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#121 | |
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Registered User
Join Date: Jun 2004
Location: Tucson, AZ
Posts: 2,649
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Quote:
Simple: from the first and second order analysis of forces in bike/rider system. From the complete lack of data making any correlation whatsoever between bike stiffness and improved performance. Math. Science. Look 'em up, and give 'em a try. People actually use it in the real world. |
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#122 | |
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Join Date: Dec 2007
Posts: 3,840
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#123 | |
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Registered User
Join Date: Jun 2007
Location: You are here => X
Posts: 10,494
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Quote:
Interesting logic for he who decries having an opinion when there is no data to support it... ![]()
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#124 | |
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Registered User
Join Date: Jun 2006
Posts: 317
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Quote:
I didn't perform an experiment. I used the known values of stiffness and computed the theoretical losses. But yes, you made one of my points for me. The losses are generally too small to be measured... ![]() This is how I calculated the losses: - Assume the stiffness values (expressed as k = N/mm) represent a linear, spring relationship. And it should because there are no non-linear elements. - The energy stored in a spring (and subsequently lost) is equal to 0.5kx^2 where x is the displacement. - The amount of displacement can be estimated from F = kx and P = Tw, where P is power, T is torque, and w is the rotational speed of the cranks. - For a given power output and cadence, you can figure the average torque on the crank. - Assuming the instantaneous peak torque is ~ 4 times average (that's generous) and using a force diagram, you can calculate the force that goes into bending the frame (i.e., pushing on our model of a spring) - This force gives you the energy stored in the spring as described above: 0.5kx^2 and all that. - This energy loss happens twice every rotation of the cranks, which happens 2cadence/60 seconds. - Therefore, the power lost is equal to Energyx30/cadence Watts. - Divide that by the original power input and there's your efficiency. I found that using this model, which should be accurate by way better than an order of magnitude, the efficiency of a bike frame is ~99.95%. That might change by ~0.025% depending on whether you have a super stiff or super flexible frame. John Swanson www.bikephysics.com |
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#125 |
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Registered User
Join Date: Dec 2007
Posts: 3,840
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Maybe alienator is just confused with what inferences can or cannot be drawn from "lack of data". Case in point - there is no data showing that string theory is right. Hence, string theory should be wrong. Right, alienator?
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#126 |
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Registered User
Join Date: Jun 2006
Posts: 317
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Oh yeah. And the efficiency is the same whether you're putting out 12 or 1200 Watts. The system is incredibly linear over a wide range of inputs.
John Swanson www.bikephysics.com |
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#127 | |
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Join Date: Dec 2007
Posts: 3,840
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#128 |
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Registered User
Join Date: Apr 2005
Location: Toronto Canada
Posts: 474
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I'm not pretending to understand string theory; however, I believe there are 6 different theories, all requiring many more dimensions than the four we live with.
They can't all be right. |
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#129 | |
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Join Date: Dec 2007
Posts: 3,840
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#130 | |
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Registered User
Join Date: Jun 2006
Posts: 317
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Quote:
Nah. You don't really need a damping term because you don't care *where* the losses are. It's enough to know that any energy you put into this spring system is lost. Besides, the only effect a damping mechanism would have is to improve the overall efficiency... John Swanson www.bikephysics.com |
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#131 | |
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Join Date: Jun 2007
Location: You are here => X
Posts: 10,494
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Quote:
And how is your model able to determine the difference between a "noodly" frame and a very stiff frame. I can't see where the frame properties are accounted for in your model? I need more time to go through and understand your model though. Thanks in any case, John, for your explanation.
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#132 | |
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Join Date: Dec 2007
Posts: 3,840
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#133 | |
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Registered User
Join Date: Jun 2006
Posts: 317
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Quote:
I know that this was a quick summary and perhaps not the easiest to "digest". But hopefully I can answer your questions. The value of k comes directly from published data on frame stiffness. To be honest, I can't remember where I got my numbers, but I think it was from the famous "Tour" testing. I then use k with the estimated F (from the Torque, power, cadence, and force diagrams) to calculate x. x = F/k From there, I can calculate the energy loss: E = 0.5kx^2 And with a few more sums, I get the overall efficiency. I'll try to find my old, longwinded posts on the subject. If I can't find them, maybe I'll write them all out again. But don't hold your breath, I've been busy lately and I'm feeling lazy. John Swanson www.bikephysics.com |
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#134 | |
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Join Date: Dec 2007
Posts: 3,840
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#135 | |
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Join Date: Jun 2007
Location: You are here => X
Posts: 10,494
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Quote:
You have a force on the crank. The only way to know how much of that force goes into deflecting the frame is to know the properties of the frame. The energy will be stored in the path of least resistence first. Its not until the force of the spring pushes back with the same force from the crank, that the drive train will start to be engaged. You need to know this F= kx of the frame, which is not the same as the F (force) of the pedal force. Correct me where I am wrong please. The "x" value is important IMO because if you have a high "x" value of the frame (high deflection ie. a "noodly" frame) then more time may be required to deflect the frame before it resists the pedal force. This will be a more significant part of the pedal rotation arc than in the case of a stiffer frame, which can push back against the pedal force quicker. I need to think more about your model though. At first glance, I am struggling with understanding how you accounted for the stiffness modulus/properties of the frame, to get your 0.05% difference betweeen the two.
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