Rotating vs non-rotating mass.
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I think you guys are getting distacted. Obivously energy is always conserved. Apart from certain loss processes (drag, friction, etc) energy will always remain within the system.
However, the body is primarily restricted by the power it can deliver, not the energy. It doesn't take any more energy to move an elephant up and down a ladder than it does a paperclip (zero in both cases), but your body will waste a lot of energy in order to muster the necessary power to move the elephant.
Furthermore, it's better to retain control over acceleration/deceleration with your legs. If you invest energy in getting a large wheel up to speed then you risk losing that energy if you need to brake, but if you keep the energy in your muscles then you don't risk as much. On average the higher risk should translate to more energy lost due to braking.
However, the body is primarily restricted by the power it can deliver, not the energy. It doesn't take any more energy to move an elephant up and down a ladder than it does a paperclip (zero in both cases), but your body will waste a lot of energy in order to muster the necessary power to move the elephant.
Furthermore, it's better to retain control over acceleration/deceleration with your legs. If you invest energy in getting a large wheel up to speed then you risk losing that energy if you need to brake, but if you keep the energy in your muscles then you don't risk as much. On average the higher risk should translate to more energy lost due to braking.
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Originally Posted by dalmore
Looking at energy can also be misleading. Consider that whether a biker rides up a hill or pushes the bike up the hill, the energy is the same but the experience is quite different.
Originally Posted by dalmore
I think the weight of wheels and tires have a constant effect on bikes that is greater than the effect that same amount of weight would have elsewhere on the bike. I tried to explain the idea with the example of a lever and failed. (I still maintain that's valid but I'll drop that for now.) Let me try again with a different aproach.
We all agree that rotating mass has an effect on acceleration to a greater degree than non rotating mass. We all agree that the forces of friction (from various sources) and aerodynamic drag are acting to prohibit forward movement of the bike. These forces are constant - if you stop applying power, these forces cause a bike to slow down.
We all agree that rotating mass has an effect on acceleration to a greater degree than non rotating mass. We all agree that the forces of friction (from various sources) and aerodynamic drag are acting to prohibit forward movement of the bike. These forces are constant - if you stop applying power, these forces cause a bike to slow down.
Originally Posted by dalmore
Now consider that power from the biker is not being applied constantly like gravity or a rocket engine. Instead power is being applied in pulses. So the bike is in a constant cycle of acceleration and deceleration.
Perhaps you think the pulses are so short that they don't matter. Well regardless of the cadence, a bike with a standard crank and plaform pedals is only under power about half the time. 1/4 of the time from the left foot pushing down on the pedal from about 90 to 180 degrees and 1/4 of the time from the right foot pushing down on the pedal from about 90 to 180. I think that does matter.
Perhaps you think the pulses are so short that they don't matter. Well regardless of the cadence, a bike with a standard crank and plaform pedals is only under power about half the time. 1/4 of the time from the left foot pushing down on the pedal from about 90 to 180 degrees and 1/4 of the time from the right foot pushing down on the pedal from about 90 to 180. I think that does matter.
All you need to recognize is that kinetic energy is kinetic energy. It can be stored as forward motion, and it can be stored in a rotating object. It doesn't matter which. Consider the example of the bike with massive flywheel wheels. At speed, with each power pulse I would put most of the energy delivered into rotational kinetic energy. Very little would go into translational kinetic energy, so I would experience very little speed change, but I have stored the same amount of energy. Between pulses the very slightest of slowing the the flywheel will deliver enough energy to overcome friction and drag. So I would experience very little slowing between pulses. Note, though, that there is not more power going into the system then there is in the light wheel case.
Note to all respondees: please don't get on my case as advocating giant flywheel wheels. I'm not. They are just a specific example that is useful because they are so extreme!
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Originally Posted by makeinu
I think you guys are getting distacted. Obivously energy is always conserved. Apart from certain loss processes (drag, friction, etc) energy will always remain within the system.
However, the body is primarily restricted by the power it can deliver, not the energy. It doesn't take any more energy to move an elephant up and down a ladder than it does a paperclip (zero in both cases), but your body will waste a lot of energy in order to muster the necessary power to move the elephant.
Furthermore, it's better to retain control over acceleration/deceleration with your legs. If you invest energy in getting a large wheel up to speed then you risk losing that energy if you need to brake, but if you keep the energy in your muscles then you don't risk as much. On average the higher risk should translate to more energy lost due to braking.
However, the body is primarily restricted by the power it can deliver, not the energy. It doesn't take any more energy to move an elephant up and down a ladder than it does a paperclip (zero in both cases), but your body will waste a lot of energy in order to muster the necessary power to move the elephant.
Furthermore, it's better to retain control over acceleration/deceleration with your legs. If you invest energy in getting a large wheel up to speed then you risk losing that energy if you need to brake, but if you keep the energy in your muscles then you don't risk as much. On average the higher risk should translate to more energy lost due to braking.
To move a mass M, up a ladder, increasing it's height by h, in a gravitational field with gravitaional acceleration g, will take energy M*g*h. So, if an elephant is a mass M and a paperclip is mass m, then the difference in energy required would be (M-m)*g*h.
Power is energy per unit time. It is the rate of energy delivered, or extracted from a system. You are right in that a rider will be limited in how much energy he can deliver per unit time. His power does have some finite limit.
Braking is an issue. In the other discussions I was arguing that in near steady state, you get the energy out of the system, in overcoming drag and friction, that you put in. If you hit the brakes, then all that energy goes to heat. But remember, hitting the brakes you give up kinetic energy from ALL sources. That includes the translational kinetic energy. The translational kinetic energy of a 150 pound biker on a 25 pound bike dwarfs the rotational kinetic energy in the rotating wheels. If you are doing nothing but start and stop, your wheels are a small part of your worries!
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Originally Posted by Speedo
Well, no and yes. None of the friction and drag forces are "constant". Bearing friction will be proportional to rotation rate, and hence speed. Aerodynamic drag is proportional to the square of the relative air speed. I think that tire rolling resistance is proportional to speed, but don't know for sure. But, yes I agree that on level ground, in no wind, if you stop applying power they will cause the bike to slow down.
Originally Posted by Speedo
Okay, we are at the point where we agree that the bike is "up to speed".
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Originally Posted by Speedo
Even more different if (since this is in folding bikes) the biker folds the bike puts it on his back and carries it up the hill. But in any of those cases examining the energy is useful. It's just a technique, it reveals relationships in the system.
Originally Posted by Speedo
Okay, we are at the point where we agree that the bike is "up to speed". In getting the bike up to speed I paid a penalty for rotating vs non-rotating mass. Now I'm up to speed, and I deliver power to the system in a non-constant way. In the subjective way that I experience this, unless I am piston pedalling up a hill, I don't experience this as pulses. Why not? Well, we need to look at (sorry ) energy. The inertia of the system, that is, the energy stored as kinetic energy smooths the motion over the non-constant input power. We aren't really in a steady state, but have small variations around a given speed. With each power pulse the energy delivered is distributed between heat (friction, and drag) and kinetic energy (we speed up a bit). In the between pulse period, the kinetic energy goes to heat (friction and drag) and we slow down a bit.
Originally Posted by Speedo
All you need to recognize is that kinetic energy is kinetic energy. It can be stored as forward motion, and it can be stored in a rotating object. It doesn't matter which. Consider the example of the bike with massive flywheel wheels. At speed, with each power pulse I would put most of the energy delivered into rotational kinetic energy. Very little would go into translational kinetic energy, so I would experience very little speed change, but I have stored the same amount of energy. Between pulses the very slightest of slowing the the flywheel will deliver enough energy to overcome friction and drag. So I would experience very little slowing between pulses. Note, though, that there is not more power going into the system then there is in the light wheel case.
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Originally Posted by dalmore
They most certianly are constant in the sense that they are not pulsing.
Originally Posted by dalmore
It's obvious that you are not getting it. The bike is never at a constant speed. Never. It's either speeding up or slowing down.
I'm not claiming that the bike is at constant speed. I'm only saying that if you look at what happens as the bike speeds and slows with the pedal pulsing there is energy that goes into kinetic energy on the speed up, that comes out on the slow down. If the bike had no kinetic energy, then it would stop dead as soon as no power was put in. But the kinetic energy of the bike goes toward overcoming friction, rolling resistance and aero drag, so the bike continues to move forward (slowing as it goes as the kienetic energy is turned to heat). Some of that kinetic energy disappated is the rotational kinetic energy of the wheels.
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Originally Posted by Speedo
Uh, sorry, but you don't seem to be clear on energy, power, or the realtionship between them.
Originally Posted by Speedo
To move a mass M, up a ladder, increasing it's height by h, in a gravitational field with gravitaional acceleration g, will take energy M*g*h. So, if an elephant is a mass M and a paperclip is mass m, then the difference in energy required would be (M-m)*g*h.
The energy required to go up the ladder is proportional to the maximum power. That is why you intuitively considered only the energy required to go up the ladder and not the total energy at the end of the day. Formally this is the maximum power.
Likewise, in the case of bicycle wheels, we need to consider the energy required to get up to speed (not the total energy at the end of the journey) because this is proportional to the peak power provided by your legs.
Originally Posted by Speedo
Power is energy per unit time. It is the rate of energy delivered, or extracted from a system. You are right in that a rider will be limited in how much energy he can deliver per unit time. His power does have some finite limit.
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Originally Posted by Speedo
If what you say below is true, that the bike is never at a constant speed then they must be pulsing. They are proportional to the speed, or the square of the speed. As the speed changes, they change.
Originally Posted by Speedo
No, no, yesterday was Valentines Day. I did!
Originally Posted by Speedo
I'm not claiming that the bike is at constant speed. I'm only saying that if you look at what happens as the bike speeds and slows with the pedal pulsing there is energy that goes into kinetic energy on the speed up, that comes out on the slow down. If the bike had no kinetic energy, then it would stop dead as soon as no power was put in. But the kinetic energy of the bike goes toward overcoming friction, rolling resistance and aero drag, so the bike continues to move forward (slowing as it goes as the kienetic energy is turned to heat). Some of that kinetic energy disappated is the rotational kinetic energy of the wheels.
Speedo
Speedo
Originally Posted by speedo
While a rotating mass requires both the translational energy and the rotational energy to get up to speed.
Et+Er=0.5*M*V^2+0.5*M*V^2 = M*V^2; twice the non-rotating energy.
Et+Er=0.5*M*V^2+0.5*M*V^2 = M*V^2; twice the non-rotating energy.
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Originally Posted by dalmore
I'm not sure where the disconnect in our terminology blies. But the air causes aerodynamic drag does not vanish for an instant while I'm not appliying force on the pedal. That air is still resisting the forward movement of the bike and causing it to slow. If that's not "constant" perhaps "consistent" is a better word.
Originally Posted by dalmore
Exactly!! And because of this the rotating mass is ALWAYS having more of an effect that non-rotating mass. After all you did a fine job of proving that back in Post number 1
Okay, I'm on the bike. I'm "at speed". "At speed" is near constant, but will vary with how I am pushing on the pedals. With each push on the pedals I add kinetic energy. I am adding kinetic energy not just in translational kinetic energy, but in rotational kinetic energy of the wheel. There is not only translational momentum, but angular momentum as well. Just as in the sled case, it is the momentum that carries us forward between pushes. The fact that some of your push energy went into angluar momentum means that at that it did not go into translational momentum, so your speed increase at that push was not as much at the push. BUT that angular momentum will now help carry you through the non-push interval, and your speed will not decrease as much.
When you are trying to maintain speed, what you put into angular momentum in little pulses, comes back to you, helping carry you forward, between the pulses. You don't lose because of it.
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Originally Posted by makeinu
Yes, it reveals precisely that you are leaving out the most important energies. It reveals that smaller wheels, like gearing, weight, and almost everything else about a bicycle are not meant to reduce mechanical losses, but biomechanical losses. It reveals that we are better off considering the power than the energy.
Originally Posted by makeinu
It smooths the pulse at the output. The input is still very much experiencing pulses, which affects the sources ability to generate energy with minimal losses. Matching the load seen at the input to the source is the most important factor and it is one you are completely ignoring. It's the entire reason for cycling in the first place!
Originally Posted by makeinu
The linear acceleration of the bike is not magically reduced to compensate.
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Originally Posted by makeinu
What do I need to clarify?
As I noted earlier:
I'm always happy to concede that light is better than heavy. My only claims are that:
1) When accelerating the bike it is, in fact, true that a pound in the wheels is like two on the bike.
2) After the bike is up to speed, there is no continuing penalty due to the fact that the mass of the wheel is rotating.
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ok I guess I see what you are saying on this point ... For the sake of clarity say I'm averaging a constant speed of 20 mph by bouncing between 21 and 19 mph. You are saying that the rotational energy change when dropping from 21 mph to 19mph is equal to the rotational energy change of going back from 19 to 21 so it's a net zero game. ok, I can swallow that.
BUT that is not to say that I agree that rotating mass is the same as non rotating mass except when accelerating. Only that I don't have the math skills to argue the point.
BUT that is not to say that I agree that rotating mass is the same as non rotating mass except when accelerating. Only that I don't have the math skills to argue the point.
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Originally Posted by Speedo
Energy is important as an analysis tool to understand the inter-relationships between the parts.
Originally Posted by Speedo
The input is the cyclist adding energy in the most efficient way they can manage.
Originally Posted by Speedo
I'm only showing that that energy, once added is not squandered by rotating masses.
Originally Posted by Speedo
No, it's not magic. It's physics.
Originally Posted by Speedo
You know, at some point above I introduced the concept of massive flywheel wheels to help with the idea of angular momentum, and energy stored in the rotating mass. They were just an example. I'm not recommending that people go out and put massive wheels on their bikes. I'm sorry for any misunderstanding.
Originally Posted by Speedo
I'm always happy to concede that light is better than heavy.
Originally Posted by Speedo
1) When accelerating the bike it is, in fact, true that a pound in the wheels is like two on the bike.
2) After the bike is up to speed, there is no continuing penalty due to the fact that the mass of the wheel is rotating.
2) After the bike is up to speed, there is no continuing penalty due to the fact that the mass of the wheel is rotating.
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I'm with you on this one Speedo.
Looks like it is going to require a detailed simulation to decide it. I have a simulator, just need the math to put into it. I'll see if I can squeeze in the time. Or maybe you can furnish a starting point?
We will need equations for:
forward motion, with drag from wind resistance;
model of torque supplied by legs on pedals, I am thinking a sine wave with variable amplitude and offset may do here;
angular momentum converted to linear momentum as a function of wheel diameter, with wheel moment of inertia variable;
maybe some drag from bearings;
That will probably do.
Then the sim should show if the terminal velocity for a steady state torque model for cases of different wheels is different.
[edit] An approach from conservation of energy is going to be most reliable and easy.
Looks like it is going to require a detailed simulation to decide it. I have a simulator, just need the math to put into it. I'll see if I can squeeze in the time. Or maybe you can furnish a starting point?
We will need equations for:
forward motion, with drag from wind resistance;
model of torque supplied by legs on pedals, I am thinking a sine wave with variable amplitude and offset may do here;
angular momentum converted to linear momentum as a function of wheel diameter, with wheel moment of inertia variable;
maybe some drag from bearings;
That will probably do.
Then the sim should show if the terminal velocity for a steady state torque model for cases of different wheels is different.
[edit] An approach from conservation of energy is going to be most reliable and easy.
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Originally Posted by makeinu
Not when you leave out the most important energies, such as the energy lost by the body at a given power level.
The rider outputs his normal power level. A bike with relatively heavier wheels acclerates more slowly, so takes longer getting to speed. Once at speed the rider is again providing the same amount of power, and riding the same speed. You can say that the overall consumed slightly more energy because the rider out put the same amount of power and thus lost time in the accelerations, or preserved the acceleration time by outputing more power. In either case it is not a dramatic difference.
Originally Posted by makeinu
Which is more efficient with the smaller wheel.
Originally Posted by makeinu
So the energy will be squandered in the brakes via the excess momentum and in the heating of your muscles due to the increased power requirement.
Originally Posted by makeinu
The linear acceleration certainly isn't physically reduced to compensate either. At a given cadence, the bike will only go slower if you reduce the gear. Otherwise you will have to pedal harder, just like you have to pedal harder with a heavier bike, just like you have to pedal harder when going up hill. Pedaling harder and deviating from optimal cadence both waste more biomechanical energy. Therefore using a bigger wheel wastes more biomechanical energy.
[QUOTE=makeinu]I'm not saying that you're recommending that people go out and put massive wheels on their bikes. I'm saying that the fact that larger wheels do not themselves dissipate energy is irrelevant to the conclusion that a bike with larger wheels will waste more energy.[/QUOTETE]
Do you think that we are having a discussion about wheel diameter? I don't really have anything to say about wheel diameter.
Originally Posted by makeinu
Yeah, but you are so occupied with analyzing the energy that you're missing the reason why light is better than heavy. Your missing the most important inter-relationships which you claim your energy analysis is so helpful to understand.
Originally Posted by makeinu
Ok, but the bike will most likely never be "up to speed". Most of the time riding is probably spent pedaling/accelerating and braking.
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Originally Posted by Speedo
Nowhere have I said that the rider would have to provide more power then they otherwise would. I have no idea where you've gotten that idea from.
The rider outputs his normal power level. A bike with relatively heavier wheels acclerates more slowly, so takes longer getting to speed. Once at speed the rider is again providing the same amount of power, and riding the same speed. You can say that the overall consumed slightly more energy because the rider out put the same amount of power and thus lost time in the accelerations, or preserved the acceleration time by outputing more power. In either case it is not a dramatic difference.
The rider outputs his normal power level. A bike with relatively heavier wheels acclerates more slowly, so takes longer getting to speed. Once at speed the rider is again providing the same amount of power, and riding the same speed. You can say that the overall consumed slightly more energy because the rider out put the same amount of power and thus lost time in the accelerations, or preserved the acceleration time by outputing more power. In either case it is not a dramatic difference.
Originally Posted by Speedo
Do you think that we are having a discussion about wheel diameter? I don't really have anything to say about wheel diameter.
Originally Posted by Speedo
I'm always happy to concede that lighter is better.
Originally Posted by Speedo
If you are spending all of your time accelerating and then braking then you have my sympathy. But if that's the case the energy in and out of the wheel angular momentum will be overwhelmed by the linear momentum swings.
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Originally Posted by makeinu
I got the idea that the rider would have to provide more power from the physics of the situation. If you fix the power provided by the rider then the rider's candence must be reduced to compensate for the reduced acceleration.
Originally Posted by makeinu
As we've already established. The relevant difference between larger and smaller wheels is the difference in rotating weight, which is what this whole thread is about. All else being equal larger wheels are heavier wheels and smaller wheels are lighter wheels.
Also, there must be some other things coming into play, otherwise we's all be riding those bikes that use skateboard wheels! Time trial bikes use smaller wheels than 700C. Maybe that's the optimum. I don't really have a strong opinion one way or the other in the big vs small wheels.
Originally Posted by makeinu
Then why do you keep going on about the mechanical energy being independent of the rotating mass?
Originally Posted by makeinu
Either the total mechanical energy is important and, since rotating weight does not affect the total mechanical energy, rotating weight is unimportant or the total mechanical energy is irrelevant and lighter is better. Lighter is better because the conservation of energy you keep talking about is irrelevant.
Originally Posted by makeinu
Obviously small changes in weight will give small changes in performance regardless of whether the weight is linear or rotating, but braking and accelerating must be awfully popular among most cyclists. Why else would light weight and low momentum be considered so important?
As to your second, well, my party line has been lighter is better. How light? Damned if I know. I have a friend who insists on spending thousands of dollars every year to have the latest lightest widget. I suppose he's got the dosh, and likes to bike, so what else is he going to spend it on? I have other friends who will ride nothing but 25 year old bikes that are as much as 6 or 7 pounds heavier than a middle of the line new bike. I must admit that I learned much about the mechanics of bikes to puncture Mr. Lightbike's claims about his nanogram wheels!
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Originally Posted by jur
I'm with you on this one Speedo.
Looks like it is going to require a detailed simulation to decide it. I have a simulator, just need the math to put into it. I'll see if I can squeeze in the time. Or maybe you can furnish a starting point?
Looks like it is going to require a detailed simulation to decide it. I have a simulator, just need the math to put into it. I'll see if I can squeeze in the time. Or maybe you can furnish a starting point?
On the other hand, I've never been one to let practical considerations stand in the way of writing equations! I take the challenge!
I am going away this weekend. Maybe next week I can put something together. Do you want equations? Are you going to put this into Matlab or something similar? I have Matlab and can write code that can be integrated by their differential equation solver.
If Dalmore and makineu (I think they are the last who haven't been driven away by the pedantry) are interested we can post the pieces here.
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Originally Posted by Speedo
Why? A slowly accelerating rider is going through the same range of speeds as the fast accelerating rider just a lower rate. The range of strategies for matching available power to load (standing, shifting gears, ...) are available to be used by any rider.
Originally Posted by Speedo
The thread is about rotating vs non-rotating mass. Some posters, yourself, included have made that claim. I would agree that if I were out to make the lightest wheels possible, I'd go for smaller rims, but that doesn't mean that small wheels must be lighter. On my small wheels I run wider tires and the rim itself is wider. I may have to try measuring, but I would not immediately conclude that my 406 wheels (and tires) are lighter than my 700Cs.
Also, there must be some other things coming into play, otherwise we's all be riding those bikes that use skateboard wheels! Time trial bikes use smaller wheels than 700C. Maybe that's the optimum. I don't really have a strong opinion one way or the other in the big vs small wheels.
Also, there must be some other things coming into play, otherwise we's all be riding those bikes that use skateboard wheels! Time trial bikes use smaller wheels than 700C. Maybe that's the optimum. I don't really have a strong opinion one way or the other in the big vs small wheels.
Originally Posted by Speedo
I don't think it will convince anyone who isn't ready to be convinced. The model is going to be a set of diferential equations. People will have to buy the model as well as the idea of numerically integrating the equations to get a result.
On the other hand, I've never been one to let practical considerations stand in the way of writing equations! I take the challenge!
I am going away this weekend. Maybe next week I can put something together. Do you want equations? Are you going to put this into Matlab or something similar? I have Matlab and can write code that can be integrated by their differential equation solver.
If Dalmore and makineu (I think they are the last who haven't been driven away by the pedantry) are interested we can post the pieces here.
Speedo
On the other hand, I've never been one to let practical considerations stand in the way of writing equations! I take the challenge!
I am going away this weekend. Maybe next week I can put something together. Do you want equations? Are you going to put this into Matlab or something similar? I have Matlab and can write code that can be integrated by their differential equation solver.
If Dalmore and makineu (I think they are the last who haven't been driven away by the pedantry) are interested we can post the pieces here.
Speedo
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Originally Posted by makeinu
What's there to simulate? Everything is analytically solvable. It's just boils down to how large the various effects are when subject to real world nonidealities.
If you have a solution feel free to contribute it!
Speedo
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Originally Posted by Speedo
I don't think it will convince anyone who isn't ready to be convinced. The model is going to be a set of diferential equations. People will have to buy the model as well as the idea of numerically integrating the equations to get a result.
On the other hand, I've never been one to let practical considerations stand in the way of writing equations! I take the challenge!
I am going away this weekend. Maybe next week I can put something together. Do you want equations? Are you going to put this into Matlab or something similar? I have Matlab and can write code that can be integrated by their differential equation solver.
If Dalmore and makineu (I think they are the last who haven't been driven away by the pedantry) are interested we can post the pieces here.
Speedo
On the other hand, I've never been one to let practical considerations stand in the way of writing equations! I take the challenge!
I am going away this weekend. Maybe next week I can put something together. Do you want equations? Are you going to put this into Matlab or something similar? I have Matlab and can write code that can be integrated by their differential equation solver.
If Dalmore and makineu (I think they are the last who haven't been driven away by the pedantry) are interested we can post the pieces here.
Speedo
The diff. equations can be easily converted to Laplace (s-domain) format. But perhaps it is easiest, instead of constructing a diff eq model and putting that in, to construct a model with all the various pieces connected with a block diagram format.
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Originally Posted by Speedo
I wondered if that were true. It might be doable if one assumed constant input power, but one of the questions to be addresssed was what happend in the case of non-constant input. The pulsing pedal stroke case. It is a periodic input, maybe Fourier analysis. Not being very smart, I often resort to numerical integration.
If you have a solution feel free to contribute it!
If you have a solution feel free to contribute it!
However, I still think the most important factor is how efficiently the body can deliver power for different loads. Biomechanical losses are very tricky to analyze.
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As things currently stand 700c wheels are more often than not lighter than 20"/16" wheels - this is because of the r&d that goes into racing. Look at some of the weights on weight weenies (if you are really that sad!).
If you want to see heavy rotating masses check out this guy and his machine:
https://www.wolfgang-menn.de/sosenka.htm
If you want to see heavy rotating masses check out this guy and his machine:
https://www.wolfgang-menn.de/sosenka.htm
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Well, I have a write up of the equations. The basic differential equation is based on solving an equation of the power sources and the power sinks for the bike acceleration. The bike acceleration can then be integrated in whatever tool you have available to get speed vs time.
The model includes a pedal power model, rotating and non-rotating inertia, a hill (if desired!), and aerodynamic drag. The model doesn't include rolling resistance and bearing friction. I found references for those terms, but thought that going without them would be better for a start. I'm not sure there is a closed form solution to the differential equation. It's complicated enought that I'm just going to go after it numerically.
What I have is a Word document that has been converted to pdf. I used Microsoft equations; this won't look very good in plain text. I'm not sure if I can paste either of those here. I think I can covert the individual pages to an image. If I can't turn it into jpegs, I'll just try sending it to interested parties...
Speedo
The model includes a pedal power model, rotating and non-rotating inertia, a hill (if desired!), and aerodynamic drag. The model doesn't include rolling resistance and bearing friction. I found references for those terms, but thought that going without them would be better for a start. I'm not sure there is a closed form solution to the differential equation. It's complicated enought that I'm just going to go after it numerically.
What I have is a Word document that has been converted to pdf. I used Microsoft equations; this won't look very good in plain text. I'm not sure if I can paste either of those here. I think I can covert the individual pages to an image. If I can't turn it into jpegs, I'll just try sending it to interested parties...
Speedo
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I am off on my 3 week cycle tour of Tassie tomorrow, so won't be able to look at this until end March. I also came up with a block diagram (scribbled on paper), so we can compare notes when I get back.