Jobst Brandt and how wheels hold load
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Putting this another way, do this thought experiment. Hang a weight on a spring. Hook another spring with a platform underneath the weight so that the two springs are pulling on the weight up and down. Different weights will equilibrate at different heights, but no matter what weight you use, there is no change in energy so long as the springs aren't bottomed out. Is there? Yes weight is moving up and down and force and motion define change in energy, but the opposite is taking place inside the springs. Unless I am mistaken that is a simplified model of the wheel question we are discussing.
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note that the steel rod in this simpler case is very analogous to the spokes in a wheel. Both are the elements that are supplying the preload to other elements in the system (rim in the case of the wheel, the cement block in the simpler example). The fact that the rod loses spring tension energy when a load is applied shows that there's a fundamental problem with your assumption that the spoke tension energy in a wheel must increase when a load is applied. Neither the steel rod nor the spokes are the only elements in their respective systems. You accept this for the rod/block system but are not acknowledging it for the spokes/rim/hub system.
The spoke/rim/hub system is more complicated to understand. If you do the proper finite element analysis of it you'll find that a few spokes (those at the bottom) lose a lot of energy while some others gain a tiny amount, but the sum of all the spoke tension energy does decrease.
The spoke/rim/hub system is more complicated to understand. If you do the proper finite element analysis of it you'll find that a few spokes (those at the bottom) lose a lot of energy while some others gain a tiny amount, but the sum of all the spoke tension energy does decrease.
Well explained.
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By definition tension means force pulling on the ends of an object. Isn't the 50 N weight pulling on the top spoke?
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Putting this another way, do this thought experiment. Hang a weight on a spring. Hook another spring underneath the weight so that the two springs are pulling on the weight up and down. Different weights will equilibrate at different heights, but no matter what weight you use, there is no change in energy so long as the springs aren't bottomed out. Is there? Yes weight is moving up and down and force and motion define change in energy, but the opposite is taking place inside the springs. Unless I am mistaken that is a simplified model of the wheel question we are discussing.
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No, because you relieve potential energy inside the lower spring...assuming you are pulling down. You are exerting energy, but the spring has less.
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At the same time, similar thing happens in the hub with preloaded bearings.
That's why it all works so nicely and lasts long. That is also one of the reasons why, when spokes (or bearings) come loose - damage quickly happens.
Tyre and rim do not have this "luxury", so they get all the beating directly, and without any relief (of course, the whole wheel, including the rim, does enjoy some relief from tyre flex working as a shock absorber).
Last edited by Bike Gremlin; 08-20-16 at 02:06 PM.
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The lower spoke doesn't lose any tension until the hub moves down. That is like relieving the pull on a spring. And when the hub moves, the upper spoke increases in tension by 50 N. The upper increases to 150 as the lower decreases to 50.
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I could easily settle this, seeing as how I stayed at a Holiday Inn last night, but you guys are having fun kicking this around so why should I rain on the parade.
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Note that the steel rod in this simpler case is very analogous to the spokes in a wheel. Both are the elements that are supplying the preload to other elements in the system (rim in the case of the wheel, the cement block in the simpler example). The fact that the rod loses spring tension energy when a load is applied shows that there's a fundamental problem with your assumption that the spoke tension energy in a wheel must increase when a load is applied. Neither the steel rod nor the spokes are the only elements in their respective systems. You accept this for the rod/block system but are not acknowledging it for the spokes/rim/hub system.
The spoke/rim/hub system is more complicated to understand. If you do the proper finite element analysis of it you'll find that a few spokes (those at the bottom) lose a lot of energy while some others gain a tiny amount, but the sum of all the spoke tension energy does decrease.
The spoke/rim/hub system is more complicated to understand. If you do the proper finite element analysis of it you'll find that a few spokes (those at the bottom) lose a lot of energy while some others gain a tiny amount, but the sum of all the spoke tension energy does decrease.
If you apply the same logic to your example with concrete then the concrete does not deform with extra load and the tension of the steel rod does not change.
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50 N is pushing the hub down, reducing the tension of the bottom spoke by the same amount. So while the 50 N form the weight does increase tension of the upper spoke, the bottom one is pushing by 50 N less force - so the tension of the upper spoke remains the same.
At the same time, similar thing happens in the hub with preloaded bearings.
That's why it all works so nicely and lasts long. That is also one of the reasons why, when spokes (or bearings) come loose - damage quickly happens.
Tyre and rim do not have this "luxury", so they get all the beating directly, and without any relief.
At the same time, similar thing happens in the hub with preloaded bearings.
That's why it all works so nicely and lasts long. That is also one of the reasons why, when spokes (or bearings) come loose - damage quickly happens.
Tyre and rim do not have this "luxury", so they get all the beating directly, and without any relief.
This is really ironclad.
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In addition to that - if the lower spoke looses tension by amount of X N, the upper spoke gets 100 N + 50 N (load) - X N (the amount of lost tension from the lower spoke).
The X is dangerously close to the load applied.
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Rim slightly deforms at the lowest part. That allows for the lower spoke to loose some tension.
In addition to that - if the lower spoke looses tension by amount of X N, the upper spoke gets 100 N + 50 N (load) - X N (the amount of lost tension from the lower spoke).
The X is dangerously close to the load applied.
In addition to that - if the lower spoke looses tension by amount of X N, the upper spoke gets 100 N + 50 N (load) - X N (the amount of lost tension from the lower spoke).
The X is dangerously close to the load applied.
We were ignoring deformation. If you consider deformation, you have to consider that the top of the rim flattens too.
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Please don't get offended, but lose is spelled with only one o. I figured that if this were going to continue for a while, I could either mention it or go crazy.
We were ignoring deformation. If you consider deformation, you have to consider that the top of the rim flattens too.
We were ignoring deformation. If you consider deformation, you have to consider that the top of the rim flattens too.
Still, with a perfectly rigid rim, there remains the amount of lowered tension of the lower spoke, that is deducted from the 50 N increase. How much is it? Probably about 50 N.
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But it is added back on the upper spoke. Why do you keep ignoring that? Otherwise the two spokes wouldn't meet each other...with the hub between them of course. You are double dipping the reduction of tension in the lower spoke, saying the lower spoke has reduced tension, AND you have to subtract it from the upper spoke as well. You can't consider it twice.
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100 N each spoke. OK?
50 N load.
If the lower spoke looses tension with that load, the upper spoke gains tension: 100 N minus lost tension of the lower spoke, plus the added 50 N load. That results in less than 150 N. Exactly 100 N.
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I think I was wrong! I wasn't considering the total forces on each side had to be the same. Some serious simultaneous equations needed. Let me work on it.
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I assume that the rim is very flexible but incompressible (this is very close to what happens in classical low profile rims). That way it can not store any energy.
If you apply the same logic to your example with concrete then the concrete does not deform with extra load and the tension of the steel rod does not change.
If you apply the same logic to your example with concrete then the concrete does not deform with extra load and the tension of the steel rod does not change.
Concrete is not easily compressed, but if a preload is applied using the steel rod and a weight (wt. < preload) is then applied on top of it the result is that the tension in the rod is reduced because of the weight.
A paper giving an FEA of bicycle wheels was already presented at:
https://www.ewp.rpi.edu/hartford/~ern...inalReport.pdf
As expected it shows large reductions in tension of a few spokes at the bottom of the wheel and much smaller increases in other spokes. There's a table with the forces on p. 17 and you could calculate the corresponding stored energies. But just glancing at the table makes it clear that the sum of the spoke stored energies went down when the load was applied.
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If concrete does not compress then the tension in the rod will not decrease.
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If you want to dispute the FEA studies of rim loading that have been done, then you need to either show exactly where their errors are or do your own study that supports your claim. In the latter case we'd then need to examine both yours and the previous ones to see where they differ and which one should be trusted. Just repeating the claim based on energy conservation when it's clear that the spokes by themselves do not constitute a closed and isolated system is not convincing.
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As I said before, I thought we were interested in real materials in the real world - not some fictitious material. I said that concrete doesn't compress easily - not that there is no compression at all.
If you want to dispute the FEA studies of rim loading that have been done, then you need to either show exactly where their errors are or do your own study that supports your claim. In the latter case we'd then need to examine both yours and the previous ones to see where they differ and which one should be trusted. Just repeating the claim based on energy conservation when it's clear that the spokes by themselves do not constitute a closed and isolated system is not convincing.
If you want to dispute the FEA studies of rim loading that have been done, then you need to either show exactly where their errors are or do your own study that supports your claim. In the latter case we'd then need to examine both yours and the previous ones to see where they differ and which one should be trusted. Just repeating the claim based on energy conservation when it's clear that the spokes by themselves do not constitute a closed and isolated system is not convincing.
So I don't understand your point very much. I've said that a couple of times that some parts of the system can lose energy. It's the system as a whole that can't. Either be it a rod with the concrete block or spokes with a rim.
Whether the rim can store much energy is another question.
And I'm not disputing the FEA studies. In fact I've seen it as such that supports my claims. It does look like the total energy of spokes decreases so the rim plays greater role than I thought. I'll have to think about it.
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Like a powermeter. you don't need to measure all the places where power is dissipated (aero loss, elevation gain, rolling friction, etc.) to calculate the power out of your legs. You can simply measure the force and deflection of a load component and calculate power directly. Same calculation as above, in fact.
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