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USnavy
Mar 14, 2012, 8:16 AM
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I recently purchased a 500Hz. strain gauge analyzer and 5000 lbs load cell that I can use in the field with my laptop, so I decided to do some testing on TR falls today. This is just some quick non-scientific testing to familiarize myself with the equipment, so don’t take anything in here too seriously. I took six falls of varying length and catch method (i.e. hard catch, soft catch, ect.). The graphs below represent the most serious of the six falls. Basically I wanted to determine what would be the highest impact force I could produce on the anchor while top roping without doing something extremely dumb, like taking a huge TR whipper on static rope. Here are the specs: -160 lb climber -175 lb belayer -Mechanically locking belay device -9.9mm Maxim Glider, 9.5 kN impact force rating, 29% dynamic elongation, 5% static elongation -Hard catch (the belayer just stood there and locked off) -50 feet of rope out, 12 foot free fall, 20 foot total fall distance (approximate, not measured) To start with, some really crappy pictures of the set up: Next, the fall graphed out: This next graph represents the loading that was in the upper 50% of the fall range. The peak load was just shy of 700 lbs. so this graph shows the loading above 350 lbs. The numbers on the X axis represent the duration in milliseconds multiplied by ten. This last graph captures what I am going to call the “high” or “mean peak” meaning it shows how long the force stayed in the upper 10% range of the fall range, or above 600 lbs. This graph would be useful to compare different falls of the same fall factor, but different fall lengths, because it shows how long the anchor experiences the peak force of the fall. As you can see the loading on the anchor was only in the top 10% for 160mS. So the maximum impact force on the anchor with a 12 foot free fall on TR was 3.09 kN. Keep in mind, I pulled out a fair amount of slack before I let go and my belayer gave me an intentionally hard catch. So your average TR fall will likely produce less of an impact force on the anchor, unless you weight a lot more than me.
(This post was edited by USnavy on Mar 14, 2012, 10:21 AM)
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moose_droppings
Mar 14, 2012, 3:03 PM
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USnavy wrote: I recently purchased a 500Hz. strain gauge analyzer and 5000 lbs load cell that I can use in the field with my laptop, so I decided to do some testing on TR falls today. This is just some quick non-scientific testing to familiarize myself with the equipment, so don’t take anything in here too seriously. I took six falls of varying length and catch method (i.e. hard catch, soft catch, ect.). The graphs below represent the most serious of the six falls. Basically I wanted to determine what would be the highest impact force I could produce on the anchor while top roping without doing something extremely dumb, like taking a huge TR whipper on static rope. Here are the specs: -160 lb climber -175 lb belayer -Mechanically locking belay device -9.9mm Maxim Glider, 9.5 kN impact force rating, 29% dynamic elongation, 5% static elongation -Hard catch (the belayer just stood there and locked off) -50 feet of rope out, 12 foot free fall, 20 foot total fall distance (approximate, not measured) To start with, some really crappy pictures of the set up: [img]http://img209.imageshack.us/img209/5091/1001093b.jpg[/img] [img]http://img696.imageshack.us/img696/5688/1001096h.jpg[/img] Next, the fall graphed out: [img]http://img338.imageshack.us/img338/8853/totalg.jpg[/img] This next graph represents the loading that was in the upper 50% of the fall range. The peak load was just shy of 700 lbs. so this graph shows the loading above 350 lbs. The numbers on the X axis represent the duration in milliseconds multiplied by ten. [img]http://img3.imageshack.us/img3/5476/53675516.jpg[/img] This last graph captures what I am going to call the “high” or “mean peak” meaning it shows how long the force stayed in the upper 10% range of the fall range, or above 600 lbs. This graph would be useful to compare different falls of the same fall factor, but different fall lengths, because it shows how long the anchor experiences the peak force of the fall. As you can see the loading on the anchor was only in the top 10% for 160mS. [img]http://img52.imageshack.us/img52/2038/peek10.jpg[/img] So the maximum impact force on the anchor with a 12 foot free fall on TR was 3.09 kN. Keep in mind, I pulled out a fair amount of slack before I let go and my belayer gave me an intentionally hard catch. So your average TR fall will likely produce less of an impact force on the anchor, unless you weight a lot more than me. Thanks for your time and work. Now, who the hell one starred this effort. Stand up and out yourself and why. I don't use the star system but thought I'd counter there one star with a five star.
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jt512
Mar 14, 2012, 3:44 PM
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The three figure shows the peak at about 40, 22, and 11, respectively. Can you clarify what the units of the horizontal axes are in each of the figures, and explain why peak occurs at different values? Jay
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skurdeycat
Mar 14, 2012, 4:20 PM
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Can you measure the force exerted by the climbers fist on the belayers face after a 20ft toprope fall? Skurdey
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LostinMaine
Mar 14, 2012, 4:21 PM
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Good stuff. Thanks for posting. In the future, like Jay points out, your figures need a bit of work. Label all axes for each figure - that little bit of time spent helps to strengthen all of the time spent previously generating data to populate the figures. I'm curious about consistency, though. Have you tried taking the same fall with the same style catch multiple times and plotting the results? I wonder what kind of variance you might find.
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MFC
Mar 14, 2012, 4:22 PM
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Thanks for posting this up - very interesting. If I may, I have a question/suggestion. According the the standard equation for impact force, a fall on a top rope with zero fall factor (basically just weighting the rope) will produce a peak force on the rope (and felt by the climber) of twice his body weight before returning to just one body weight. Most climbers I have talked to find this to be unbelievable/untrue. Next time you run some tests, could you measure the peak load from a fall factor=zero fall on a top rope? Thanks. I look forward to further test results.
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LostinMaine
Mar 14, 2012, 4:22 PM
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skurdeycat wrote: Can you measure the force exerted by the climbers fist on the belayers face after a 20ft toprope fall? Skurdey Sure. What's the mass of the fist and what is its acceleration?
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amarius
Mar 14, 2012, 4:49 PM
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Not the OP, but here is quick answer. If just hanging off the top anchor with full mass of M, the top anchor attachment will experience 2*M*g force. This is, most likely, a bit hard to believe :) So, to simplify this a bit - hanging off the top anchor could be reconfigured as a fixed pulley
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MFC
Mar 14, 2012, 5:29 PM
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I am not referring to the "pulley effect" of the top piece of pro. If the standard equation of impact force is true/accurate then weighting the top rope (FF=0)produces an instantaneous impact force of 2x body weight, and the pulley effect would effectively double that (neglecting friction at the carabiner). My original question was to verify that the impact force equation is valid or not for zero fall factor on a top rope.
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amarius
Mar 14, 2012, 5:50 PM
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FF=0 is equal to static loading. It is a bit easier to understand this if there is no friction on the system. Climber rope pulls down with M*g Belayer rope pulls down with M*g - remember, no frictional losses. Why are these two forces equal? If they were not equal, according to Newton's Laws, something would have to be moving, and we are talking about a static load. Climber rope pulls down with M*g, belayer rope pulls down with M*g, anchor pulls up with 2*M*g. Why 2*M*g - nothing is moving, forces have to be cancel out, two M*g down, the one going up must be equal to the sum. As a matter of fact, if one examines the Force vs time over longer period, the one with force oscillation, observation that the loading settles around 300lb is quite obvious, with swings to above ~325 and below 250. Why 300lb, and not 320lb? - possible explanations - additional friction somewhere, i.e. climber touching something, rope rubbing against the rock, instrument not calibrated/erroneous. BTW, I am not implying calibration or erroneous reading issues, the possibility is just listed Adding rope over the couple of carabiners friction doesn't change the final static loading on the anchor, but the forces get too complicated for the verbal analysis Hope this helps
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MFC
Mar 14, 2012, 6:15 PM
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I believe Richard Goldstone's article " Standard Equation for Impact Force" is still on the rockclimbing.com forum archives. I hope this address is still accurate: http://www.rockclimbing.com/cgi-bin/forum/gforum.cgi?do=post_attachment;postatt_id=2957; It is a good read!
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jt512
Mar 14, 2012, 6:22 PM
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amarius wrote: FF=0 is equal to static loading. No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight.
In reply to: As a matter of fact, if one examines the Force vs time over longer period, the one with force oscillation, observation that the loading settles around 300lb is quite obvious, with swings to above ~325 and below 250. Why 300lb, and not 320lb? The simplest explanation would be because of friction between the rope and the top carabiners.
In reply to: Adding rope over the couple of carabiners friction doesn't change the final static loading on the anchor . . . Yes it does. It reduces the tension in the rope on the belayer's side of the anchor.
In reply to: Hope this helps Hope springs eternal. Jay
(This post was edited by jt512 on Mar 14, 2012, 6:24 PM)
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cracklover
Mar 14, 2012, 6:36 PM
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amarius wrote: FF=0 is equal to static loading. It is a bit easier to understand this if there is no friction on the system. Climber rope pulls down with M*g Belayer rope pulls down with M*g - remember, no frictional losses. Why are these two forces equal? If they were not equal, according to Newton's Laws, something would have to be moving, and we are talking about a static load. Climber rope pulls down with M*g, belayer rope pulls down with M*g, anchor pulls up with 2*M*g. Why 2*M*g - nothing is moving, forces have to be cancel out, two M*g down, the one going up must be equal to the sum. As a matter of fact, if one examines the Force vs time over longer period, the one with force oscillation, observation that the loading settles around 300lb is quite obvious, with swings to above ~325 and below 250. Why 300lb, and not 320lb? - possible explanations - additional friction somewhere, i.e. climber touching something, rope rubbing against the rock, instrument not calibrated/erroneous. BTW, I am not implying calibration or erroneous reading issues, the possibility is just listed Adding rope over the couple of carabiners friction doesn't change the final static loading on the anchor, but the forces get too complicated for the verbal analysis Hope this helps I'm just curious - why would you want to embarrass yourself by putting this in print? GO
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amarius
Mar 14, 2012, 6:51 PM
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Thanks for you corrections. I have to agree, I made erroneous statements. Tension on the belayer side is defined by the Capstan equation Tbelayer=Tclimber*exp( - miu * angle) miu - is the friction coefficient between the surfaces, angle in radians is how much arc coverage surface provide. In the most general case miu is different for dynamic and static friction. Dynamic friction values are, typically, lower. Force on the anchor would then be Tbelayer+Tclimber Rough estimations are just that since rope friction over carabiners should depend on the construction of the rope and carabiners - that is very specific to set up. Two carabiner setup will result in angle > pi, exact value depending on the angle that carabiners form. miu is a bit more difficult - published values range from .15 to .25 So, for angle of pi ( 3.14), miu of ( .15/.2/.25 ) Tanchor = (259 245 232) lb of force, for the 160lb climber Not quite the same as the measurement. As a general observation - lower friction will result in higher anchor loading. Two extreme cases - no friction - Tanchor == 320lb, the pulley - super friction - belayer ends is unloaded ( aka rope tied directly to the anchor ) Tanchor=160lb. Just to clarify - that is the static loading value. As jt512 pointed out, FF=0 will include the rope stretching out.
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bigo
Mar 14, 2012, 7:16 PM
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jt512 wrote: ...Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. I don't disagree, Hooke's law is specific to stiffness only, but I believe the above only stands true for an un-damped response which seems like a pretty rough assumption for a FF=0 fall. I would definitely agree that friction at the top biners causes the anchor load to not equal 2x the climber weight.
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dan2see
Mar 14, 2012, 7:27 PM
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Great stuff, USN! Real data, in a real situation, simply presented. Your experiment surpasses the thousands of myths and millions of words about anchor dynamics.
Daniel the scientist wrote: Why do climbing engineers have hunched shoulders, and sloping foreheads? When you ask one to describe the real forces on a TR anchor, he'll hunch his shoulders and say "I don't know". When you show him USN's experiment, he'll slap his forehead and say "I knew it!"
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skurdeycat
Mar 14, 2012, 7:28 PM
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Good lord. There isn't a single post is this thread that is completely accurate, except perhaps the OP, and the one linking to rgold. I don't know where to start. Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). There is no friction, rope elongation, pulley effect, nothing else to consider. If the climber or belayer is touching the rock or ground, the force will be less. aargh, you folks scare me.
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bigo
Mar 14, 2012, 7:48 PM
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skurdeycat wrote: Good lord. There isn't a single post is this thread that is completely accurate, except perhaps the OP, and the one linking to rgold. I don't know where to start. Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). There is no friction, rope elongation, pulley effect, nothing else to consider. If the climber or belayer is touching the rock or ground, the force will be less. aargh, you folks scare me. Go belay someone half your weight and try to lift your legs off the ground while they are hanging free on the rope.
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healyje
Mar 14, 2012, 7:54 PM
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I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts.
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jt512
Mar 14, 2012, 8:01 PM
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skurdeycat wrote: Good lord. There isn't a single post is this thread that is completely accurate, except perhaps the OP, and the one linking to rgold. I don't know where to start. Nor where to stop, unfortunately for you.
In reply to: Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). There is no friction, rope elongation, pulley effect, nothing else to consider. No friction? I think you need to think that through a little more.
In reply to: aargh, you folks scare me. Is that your best pirate voice? At least it's better than your physics. Jay
(This post was edited by jt512 on Mar 14, 2012, 8:12 PM)
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jt512
Mar 14, 2012, 8:05 PM
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cracklover wrote: I'm just curious - why would you want to embarrass yourself by putting this in print? I hope that wasn't all you got, because you need something left for skurdeykat. Jay
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kennoyce
Mar 14, 2012, 8:06 PM
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skurdeycat wrote: Good lord. There isn't a single post is this thread that is completely accurate, Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). Quoted for posterity.
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boadman
Mar 14, 2012, 8:16 PM
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jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that?
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jt512
Mar 14, 2012, 8:20 PM
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boadman wrote: jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that? Pretty sure. We're talking plain vanilla Hooke's Law. No dampening. Jay
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kennoyce
Mar 14, 2012, 8:22 PM
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boadman wrote: jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that? I don't know about Jay, but I am, FF = distance of fall (before the rope starts to catch you)/amount of rope (before the rope starts to stretch), so if there is 0 slack, and 0 tension, and a full 200 ft of rope out, the FF will be 0/200 = 0, but the rope will certainly stretch quite a bit before you come to a stop.
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healyje
Mar 14, 2012, 8:31 PM
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jt512 wrote: healyje wrote: [image]http://img209.imageshack.us/img209/5091/1001093b.jpg[/image] I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts. *facepalm* *facepalm* - exactly.
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boadman
Mar 14, 2012, 8:37 PM
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jt512 wrote: boadman wrote: jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that? Pretty sure. We're talking plain vanilla Hooke's Law. No dampening. Jay For the climber at the instant he came to rest, the force would be: -kx = mg How do you get 2xthe climbers (I assume you meant mass?) "weight" out of that? Were you thinking about the load the anchor would see? I could understand that, I think.
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bigo
Mar 14, 2012, 10:01 PM
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boadman wrote: jt512 wrote: boadman wrote: jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that? Pretty sure. We're talking plain vanilla Hooke's Law. No dampening. Jay For the climber at the instant he came to rest, the force would be: -kx = mg How do you get 2xthe climbers (I assume you meant mass?) "weight" out of that? Were you thinking about the load the anchor would see? I could understand that, I think. You are thinking statics, but this is a dynamic system. Also, Jay was scrupulous and said as Hooke's law would predict, so it is not what what you see with a actual top-rope that includes friction/dampening. From http://en.wikipedia.org/wiki/Fall_factor which comes from http://en.wikipedia.org/.../Harmonic_oscillator
(This post was edited by bigo on Mar 14, 2012, 10:04 PM)
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dan2see
Mar 14, 2012, 10:02 PM
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kennoyce wrote: boadman wrote: jt512 wrote: No, it isn't. A fall factor of 0 is a fall. It occurs when you fall on a rope with no slack and no initial tension—for example, an idealized top rope fall. Hooke's Law predicts that the maximum impact force on the climber will be two times his weight. Jay Sure about that? I don't know about Jay, but I am, FF = distance of fall (before the rope starts to catch you)/amount of rope (before the rope starts to stretch), so if there is 0 slack, and 0 tension, and a full 200 ft of rope out, the FF will be 0/200 = 0, but the rope will certainly stretch quite a bit before you come to a stop. It's a fall. No it's a fall-factor. It's Hooke's Law. No it's pulley effect. You're wrong. I'm right. It's a nitter! No, it's a natter! Sheesh! Well, boys, I think the OP's reality check is refreshing and informative. But there's them that can, and there's them that criticize. Now shut up, watch, and learn something. So there! -- --
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ptlong2
Mar 14, 2012, 10:16 PM
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boadman wrote: For the climber at the instant he came to rest, the force would be: -kx = mg Boadman, the maximum force doesn't occur when the climber comes to rest. In fact, with just Hooke's Law (no damping) the climber never comes to rest. The point of equilibrium you are thinking of would be if a climber were gently set onto the rope, no fall at all. If he instead falls, even FF=0, he will fall past the point of equilibrium where x=mg/k and stretch the rope further. It's easy enough to calculate. If the climber falls a distance x the potential energy is mgx. This has to equal the potential energy of the rope which is 1/2*k*x^2. Solve for x and you have x=2mg/k. So, F=kx=2mg.
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boadman
Mar 14, 2012, 10:28 PM
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That makes sense, thanks.
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skurdeycat
Mar 15, 2012, 1:07 AM
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jt512 wrote: skurdeycat wrote: Good lord. There isn't a single post is this thread that is completely accurate, except perhaps the OP, and the one linking to rgold. I don't know where to start. Nor where to stop, unfortunately for you. In reply to: Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). There is no friction, rope elongation, pulley effect, nothing else to consider. No friction? I think you need to think that through a little more. In reply to: aargh, you folks scare me. Is that your best pirate voice? At least it's better than your physics. Jay Shoot, one missing word and I'm proof of my own statement. Hanging on toprope (the climber and belayer have stopped, the calculus fun is over), the MAXIMUM possible force on the anchor is the weight of everything hanging from it. I sincerely do appreciate the work you guys do and share here, but sometimes the original question wasn't complicated, and the answer isn't either.
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loginatnine
Mar 15, 2012, 2:16 AM
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ptlong2 wrote: It's easy enough to calculate. If the climber falls a distance x the potential energy is mgx. This has to equal the potential energy of the rope which is 1/2*k*x^2. Solve for x and you have x=2mg/k. So, F=kx=2mg. Your analysis here is valid for a FF=0 where the rope stretch will be equal to the fall height. That's x in your equation. In a real fall, it will be something like mg(H+x) = 1/2*k*x^2 where x is the rope stretch and H is the length of the fall before the climber is catch by the rope.
(This post was edited by loginatnine on Mar 15, 2012, 2:18 AM)
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USnavy
Mar 15, 2012, 5:34 AM
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jt512 wrote: The three figure shows the peak at about 40, 22, and 11, respectively. Can you clarify what the units of the horizontal axes are in each of the figures, and explain why peak occurs at different values? Jay Those units were chosen for me by Excel and I cant figure out how to change them. Anyway, they are row numbers. Because the strain gauge conditioner software creates a new row every 10mS, those units also represent time. Specifically, they are the duration multiplied by ten. So if you are looking at the waveform and notice a particular point starts out at say 30 and ends at say 60, that means it covered 300mS total. The reason why the peaks are at different intervals is because Excel uses the starting row number from the dataset I selected as one, not the start of the entire dataset. The entire dataset has over 150,000 points, so scroll through the data to the dataset that’s relevant to the fall I want to view, and I graph just the points I want. So for example, the data I want may land in rows 120,000 – 121,000. So when I chart out the rows in 120k - 121k, the graph shows 1 - 1,000 instead of 120k-121k because I only selected 1,000 rows. This is an example of the dataset that exists in the .csv file generated by my strain gauge conditioner software: 730321 347.9256 730331 350.5929 730341 355.9004 730351 365.2213 730361 374.1467 730371 377.9456 730381 380.442 730391 383.4596 730401 388.9277 730411 394.7827 730421 401.5505 730431 407.5202 730441 414.8244 730451 422.0302 730461 425.8789 730471 428.9844 730481 433.2427 730491 434.0447 730501 438.4572 The number on the left indicate the time stamp, in mS, generated by the strain gauge software. The numbers on the right are the readings, in lbs. The rows are not listed above. What I am trying to get Excel to do is list the time stamps on the X axis and the load values on the Y axis, but I cant figure out how to get Excel to do this. It wont let me change the X axis values, it forces me to use the row numbers.
LostinMaine wrote: In the future, like Jay points out, your figures need a bit of work. Label all axes for each figure - that little bit of time spent helps to strengthen all of the time spent previously generating data to populate the figures. I'm curious about consistency, though. Have you tried taking the same fall with the same style catch multiple times and plotting the results? I wonder what kind of variance you might find. I would like to, but I don’t know how. I am kind of an Excel noobie, I don’t use the program that much. If you can tell me how to label the axis’s, I will change them. Yes I have tried taking multiple falls. Here is a graph of the entire data set (150,000+ points!), including all the falls I took yesterday: However, keep in mind, they were not all of the same catch type. Some of the falls were identical, but I was changing the catch types and fall distances, so its not accurate data. I will answer your question in further detail at the end of this post.
MFC wrote: Next time you run some tests, could you measure the peak load from a fall factor=zero fall on a top rope? Thanks. I look forward to further test results. Yes I can, later. That’s already somewhat related to a plan I have. I intend to test the differences in impact force between low and high elongation ropes when the climber takes a rope stretch only lead fall (such as in the case of aid climbing).
healyje wrote: I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts. There is to the left, in the dihedral. The dihedral is a trad route; however that’s a separate route. The sport route climbs the aręte. This is just a noob climbing area, its short and the routes are easy, the FA just wanted to make a playground for the kids to play on, sorta speak. Anyway, this post marks the start of a detailed and complex study I would like to make regarding the impact forces related on lead falls. Today I went out and took some real lead falls on the load cell and captured some data. I will make another post about that later. But there is a lot I need to do. I want to compare soft and hard catches, low and high fall factors, high and low elongation ropes, heavy and light climbers, and highline falls. Then I want to compare everything to each other, in a thesis paper and on video. However that’s going to takes hundreds of hours of research and testing and countless lead falls, so it will take some time. It is also going to be rather tricky to isolate all the variables to get accurate results. I have to measure out the rope and fall distance every time to calculate the true fall factor, I have to retie the knot after each fall, I have to let the rope rest, I have to isolate belay device slippage and take into account rope drag, the list goes on and on and on of variables that have to be isolated to be able to truly compare lead falls in a synthesized setting. But first I need to understand what I am looking at in the graphs. Specifically I need to figure out how to determine when the fall is fully arrested so I can accurately calculate how long the fall duration is. There is also another issue that I don’t understand, I will explain that problem in the next thread that includes data on lead falls.
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guangzhou
Mar 15, 2012, 9:34 AM
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Very happy people like you enjoy this stuff, it means I will never have to. Instead, I can spend all those hours climbing. Eman
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skurdeycat
Mar 15, 2012, 11:57 AM
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You are probably using the Line Chart in Excel, if you use the scatter plot (choose the scatter option with lines and no markers) then Excel should plot the x-axis the way you want. While it wouldn't matter in this case, a Line Chart assumes all x-axis readings are equally spaced, a scatter plot will properly space them. In Office 2007 or later, to add axes titles, click on the chart and go to the Layout tab on the Ribbon.
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LostinMaine
Mar 15, 2012, 4:06 PM
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So you don't waste your time, do you know a statistician that you can talk to... or anyone who has taken a sampling design course? You want replication of each fall type and each catch type to get any useful conclusion. My suspicion is that because of friction in the system and the "real-world" nature of the testing you will get some funky impact force outliers that will need to be balanced by a fair number of replicates (within each fall-catch category). Otherwise, you will do all of this and not get much useful other than some cool figures to consider. As a side, if you PM me a link to your CSV file, I can make some figures for you.
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cracklover
Mar 15, 2012, 6:12 PM
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jt512 wrote: cracklover wrote: I'm just curious - why would you want to embarrass yourself by putting this in print? I hope that wasn't all you got, because you need something left for skurdeykat. Jay I don't see why. I assume you're talking about this post:
skurdeycat wrote: Hanging without bouncing on toprope, the force on the ANCHOR is the sum of the weight of the belayer, the climber, the rope and if you want to be really picky, the masterpoint biner(s). There is no friction, rope elongation, pulley effect, nothing else to consider. If the climber or belayer is touching the rock or ground, the force will be less. ... it may be the "wrong" question he's answering, it may even be misleading, but it's not substantively incorrect. What I found so puzzling in amarius' post was his proud parade of his own ignorance, as if it was a bright shining flag to rally around. Skurdy, otoh, is just making a factual statement: At rest, climber weight plus belayer weight, assuming both are hanging, equals force on the anchor. True, this is not a particularly enlightening point, but it's nothing to be embarrassed about. G
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camhead
Mar 15, 2012, 6:21 PM
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guangzhou wrote: Very happy people like you enjoy this stuff, it means I will never have to. Instead, I can spend all those hours climbing. Eman Yes. I'll never understand the obession with gear, though if you're into it, more power to you. I'm just thinking of this line, however, in an article that's been going around about different climbing types, in which it describes the "Widgeteer":
In reply to: Ironically, though Widgeteers are well-versed in the intricacies of load distribution, impact force, and lobe geometry, they rarely have as keen a grasp of the physiological techniques of climbing itself.
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jt512
Mar 15, 2012, 7:20 PM
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USnavy wrote: jt512 wrote: The three figure shows the peak at about 40, 22, and 11, respectively. Can you clarify what the units of the horizontal axes are in each of the figures, and explain why peak occurs at different values? Jay Those units were chosen for me by Excel and I cant figure out how to change them. Anyway, they are row numbers. Because the strain gauge conditioner software creates a new row every 10mS, those units also represent time. Specifically, they are the duration multiplied by ten. So if you are looking at the waveform and notice a particular point starts out at say 30 and ends at say 60, that means it covered 300mS total. The reason why the peaks are at different intervals is because Excel uses the starting row number from the dataset I selected as one, not the start of the entire dataset. The entire dataset has over 150,000 points, so scroll through the data to the dataset that’s relevant to the fall I want to view, and I graph just the points I want. So for example, the data I want may land in rows 120,000 – 121,000. So when I chart out the rows in 120k - 121k, the graph shows 1 - 1,000 instead of 120k-121k because I only selected 1,000 rows. This is an example of the dataset that exists in the .csv file generated by my strain gauge conditioner software: 730321 347.9256 730331 350.5929 730341 355.9004 730351 365.2213 730361 374.1467 730371 377.9456 730381 380.442 730391 383.4596 730401 388.9277 730411 394.7827 730421 401.5505 730431 407.5202 730441 414.8244 730451 422.0302 730461 425.8789 730471 428.9844 730481 433.2427 730491 434.0447 730501 438.4572 The number on the left indicate the time stamp, in mS, generated by the strain gauge software. The numbers on the right are the readings, in lbs. The rows are not listed above. What I am trying to get Excel to do is list the time stamps on the X axis and the load values on the Y axis, but I cant figure out how to get Excel to do this. It wont let me change the X axis values, it forces me to use the row numbers. You should convert the timestamp in Excel to a meaningful 0-based time unit and redo the figures so that the horizontal axis is time. You need to do an X–Y scatterplot, and your data range should be the two columns of data: time and force. It's been a long time since I've used Excel, but if it still (mal)functions the way it used to, if you put the variable names in the first row of each column in your dataset and include that rowin the data range for the figure, Excel will use them as axis labels automatically. (Don't skip a row between the variable names and the data.) If not, you can edit the axis lables manually, as Skurdeykat explained. Jay
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jt512
Mar 15, 2012, 7:24 PM
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USnavy wrote: healyje wrote: I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts. [T]he FA just wanted to make a playground for the kids to play on, sorta speak. Does anybody know how to air-pop popcorn?
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njrox
Mar 15, 2012, 7:32 PM
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camhead wrote: Yes. I'll never understand the obession with gear, though if you're into it, more power to you. I'm just thinking of this line, however, in an article that's been going around about different climbing types, in which it describes the "Widgeteer": Ironically, though Widgeteers are well-versed in the intricacies of load distribution, impact force, and lobe geometry, they rarely have as keen a grasp of the physiological techniques of climbing itself. haha, great link!
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miklaw
Mar 15, 2012, 10:46 PM
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Anyway, good work and congrats for doing something. Falling from the top rope anchor with 12' of slack, falling 12' (then rope strech adding another 8' to amke 20' of distance all up) is the same as a lead fall from 6' above the belay; they are both factor 0.24 falls. 3 kN is about the ballpark figure bandied around fro a hard sport fall. At that level light belayers will be up at the first draw, did you tie down? (and how come you guys are so light, don't you know that's cheating?) mikl
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TonyB3
Mar 19, 2012, 7:51 PM
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So USFlotsam has bought an expensive toy to replicate tests that have been conducted by myriad professional institutions with engineers capable of analyzing the data. Woo! The OP is worthless because of the lack of any sort of comprehensive analysis or controls. All he wants is to fool some n00b into thinking he is some sort of expert, when in fact nothing could be further from the truth.
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blueeyedclimber
Mar 19, 2012, 8:09 PM
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jt512 wrote: USnavy wrote: healyje wrote: I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts. [T]he FA just wanted to make a playground for the kids to play on, sorta speak. Does anybody know how to air-pop popcorn? I can do that, as long as it doesn't involve math or excel spreadsheets. Josh
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chadnsc
Mar 19, 2012, 8:38 PM
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blueeyedclimber wrote: jt512 wrote: USnavy wrote: healyje wrote: I find it a bit hard to believe there isn't decent pro to be had below or to the left of both these bolts. [T]he FA just wanted to make a playground for the kids to play on, sorta speak. Does anybody know how to air-pop popcorn? I can do that, as long as it doesn't involve math or excel spreadsheets. Josh You're screwed Josh, good air-popped popcorn involves both math and an excel spreadsheet.
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guangzhou
Mar 25, 2012, 9:01 AM
Post #48 of 51
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I am amazed this was made a sticky. Really, is RC.com getting desperate. Really should let this get buried before people think the OP actually knows what his doing and talking about.
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majid_sabet
Mar 25, 2012, 3:43 PM
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good work commando,( assuming you really did this yourself and did not fool someone else to do it for you). next time you are in the valley, stop by and I'll get you a free coffee at the lodge. what brand was the load cell and the receiver ( does it offer serial or USB output )?
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USnavy
Mar 26, 2012, 6:57 AM
Post #51 of 51
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majid_sabet wrote: good work commando,( assuming you really did this yourself and did not fool someone else to do it for you). next time you are in the valley, stop by and I'll get you a free coffee at the lodge. what brand was the load cell and the receiver ( does it offer serial or USB output )? The conditioner is made by Mantracourt, it is called the DSCUSB. http://www.mantracourt.co.uk/products/signal-converters/usb-load-cell-converter The load cell is from AnyLoad in Canada, its a 5000 lbs. alloy cell, standard issue, nothing special. It has a USB connection, but it communicates using a serial interface, not that it really matters. For all intents and purposes, it is a USB device. I will be in the Valley in June and I will come seek you out if you are there.
(This post was edited by USnavy on Mar 26, 2012, 7:09 AM)
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