if you will only use them correctly, you will come out unscathed.

So if you panic when you fall, you're screwed. If you practice falling and react corectly and quickly, you are not screwed.

IF you want to know more about what I think on this subject, look at the first two pages of this thread. All the examples I gave of how to take these falls were based on actually taking such falls myself. I'm a firm believer in the Arno School of Falling Practice and using your head to judge the falling consequences BEFORE you are in the fall.

BTW, I don't mean to sound like a butthead, I just feel like crap today, LOL


billl7


Jan 20, 2006, 7:31 PM
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I don't blame you for wanting to model, and it woud be interesting, but in the end, when you take the fall two things will matter: Are you in a good falling position and have you got a plan for meeting the wall?

But modeling looks so attractive to someone new to leading, who hasn't yet fallen on lead, who generally climbs on routes that aren't very close to vertical such that a pendulum would probably involve a lot of contact with the rock along the way before the possible impact. I guess I'm just trying to live vicariously through math and experience of others.

Peace, Bill


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Edit: the following comments are no longer relevant. They referred to an earlier graph, not the one now pictured above.

I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

Note that for pendulum falls originating from a short horizontal distance, you will always be on the "downside" of the curve. If you fall from say 5 feet straight out horizontally from your highest pro, you will almost certainly have at least 7.8 inches of slack in the rope (13% of 5 feet), if there is much total rope in the system at all, and therefore any additional slack in the rope would reduce the horizontal velocity, given the above model.

Jay


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Jan 20, 2006, 7:56 PM
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http://www.popupbooks.net/coverW/W99.jpg


Partner cracklover


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In reply to:
In reply to:
In reply to:
Throw in a soft catch and there would be even less and weaker oscillations as well (where's Jay! he's probably going to miss another opportunity to crow!! :) ).
Actually, I introduced the soft catch way back on page 3. Unfortunately, curtis_g agreed with me, causing me to lose all credibility. :)
My bad. :)

Which do you think typically causes more pendulum elongation: belay slippage or plain rope stretch? That probably needs some qualification but I'm too lazy right now.

No, it's a good question, and doesn't require qualification. I think that the answer of which is more important depends on how much rope is out and the fall factor. For example, in a long, low fall-factor fall, the rope might stretch a good deal relative to the "diameter" of the pedulum arc, while the belayer would let out almost no slack (again, relatively speaking). So in this case, the force absorbed by the rope is much more important. Alternatively, in a short, high fall-factor fall, there is very little force that the rope can absorb, and the belayer is going to let rope slip whether they like it or not - probably a significant amount (relative to the amount of rope involved in the fall). In this case, the force absorbe by the soft catch may be relatively more important. Sorry if I'm just raising more questions rather than answers!

But here's the main point I wanted to make: Clearly rope slippage and rope stretch occupy the same category. You've attempted to account for the role of this category in absorbing some of the added kinetic energy that additional slack creates. Let's assuming you've done this correctly. So if you wanted to take into effect a soft catch, you'd just increase this effect. But I believe there is an addition issue that needs to be taken into effect!

A classical pendulum operates in the way it does only because the net energy in and out is zero. I believe that the energy absorbed by rope, both through stretch and through friction over top biner, belay biner, and around belay device, will change the entire system.

Take a simple spring pedulum. Drop a weight attached to a spring straight down, and it will drop until the maximum tension builds in the spring, at which point the weight will stop, and then move up again until it reaches the top position again. It will oscilate up and down. This is the same basic principle as the pendulum. Now imagine that you coat the spring in peanut butter. The weight drops to the bottom, but never makes it all the way back up again. It may barely bounce at all. This is the system we're really looking at. What is the speed of the falling climber when they hit the wall? Well, what is the speed of the weight attached to the peanut butter coated spring when it passes the mid-point? I don't know. But I do know that it's lower than the speed at which it would pass the mid-point if the spring were not coated with peanut butter. I'm sorry I have to leave the math to those more capable, but I think the principle of what I'm suggesting may be right on.

As a further thought experiment, picture an infinitely stretchy rope with no slack as the climber falls and the pedulum begins. The rope simply stretches, the climber falls straight down, and never hits the wall at all! What happens when a highly dampened, highly stretchy spring is in this position? I suspect that the force with which the climber hits the wall is less, as there is more dampening in the system.

GO


billl7


Jan 20, 2006, 8:41 PM
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I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

I may be misunderstanding you but ... multiply R by the amount of the horizontal traverse before the fall. Take that number and subtract the horizontal travese. This gets on the amount of slack added.

So the point on the line to the right of the spike where the line crosses "1" - that would be about one hundred and eighty percent of the horizontal traverse as added slack.


jt512


Jan 20, 2006, 9:10 PM
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I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

I may be misunderstanding you but ... multiply R by the amount of the horizontal traverse before the fall. Take that number and subtract the horizontal travese. This gets on the amount of slack added.

So the point on the line to the right of the spike where the line crosses "1" - that would be about one hundred and eighty percent of the horizontal traverse as added slack.

Since we agree on what R is, you must be misunderstanding me.

Jay


antiqued


Jan 20, 2006, 9:56 PM
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For the modelers:

PS - how do you get graphs into these things?

I never practiced physics, and don’t have enough time on his hands to really do this justice.

First, regarding Whoa’s analysis. I got the same results he did working from what I thought were his assumptions, before the introduction of “R”. Since Excel rebels against sub expressions dividing by zero – even when the whole expression is non-infinite, I just matched to that point. When I plot up my equations and his equations, I get the same numbers. However, when he says that the key is to let 41% of L as slack, I find that 40% of L is the worst swing, and more slack reduces swing. If the tick marks on Whoa’s graph indicate units, then the total (grey line) seems to peak around 0.4.

Note in my equations I use R as rope length (see Daithi’s diagram) , not as a ratio – the rope length is too useful a value for me to ignore.

Daithi –
I don’t understand why your assumption of no radial momentum should come out different from Whoa’s assumption of dropping all rope direction velocity and taking the tangential velocity. I suspect that you made an error somewhere, since your prediction of 40% more impact velocity (96% more impact energy) would require at least twice the total fall as a taught pendulum, with all fall energy converted to swing– ie slack must equal L, so h=2*L, and slack = 1.24 and nu = 26.6degrees (not slack = 13% and nu=60). Perhaps nu and 90-nu are switched somewhere.

Orthogonal Vy=sqrt(2Gh) Vx = 0; Vtan = V* sin nu ; Vrad = V*cos nu
Radial Vr^2+Vt^2 =2Gh; Vt=Vsin nu; Vr = Vcos nu


Pendulum model – rigid rope when loaded
L – horizontal runout from pro
h – length of free fall before rope is taut
R – rope length = sqrt(h^2+L^2)
S – slack = R-L

Velocity at ‘contact point’ V= sqrt(2Gh)
Tangential velocity = Vtan = V*L/R
Tangential energy Etan=m*V^2 * L^2 /(2*R^2)
Additonal Pendulum energy after ‘contact point’
Epen = mg(R-h)

Eswing = Epen + Etan


http://


antiqued


Jan 20, 2006, 10:08 PM
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For the empiricists:

I haven't survived any big pendulums since ElCap. I just tweaked my ankle off a gym roof last weekend on a small pendulum - tight belay.

The key is obviously to have the braking force occur primarily while the climber is under, rather than to the side of the protection. Just putting slack in does this with modest effectiveness- the braking starts the same distance off to the side as without any slack, but the rope angle is better. However, if "Jay" jumps a little late (after or as a bit of force is applied to the faller), this force will start the climber swinging under the pro - when "Jay's" jump is finished, he brakes the climber under the bolt, and minimal swing occurs.

I don't jump, I try to start braking, then let a little slip and step forward, hoping for the same effect - start the pendulum, delay braking a little to allow the climber to get closer to the plumb line.

Back to your irregularly scheduled equations.


antiqued


Jan 20, 2006, 10:13 PM
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For the empiricists:

I haven't survived any big pendulums since ElCap. I just tweaked my ankle off a gym roof last weekend on a small pendulum - tight belay.

The key is obviously to have the braking force occur primarily while the climber is under, rather than to the side of the protection. Just putting slack in does this with modest effectiveness- the braking starts the same distance off to the side as without any slack, but the rope angle is better. However, if "Jay" jumps a little late (after or as a bit of force is applied to the faller), this force will start the climber swinging under the pro - when "Jay's" jump is finished, he brakes the climber under the bolt, and minimal swing occurs.

I don't jump, I try to start braking, then let a little slip and step forward, hoping for the same effect - start the pendulum, delay braking a little to allow the climber to get closer to the plumb line.

Back to your irregularly scheduled equations.


cchildre


Jan 20, 2006, 10:58 PM
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I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ?


cause from the way you are writing it sounds like you have not done it very much.

Well, why would it matter? This is a matter of physics and is not strictly related to climbing alone IMO.

Further, I don't think I want to hear advice from someone who takes big pendulums on a regular basis, even if done safely. I am trying to limit my experience on this issue.

Straight Answer: none


billl7


Jan 21, 2006, 12:22 AM
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I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

I may be misunderstanding you but ... multiply R by the amount of the horizontal traverse before the fall. Take that number and subtract the horizontal travese. This gets on the amount of slack added.

So the point on the line to the right of the spike where the line crosses "1" - that would be about one hundred and eighty percent of the horizontal traverse as added slack.

Since we agree on what R is, you must be misunderstanding me.

Jay
Okay, it's now inexplicably clearer that you refer to the slope leading up to the spike from starting at no slack.

Trying to back out height from a V-ratio of 1.4, h = (v^2)/(2*g);
assuming units are such that g = 9.81 m/s^2,

h = (1.4*4.429)^2/(2*9.81) ~= 1.96

Doesn't the chart indicate an h of ~1.13 for the spike? And the h of 1.96 assumes perfect transfer of energy from vertical to horizontal. If it is not so efficient as in the model then in reality a larger h is needed rather than smaller?

Sorry if someone has been following my many edits. But it's Friday night and I figure everyone else is off doing something better as I should be. :oops:


whoa


Jan 21, 2006, 5:40 PM
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Thanks, antiqued. I think we do agree on the model. And you're right that my "R" (which was the ratio of the free-fall to my "L", which was the horizontal distance from the piece) is not as useful as as the amount of slack as a percentage of "L".

So let's look at the more interesting quantity. Again I'll show all my work so that my errors can be found easily.

http://groups.msn.com/...=4675556899514017039

a = fall distance
b = horizontal distance from last piece
c = total length of rope

We want to know how the energy at the wall varies with the amount of slack let out, which is (c-b)/b, or ((c/b)-1). Let S = c/b. Same assumptions as before.

Energy at the wall for no slack (i.e., S=1) = mGb.
Velocity at ‘contact point’ V = sqrt(2Ga)
Tangential velocity = V*b/c = sqrt(2Ga)*b/c
Tangential energy = mGab^2/c^2 = mGb * sqrt(c^2-b^2)*b/c^2
= mGb * sqrt(1 - b^2/c^2)*b/c = mGb * [sqrt(1-1/S^2)/S]
Additonal Pendulum energy after ‘contact point’
Ependulum = mG(c-a) = mG(c - sqrt(c^2-b^2))
= mGb * (c/b - sqrt(c^2/b^2 - 1)) = mGb (S - sqrt(S^2 - 1))

I've plotted how the energy at the wall depends on (S-1). So the functions are:

sqrt(1-1/(x+1)^2)/(x+1)
(x+1) - sqrt((x+1)^2-1)
sqrt(1-1/(x+1)^2)/(x+1) + (x+1) - sqrt((x+1)^2-1)

http://groups.msn.com/...=4675556978528778538

From this plot, it looks like (on the current assumptions) letting out a little slack is a tiny bit bad (the worst is at 10% slack, where you gain 2% energy), and letting out 20% or more of the original length starts to get good. At 25% you reduce final energy 2%; at 50% slack you reduce it 12%; 100% slack, 30% reduction.

Enough of that! Off to do some bouldering, where pendulum falls are relatively uncommon.


dirtineye


Jan 21, 2006, 6:19 PM
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I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ?


cause from the way you are writing it sounds like you have not done it very much.

Well, why would it matter? This is a matter of physics and is not strictly related to climbing alone IMO.

Further, I don't think I want to hear advice from someone who takes big pendulums on a regular basis, even if done safely. I am trying to limit my experience on this issue.

Straight Answer: none

You, and the rest of the modelers, are making the classic mistake of treating a comples active organism as if it were an inanimate nonreacting object. Can't really blame you for that, because to make a really good model of a falling climber who reacts to the situation would be beyond what most people could do or comprehend or solve. I am NOT saying I could do it mind you!

As a first step though, you modelers should try throwing in a damper on your falling object that will represent the energy absoption of the legs meeting the wall correctly. Good luck with that unless you know a good bit of classical mechanics and possibly PDE if you want to get serious. You need at least three variables

BTW, limiting your experience with falling in a controlled environment, so that you will be ready for one in a less controlled environment, is foolish, but that 's your business.


cintune


Jan 21, 2006, 6:30 PM
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More study is needed.
http://www.chronologictiming.com/wile.jpg


billl7


Jan 21, 2006, 7:55 PM
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I just have to know, how many of you posting in this thread lately have taken any big pendulums and done it safely ?

cause from the way you are writing it sounds like you have not done it very much.
.... This is a matter of physics and is not strictly related to climbing alone IMO. ....

... to make a really good model of a falling climber who reacts to the situation would be beyond what most people could do or comprehend or solve. I am NOT saying I could do it mind you!

As a first step though, you modelers should ....

The question folks are trying to answer with models was whether paying out slack makes a difference in energy at impact.

BTW dirtineye, there's no rule that one has to live up to their username. :wink:

Bill


healyje


Jan 21, 2006, 10:51 PM
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Models are useless - we need to have thirty RC volunteers do repeated 40 foot pendulums into a dihedral with varying amounts of slacked belay both with feet and backs to the wall and then tally the results.

I can't believe you guys are still going on over this one given it has an incredibly high "duh" factor...


daithi


Jan 22, 2006, 12:10 AM
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I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

And with good reason! It's wrong. I have edited my original post.

In reply to:
I don’t understand why your assumption of no radial momentum should come out different from Whoa’s assumption of dropping all rope direction velocity and taking the tangential velocity. I suspect that you made an error somewhere...

You are correct. I made a very simple algebraic mistake. I really should have checked it first before posting. I have updated my original post.

The shame of fucking up something so simple! :oops:

Here is an extract from the edited post.

The actual increase at the worst possible case, which is a 7% increase of slack, is only 2% in energy or approximately 1% in impact velocity at the wall. This is not significant enough to warrant ever refusing to give slack to a falling climber, since in a real system slack will always be favourable when we take into account rope stretch that takes place over a finite time, as opposed to instantaneously and that 20% slack is very easily achievable! At 20% slack and above the impact force dramatically reduces with increasing slack.


dutyje


Jan 22, 2006, 3:06 AM
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I haven't survived any big pendulums since ElCap.

How many pendulums did you fail to survive since ElCap? ;)

PTI. Everyone else, please resume your nerdity.


cchildre


Jan 23, 2006, 8:04 PM
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[quote="dirtineye]BTW, limiting your experience with falling in a controlled environment, so that you will be ready for one in a less controlled environment, is foolish, but that 's your business.
You do have a point here. Learning to control a fall in a controlled enviroment does have it's merit, but that was not exactly what I intended to communicate with my post. My desire is to not fall, and avoiding them is one of my highest priority.

As far as the modeling guys here and their exercise to calculate the forces that play into a fall and pendlum and examine how the varibles effect these forces is a good thing. So for the 'modelers' they look to reproduce the problem on paper so no one gets killed. From your post, and correct me if I am wrong, but it seems that you would prefer to take some guys out in a 'controlled' enviroment and conduct real world experiments with out ever considering the possibilities an easy calculation might reveal before risking anyones life.

Total aside from the whole discussion...sort of. Bartender enlists five friends to join him in a pendlum off a bridge where they will be harnessed to a steel cable and be picked up by a boat. Bartender adds up eveyones weight and it was around 1000 pounds. So the genius buys 1200 pound test cable, a little over for 'safety'. Mr. Brightness did not think to calculate the force generated by the falling bodies that would build and peak at the very bottom of the swing, far beyond the 1200 pounds he had purchased. One girl opted out and they lost even more weight but the cable still broke just as they began to ascend on the other side of the swing and hit the water, and a few broken bones and two people not breathing. They revived everyone, and this jag is still wanting to do more swings, even though he narrowly avoided killing anyone. Anyone see it?


jt512


Jan 23, 2006, 8:24 PM
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I have trouble believing that the slope is so steep. It doesn't seem reasonable that a tiny increase in slack would increase the impact force by nearly 40%.

And with good reason! It's wrong. I have edited my original post.

In reply to:
I don’t understand why your assumption of no radial momentum should come out different from Whoa’s assumption of dropping all rope direction velocity and taking the tangential velocity. I suspect that you made an error somewhere...

You are correct. I made a very simple algebraic mistake. I really should have checked it first before posting. I have updated my original post.

The shame of f---ing up something so simple! :oops:

Here is an extract from the edited post.

The actual increase at the worst possible case, which is a 7% increase of slack, is only 2% in energy or approximately 1% in impact velocity at the wall. This is not significant enough to warrant ever refusing to give slack to a falling climber, since in a real system slack will always be favourable when we take into account rope stretch that takes place over a finite time, as opposed to instantaneously and that 20% slack is very easily achievable! At 20% slack and above the impact force dramatically reduces with increasing slack.

Okay, these results are much more believable. So, as a rule, we should give the climber more than 20% slack, relative to the their horizontal lead-out.

Jay


Partner rgold


Jan 23, 2006, 9:18 PM
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I've enjoyed reading this thread, and wish I could have contributed, but work on other projects with looming deadlines made it impossible for the moment. In the absence of a real contribution, I feel bad about expressing misgivings about what has been done; nonetheless I'm wary of deductions made from models that use a completely inelastic rope.

First of all, these models are physically impossible, a fact their proposers acknowledge but do not view as a deal-breaker. The models have a jump discontinuity in the velocity vector of the falling climber at the moment the rope goes taut, requiring an infinite force in order to achieve the jump. Any actual situation that approached these models would end with the breaking of gear before the climber pendulumed into the wall, rendering any conclusions about that impact rather moot.

Second, the ability of the rope to absorb energy by stretching might well have a significant effect on the kinetic energy of the penduluming climber and so on the severity of the impact experienced. Whether the rigid cable model provides, in some sense, a good approximation to the elastic rope model is not clear to me. Perhaps it doesn't.

It doesn't seem to me (not having tried yet) to be especially hard to write down the differential equations for a strechable pendulum obeying Hooke's law; I'll try to do this when I can, unless someone beats me to it. It is certain that these equations won't have a closed-form solution, but we have solvers nowadays that can provide very good numerical information and draw lovely phase portraits, and this data should be enough to make reasonable and realistic conclusions about adding slack to a pendulum fall belay.


Partner cracklover


Jan 23, 2006, 9:45 PM
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It doesn't seem to me (not having tried yet) to be especially hard to write down the differential equations for a strechable pendulum obeying Hooke's law; I'll try to do this when I can, unless someone beats me to it.

If you do, please put some thought into how you might account for a soft catch while you're at it. It seems as if a soft catch would amplify the results you see from rope stretch. In other words: further add to the length of the pedulum and convert kinetic energy to heat.

Cheers and thanks in advance!

GO


daithi


Jan 23, 2006, 10:44 PM
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It doesn't seem to me (not having tried yet) to be especially hard to write down the differential equations for a strechable pendulum obeying Hooke's law;

Here's my guess. It is written in polar coordinates r, and q (theta).

Equation of motion of pendulum:

d^2q/dt^2 = -g/r sin q [eqn. 1]

Edited: rgold pointed out a mistake. Changed l to r in [eqn. 1]. For a derivation of this see my later post.

Hooke's Law in cartesian coordinates.

d^2x/dt^2 = -(k/m) x + g

Write d^2x/dt^2 in polar coordinates where r_hat is the unit vector in the r direction. (x = rcosq and y = rsinq).

d^2x/dt^2 = (d^2r/dt^2 - r (dq/dt)^2) r_hat

The second derivative in the q_hat direction is zero, since the spring constant of the rope only acts in the r_hat direction. The gravity force acting in the r_hat direction is g cos q. Hooke's law then becomes,

(d^2r/dt^2) = -(k/m)*r + (g*cos q) + (r*(dq/dt)^2) [eqn. 2]

There we have two differential equations [eqns. 1,2] in polar coordinates to describe the motion.

Anyone get anything else?

Edited to add: If we ignore the (dq/dt)^2 term in [eqn. 2] and introduce two dummies variables the above equations can easily be reduced to first order ODE's. They can then be solved using a time marching approach. Not too sure if that is a valid assumption though.

Edited: Changed r cos q to r since deformation can only take place in r in [eqn. 2].

Edited: After thinking about it, we can't ignore the (dq/dt)^2 term. Physically this is the centrifugal force (or whatever you wish to call it!)

In reply to:
Whether the rigid cable model provides, in some sense, a good approximation to the elastic rope model is not clear to me. Perhaps it doesn't.

As for the previous model it is correct in the limit as the fall factor goes to zero (no elongation of the rope). Like any idealised physical model, the limitations should be known.


Partner kimgraves


Jan 23, 2006, 11:13 PM
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Interesting discussion - Just want to be notified when updated. Thanks.


Partner rgold


Jan 24, 2006, 5:22 AM
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Equation of motion of pendulum:

d^2q/dt^2 = -g/l sin q [eqn. 1]

I don't think this is the right thing to use for the stretchable pendulum; it is derived assuming the pendulum length L is constant. In that derivation, if L is a function of t rather than a constant, then the product rule will have to be invoked and, in addition to L, L' will also have to appear.


whoa


Jan 24, 2006, 7:09 AM
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Yeah. Instead, just keep track of the axial rope force and gravity, which are the only forces we're including (ignoring wall-friction, wind resistance, . . .).

I've written a little simulator in an excel spreadsheet that just calculates the motion millisecond by millisecond and draws a couple of charts. You can adjust the assumptions, including the amount of slack, the rope stretchiness (from which we get the spring constant, allowing that longer ropes have smaller k's), and, crucially, a damping factor (ropes are damped oscillators because of internal friction). I assumed that unlike a spring, there is no rope force when the rope is compressed (slack).

I did a sanity check with near-zero stretchiness and zero slack, and it is pretty darned close to the theoretical value (e=mGh). But I haven't played with it much more than that.

Anyway, it's at http://merv.stanford.edu/pendulumfall.xls if anyone wants to check it out and maybe fiddle with it.


cintune


Jan 24, 2006, 12:51 PM
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daithi


Jan 24, 2006, 3:23 PM
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In reply to:
In reply to:
Equation of motion of pendulum:

d^2q/dt^2 = -g/l sin q [eqn. 1]

I don't think this is the right thing to use for the stretchable pendulum; it is derived assuming the pendulum length L is constant. In that derivation, if L is a function of t rather than a constant, then the product rule will have to be invoked and, in addition to L, L' will also have to appear.

Edited: Sorry rgold ignore all the nonsense that was here in this post before. You were correct.

We start with the differential equation

d^2x/dt^2 = (-k/m)*x + g

Write in terms of r and q.

The r component is [eqn. 2]

The theta component should be written as:

d^2q/dt^2 = -g/r sin q - ((2/r)*(dr/dt)*(dq/dt))) [eqn. 1]

The additional term on the right hand side is due to the r not being constant in the moment of inertia so it is the second derivative of the product of r^2 and angle. When dr/dt is zero this reduces to the normal predulum equation.

Man that was a lot more complicated than I thought it would be.


daithi


Jan 24, 2006, 3:37 PM
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The forces in a two-dimensional elastic pendulum are due to gravity and Hooke's Law:

In reply to:
Yeah. Instead, just keep track of the axial rope force and gravity, which are the only forces we're including (ignoring wall-friction, wind resistance, . . .).



What delcross and whoa have neglected in their models of an elastic pendulum is the "centrifugal" force which in addition to gravity acts against the spring. Even the non-mathematical amongst you will be able to appreciate that the faster you swing the rope around the more it will stretch.

If we have a look at the differential equations again.

In the theta direction:
d^2q/dt^2 = -g/r sin q [eqn. 1]

In the radial direction:
(d^2r/dt^2) = -(k/m)*r + (g*cos q) + (r*(dq/dt)^2) [eqn. 2]

Here we have two differential equations in two variables r and theta (q). For the non-mathematical amongst you (who I presume will have left long ago!) I will attempt to explain the terms.

The first equation basically says the angular acceleration is caused by the component of gravity acting in this direction. There is no other force acting in this direction.

The second equation basically says that the acceleration in the radial direction is equal to the component of gravity acting in line with the rope and the centrifugal force (which also acts in line with the rope). These two forces are counteracted (minus sign) by the spring force in the rope (the first term on the right hand side).


whoa


Jan 24, 2006, 3:51 PM
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Daithi, there is no centrifugal force on the climber. The only forces on the climber are gravity, which pulls down, and the rope, which pulls radially. If you swing a weight around on a rope, there is not some new force on the object pulling it away from you. It is going tangent to you and a force is required to accelerate it towards you to keep it the same distance from you; the rope provides that force.

Probably there is some equivalent way to think of the situation as involving a centrifugal force (despite the common physicists' claim that there's no such thing as centrifugal force). But I don't think there's any force missing from the model. At least I'm not yet convinced.

I look forward to studying delcross's work (thanks!), but I can't until later...


daithi


Jan 24, 2006, 4:51 PM
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If you swing a weight around on a rope, there is not some new force on the object pulling it away from you. It is going tangent to you and a force is required to accelerate it towards you to keep it the same distance from you; the rope provides that force.

What happens if I speed up? The distance increases. Anyway the difference arises because you have chosen to model the motion in catesian coordinates (not that it's incorrect it just makes understanding curved motion a bit less intuitive).

Why have to chosen to model it in cartesian coordinates? In my mind it is a lot easier to understand what is happening physically if you describe it as a polar motion (as both of us did before).

If you derive the equations of motions from first principles in polar coordinates you get the addition of this (dq/dt)^2 term (the centrifugal force term). This is not my assumption or addition, it comes out in the maths. But don't take my word for it. Derive the equations of motion for yourself from first principles and see what you get. I would be interested to see someone else's equations of motion.


whoa


Jan 24, 2006, 5:41 PM
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I dunno, it seems intuitive enough in x-y coordinates to me. Wouldn't be hard to do something similar on a spreadsheet in polar coordinates. Either way, it's nice to be able to see the trajectories charted to get a sense of what's going on with different assumptions.


cintune


Jan 24, 2006, 10:47 PM
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daithi


Jan 25, 2006, 2:39 AM
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In reply to:
In reply to:
(d^2r/dt^2) = -(k/m)*r + (g*cos q) + (r*(dq/dt)^2) [eqn. 2]

Almost, but you left out a term in the first equation for the coupling between r and q. Try this instead: write down the Lagrangian and from that derive the equations of motion.

I agree. See my revised post above.

d^2q/dt^2 = -g/r sin q - ((2/r)*(dr/dt)*(dq/dt))) [eqn. 1]


antiqued


Jan 26, 2006, 1:34 AM
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I have further refined a SS model with some help from Whoa’s work. My previous model was broader in that it covered arbitrary rope length, lead out distance, lead across distance and slack (frictionless biners). While it imitated a lead fall reasonably well (elongation and impact force) and also gave decent results for a taut pendulum fall, it did not add up the energy balance closely enough - there was a 5-10% surplus of energy stored in the rope.

I took some hints from Whoa’s SS and got to a better energy balance, and then pulled in the damping coefficient approach he used. I could not get reasonable combinations of impact force, elasticity and rope stretch for the standard UIAA fall. Any damping coefficient that produced a reasonable ‘one rebound only’ motion forced unreasonably high elasticity to minimize impact force, and failed to extend the rope sufficiently. I then introduced an additional term, a hysteresis effect, in which the stretched rope does not exert its full elastic tension while contracting during the rebound upwards. This SS does a reasonable casual impression of the UIAA standards for static elongation and impact force. Since the UIAA fall has little rope on the static side of the biner, and the pendulum falls we are looking at don’t stretch too much, the frictionless biner assumption probably does not change these results too much.

The predictions for pendulum energy in the x direction – that is the energy of collision into a wall under a roof, for example when falling off above the roof:

Rope distance belayer to last pro – 8m
Climber height above pro – 1m
Lateral distance of climber from pro – 2m

Rope Slack – Wall impact energy
0 m 1.95kJ (“steel” rope – minimal stretch calculates as 2.29kJ for this fall)
0.1 1.89
0.2 1.83
0.5 1.64
0.75 1.48
1 1.36
1.5 1.16
2 1.02
3 0.82
4 0.68

I still don’t think that this accurately represents best practice – it is all “hard catch” still, and I don’t think that most people are giving a metre of slack or more. I’m pretty damn sure they aren’t jumping that high. But best practice seems to reduce the swing to nearly zero.

(delcross - this stepwise model has the nerve to predict that 85% of the gravitational energy is converted to swing for a "steel" rope)

But it is another step in some direction – unfortunately, work calls, and fortunately, I have a long vacation weekend coming up, so I won’t be able to follow through much for a while.


healyje


Jan 26, 2006, 9:18 AM
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When you guys get done please post one with the bottom line for us mere mortals. It would seem common sense though that you could take a bunch of steam out of a pendulum with enough slack and air space to play in - but who knows, I could be completely wrong...


azrockclimber


Jan 26, 2006, 1:55 PM
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haha..okay.

Easy answer, A pendulum fall can be just as bad as decking on the ground... Avoid it, protect yourself, protect your second, and try not to take the hit on the side of your body of you do fall into a wall on a pendulum swing. Vital organs are more exposed there.

And, if you have time to do the calculations in the other posts, bring a graphing calculator when you climb....who doesn't..it just makes it more fun. ya know!!???


whoa


Feb 1, 2006, 11:39 PM
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Well I do not yet share that conclusion based on my spreadsheet which included modeling the damping effect of the rope. I think we still need to model the actual features of climbing ropes better. It may well turn out that reasonable amounts of slack are good, but I think it's too soon to conclude anything.

Certainly it would be crazy for anyone to rely on our half-assed work on this for actual decisions about safety.


trenchdigger


Feb 1, 2006, 11:53 PM
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Now, I'm too lazy to actually do the work to look into it, but I would propose that a softer catch via a dynamic belay would be much more effective at reducing horizontal (swinging) speed than simply adding slack to the system. Just another bone to chew on...


jt512


Feb 2, 2006, 12:12 AM
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In reply to:
In reply to:
At 20% slack and above the impact force dramatically reduces with increasing slack.

In reply to:
Okay, these results are much more believable. So, as a rule, we should give the climber more than 20% slack, relative to the their horizontal lead-out.

To get a 10% reduction one needs to provide 68% slack. To put this in perspective, a 15 foot traverse results in a speed of about 21 mph at the bottom of the swing.

What is the speed at the bottom of the arc if the traverse is 4 feet and there is no slack in the rope?

Jay


cintune


Feb 2, 2006, 12:13 AM
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Conclusion: Adding slack to a pendulum fall is not a practical means for reducing the speed of the swing.

- This being the case, which it may or may not I suppose, there may still be other quantifiable benefits to the practice. No matter what, every foot-per-second-slower the impact, the less potential damage. Difference between bad sprains or bruises and broken bones. second, giving slack to add even a little more reaction-time to work with can't hurt. Thirdly, it's a shorter lower-off and carry out, if it comes to that.


rockkid55


Feb 2, 2006, 1:58 AM
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Umm........I'm trying to think of something funny to add to this post, but I doubt that anyone is reading this far into a MATH post. So.

I'll just go away now.


daithi


Feb 2, 2006, 3:09 AM
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Here is another calculation done modelling the elasticity (very simply)! It was done over a week ago but due to being very busy I didn't have time to post it until now. Sorry.

The physical system this time has replaced the perfectly rigid connection with a spring of stiffness k. The relevance of this physical model to an actual climbing situation is of course very debatable. The dynamic response of a rope is not that of a linear spring! However, it should serve at least some use to understand the effect of elasticity.

http://www.rockclimbing.com/...p.cgi?Detailed=68520

The angle q (theta) is the angle from the vertical, r is the time dependent length of the rope and r0 is the initial length of the rope, which corresponds to the equilibrium position of the spring when there is no force applied.

The differential equations solved were:

d^2q/dt^2 = -g/r sin q - ((2/r)*(dr/dt)*(dq/dt))) [eqn. 1]
(d^2r/dt^2) = -(k/m)*(r-r0) + (g*cos q) + (r*(dq/dt)^2) [eqn. 2]

By defining two new variables u and v as,
dr/dt = u; dq/dt = v,
equations (1) and (2) can be reduced to first order differential equations. Therefore, we have four coupled first order differential equations to solve. I used a 4th order Runge-Kutta method to solve the coupled differential equations. The timestep size was 1E-03 and the equations were marched in time until q = 0 (the point of impact with the wall).

The spring constant is defined as k = EA/r0, where E is Young's modulus and A is the cross sectional area of the rope (I assumed a 10.5 mm rope). Young's modulus was taken to be 2.36E08 N/m^2. The mass was assumed to be 80 kg (UIAA mass). A test was done at initial values of q = 0, r0 = 1 m and a distance dropped of 1.71 m. This corresponds to a vertical fall with a fall factor of 1.71 (the UIAA drop test). The model predicted a peak force at the point the mass stopped of 7.45 kN at an elongation of 40%. The actual experimental figures for the UIAA drop test at a fall factor of 1.71 are 7.4 kN at an elongation of 37% for my Beal rope. Therefore, the value of k is reasonably physical. However, it should be noted that although the peak values are realistic at the point when the mass stops moving, the time dependent motion is not physical as there is no damping.

An example of the trajectory of the elastic pendulum compared to the ideal pendulum is shown below at R = 1 showing the increase falling distance due to the elastic deformation.

http://www.rockclimbing.com/...p.cgi?Detailed=68523

Shown below are the results of the impact velocity at the wall compared to the original model. The impact velocities (r dq/dt) have again been normalised wrt 4.429 m/s, which is the impact velocity of an idealised pendulum at R = 1.

http://www.rockclimbing.com/...p.cgi?Detailed=68521

It should also be noted that in this graph, for the elastic pendulum, R is the initial length of rope at t = 0. Below are some conclusions.

1. Initially at R = 1 there is a slight decrease in the impact velocity even though the mass has fallen a greater distance. The initial velocity and acceleration at this condition are zero, i.e. a pure pendulum.

2. As R increases there is more vertical fall distance and therefore more initial velocity in the pendulum. The rope in the original model performed perfectly in that it absorbed all the linear momentum in the direction of the rope instantaneously at the start of the pendulum. In this revised model it initially absorbs less linear momentum and it is spread out over a finite time interval.

3. The combination of this effect and the increased falling distance due to the elongation results in higher impact velocities at the wall.

4. According to this we need to let out over twice as much slack as the horizontal distance before a decrease is seen in the impact velocity. This is a lot more than the 20% increase in slack with our 'perfectly' performing rope.

Some comments on damping:
In reality the climbing rope is likely to exhibit viscoelastic damping and be over-damped. The damping will probably depend on static pre-load, frequency, dynamic strain rate etc. The Young's modulus will be a complex quantity containing a real part (the elastic behaviour) and an imaginary part (the dissipative term). I have not seen any experimental time dependent data for a kernmantle rope so I really have no idea of the magnitude of the real and imaginary parts of the complex modulus.

As always I cannot guarantee this is devoid of errors!


curt


Feb 2, 2006, 3:17 AM
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In reply to:
In reply to:
In reply to:
In reply to:
- initial slack makes negligable (in theory, if not zero) difference

If it makes no difference ito you in theory, you need to find another theory.

Jay

Dear Jay, I will restate...with initial slack in the system (your rope), you will only increase your vertical fall velocity and THEN translate it into the SAME AMOUNT of horizontal velocity


By looking at the extreme case suggested by Curt, an infinitie amount of slack, it can be seen that you are wrong. The horizontal velocity would be 0 (and, incidentally, the fall factor would only be 1). So, assuming, as we should, until someone proves otherwise (using real equations), that the relationship between slack and horizontal velocity is monotonic, then the more slack in the rope, the less the horizontal velocity.

Edit: Actually, in daithi's model the realtionship is not monotonic.

Jay

I agree with this. The only reason I said that the correct answer was "situational" is because, in real life, feeding out additional slack could cause the climber to hit a ledge or something similar below--perhaps with worse consequences than the initial pendulum fall itself.

Curt


jt512


Feb 2, 2006, 8:45 PM
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4. According to this we need to let out over twice as much slack as the horizontal distance before a decrease is seen in the impact velocity. This is a lot more than the 20% increase in slack with our 'perfectly' performing rope.

And, based on practical climbing experience, I'm back to not believing the results.

Jay


daithi


Feb 2, 2006, 9:36 PM
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4. According to this we need to let out over twice as much slack as the horizontal distance before a decrease is seen in the impact velocity. This is a lot more than the 20% increase in slack with our 'perfectly' performing rope.

And, based on practical climbing experience, I'm back to not believing the results.

Jay

This very simplified model is only a tiny part of the real life situation (and I still make no guarantees of it being correct). For example here is a plot of the increase in time to impact with increase in R.

http://www.rockclimbing.com/...p.cgi?Detailed=68803

The worst case scenario in terms of increase in impact velocity is R = 1.36, which corresponds to an increase in time to impact of 22%.

In real world situation the chances of injuring oneself is related to how well one absorbs the impact. Therefore, I think the increase in time is all important in avoiding injuries not necessarily the increase in impact velocity. I personally would prefer to take a higher impact that I was prepared for as opposed to a slightly less severe impact that I hadn't quite got into position to absorb the impact.


daithi


Feb 2, 2006, 9:47 PM
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4. According to this we need to let out over twice as much slack as the horizontal distance before a decrease is seen in the impact velocity. This is a lot more than the 20% increase in slack with our 'perfectly' performing rope.

And, based on practical climbing experience, I'm back to not believing the results.

Jay

This very simplified model is only a tiny part of the real life situation (and I still make no guarantees of it being correct). For example here is a plot of the increase in time to impact with increase in R.

http://www.rockclimbing.com/...p.cgi?Detailed=68803

The worst case scenario in terms of increase in impact velocity is R = 1.36, which corresponds to an increase in time to impact of 22%.

In real world situation the chances of injuring oneself is related to how well one absorbs the impact. Therefore, I think the increase in time is all important in avoiding injuries not necessarily the increase in impact velocity. I personally would prefer to take a higher impact that I was prepared for as opposed to a slightly less severe impact that I hadn't quite got into position to absorb the impact.


daithi


Feb 2, 2006, 10:04 PM
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delcross,

Out of curiosity what force and elongation does your values of modulus and damping coefficient produce at the end of a vertical fall with a fall factor of 0.25? Based on simple analysis I would consider values of somewhere around 2.8 kN and elongation of around 14 % to be physical. I would be interested to see what your model predicts. Thanks.

 

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