
shockabuku
Jul 13, 2011, 6:02 AM
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Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor?





notapplicable
Jul 13, 2011, 7:00 AM
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I was wondering about that the other day as well.





j_ung
Jul 13, 2011, 7:06 AM
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I'm probably about to show my ignorance of all things physics, but things being equal, I would expect it not to change at all. Curious to hear an actual answer.





shockabuku
Jul 13, 2011, 7:18 AM
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j_ung wrote: I'm probably about to show my ignorance of all things physics, but things being equal, I would expect it not to change at all. Curious to hear an actual answer. Ideally, it shouldn't. But, life being less than ideal...





puravida9539
Jul 13, 2011, 8:15 AM
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The climber's speed will be greater with the longer falls, so I would assume that would raise the force. However, the longer the amount of rope, the greater effect the dynamic properties of the rope will have. However, for a fall on static gear the distance would make a huge amount of difference. For a fall on static gear, there is nothing to absorb the extra distance/speed. Farther fall = faster fall = harder impact.





sungam
Jul 13, 2011, 8:28 AM
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shockabuku wrote: j_ung wrote: I'm probably about to show my ignorance of all things physics, but things being equal, I would expect it not to change at all. Curious to hear an actual answer. Ideally, it shouldn't. But, life being less than ideal... Well, the average acceleration before the catch started would be higher for the shorter fall then for the longer fall, since the longer fall reaches higher speeds and thus air resistance becomes less negligible. Dunno how that would carry through, though.





cracklover
Jul 13, 2011, 9:13 AM
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shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO





cracklover
Jul 13, 2011, 9:16 AM
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puravida9539 wrote: The climber's speed will be greater with the longer falls, so I would assume that would raise the force. However, the longer the amount of rope, the greater effect the dynamic properties of the rope will have. However, for a fall on static gear the distance would make a huge amount of difference. For a fall on static gear, there is nothing to absorb the extra distance/speed. Farther fall = faster fall = harder impact. Look up Fall Factor. GO





cracklover
Jul 13, 2011, 10:01 AM
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For example, this study found that "The Figure8 follow through knot absorbs an equivalent of nearly 1.5 meters of rope." http://amga.com/...al_Failure_Paper.pdf Assuming for the moment that it was that simple*, what would that mean in practice? Let's say you fall five feet with ten feet of rope out. A simple calculation would say that you would have a FF 0.5 fall. If we want to put some hard numbers on it, we could us Jay's calculator to say that the top piece would feel 9.6kN. Now let's include that equivalent 1.5 meters for rope tightening. That means you effectively fall five feet on fifteen feet of rope, reducing the FF to .33. Our "improved" model, including knottightening, now says the top piece would feel 8.2kN. So adding the knot tightening reduces the peak force by 1.4 kN, or 15% Now what if we look at a longer fall with the same fall factor? Let's say you fall ten feet with twenty feet of rope out. Again, FF = .5, which gives us a simple number of 9.6kN on the top piece. Now when we include that 1.5m (or 5 feet) of knot tightening to get an "improved" FF, we get 10/25, or ff = 0.4, or 8.8kN. So for the longer fall, the knot only reduced the peak load by 0.8kN, or 8%. This is because as you fall farther, for a given fall factor, all the rope available to absorb the fall increases except the rope in your knot. So the farther you fall, the less the knot tightening will help. The same is true for all the other small factors (stretching runners, body deformation, etc). Hope that makes sense to all? GO * Evidence from other studies suggests it's slightly more complex: http://web.mit.edu/...d_order_rope_fit.pdf





shockabuku
Jul 13, 2011, 11:15 AM
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cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though.





redlude97
Jul 13, 2011, 11:20 AM
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Some other practical points, with more rope out in general the rope drag increases which in turn increases the effective "fall factor" by decreasing the effective rope out in the system because of friction limiting the rope stretch on the belayer side. This in general increases the total force felt by the top piece.





cracklover
Jul 13, 2011, 12:16 PM
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Redlude  true. Your factor and mine will both are in the same direction, so it seems that longer falls will produce higher effective peak forces, for a given FF.
shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Not sure what you're getting at, then. All other factors being ignored, peak force is simply predicted by the fall factor and the rope modulus. To the best of my knowledge, to the degree that other factors are either eliminated or integrated, the measurements bear this out. GO





Rudmin
Jul 13, 2011, 1:07 PM
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Instead of putting the screamer on every piece, why not just connect the screamer to the climber? Between the harness and the rope. It can be backed up with slack rope if need be.





cracklover
Jul 13, 2011, 2:03 PM
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shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Let me put it another way. The kinetic energy of a falling body is the force of gravity on that object times the distance it falls. IOW, kinetic energy is directly proportional to fall distance. IOW, you can say that for any object, the energy is equal to the fall distance times a constant. So, if FF is fall distance / rope, then for a given FF, the rope is always proportional to the fall distance, which is proportional to the energy. So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ignoring air resistance and friction and all that jazz, the rope puts the same peak force on your gear for any given FF. Make sense? GO





shockabuku
Jul 14, 2011, 7:24 AM
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cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Let me put it another way. The kinetic energy of a falling body is the force of gravity on that object times the distance it falls. IOW, kinetic energy is directly proportional to fall distance. IOW, you can say that for any object, the energy is equal to the fall distance times a constant. So, if FF is fall distance / rope, then for a given FF, the rope is always proportional to the fall distance, which is proportional to the energy. So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ignoring air resistance and friction and all that jazz, the rope puts the same peak force on your gear for any given FF. Make sense? GO I understand most of what you're saying. I would still like to see some data on a case where these other factors aren't involved. Strictly speaking you're confusing potential energy (mgh) with kinetic energy (.5mv^2). This I don't understand "the rope is always proportional to the fall distance, which is proportional to the energy." This statement "So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ..." seems only to lead to this conclusion "the rope puts the same peak force on your gear for any given FF." if the rope is in a linear force vs. distance relationship. I suspect that breaks down with greater fall factors, but I don't know for sure.
(This post was edited by shockabuku on Jul 14, 2011, 7:40 AM)





cracklover
Jul 14, 2011, 9:01 AM
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shockabuku wrote: cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Let me put it another way. The kinetic energy of a falling body is the force of gravity on that object times the distance it falls. IOW, kinetic energy is directly proportional to fall distance. IOW, you can say that for any object, the energy is equal to the fall distance times a constant. So, if FF is fall distance / rope, then for a given FF, the rope is always proportional to the fall distance, which is proportional to the energy. So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ignoring air resistance and friction and all that jazz, the rope puts the same peak force on your gear for any given FF. Make sense? GO I understand most of what you're saying. I would still like to see some data on a case where these other factors aren't involved. Strictly speaking you're confusing potential energy (mgh) with kinetic energy (.5mv^2). I am? How so? The kinetic energy, ignoring air resistance, is exactly related to distance fallen.
In reply to: This I don't understand "the rope is always proportional to the fall distance, which is proportional to the energy." Okay, let's take FF = 1. If we double the distance fallen, we double the amount of rope, right? With me so far? And would you agree that for every other FF that holds true? That takes care of the first two thirds of that sentence: "the rope is always proportional to the fall distance". Then if you also agree that that the kinetic energy is equal to the fall distance times a constant.... It must be that "the rope is always proportional to the fall distance, which is proportional to the energy." IOW, as long as you don't change gravity, the springiness of the rope, the fall factor, or the mass of the climber, the energy of the climber will always vary in exact proportion to the amount of rope available to catch the fall.
In reply to: This statement "So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ..." seems only to lead to this conclusion "the rope puts the same peak force on your gear for any given FF." if the rope is in a linear force vs. distance relationship. I suspect that breaks down with greater fall factors, but I don't know for sure. What do you mean "a linear force vs distance relationship"? The question is simply this: If you ask twice the length of rope to dissipate twice the amount of energy, how can it know there is any difference? As far as the rope is concerned, it is doing exactly the same amount of work per inch. GO





jt512
Jul 14, 2011, 9:17 AM
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ptlong2 wrote: shockabuku wrote: I would still like to see some data on a case where these other factors aren't involved. These data are taken from a paper by Martyn Pavier. The selected drops were performed with a 70kg steel mass and the belay was tied off. It appears that with the "other factors" removed the length of fall has no significant effect on maximum tension, at least over this limited range. For real life falls I would wonder about the effects of belay device and belayer behavior. Maybe I'm missing something, but that chart of the Pavier data doesn't seem to address the original question—what is the relationship between the fall length and the maximum impact force for a given fall factor—very well. The only fall factor where we have data for multiple fall lengths is 1.00. Here the impact force increases slightly as the fall length increases from 1 to 2 m. However, at FF = 0.90 there appear to be three drops of the same length, whose range of impact forces appears to be about the same as the range at FF = 1.00, so what could be interpreted as an increasing relationship here could be due to random error. It seems like what we need in order to answer the original question is a dataset with multiple drops at a constant fall factor over a greater range of fall lengths. Edit: Is the impact force in the chart for the "climber's" side of the rope? Have you compared the Pavier data to that predicted by the "standard" model? Do you know the rope modulus or impact force rating of the rope? Jay
(This post was edited by jt512 on Jul 14, 2011, 9:25 AM)





cracklover
Jul 14, 2011, 10:02 AM
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Looks to me like at approx FF1, there are four data points, each of which, within a small error factor, show the same force. Edited to add, at FF 0.85, there are also two data points showing the same thing. BTW, this appears to be a link to the data referenced above: http://personal.strath.ac.uk/...w.mclaren/Pavier.pdf (see table 2) GO
(This post was edited by cracklover on Jul 14, 2011, 10:13 AM)





cracklover
Jul 14, 2011, 10:42 AM
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Hmm... in the experimental method used "the rope was tied to the trolley." So the knot *should* have an affect. Which means that longer drops should, according to what I stated earlier, give a slightly higher peak force. However, there is this: "Table 2 provides results of the number of fallstofailure and the maximum tension recorded in the rope..." That "maximum tension" could be interpreted in either of two ways, either the peak force, averaged over the course of the multiple drops it took to break the rope, or the highest peak force measured over the course of drops required to break the rope. If it's the latter, then the force listed in the chart for each data point is only the force from the one fall in which the knot was mostly tensioned after several drops, since the peak force would increase as the knot gets set tighter. GO





shockabuku
Jul 14, 2011, 1:27 PM
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cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Let me put it another way. The kinetic energy of a falling body is the force of gravity on that object times the distance it falls. IOW, kinetic energy is directly proportional to fall distance. IOW, you can say that for any object, the energy is equal to the fall distance times a constant. So, if FF is fall distance / rope, then for a given FF, the rope is always proportional to the fall distance, which is proportional to the energy. So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ignoring air resistance and friction and all that jazz, the rope puts the same peak force on your gear for any given FF. Make sense? GO I understand most of what you're saying. I would still like to see some data on a case where these other factors aren't involved. Strictly speaking you're confusing potential energy (mgh) with kinetic energy (.5mv^2). I am? How so? The kinetic energy, ignoring air resistance, is exactly related to distance fallen. Kinetic energy is the energy of motion  it starts out as zero when the fall begins and grows as the climber's speed of fall increases. The maximum kinetic energy will not be equal to the original potential energy because the climber starts to slow down as the rope begins to get tight. There is gravity pulling down and the rope pulling up at the same time while the climber is slowing to a stop. I think what you mean to say is correct, that the total energy for the rope to absorb or dissipate is the potential energy which is determined by total fall length.
In reply to: In reply to: This I don't understand "the rope is always proportional to the fall distance, which is proportional to the energy." Okay, let's take FF = 1. If we double the distance fallen, we double the amount of rope, right? With me so far? And would you agree that for every other FF that holds true? That takes care of the first two thirds of that sentence: "the rope is always proportional to the fall distance". Then if you also agree that that the kinetic energy is equal to the fall distance times a constant.... It must be that "the rope is always proportional to the fall distance, which is proportional to the energy." IOW, as long as you don't change gravity, the springiness of the rope, the fall factor, or the mass of the climber, the energy of the climber will always vary in exact proportion to the amount of rope available to catch the fall. I didn't understand that you meant the length of rope.
In reply to: In reply to: In reply to: This statement "So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ..." seems only to lead to this conclusion "the rope puts the same peak force on your gear for any given FF." if the rope is in a linear force vs. distance relationship. I suspect that breaks down with greater fall factors, but I don't know for sure. What do you mean "a linear force vs distance relationship"? The springiness of the rope  I was talking about if it changes due to being overstretched. I don't know if all ropes stay in the linear regime up through factor two falls for all amounts of falling mass. If not, your argument breaks down. The linear spring model (force=constant*change in length) for a rope only works for a certain percentage of stretch of the rope. So long as this model holds then for every additional foot of stretch there is the same additional amount of associated tension in the rope. Beyond the linear range (hard fall), for the same amount of stretch, the added tension in the rope grows nonlinearly  maybe like force=constant*(change in length)^2. This means each additional foot of stretch incurs a greater additional tension than the last foot.





cracklover
Jul 14, 2011, 2:44 PM
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shockabuku wrote: cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: cracklover wrote: shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? Yes, all other things being equal, the longer fall will have a slightly higher peak force. The reason for that is simple. Aside from the rope, there are a lot of other things that can "absorb" some energy, such as the sling on the top piece, the climber's body, and most importantly, the knot tightening. But each of these can absorb a set amount of energy, and unlike the rope, they don't scale with the length of fall. A small fall will have a smaller amount of kinetic energy that must be "absorbed", and a larger fraction of that will be absorbed by those various other items, leaving a smaller fraction for the rope, and thus a smaller impact force on the top piece. In a large fall, the overall percent of the energy they can convert to heat is much smaller relative to the total amount of kinetic energy, so the rope must absorb essentially all of the energy, putting a higher force on the top piece of gear. I've only seen one study that looked at how much energy the knot could absorb. Practically speaking, for falls over say ten or fifteen feet, I don't think it made much difference, but if you like I can try to track down that study for you. GO You bring up some practical points that I hadn't considered though I'm still interested in the case where those factors are negligible (lab case). I was asking this question because of the thread about Screamers. It linked to some BD research on Screamers that did some test falls of two different fall factors onto different types of slings, screamers, etc. They didn't vary the fall length within the same fall factor though. Let me put it another way. The kinetic energy of a falling body is the force of gravity on that object times the distance it falls. IOW, kinetic energy is directly proportional to fall distance. IOW, you can say that for any object, the energy is equal to the fall distance times a constant. So, if FF is fall distance / rope, then for a given FF, the rope is always proportional to the fall distance, which is proportional to the energy. So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ignoring air resistance and friction and all that jazz, the rope puts the same peak force on your gear for any given FF. Make sense? GO I understand most of what you're saying. I would still like to see some data on a case where these other factors aren't involved. Strictly speaking you're confusing potential energy (mgh) with kinetic energy (.5mv^2). I am? How so? The kinetic energy, ignoring air resistance, is exactly related to distance fallen. Kinetic energy is the energy of motion  it starts out as zero when the fall begins and grows as the climber's speed of fall increases. The maximum kinetic energy will not be equal to the original potential energy because the climber starts to slow down as the rope begins to get tight. There is gravity pulling down and the rope pulling up at the same time while the climber is slowing to a stop. I think what you mean to say is correct, that the total energy for the rope to absorb or dissipate is the potential energy which is determined by total fall length. How is that different from what I did say? When calculating fall factor, you look at the distance the climber fell before the rope starts to catch.
In reply to: In reply to: In reply to: In reply to: This statement "So if you agree that any given section of rope should be able to absorb X amount of energy in the same way that double the amount of rope would absorb double the energy, then, ..." seems only to lead to this conclusion "the rope puts the same peak force on your gear for any given FF." if the rope is in a linear force vs. distance relationship. I suspect that breaks down with greater fall factors, but I don't know for sure. What do you mean "a linear force vs distance relationship"? The springiness of the rope  I was talking about if it changes due to being overstretched. I don't know if all ropes stay in the linear regime up through factor two falls for all amounts of falling mass. If not, your argument breaks down. The linear spring model (force=constant*change in length) for a rope only works for a certain percentage of stretch of the rope. So long as this model holds then for every additional foot of stretch there is the same additional amount of associated tension in the rope. Beyond the linear range (hard fall), for the same amount of stretch, the added tension in the rope grows nonlinearly  maybe like force=constant*(change in length)^2. This means each additional foot of stretch incurs a greater additional tension than the last foot. I think you are confused. For a given FF, a rope will always stretch the same amount per foot of rope. GO





cracklover
Jul 14, 2011, 3:11 PM
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This seems to be the problem:
shockabuku wrote: The springiness of the rope  I was talking about if it changes due to being overstretched. I don't know if all ropes stay in the linear regime up through factor two falls for all amounts of falling mass. If not, your argument breaks down. I don't know what, exactly, you think I am saying is linear, but I'm pretty sure you're referring to something else. So let me clarify. Ignoring the other factors such as knot tightening, for a given fall factor, a given rope will always stretch the same percentage. That's because the ratio between kinetic energy and rope will be constant. And it's precisely the percent stretch in the rope that gives you the force on the gear, which is why that force is (again, ignoring those other factors) always constant (for a given rope, fall factor, and mass.)
In reply to: The linear spring model (force=constant*change in length) for a rope only works for a certain percentage of stretch of the rope. So long as this model holds then for every additional foot of stretch there is the same additional amount of associated tension in the rope. Beyond the linear range (hard fall), for the same amount of stretch, the added tension in the rope grows nonlinearly  maybe like force=constant*(change in length)^2. This means each additional foot of stretch incurs a greater additional tension than the last foot. Yes, this paper I referenced earlier: http://web.mit.edu/...d_order_rope_fit.pdf discusses that, if you're interested. But I don't see how that has any bearing on the topic. GO





ptlong2
Jul 14, 2011, 5:23 PM
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jt512 wrote: Maybe I'm missing something, but that chart of the Pavier data doesn't seem to address the original question—what is the relationship between the fall length and the maximum impact force for a given fall factor—very well. You're right, it doesn't demonstrate it very well. But I was reasoning that because the data show a linear relationship between fall factor and maximum tension, regardless of fall length, they support the notion that fall length doesn't matter (in this circumstance). The fact that longer fall lengths appear for both higher and lower fall factors bolsters the argument. But it is still somewhat weak.
In reply to: Edit: Is the impact force in the chart for the "climber's" side of the rope? Have you compared the Pavier data to that predicted by the "standard" model? Do you know the rope modulus or impact force rating of the rope? It's the rope tension, hence the climber's side. The model does not have a single modulus; rather there are two moduli and a damping constant. But I believe one still gets a linear FF to max tension relationship from the model so one could come up with an effective modulus for this purpose. It would be something around 25 kN.





jt512
Jul 14, 2011, 6:46 PM
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ptlong2 wrote: jt512 wrote: Maybe I'm missing something, but that chart of the Pavier data doesn't seem to address the original question—what is the relationship between the fall length and the maximum impact force for a given fall factor—very well. You're right, it doesn't demonstrate it very well. But I was reasoning that because the data show a linear relationship between fall factor and maximum tension, regardless of fall length, they support the notion that fall length doesn't matter (in this circumstance). The fact that longer fall lengths appear for both higher and lower fall factors bolsters the argument. But it is still somewhat weak. Interestingly, there appears to be an interaction between fall length and fall factor in the data. I'll expand upon that in my next post. Jay





jt512
Jul 14, 2011, 7:15 PM
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I have analyzed all the data in Table 2 in the Pavier paper (from which ptlong2's figure was apparently derived) for which the belay connection was tied off (N=27), in order to investigate whether there is a relationship between fall length and maximum impact force after the the effect of the fall factor is accounted for. There is such a relationship (at least in this dataset), and surprisingly, it's nonlinear. Method: I used multiple linear regression models with maximum impact force as the dependent variable. In the first model, I included as independent variables fall factor, fall length, mass, and carabiner radius (which was coded as a 3level factor to allow for a possible nonlinear relationship with impact force). Regression diagnostics strongly suggested a nonlinear effect of fall length on impact force. To account for this I ran a second model in which I added a term for an interaction between fall length and fall factor. Carabiner radius was not significantly associated with impact force, and excluding if from the model had essentially no effect on the results, and so, for simplicity, I excluded it from the final model. Results: The initial model assumed that if there was an independent relationship between impact force and fall length after controlling for fall factor, mass, and carabiner radius, that the relationship would be linear. Although this model seemed to fit the data well (adjusted Rsquare=0.984), regression diagnostics indicated that there was a nonlinear relationship between fall length and fall factor, and so a linear model was not appropriate. The following figure shows these regression diagnostics (click to enlarge). The panels show excellent linear relationships with impact force for fall factor and mass, but not for fall length (bottom right quadrant). The linear model (red dashed line) overestimates the impact force when the fall length is low or high, and underestimates the impact force when the fall length is intermediate. This implies that a model in which fall length had a quadratic relationship with impact force independent of the fall factor would be a better fit to the data. But this seems nonsensical. It would mean that, for a given fall factor, both short and long falls would have lower impact forces than middlesized falls. A more plausible explanation is that the effect of fall length on impact force depends on the fall factor itself, and thus the model should include a term to account for an interaction between fall length and fall factor. The regression diagnostics for this interaction model are shown below (click to enlarge). Comparing these diagnostic plots with those for the strictly linear model shows the fit is improved for all variables. The fits for mass and fall factor, which were quite good in the linear model, are now essentially perfect, and the fits for fall length (lower left) and the interaction between fall length and fall factor (lower right) are excellent. This model also improved the adjusted Rsquare to 0.997. The final fitted regression model is: impact force = –1.29 + 0.0523*mass + 4.23*ff + 0.353*length – 0.335*length*ff where mass is in kg, "length" is the length of the fall in meters, and ff is the fall factor. The last term in the model represents the interaction between length and fall factor. All regression coefficients were highly significant (P < 0.00001). The following scatter plot of the observed and modelpredicted impact force vs. fall factor shows how well the model fits the data (click to enlarge). Notice how close the predicted values (red circles) are to the observed values (black discs). To better understand the interaction between fall length and fall factor, that is, how the effect of fall length on impact force depends on the fall factor, we can factor out the fall length from the last two terms in the previous equation. Doing so allows us to express the regression equation as impact force = –1.29 + 0.0523*mass + 4.23*ff + (0.353 – 0.335*ff)*length . This shows that the effect of fall length on impact force is a linear function of the fall factor: for each meter of fall length, the impact force is increased by 0.353 kN less 0.335 kN times the fall factor. Since 0.353 is close to 0.335, the effect of fall length on impact force reverses at a fall factor of about 1. For fall factors less than 1, the longer the fall length, the higher the impact force; for fall factors greater than 1, the longer the fall length, the lower the impact force. Limitations: In a small dataset such as this, model overfitting is a risk. The results should be considered food for thought rather than definitive. Conclusion: In this dataset, fall length had a significant nonlinear relationship with maximum impact force after the effects of fall factor and falling mass were taken into account. This nonlinearity can be modeled as an interaction between fall length and fall factor in which, for fall factors less than 1, the longer the fall is, the higher the impact force is; and for fall factors greater than 1, the longer the fall is, the lower the impact force is. These results should be interpreted with caution due to the limited number of data points available for analysis. Jay
(This post was edited by jt512 on Jul 14, 2011, 8:58 PM)





dagibbs
Jul 14, 2011, 7:37 PM
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Thanks for the very thorough analysis, Jay.





shockabuku
Jul 15, 2011, 7:12 AM
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Thanks for the analysis. Unfortunately I can't see your plots right now  I think your server is down. I wonder if the results have to do with friction at the biner (top piece) not allowing the belay side of the rope to interact as well as the climber's side.





cracklover
Jul 15, 2011, 8:29 AM
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Jay, you lost me at one of your early graphs. Could you explain what you're plotting in this one labeled Component+Residual(force) by Length? Thanks! GO





jt512
Jul 15, 2011, 9:07 AM
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cracklover wrote: Jay, you lost me at one of your early graphs. Could you explain what you're plotting in this one labeled Component+Residual(force) by Length? Thanks! GO Each of the "Residual + Component" plots shows the relationship between impact force and the variable on the horizontal axis, after controlling for the effects of all other independent variables in the model. So, what the panel for Length in the first set of plots is showing is that after controlling for the effects of the other terms in the model, the relationship between impact force and fall length is curvilinear. Jay





ptlong2
Jul 15, 2011, 10:33 AM
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Nice work, Jay. I had originally noticed that there seemed to be a trend in the fall length to tension numbers but suspected that it was too small to be above the noise. I'm still not convinced this isn't the case. You may simply have found a nice mathematical fit that has no greater significance. It's hard to say without more data. What physical interpretation is there for a reduced tension with increasing fall length for FF > 1?





jt512
Jul 15, 2011, 11:00 AM
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ptlong2 wrote: Nice work, Jay. I had originally noticed that there seemed to be a trend in the fall length to tension numbers but suspected that it was too small to be above the noise. I'm still not convinced this isn't the case. You may simply have found a nice mathematical fit that has no greater significance. It's hard to say without more data. What physical interpretation is there for a reduced tension with increasing fall length for FF > 1? Beats me. The effect is small, but it's there. The only reason we can see is that there is so little noise in the data. In fact, the data seem almost too good to be true. The effect may have something to do with the design of the experiment, or who knows, it may be real and generalizable to experiments involving solid falling masses with fixed belay. Jay








jt512
Jul 15, 2011, 2:43 PM
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ptlong2 wrote: jt512 wrote: The effect is small, but it's there. The only reason we can see is that there is so little noise in the data. In fact, the data seem almost too good to be true. The effect may have something to do with the design of the experiment, or who knows, it may be real and generalizable to experiments involving solid falling masses with fixed belay. I'll bet it's an artifact of some sort. Here are some more data, taken from a paper that is mostly about static ropes but includes drops with a 10.6mm dynamic. "Fall Factors & Life Safety Ropes: a closer look" Chuck Weber, PMI Quality Manager ITRS 2001 Looking at just the dynamic rope data, there appears to be a nonlinear relation between fall length and impact force, as there was in the Pavier data. In the Pavier data, there were two models that explained the data equally well from a statistical perspective: a quadratic relationship between fall length and impact force that was independent of fall factor, or an interaction between fall length and fall factor. I chose the latter because I thought the former was implausible. Why, given the fall factor, would intermediate length falls produce higher impact forces than both shorter and longer falls? But this is what we see in the PMI data. There is a slight drop off in the impact force for the longest fall in the first three panels. With just fall factor and fall length in the model, the adjusted Rsquared for the PMI data is 0.951. Adding a quadratic term for fall length increases the adjusted Rsquared to 0.963, with a pvalue for the quadratic term of 0.049. So we now have two datasets that show a nonlinear relationship between fall length and impact force that can be modeled as a quadratic effect that is independent of fall factor. Jay





ptlong2
Jul 15, 2011, 4:11 PM
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jt512 wrote: Why, given the fall factor, would intermediate length falls produce higher impact forces than both shorter and longer falls? But this is what we see in the PMI data. There is a slight drop off in the impact force for the longest fall in the first three panels. Maybe, but it could simply be noise. Look at the data for the low stretch ropes. Sometimes one goes up and the other down, then it's reversed for a different case. What is the most likely explanation for that?





jt512
Jul 15, 2011, 4:38 PM
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ptlong2 wrote: jt512 wrote: Why, given the fall factor, would intermediate length falls produce higher impact forces than both shorter and longer falls? But this is what we see in the PMI data. There is a slight drop off in the impact force for the longest fall in the first three panels. Maybe, but it could simply be noise. Look at the data for the low stretch ropes. Sometimes one goes up and the other down, then it's reversed for a different case. What is the most likely explanation for that? I don't know. I don't think we should bring lowstretch ropes into the analysis, either formally or informally. I wouldn't assume a priori that the results of lowstretch ropes should be applicable to dynamic ropes. I suspect that the effect observed in the Pavier data could have something to so with their methodology. As far as I can tell, they performed multiple drops on the same rope until failure, and recorded the highest impact force observed on any of those drops. That's different than performing one drop per rope sample, and recording the maximum impact force. There are likely to be more variables that affect when a rope breaks after multiple drops than affect what the maximum impact force is on a single drop, and therefore I think it's plausible that there could be more a complicated relationship between fall length and impact force in the former case than in the latter. Jay
(This post was edited by jt512 on Jul 16, 2011, 3:13 PM)





ptlong2
Jul 15, 2011, 5:34 PM
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jt512 wrote: ptlong2 wrote: Look at the data for the low stretch ropes. Sometimes one goes up and the other down, then it's reversed for a different case. What is the most likely explanation for that? I don't know. I don't think we should bring lowstretch ropes into the analysis, either formally or informally. I wouldn't assume a priori that the results of lowstretch ropes should be applicable to dynamic ropes. The reason I mentioned it was to suggest that the accuracy of their data is probably not high enough to give too much credence to the slight downturn in in the plots.
In reply to: I suspect that the effect observed in the Pavier data could have something to so with their methodology. As far as I can tell, they performed multiple drops on the same rope until failure, and recorded the highest impact force observed on any of those drops. That's different than performing one drop per rope sample, and recording the maximum impact force. There are likely to be more variables that affect when a rope breaks after multiple drops than affect what the maximum impact force is on a single drop, and therefore I think it's plausible that there could be more a complicated relationship between fall length and impact force in the former case than in the latter. Who knows what Pavier did? Look at Powick's results: there's one case where the first drop peak is lower for the shorter fall but the maximum peak is lower for the longer fall. Do you really find the evidence for a dropoff in tension statistically compelling?





jt512
Jul 15, 2011, 7:44 PM
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ptlong2 wrote: jt512 wrote: ptlong2 wrote: Look at the data for the low stretch ropes. Sometimes one goes up and the other down, then it's reversed for a different case. What is the most likely explanation for that? I don't know. I don't think we should bring lowstretch ropes into the analysis, either formally or informally. I wouldn't assume a priori that the results of lowstretch ropes should be applicable to dynamic ropes. The reason I mentioned it was to suggest that the accuracy of their data is probably not high enough to give too much credence to the slight downturn in in the plots. In reply to: I suspect that the effect observed in the Pavier data could have something to so with their methodology. As far as I can tell, they performed multiple drops on the same rope until failure, and recorded the highest impact force observed on any of those drops. That's different than performing one drop per rope sample, and recording the maximum impact force. There are likely to be more variables that affect when a rope breaks after multiple drops than affect what the maximum impact force is on a single drop, and therefore I think it's plausible that there could be more a complicated relationship between fall length and impact force in the former case than in the latter. Who knows what Pavier did? Look at Powick's results: there's one case where the first drop peak is lower for the shorter fall but the maximum peak is lower for the longer fall. Do you really find the evidence for a dropoff in tension statistically compelling? I haven't really looked at Powick's results. But, at this point, between the Pavier data and the PMI data (including the static and lowelongation rope data), I'd say that the evidence favors the existence of a nonlinear relationship between fall length and impact force after the effect of fall factor is taken into account. Looking at the PMI data, the overall impression is that the effect of fall length decreases as the fall length increases. Whatever is going on in the Pavier data, it isn't random. He has hardly any random error in his data at all. The pattern in the lower right panel in my first set of residual plots is almost certainly a systematic departure from linearity. What caused it, I don't know. It could be systematic error or something meaningful in the context of Pavier's methodology, but not elsewhere. Edit: The residual effect of fall length on impact force was observed because the model wrongly assumed that there should be a linear relationship between maximum impact force and fall factor. See my next post. Jay
(This post was edited by jt512 on Jul 16, 2011, 3:15 PM)





jt512
Jul 16, 2011, 12:38 PM
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ptlong2 wrote: shockabuku wrote: I would still like to see some data on a case where these other factors aren't involved. These data are taken from a paper by Martyn Pavier. The selected drops were performed with a 70kg steel mass and the belay was tied off. It appears that with the "other factors" removed the length of fall has no significant effect on maximum tension, at least over this limited range. For real life falls I would wonder about the effects of belay device and belayer behavior. So, this ^^^^ turned out to be a red herring that sent me on a wild goose chase of mixing metaphors and looking for a residual effect of fall length on impact force. Why would you expect there to be a linear relationship between fall factor and maximum impact force in the first place? The standard relationship is given by where F is the impact force, w is the climber's weight, k is the rope modulus, and r is the fall factor. Pavier's observed impact forces are almost perfectly correlated with the values predicted from this model. Using linear regression, I compared the impact forces observed by Pavier with those predicted by the standard model above (Pavier, Table 2, Belay condition = "tied off", N=27). It was difficult to tell from Pavier's paper what value should be used for the rope modulus k, and the fit depends slightly on the value chosen. Using k = 30.9 (equivalent to a rope with an impact force rating of 10.1 kN), results in a regression coefficient, or slope, of 1 and an intercept of –0.62; in other words, the standard model overestimates the impact force by a constant 0.62 kN. This model almost perfectly fits the data, as assessed by an rsquared value of 0.995. Interestingly, cracklover sent me a copy of an analysis he did that did show a residual effect of fall length after accounting for the impact force explained by the standard model, but I'm not seeing it in my analysis. Jay
(This post was edited by jt512 on Jul 25, 2011, 10:27 PM)

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ptlong2
Jul 18, 2011, 11:46 AM
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jt512 wrote: Why would you expect there to be a linear relationship between fall factor and maximum impact force in the first place? Because it looked linear! It is curious and humbling how both of us were so easily duped by my blunder. We both knew it was a square root relationship. If only we'd taken a moment to look at Figure 1 in your paper on the subject. Sorry for the wild goose chase. It's not all wasted effort though. Your comparison with the standard model might be of interest. We don't have the hang tag specs for the rope which the standard model methodology calls for, but if his data are so good I'm curious why you didn't use Pavier's own 80kg factor 1.77 drop data for the maximum impact force? Since the frictionadjusted model in your paper predicts even higher tensions it could be that by leaving out some other factor it is "correcting" in the wrong direction. Maybe this discrepency is accounted for by Pavier's model. I could have sworn I had investigated this and determined that an effective modulus could be used for the ff to peak tension relationship. But I can't find this work so perhaps I'm thinking of something else. It isn't terribly difficult to code Pavier's model, at least not for the simple onerunner 180 degree angle case. EDIT: I found a piece of what I'd done before, a graph that compared belayerside tension to fall factor for the following models: standard, Attaway's (aka frictionadjusted), Attaway's corrected for his approximation, and Pavier's. The Pavier model diverged significantly from all of the other three.
(This post was edited by ptlong2 on Jul 18, 2011, 12:23 PM)





cracklover
Jul 18, 2011, 12:41 PM
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ptlong2 wrote: jt512 wrote: Why would you expect there to be a linear relationship between fall factor and maximum impact force in the first place? Because it looked linear! It is curious and humbling how both of us were so easily duped by my blunder. We both knew it was a square root relationship. If only we'd taken a moment to look at Figure 1 in your paper on the subject. Sorry for the wild goose chase. It's not all wasted effort though. Your comparison with the standard model might be of interest. We don't have the hang tag specs for the rope which the standard model methodology calls for, but if his data are so good I'm curious why you didn't use Pavier's own 80kg factor 1.77 drop data for the maximum impact force? Since the frictionadjusted model in your paper predicts even higher tensions it could be that by leaving out some other factor it is "correcting" in the wrong direction. Maybe this discrepency is accounted for by Pavier's model. I could have sworn I had investigated this and determined that an effective modulus could be used for the ff to peak tension relationship. But I can't find this work so perhaps I'm thinking of something else. It isn't terribly difficult to code Pavier's model, at least not for the simple onerunner 180 degree angle case. EDIT: I found a piece of what I'd done before, a graph that compared belayerside tension to fall factor for the following models: standard, Attaway's (aka frictionadjusted), Attaway's corrected for his approximation, and Pavier's. The Pavier model diverged significantly from all of the other three. Well, I was chasing no such geese in my analysis. I was completely comparing apples to apples. Let me know if you'd like me to put this stuff online. GO





cracklover
Jul 18, 2011, 1:38 PM
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Edits inserted in red Here you go, I put it in an online document: https://spreadsheets.google.com/...E&hl=en_US#gid=0 The number for the model_tension comes by plugging all the numbers given in pavier's chart into the standard rope model equation. The only number not provided in his paper is the modulus for the rope. For that I simply assumed a modulus that would provide an average difference of zero. Any other modulus would work equally well, it makes no difference.It turns out that while small changes in modulus make no difference, as the modulus gets over ten, the effect I found disappears. If one assumes a still higher modulus, the affect actually reverses! So, for pavier's setup, it appears that the shorter the fall, the higher the force, relative to the standard model, and the longer the fall, the lower the force (again, relatively).Again, only at the modulus I used. Note that this observed difference is quite small! The largest difference is a few percent. So, to answer the OP's question, at least in Pavier's setup, the FF is almost entirely predictive of the impact force, but there is also a very small (at most a couple percent of the force) change depending on the actual fall length.There is no strong evidence for any relationship between fall distance and force, except as it relates to fall factor. GO
(This post was edited by cracklover on Jul 19, 2011, 8:29 AM)





cracklover
Jul 18, 2011, 1:49 PM
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jt512 wrote: The standard model ... almost perfectly fits the data, as assessed by an rsquared value of 0.995. Interestingly, cracklover sent me a copy of an analysis he did that did show a residual effect of fall length after accounting for the impact force explained by the standard model, but I'm not seeing it in my analysis. Jay Well you certainly won't see it in that graph, because, as you say, his data almost perfectly fits the model. It's only if you look at the delta force between what the model predicts and his data shows that you can see that at any given FF there is a small but real difference. As I mentioned in my post above, the difference is at most a few percent. Edited to add the graph inline for those who just want to see the result: GO
(This post was edited by cracklover on Jul 18, 2011, 2:02 PM)





dynosore
Jul 18, 2011, 3:57 PM
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shockabuku wrote: Has anyone seen any data on how the maximum impact force changes (or doesn't change) as fall length increases for a constant fall factor? One thing rarely discussed is the total energy to be absorbed in a fall. Yes, a 10 foot and 40 foot factor one fall will have very similar peak forces, all other things being equal. But what about the duration of those forces? Maybe a cam starts to skid at 5kn in a bad placement. The 5kn force is only exceeded for say, 0.1 sec in a 10 foot F1 fall, but in a 40 foot fall it's exceeded for several times that long. Maybe that's the difference between the cam skipping all the way out and not. Hope that makes sense, I'm in a bit of a hurry.





jt512
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cracklover wrote: jt512 wrote: The standard model ... almost perfectly fits the data, as assessed by an rsquared value of 0.995. Interestingly, cracklover sent me a copy of an analysis he did that did show a residual effect of fall length after accounting for the impact force explained by the standard model, but I'm not seeing it in my analysis. Jay Well you certainly won't see it in that graph, because, as you say, his data almost perfectly fits the model. It's only if you look at the delta force between what the model predicts and his data shows that you can see that at any given FF there is a small but real difference. By "not seeing it in my analysis," I meant that a plot of the residuals (ie, the observed minus the predicted impact force) from the aforementioned model vs fall length shows no relationship. This is plotted in the following figure. The depicted regression line is not significant (pvalue = 0.20). Jay
(This post was edited by jt512 on Jul 19, 2011, 6:56 AM)





cracklover
Jul 18, 2011, 8:47 PM
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Registered: Nov 14, 2002
Posts: 10158

jt512 wrote: ptlong2 wrote: cracklover wrote: [IMG]http://i53.tinypic.com/miz70i.png[/IMG] Cracklover, since the fall length and fall factor are not independent in Pavier's data it is hard to know whether the effect you think you see is due to one or the other or both. In addition, the effect is rather sensitive to the choice of rope modulus. The following figure shows the difference between the impact force predicted by the standard model and the observed impact force vs fall length, using various values for the rope modulus. The rope modulus is represented by U the rope's UIAA impact force rating (click to enlarge). Jay Wow, that's fascinating! Thanks for the second set of eyes. I'll have to look that over. While a modulus that high is beyond what a new dynamic rope could ever have, Pavier has that key phrase "maximum tension" which suggests that he may be reporting the tension after the rope is nearly shot from multiple repeated drops. I don't know, perhaps a modulus could get that high in those conditions. GO





cellige
Jul 25, 2011, 9:45 PM
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Registered: Dec 2, 2010
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While I would love to see the solution to these differing data sets, I have another question pertaining to the topic. Has anyone investigated the difference in friction in the system under different velocities? A longer fall should build up much more heat for example on the top carabiner. What effect would this have? Also, considering ropes reach their elasticity limits first about 10 feet from their knot (correct me if that is wrong, but I remember rope manufacturers reporting this), would a longer fall put more good rope of an older rope on the higher force side of the top piece and thus reduce the force on the top piece? Just a wild thought. I was keen to hear more about rope drag in all of this, because it seems that could be a significant factor since it is in the top portion of a pitch you could see the longest falls if your spacing your gear farther and farther apart. Your discussion on the reported data however is very interesting, thanks for the time and insight.








