Wind Power Vehicle Traveling Down Wind Faster Than The Wind

In summary: This is the part where I post the equations and simulation to show that it is possible to go faster than the wind with a propeller driven by the wheels.
  • #71
What I meant is that since the cart is moving faster than the wind, which can be seen from the countless videos, there must be a net thrusting force coming from somewhere. What I am trying to say is that just multiplying the force from the wheels shouldn't matter and I am trying to get an explanation why it does.

Imagine you are freewheeling on a regular car, except it has no air resistance and can convert motion to electricity or do pretty much anything else at 100% efficiency. There is a machine on board that produces photons and it has a flywheel connected to the wheels. The device can shoot out photons with more energy at a lower rate, increasing the thrusting force per photon, or shoot them out at any other combination. Do you agree that in such a scenario the best that is achievable at 100% efficiency is that the cart will maintain it's speed?

In the case of the wind cart, the fact that the force is multiplied somehow causes a net thrusting force on the cart, despite the fact that the power at both ends is the same. Let's make the car shoot out photons with more force but at a lower rate, increasing the force. Does the hypothetical car start accelerating? Then why does the wind cart accelerate when you multiply force, after all, the energy lost by drag and the energy used for propulsion are equal in both scenarios?

Does the reference frame matter regarding the power at the input and output?

A.T. said:
In the ground frame the equation does apply as you suggest:

power_air_to_cart = true_wind_speed x thrust

In the cart's frame:

power_ground_to_cart = ground_speed x wheel_drag
power_cart_to_air = air_speed x thrust

They should be still equal as far as I understood. If you just think about it, any energy used by the propeller to propel the air particles has to come from the wheels, because that is what moves the propeller.

Another question I have regarding the diagram. Shouldn't the path of the blade be at a right angle to the wind and vehicle speed when it is moving directly downwind? Or is the propeller supposed to not point directly upwind?

When the cart is at windspeed, you are right the wind will be horizontal and the wind will cause the blade to move forward, but, since in the cart's frame, the air is motionless around the cart and the propeller is moving around, the propeller is accelerating the air particles, not the other way around. Every action has an equal and opposite reaction, the propeller is at an angle and throws the particles in one direction and therefore the cart in the other. It takes energy to do that and the energy comes from the wheels. Any energy given to the air particles trying to propel itself is exactly the same energy that is taken from the cart, as the equations show, the joules per second at both ends are equivalent.
 
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  • #72
chingel said:
Any energy given to the air particles trying to propel itself is exactly the same energy that is taken from the cart, as the equations show, the joules per second at both ends are equivalent.

Yes, but the force isn't. Since the propeller is acting on the slow moving air, while the wheels are rolling on the fast moving ground (and power is force multiplied by velocity), the propeller is applying more force to the air than the ground is applying to the wheels (even though the power is the same).

I do think you're confusing yourself with reference frames here though. Pick one and stick with it - you can't jump around between them at will, especially since the energy and power balance is frame-dependent.
 
  • #73
chingel said:
there must be a net thrusting force coming from somewhere
net_thrust = prop_thurst - wheel_force
chingel said:
multiplying the force from the wheels shouldn't matter
It does matter becuse it makes:

prop_thurst > wheel_force

And that makes:

net_thrust > 0

chingel said:
Imagine you are freewheeling on a regular car, except it has no air resistance and can convert motion to electricity or do pretty much anything else at 100% efficiency. There is a machine on board that produces photons and it has a flywheel connected to the wheels. The device can shoot out photons with more energy at a lower rate, increasing the thrusting force per photon, or shoot them out at any other combination.
Why not add a flux compensator and some magnets, to make it even more complicated? It is simple classical mechanics that you don't get. So how does it help bringing photon thrusters into it? The air molecules are not massless and they are not produced on board.

You should read this very nice power analysis by uart based on molecules:
https://www.physicsforums.com/showthread.php?p=2063418

chingel said:
Does the reference frame matter regarding the power at the input and output?
Of course

chingel said:
They should be still equal as far as I understood. If you just think about it, any energy used by the propeller to propel the air particles has to come from the wheels, because that is what moves the propeller.
No, the wheels just turn the propeller. But the total motion of the propeller in the ground frame is not a pure rotation.

chingel said:
Another question I have regarding the diagram. Shouldn't the path of the blade be at a right angle to the wind and vehicle speed when it is moving directly downwind?
No, not in the ground frame.

chingel said:
Or is the propeller supposed to not point directly upwind?
The propeller axis is parallel to the true wind. The blades are not moving parallel to the true wind in the ground frame.

chingel said:
When the cart is at windspeed, you are right the wind will be horizontal and the wind will cause the blade to move forward, but, since in the cart's frame, the air is motionless around the cart and the propeller is moving around, the propeller is accelerating the air particles, not the other way around. Every action has an equal and opposite reaction, the propeller is at an angle and throws the particles in one direction and therefore the cart in the other. It takes energy to do that and the energy comes from the wheels. Any energy given to the air particles trying to propel itself is exactly the same energy that is taken from the cart, as the equations show, the joules per second at both ends are equivalent.
No. Read it again and repeat aloud:


In the cart's frame the cart doesn't have any kinetic energy

In the cart's frame the cart doesn't have any kinetic energy

In the cart's frame the cart doesn't have any kinetic energy

...
 
  • #74
chingel said:
What I meant is that since the cart is moving faster than the wind, which can be seen from the countless videos, there must be a net thrusting force coming from somewhere.
The net thrusting force is due to a combination of the tail wind and the propeller. If the wind speed is +10 mph, and the cart is moving at +15 mph, then the relative speed of the wind is -5 mph with respect to the cart, while the relative speed of the ground is -15 mph with respect to the cart. The ground speed is 3 times that of the air speed. The cart is designed to take advantage of this difference in speed, since the wheels interact with the faster moving ground and the propeller interacts with the slower moving air. If the effective gearing of the propeller is 1/2 of the ground speed, it would be accelerating the wind from -5 mph to -7.5 mph (1/2 of the -15 mph of the ground speed). Since the speed is cut in half at the propeller, the force could be doubled and power output would be the same as power input (if there were no losses). Since there are losses, either the force and/or speed of the thrust from the propeller will be a bit less, but if the cart is efficient, the speed can be enough to generate more thrust than the opposing force from the wheels, and in the case of BB, where the propeller's pitch (no load thrust speed) is set to 80% of the ground speed, equality between losses and the opposing forces occur at about 3.5x wind speed.

Does the reference frame matter regarding the power at the input and output?
Since power = force x speed, and since the reference frame affects the speed, the reference frame affects the magnitude of the power, but it doesn't affect the calculated forces (or the net force).
 
  • #75
hmmm...

This is odd. Why, if the cart is traveling directly downwind, would the wheels experience lateral load?

4:30 in the following video.

https://www.youtube.com/watch?v=LjLPPInzSzI

Seems to me that the wheels would only experience lateral load if the cart was tacking into the wind.
 
  • #76
OmCheeto said:
This is odd. Why, if the cart is traveling directly downwind, would the wheels experience lateral load?
It doesn't experience lateral load when it is traveling straight directly downwind. It experiences lateral load when it turns. He even explains that in the video: A bicycle tilts when it turns, so it doesn't have high lateral loads.
 
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  • #77
The Atom Man example in entirely different, he is actually saying that the generator uses less power to hurl those air molecules than the power that the generator delivers to thrust itself forward. Now if such a thing were true and I could somehow understand it, the increased power would indeed make the cart go forward.

He uses the thrust from the propeller to power the generator. Why does he multiply the propellers thrust with the vehicles speed to get the generators power? Shouldn't he multiply it by the propellers speed, i.e. the speed at which he propels the molecules?

With the ruler example, I can understand what happens. If the ruler is slippery and it takes a few seconds for the cart to catch up with the ruler, at ruler speed, when the ruler is stationary above the cart, the wheels that are touching the ground are going at speed x, the ruler also goes at speed x. Since the wheels are thinner in the middle, let's say their diameter is half of the parts' that touch the ground, they move at speed x/2. Since the big wheel is against the thinner parts of the wheels, it's surface also moves at speed x/2. If the big wheel and the ruler touch, the ruler is going faster than the big wheel, therefore friction will try to speed up the cart to match the ruler speed with the speed of the big wheel. I don't know how to apply this analogy to the wind cart, since at windspeed the wind is sitting still around the cart (in the cart's frame) and the propeller is moving faster, giving energy to the air, not as in the case of the ruler powered vehicle.
 
  • #78
chingel said:
The Atom Man example in entirely different,
It is exactly the same.
chingel said:
he is actually saying that the generator uses less power to hurl those air molecules than the power that the generator delivers to thrust itself forward.
The generator is not using power, it is generating power. Atom man is using that power to hurl molecules and create thrust that is twice the drag of the generator.

chingel said:
Why does he multiply the propellers thrust with the vehicles speed to get the generators power?
Because the generator works at the ground, so the ground speed is relevant for the generator power. He doesn't multiply the entire propeller thrust, just half of it, because he wants the generator drag to be only half of the prop thrust, so that he can still accelerate.


chingel said:
With the ruler example, I can understand what happens. If the ruler is slippery and it takes a few seconds for the cart to catch up with the ruler, at ruler speed, when the ruler is stationary above the cart, the wheels that are touching the ground are going at speed x, the ruler also goes at speed x. Since the wheels are thinner in the middle, let's say their diameter is half of the parts' that touch the ground, they move at speed x/2. Since the big wheel is against the thinner parts of the wheels, it's surface also moves at speed x/2. If the big wheel and the ruler touch, the ruler is going faster than the big wheel, therefore friction will try to speed up the cart to match the ruler speed with the speed of the big wheel.
Good so far.
chingel said:
I don't know how to apply this analogy to the wind cart,
As you correctly noted the top point of the blue gear will be moving slower than the ruler, if the cart moves at ruler speed. So the ruler will still push the cart forward. To translate this to the propeller you have to consider the point where the streamline intersects with the propeller blade. This point is also moving slower than the wind, if the cart moves at wind speed:

https://www.youtube.com/watch?v=FqJOVHHf6mQ


chingel said:
since at windspeed the wind is sitting still around the cart (in the cart's frame) and the propeller is moving faster, giving energy to the air, not as in the case of the ruler powered vehicle.
What do you mean by "not as in the case of the ruler powered vehicle"? You didn't even mention energy or power in our analysis of the ruler cart, so I don't know where you see the difference in that regard. You should stay consistent in the methods that you use to analyze the two systems, if you want to compare them.

Why don't you apply your energy arguments (that you use on the wind cart) to the ruler cart. You will find that the ruler cart is impossible, so your energy arguments are flawed.

You can also apply your velocity-matching arguments (that you use on the ruler cart) to the wind cart. You will find that is it trivially possible.
 
  • #79
A.T. said:
To translate this to the propeller you have to consider the point where the streamline intersects with the propeller blade. This point is also moving slower than the wind, if the cart moves at wind speed:

Could you explain it more a little bit? Where is the point, what streamline, where do they intersect?
 
  • #80
chingel said:
Could you explain it more a little bit? Where is the point, what streamline, where do they intersect?
In the http://www.youtube.com/watch?v=FqJOVHHf6mQ" the stream line is the horizontal column of air (blue with dots). The location where it meets the blade is moving slower than the air (in the ground frame), so the air is pushing forward on the blade. This corresponds to the top of the blue gear that moves slower than the ruler.
 
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  • #81
Why is the blade moving up? How long can it keep going like that? Is there a similar point when the blade is rotating instead of moving up?
 
  • #82
chingel said:
Why is the blade moving up?
For the airfoil the vertical axis in the diagram is the circumferential direction of the helix that the airfoil actually moves along. This is shown right at the begin.
 
  • #83
When I look at a helix from the side shouldn't I see it going up, then down, then up again etc? But then again it shouldn't matter in which direction the blade is going, it is always at a right angle to the wind in the cart's frame of reference?

In that sense the cart could go faster than the wind, but it is still very confusing, because there has to be an explanation for the energy questions I had. The generator uses power to hurl air molecules, the cart gains kinetic energy, but the generator is getting power from the cart's kinetic energy in the first place (in the cart's frame the energy will cause the ground and cart to match their speed, it doesn't matter, the amount of energy is the same and the effect is basically the same, the energy makes the cart slow down relative to the ground in either frame).

I have a question, let's say we are in zero gravity and we have zero air resistance. We have a machine that always outputs 500W at 100% efficiency. It is trying to accelerate a 1 kg weight. If we use different gear ratios, will the weight have different speeds at 1 second after the machine started running? Since no energy is lost in the transmission, all the 500W will go to the weight's kinetic energy, is that right? At 1 second the weight's kinetic energy will be 500J no matter what gears you use, or not? If we use 2:1 gear ratio, the weight will move half the distance, but since the machine also feels less resistance due to the mechanical advantage, it will speed up until it does work at a rate 500 J/s. Is that right?
 
  • #84
chingel said:
When I look at a helix from the side...
The diagram in not from the side. For the airfoil the vertical axis in the diagram is the circumferential direction.

chingel said:
But then again it shouldn't matter in which direction the blade is going, it is always at a right angle to the wind in the cart's frame of reference?
Yes, but in the ground frame is moving at some other angle, depending on the radial position and transmission ratio. In the diagram it is 45°.

chingel said:
but it is still very confusing, because there has to be an explanation for the energy questions I had.
Your questions make no sense. You confuse energy/power from different reference frames. You confuse energy/power with forces. etc.

chingel said:
I have a question, let's say we are in zero gravity and we have zero air resistance. We have a machine that always outputs 500W at 100% efficiency. It is trying to accelerate a 1 kg weight. If we use different gear ratios, will the weight have different speeds at 1 second after the machine started running? Since no energy is lost in the transmission, all the 500W will go to the weight's kinetic energy, is that right? At 1 second the weight's kinetic energy will be 500J
No, you cannot have a constant 500W kinetic energy increase if you accelerate from rest. That would mean infinite force at the begin:

F = P / v

chingel said:
...no matter what gears you use, or not?
No, you said that you want 500W kinetic energy increase. That determines you gear ratio to provide the needed force (see formula above)
 
  • #85
chingel said:
But then again it shouldn't matter in which direction the blade is going, it is always at a right angle to the wind in the cart's frame of reference?
Only at when the cart is at wind speed, and that ignores induced flow. In reality, at some speed below wind speed, induced flow will be zero relative to the ground and that is the only case when blade is moving at "right angle" to apparent wind. At faster than wind speed, the blade moves forward as well as at a right angle relative to the air.

chingel said:
In that sense the cart could go faster than the wind, but it is still very confusing, because there has to be an explanation for the energy questions I had. The generator uses power to hurl air molecules, the cart gains kinetic energy, but the generator is getting power from the cart's kinetic energy in the first place.
Energy is never obtained from the cart's kinetic energy. The power input and output are from the moving ground (earth) and/or the moving air depending on frame of reference. From the ground frame of reference, the air is being slowed down, so the air's kinetic energy is the power source. From the air's frame of reference, the Earth is being slowed down (a very tiny amount), so the Earth's kinetic energy is the power source. From the cart's frame of reference, it's a combination, and dependent on the cart's speed; once the cart is moving faster than the wind, then it takes kinetic energy from the earth, and adds kinetic energy to the air (relative to the cart).

Again using the cart's current velocity as a frame of reference:

power_input = ground_speed x ground_force_applied_to_wheels
power_output = thrust_speed x thrust_force_applied_to_air

For the BB, the propeller pitch is set to 80% of the ground speed. Because of losses in the power conversion through the drive train and at the propeller, the power output to the air is less than the power input from the ground. Assume the power losses are 10%, that means that 90% of the power_input is output to the air. The BB is very efficient otherwise, so the thrust force only needs to be a bit more than the opposing ground force for the BB reach it's max speed of 2.8x wind speed, where rolling resistance + aero drag + opposing ground force are equal and opposing thrust force. The 0.8 effective gearing allows the ground force to be multiplied by 1.25. For example, the losses may reduce the force multiplier to 1.12, but 12% more thrust force than opposing ground force allows the BB to go downwind faster than the wind. I don't know the actual numbers involved with forces and losses, only that under good conditions, the BB has gone 2.8x wind speed.

update - the last "official record speed" I see for BB mentions 2.8x wind speed. I don't know what the issue was for the reported 3.48x wind speed, other than it wasn't considered an "official record".
 
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  • #86
Academic said:
Well, I guess I don't have half-decent brain power because I thought about for a few minutes and couldn't come up with it. Damn my less than half decent brain...

Well, I am just a ninth grade Physical Science and Math Teacher, so I guess I will probably never have a half-decent brain. Is it ok for me to comment or ask questions on this site? I was thinking that if I could understand this, then maybe I could teach it to my students.
How can one expect a half-decent brain to understand it if a wholly-decent brain is not sure it works without actually doing an experiment to see if it will work?
I think it is reasonable to question whether it would work. I have taken several Physics courses and never recall coming across the problem. I think it natural for many to think that if a load is applied to wheels that are in some way matched to wind speed, the wheels would slow down. On the other hand all of my ninth grade students seem to understand how a sail boat can theoretically go much faster than the wind. When they asked me if it was possible to go faster downwind, I thought probably some sort of arrangement of gearing attached to a wind - mil should work. Yet as I think about even the videos (which I finally watched) and even as I think about the explanations, seems like sometimes I get it and sometimes I don't.
 
  • #87
Fun Value said:
I think it natural for many to think that if a load is applied to wheels that are in some way matched to wind speed, the wheels would slow down.
The load on the wheels is not related to wind speed, instead the load is related to the torque it takes to drive the propeller. As mentioned before this load translates into an opposing force from the ground, and this force times the the ground speed (relative to the cart) is the input power used to drive the propeller. In the meantime, the propeller interacts with the slower moving air (and not the ground), whenever the cart operates with a tailwind. This allows an effective gearing where speed is divided and torque is multiplied to result in more force from the propeller but at a lower air speed. The torque it takes to drive the propeller is related to the mass and the rate of acceleration of the air affected by the propeller (and the efficiency of the propeller).

From a ground frame of reference, the thrust produced from the propeller slows down the wind, and that is the source of energy that is consumed by the losses in the cart which are related to rolling resistance, aerodynamic drag, and losses in the drivetrain.

An example of another device that operated on a similar principle is the Brennan torpedo, which used wires that were retracted to drive propellers that drove the torpedo forwards. It was geared so that the rate of wire retraction was greater than the torpedo's forward speed (relative to a water based frame of reference), which allowed the propellers to produce more thrust than the opposing force of the retracting wires:

http://en.wikipedia.org/wiki/Brennan_torpedo

Continuing with this comparason. If there was a stream of water and the torpedo was moving down stream (and steering wasn't an issue), then the wires could be attached to a fixed base, and the torpedo would move faster than the stream. For example, a Brennan torpedo moving at 15 mph in a 10 mph stream. From the torpedoe's frame of reference, wire speed is -15 mph, water speed is -5 mph, which allows the effective wire to propeller gearing to almost 3:1, multiplying the force, dividing the speed, ...
 
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  • #88
The multiplying the force explanation makes no sense to me. So if I have the 500W engine, will using a 2:1 gear ratio make the weight accelerate faster than using a 1:1 gear ratio? After all, it also multiplies the force. I would think it does not make it accelerate faster, since nothing is lost in the transmission, all the 500W go to the weight's kinetic energy. After 1 s the weight will have 500J of kinetic energy, it's speed will be E=1/2*m*v^2; v=(2/m)^0,5=2^0,5

F=ma, but if you think about it, the gear at the weight moves slower, therefore it feels less resistance from the weight, because due to the slower speed it is trying to accelerate it slower. Then the mechanical advantage makes the engine feel even less force. So the engine speeds up until it is doing 500J of work. Is that wrong or not?

A.T. said:
No, you cannot have a constant 500W kinetic energy increase if you accelerate from rest. That would mean infinite force at the begin:

F = P / v

But that would mean that the force would have to be infinite for any power, since the v is zero.
 
  • #89
chingel said:
The multiplying the force explanation makes no sense to me. So if I have the 500W engine, will using a 2:1 gear ratio make the weight accelerate faster than using a 1:1 gear ratio?
Do you drive a real car or motorcycle? Does the car accelerate faster in first gear than it does in top gear, and is the maximum speed you can go much lower in first gear than it is in top gear?

You're focusing too much on the power issue. The only issue with power is that total power output must be less than total power input since there are always losses with most real devices.

What allows the cart to work is that the wheels interact with the ground while the propeller interacts with the air. If the air is moving with respect to the ground, then the cart can take advantage of this when going downwind, because the speed of the air will be less than the speed of the ground, no matter how fast the cart is moving. If the cart was a perfect machine, there would be no limit to how fast it could go because the difference in speed between the air and the ground wouldn't be affected by the cart. A real cart does slow down the air, but how much it needs to slow down the air depends on how efficient the cart is. The cart uses gearing (advance ratio) to take advantage of the difference in speed between air and ground so that the combined force between the wind and propeller is greater than the opposing force of the wheels that drive the propeller, and that extra bit of force allows the cart to accelerate to a faster speed unitl the other opposing forces related to rolling resistance, aerodynamic drag, and drive train losses, cancel out that extra bit of force.
 
  • #90
mender said:
But even with all the answers, sometimes it has to be explained in the right order and the right way for the light bulb to go on.

Also, for some of us, probably most of us, it takes a lot of repetition until certain facts become concrete in our minds. Still, for me, when I am not thinking correctly, it is amazing that the wind powered car can go against (or should I say “against?”) the very wind that is propelling it - kind of a concrete foundation in my mind.
While I am at it, I think a number of students might have many other ideas. For example they might wonder if a vortex is created by the propeller thereby bringing air into the center at an angle from outside the system. Maybe someone will eventually be able to demonstrate whether this and many other things happen using a wind tunnel.
I think it is good for students to try to analyze such a problem, try to figure it out for themselves before having it explained so they can see some of those false foundations upon which they have been building.
Finally I hope that I will be able to remember why I had difficulty so I can teach others.
I can admit that some things in science have become so simple that I have forgotten what I used to think before I understood it – forgotten some of the reasons students don’t get it.
 
  • #91
rcgldr said:
Do you drive a real car or motorcycle? Does the car accelerate faster in first gear than it does in top gear, and is the maximum speed you can go much lower in first gear than it is in top gear?

I thought that was due to inefficiency problems of the engine, i.e. the engine can only deliver a certain amount of force per explosion, because there is a certain amount of oxygen in the cylinder head and it can't run at very low speeds or it dies out. So that at 600 rpm it is not capable of outputting the same power as at 2000 rpm. Electric cars don't use transmissions because they don't have such problems as power depending on the rpm as much as the combustion engine does. But I am asking if the power is always the same, will the weight accelerate faster if it uses gears to multiply the force? Because I keep on reading that multiplying the force is the explanation, I don't understand it and I tend to think that multiplying the force shouldn't matter, but I am not a scientist.

I don't know any calculus so I can't do any calculations. I assume that you need calculus to calculate it out? Because as the engine applies force at a certain speed, the weight accelerates, offers less resistance, the engine has to move faster but reduce force since it only can do 500W etc and you have to use infinitely small steps because the weight is continuously accelerating. But, looking at the big picture, since no energy is lost in the transmission, all the power should go to the weight in my understanding.

Another idea I had is to put the propeller parallel to the wind and cover the bottom half with an aerodynamic shape, this way it is directly analogous to the ruler example, everything is exactly the same, but instead of the ruler pushing the top wheel the wind is pushing the propeller. Nevertheless I am still struggling with it, let's say the propeller is disconnected, then when I connect it, it uses energy to go slower than the wind and that energy does work to slow the cart down relative to the ground.
 
  • #92
Fun Value said:
It is amazing that the wind powered car can go against (or should I say “against?”) the very wind that is propelling it
Upwind carts are possible, in this case the advance ratio or the effective gearing is greater than 1, and the propeller acts as a turbine instead, drving the wheels to move the cart against the wind. Even in this case the only limitation to how fast it can move upwind depends on the efficiency of the cart, and the limitation of dealing with higher aerodynamic drag than the downwind case.

I'll assume that you mean the cart outruns the wind that propels it. However what's propelling the cart is the combination of the wind and the ground moving at different speeds. Here's another link to that youtube video posted earlier about a cart propelled by a ruler and the ground moving at different speeds, geared so that the cart moves about twice as fast at the ruler (using the ground as a frame of reference) The gearing (advance ratio) is set so that the upper wheel surface speed is about 1/2 the surface speed of the lower spools:



Getting back to the wind + ground driven cart, although the cart does move faster than the wind, the air flow from the propeller does not. From a ground frame of reference, the cart can only work when the thrust from the propeller slows down the wind. Just aft of the propeller is a compressed (and moving) volume of air, that generates equal and opposing forces to the air and to the propeller, (the magnitude of this force is equal to the thrust force of the propeller). The force applied to the propeller drives the cart forwards,while the force applied to the air slows the air down (relative to a ground frame of reference).

Again this only works because the air speed is different than the ground speed, and in a downwind situation, because relative to the cart, the air speed is less than the ground speed. Similarly, a sailboat can't move faster than the wind unless the air speed is different than the water (or land or ice) speed.

chingel said:
Electric cars don't use transmissions because they don't have such problems as power depending on the rpm as much as the combustion engine does.
That's because they are willing to sacrifice acceleration and/or top speed. Some Tesla electric cars have two speed transmissions, but they are working on some issues:

http://en.wikipedia.org/wiki/Tesla_Roadster#Transmission

An ideal electric motor produces maximum power near the middle of it's rpm range. It produces peak torque at low rpm (unless overheat protection circuitry limits the current at very low rpms), and zero torque at it's peak rpm. Scroll down to section 3.2 to see a graph of this:

http://lancet.mit.edu/motors/motors3.html

chingel said:
Because as the engine applies force at a certain speed, the weight accelerates, offers less resistance.
The resistance to acceleration relative to weight (mass) is the same regardless of speed. Force = mass x acceleration, so acceleration = force / mass. Also power = force x speed, so in the case of constant power, as speed increases, force and acceleration decrease (assuming the weight (mass) isn't changing).

Another idea I had is to put the propeller parallel to the wind and cover the bottom half with an aerodynamic shape, this way it is directly analogous to the ruler example, everything is exactly the same, but instead of the ruler pushing the top wheel the wind is pushing the propeller.
That's essentially a water wheel. If using this concept works for you, note that a propeller is more efficient than a water wheel or squirrel cage type fan, so using a propeller will produce a faster cart. You could have a sail connected to a conveyor belt that moves upwind as the cart moves downwind, then have the sail collapse on the return trip and a second sail that would deploy as the first sail collapses. Again this two sail + conveyor belt setup would be less efficient than a propeller, but if it helps you understand the concept, ...
 
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  • #93
chingel said:
After all, it also multiplies the force. I would think it does not make it accelerate faster,
...
F=ma,
You answered you own question there.

chingel said:
since nothing is lost in the transmission, all the 500W go to the weight's kinetic energy.
That is an impossible scenario that you describe here. The engine cannot deliver KE at 500W to a resting weight. If no losses are possible (perfectly rigid connection), the engine simply cannot work at 500W from rest. The power will start at 0W and then increase.

If you use a 500W laser to accelerate a perfectly reflective weight (non rigid connection), then at v=0 the reflected light has the same frequency (and thus power) that comes from the laser. So at v=0 the power that goes into the weights KE is zero.

Another reason why the increase in KE has nothing to do with "engine power": The first is frame dependent, while the later is frame independent.

chingel said:
But that would mean that the force would have to be infinite for any power, since the v is zero.
No, not for any power. For P = 0 the force can be a finite number at v = 0 and still satisfy P = F * v
 
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  • #94
chingel said:
Another idea I had is to put the propeller parallel to the wind and cover the bottom half with an aerodynamic shape, this way it is directly analogous to the ruler example,

The spool example is even simpler:

https://www.youtube.com/watch?v=E7vcQcIaWSQ

The wind powered version would need an aerodynamic shape on top.

https://www.youtube.com/watch?v=Ufk6HVWdSzE

It could potentially work, but paddle-wheels are very inefficient. Here is a real model:

https://www.youtube.com/watch?v=TcSh0qqgYKc .

I think it would have to be much bigger to go faster than wind in "normal" winds. Propellers are more efficient and thus the easier way.
 
  • #95
A.T. said:
That is an impossible scenario that you describe here. The engine cannot deliver KE at 500W to a resting weight. If no losses are possible (perfectly rigid connection), the engine simply cannot work at 500W from rest. The power will start at 0W and then increase.

Ok, but what does this mean? Let's say that for the first Planck second the power is 0 and after that it is 500W. Or let's imagine that the weight is already moving at a speed of a Planck distance per decade. Cars can still start moving and engines can start running from a stop despite the fact that the engine can't produce any power when it is at rest.

All I want to know is that assuming a zero loss frictionless massless transmission and an engine producing constant power, if we use a different gear ratio to multiply force, would the weight be moving faster after 1 second? I can't see how, because if the engine does 500W of work, it cannot go anywhere else other than the kinetic energy of the weight.

Here is a pdf I found helpful:

http://www.greglondon.com/tumbleweed/tumbleweed.pdf

But I still feel somewhat confused due to the questions I am having.
 
  • #96
  • #97
chingel said:
Cars can still start moving and engines can start running from a stop despite the fact that the engine can't produce any power when it is at rest.
Acceleration is caused by forces, not power.

chingel said:
...engine producing constant power ... because if the engine does 500W of work, it cannot go anywhere else other than the kinetic energy of the weight.
Think about a moving observer. He will see the same engine but a different change of kinetic energy of the weight.
 
  • #98
Here's as far as I've gotten with my point of view. I feel like I am on to something, but please stop me if I am headed in the wrong direction or on a dead end. Since I have taught 9th grade science for so long, I guess I am thinking at that level.

It makes sense that the vehicle could go almost the speed of the wind without the propeller. Now engage the propeller with the wheels to the ground. I think (not sure) one of three things would now happen:
1.) The propeller would cause an increase in speed if the propeller is of sufficient radius that most of the propeller is perpendicularly hitting the air at more than wind speed,
2.) The propeller would cause the vehicle to stay the same speed if the propeller radius is smaller,
3.) The propeller would cause the vehicle to slow if the propeller is even shorter.

When the propeller of sufficient radius is engaged, the vehicle can at least keep the same speed - I get that. I guess I can't prove it, but yes it does seem that the propeller would add to the speed of the vehicle. I do not see any reason it would slow it down. The perpendicular motion can only translate the velocity between wheels and ground into additional forward thrust (I think).

If the propeller is of small radius so that most of the propeller is slow, then I guess it seems like the oncoming wind from the front would tend to slow the propeller and the vehicle - wouldn't it?

Like I said, I am trying to see this from a 9th grade point of view.
 
  • #99
Fun Value said:
The propeller ... radius.
The effective gearing of the propeller is related to it's pitch. The propellers "pitch" is how far it would tend to travel forward per revolution (similar to how far a screw would move in a solid per revolution).

what_is_propeller_pitch.html

The actual effect on the air depends on the propellers radius and pitch. The radius determines the amount of air affected, and the pitch and angular (rotating) speed determine by how much the affected air is accelerated. The actual thrust speed and force depend on radius, pitch, angular speed of the propeller, and the wind speed relative to the cart.

The "effective gearing" is the ratio of thrust speed divided by the ground speed, relative to the cart. If the effective gearing is less than zero (negative), the propeller acts as a turbine to drive the wheels at less than tailwind speed. If the effective gearing is zero, the propeller acts like a sail. If the effective gearing is greater than zero and less than one, the propeller tries to make the cart go downwind faster than the wind. If the effective gearing is one (or too close to one), it could tend to limit speed (via a braking effect on the wheels). If the effective gearing is greater than one, the propeller acts as a turbine, but now in reverse and tends to move the cart into the wind (upwind).

If the propeller radius is too small, then it doesn't generate sufficient force to affect the cart more than the affect of the wind on the cart itself. The larger the radius of the propeller, the higher the forces at the propeller and the tires. If the radius of the propeller is too large, then friction between the tires and ground could be an issue.
 
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  • #100
rcgldr said:
The "effective gearing" is the ratio of thrust speed divided by the ground speed, relative to the cart. If the effective gearing is less than zero (negative), the propeller acts as a turbine to drive the wheels at less than tailwind speed. If the effective gearing is zero, the propeller acts like a sail. If the effective gearing is greater than zero and less than one, the propeller tries to make the cart go downwind faster than the wind. If the effective gearing is one (or too close to one), it could tend to limit speed (via a braking effect on the wheels). If the effective gearing is greater than one, the propeller acts as a turbine, but now in reverse and tends to move the cart into the wind (upwind).

See also that table:
http://i54.tinypic.com/2gv0kew.png
 
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  • #101
Thank you A.T. and rcgldr for all of your patient explanations and demos. I love this stuff and I am sure my students will also. For most of my students this really will have to be learned from hands on learning projects. Oh, and even my wife, a librarian is getting into this!
 
  • #102
Fun Value said:
Thank you A.T. and rcgldr for all of your patient explanations and demos. I love this stuff and I am sure my students will also. For most of my students this really will have to be learned from hands on learning projects. Oh, and even my wife, a librarian is getting into this!

Will you build a cart and demonstrate it in class?
 
  • #103
Here is another question I have.

If I put brakes on a free spinning wheel, will the wheel stop faster when I put the brakes near the edge of the wheel than when I put the brakes near the center of the wheel, assuming constant force from the brakes? I would tend to think that when I apply them closer to the edge, it would slow down faster, and as long as the ratio of speed at contact point x force stays the same, it would stop in the same time. Essentially as long as the power is the same, J/s, that is how much kinetic energy the wheel will lose. Is this idea wrong or not with the spinning wheel and brakes example?

If I read about the work-energy principle, in my understanding it says that:

http://hyperphysics.phy-astr.gsu.edu/hbase/work.html

The change in an objects kinetic energy is equal to the work done on the object. So to make the cart move faster than the wind, ie to increase the kinetic energy of cart, work has to be done on it, it's not just force. Doesn't this also mean that as long as the engine is doing 500W of work, the objects kinetic energy is increasing at a rate of 500 J/s, no matter what the gearing is?

On the other hand these same questions can be asked about the Yo-Yo or the tumbleweed example, yet I can sort of understand why they move faster than the string is pulling or wind is pushing. What is the big picture?


Is there something wrong in the tumbleweed pdf or does the author generally have a bad reputation with applying physics the wrong way?
 
  • #104
chingel said:
If I put brakes on a free spinning wheel, will the wheel stop faster when I put the brakes near the edge of the wheel than when I put the brakes near the center of the wheel, assuming constant force from the brakes?

Yes, if we assume constant force from the brakes (no brake fading, etc.), the wheel will slow down much more rapidly if I apply the force at a greater radius. We can see that in two different ways. From a force point of view, we would be applying twice as much slowing torque if we apply the force at twice the initial radius.

From an energy point of view, we can see that we're doing much more work "against" the wheel because we're applying the same force against a faster moving point on the wheel (power = energy/time = force x velocity).

I would tend to think that when I apply them closer to the edge, it would slow down faster, and as long as the ratio of speed at contact point x force stays the same, it would stop in the same time.

You're correct.

If I read about the work-energy principle, in my understanding it says that:

http://hyperphysics.phy-astr.gsu.edu/hbase/work.html

The change in an objects kinetic energy is equal to the work done on the object. So to make the cart move faster than the wind, ie to increase the kinetic energy of cart, work has to be done on it, it's not just force.

Still correct.

Doesn't this also mean that as long as the engine is doing 500W of work, the objects kinetic energy is increasing at a rate of 500 J/s, no matter what the gearing is?

Yes. But we have to be careful - we may be losing 500 J/s of energy to aerodynamic drag, rolling resistance, etc. In that case the engine could do 500 J/s all day without the car ever accelerating.

Is there something wrong in the tumbleweed pdf or does the author generally have a bad reputation with applying physics the wrong way?

I read the original document. It was riddled with shamefully wrong statements. I know he's re-written it at least once. I don't care to grade every version of it for him. But I am happy to answer any questions you have.
 
  • #105
spork said:
But I am happy to answer any questions you have.

Can you answer my question?

Where can I find Nikos's comments on the experiment?

:wink:
 

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