Work done running on an inclined treadmill

In summary: Suppose you attached a monitor to your upper...body so you could see how much work you're doing.This is not necessary - you can just use your intuition. This is not necessary - you can just use your intuition.
  • #1
harrylentil
33
5
Why does it cost roughly the same effort to run against an inclined treadmill as up a hill of the same inclination? That is neglecting the movement of the legs and the bobbing up and down as we run and the wind resistance. I remember being told in school physics that there is no work done unless a mass is accelerated or raised. To a first approximation, on a treadmill we do not ascend and we do not accelerate.
When running up a hill you are going up. So the treadmill should be nearly effortless as you are not raising a weight hence not doing work. Of course it is not effortless so where is my error?
 
Physics news on Phys.org
  • #2
harrylentil said:
Why does it cost roughly the same effort to run against an inclined treadmill as up a hill of the same inclination? That is neglecting the movement of the legs and the bobbing up and down as we run and the wind resistance. I remember being told in school physics that there is no work done unless a mass is accelerated or raised. To a first approximation, on a treadmill we do not ascend and we do not accelerate.
When running up a hill you are going up. So the treadmill should be nearly effortless as you are not raising a weight hence not doing work. Of course it is not effortless so where is my error?

It's not as hard to move on a treadmill as uphill on the ground at the same angle, but it is harder than a treadmill on the flat. Basically, the treadmill is moving part of your body (the foot and leg) downhill at each step - so, to some extent, your centre of mass. To stay at the same point on the treadmil, you have to keep moving at least some of your body upwards.

On a real hill, you have to move all your body up the whole time. And that, I think you'll find, is a lot harder than uphill on a treadmill.
 
  • #3
PeroK said:
It's not as hard to move on a treadmill as uphill on the ground at the same angle, but it is harder than a treadmill on the flat. Basically, the treadmill is moving part of your body (the foot and leg) downhill at each step - so, to some extent, your centre of mass. To stay at the same point on the treadmil, you have to keep moving at least some of your body upwards.

On a real hill, you have to move all your body up the whole time. And that, I think you'll find, is a lot harder than uphill on a treadmill.

Is it not the case that you have to keep moving your whole body upwards on a treadmill to counter the tread's movement? Say you weigh 60kg. Is the inclined treadmill not somehow forcing you to move all 60kg constantly upward (in a way I don't understand) and not just your legs?
 
  • #4
harrylentil said:
Is it not the case that you have to keep moving your whole body upwards on a treadmill to counter the tread's movement? Say you weigh 60kg. Is the inclined treadmill not somehow forcing you to move all 60kg constantly upward (in a way I don't understand) and not just your legs?

No. Your head and upper body remain essentially at the same height.
 
  • #5
PeroK said:
No. Your head and upper body remain essentially at the same height.

I'm having difficulty with this. I can see that your body mostly does not ascend on the treadmill at any time and wholly does not ascend on average (at the end of the run you are in the same place) and you seem to be saying that you do not have to work against the backward movement of the tread to stay put, except for a small component of work involving your lower body. This is not an answer I was expecting because I basically think it is false. I think you do have to work to keep your whole weight stationary against the tread. I asked the original question to find out how.
 
  • #6
harrylentil said:
I'm having difficulty with this. I can see that your body mostly does not ascend on the treadmill at any time and wholly does not ascend on average (at the end of the run you are in the same place) and you seem to be saying that you do not have to work against the backward movement of the tread to stay put, except for a small component of work involving your lower body. This is not an answer I was expecting because I basically think it is false. I think you do have to work to keep your whole weight stationary against the tread. I asked the original question to find out how.

Suppose you attached a monitor to your upper body. How would it detect that you are on a inclined treadmill? If your upper body is not moving, it's not moving.
 
  • #7
PeroK said:
Suppose you attached a monitor to your upper body. How would it detect that you are on a inclined treadmill? If your upper body is not moving, it's not moving.

If you stop working then your whole body shoots downward. To keep your whole body stationary you have to work.
 
  • #8
harrylentil said:
If you stop working then your whole body shoots downward. To keep your whole body stationary you have to work.

I can do about 6.5 km/h on a 15° treadmill at the gym. On a 15° hill, I can do about 4 km/h. There is no comparison in the effort involved. You have to do no work to stop your body falling. That is no different from standing or walking on the flat.
 
  • #9
PeroK said:
I can do about 6.5 km/h on a 15° treadmill at the gym. On a 15° hill, I can do about 4 km/h. There is no comparison in the effort involved. You have to do no work to stop your body falling. That is no different from standing or walking on the flat.

PS I was at the gym today - honestly. I did 20 minutes at 15° at an average of 6 km/h. That is about 500m of ascent in 20 mins. My normal outdoor speed on a mountain is about 600m of ascent an hour. The reason is clear: on the treadmill my upper body is not moving; on a hill, my whole body is moving upwards.
 
  • #10
PeroK said:
PS I was at the gym today - honestly. I did 20 minutes at 15° at an average of 6 km/h. That is about 500m of ascent in 20 mins. My normal outdoor speed on a mountain is about 600m of ascent an hour. The reason is clear: on the treadmill my upper body is not moving; on a hill, my whole body is moving upwards.

I admit I'm surprised.
 
  • #11
harrylentil said:
I admit I'm surprised.

It's quite different muscles as well. The uphill treadmill mostly works the calves and not much on the quads. In the mountains, it's both calves and quads that do the work. You really have to push hard to move your body up a mountain. It's much harder than the same speed on a treadmill. If I set the treadmill at my normal outdoor uphill speed of about 3 km/h it would hardly be a workout. That's just easy.
 
  • #12
PeroK said:
No. Your head and upper body remain essentially at the same height.
Completely irrelevant.

The work that is not done raising your body is done moving the treadmill belt downward. Exactly the same net work done running uphill as on an upward-slanting treadmill.
 
  • #13
jbriggs444 said:
Completely irrelevant.

The work that is not done raising your body is done moving the treadmill belt downward. Exactly the same net work done running uphill as on an upward-slanting treadmill.

The treadmill moves itself. There is no need to do any work to move the treadmill. To make it go faster, you press a button!

In any case, it is far, far easier to walk or run uphill on a treadmill than on a real hill. For example, at 15° I can comfortably do 6 km/h, which equates to 1,500m of ascent an hour. On a real hill, I would max out at 750m of ascent an hour.

1,500m of ascent an hour would make me a world-class mountain runner!
 
  • Like
Likes davenn
  • #15
jbriggs444 said:
The work that is not done raising your body is done moving the treadmill belt downward. Exactly the same net work done running uphill as on an upward-slanting treadmill.
jbriggs, I usually find your comments spot on but I think you seriously missed the boat on this one. (1) The treadmill moves exactly the same whether you are on it or not and (2) yes it DOES matter that you are not raising your center of mass.
 
  • Like
Likes davenn and PeroK
  • #16
phinds said:
jbriggs, I usually find your comments spot on but I think you seriously missed the boat on this one. (1) The treadmill moves exactly the same whether you are on it or not and (2) yes it DOES matter that you are not raising your center of mass.
Sorry, you are wrong in this case. The force of the feet on the treadmill is not irrelevant.
 
  • #17
PeroK said:
The treadmill moves itself. There is no need to do any work to move the treadmill. To make it go faster, you press a button!
Completely irrelevant. The work done by feet on belt is the same regardless of what other forces act on the belt.
 
  • #18
jbriggs444 said:
Completely irrelevant.

What isn't irrelevant is that my gentle warm-up on the treadmill is 4 km/h at 15°, which equates to 1,000m of ascent an hour and is much faster than I could do on a real hill.

There is simply no comparison. If you climbed mountains and went to the gym, you would know this for yourself.
 
  • #19
PeroK said:
What isn't irrelevant is that my gentle warm-up on the treadmill is 4 km/h at 15°, which equates to 1,000m of ascent an hour and is much faster than I could do on a real hill.
Irrelevant. The physics of the situation is what it is.
 
  • #20
jbriggs444 said:
Irrelevant. The physics of the situation is what it is.

... says he from the comfort of his armchair!
 
  • #21
Generate the free body diagram. Calculate the work done by the body on the treadmill. Pick up a pencil and calculate.
 
  • #22
jbriggs444 said:
Generate the free body diagram. Calculate the work done by the body on the treadmill. Pick up a pencil and calculate.

By that method, the work is approximately zero, as the body is not moving. On the treadmill, your centre of gravity is (approx) stationary. As one leg moves dowwards, the other moves upwards, maintaining your centre of gravity at a fixed point.

The only work is moving your limbs.
 
  • #23
PeroK said:
By that method, the work is approximately zero, as the body is not moving.
Where is that free body diagram? I did not ask for the work of the treadmill on the body. I asked for the work of the body on the treadmill.

Edit: I am interested in the real work done at the foot-belt interface rather than "center-of-mass" work done on the treadmill as a whole. Neither the runner nor the treadmill are rigid bodies. Attempting to apply conservation-of-energy arguments based on center-of-mass work will lead to erroneous conclusions -- this thread being a case in point.
 
Last edited:
  • #24
PeroK said:
That's still approximately zero, as your feet are stationary with respect to the treadmill's surface.
Pick a frame of reference and stick with it.

From the ground frame, the treadmill's surface is moving. But it seems that you wish to adopt the belt frame. That's fine. But in that frame, the runner's legs are lifting his body exactly as if he were running up a fixed incline.
 
  • Like
Likes PeroK
  • #25
Let me try this thought experiment on you. It takes the form of a series of scenarios which I claim are all equivalent to one another from the runner's point of view. I want you to identify which scenario in the series first breaks the equivalence.

1. The runner is climbing a track on a hill with a fixed incline. The track is made of a rubbery material and extends for several hundred yards up-slope.

2. The hill is mounted on an aircraft carrier steaming slowly west on calm waters as the runner runs east. The aircraft carrier maintains a speed so that the runner makes no progress compared to the water beneath. The runner does, however end his run higher than he started.

3. The aircraft carrier is still steaming west, but now it is sinking as it moves so that the runner's height above water remains constant. [Assume that the carrier maintains speed and remains upright as it sinks]. Now the runner ends his run exactly where he started.

4. Replace the long track that was fixed to the carrier with a treadmill on an island, arranging for the surface where the runner runs to be moving west and down exactly like the track surface that was on the aircraft carrier in scenario 3.
 
  • #26
Since the human body in motion is a complex system, why not simplify the matter. Consider using a Segway on the treadmill next time you are at the gym. Now it becomes a rotational work problem.
 
  • Like
Likes jbriggs444
  • #27
I didn't think my query would be controversial. I was expecting someone to explain where and how my assumption of zero work was wrong, because I thought it was wrong. I am glad to see that it might clarify a more widespread misunderstanding. I haven't seen a clear and simple explanation yet, though.
 
  • #28
harrylentil said:
I didn't think my query would be controversial. I was expecting someone to explain where and how my assumption of zero work was wrong, because I thought it was wrong. I am glad to see that it might clarify a more widespread misunderstanding. I haven't seen a clear and simple explanation yet, though.
Let's see you justify the claim of zero work. What force are you considering acting on what body?
 
  • #29
jbriggs444 said:
Where is that free body diagram? I did not ask for the work of the treadmill on the body. I asked for the work of the body on the treadmill.

Edit: I am interested in the real work done at the foot-belt interface rather than "center-of-mass" work done on the treadmill as a whole. Neither the runner nor the treadmill are rigid bodies. Attempting to apply conservation-of-energy arguments based on center-of-mass work will lead to erroneous conclusions -- this thread being a case in point.

We have:

a) a theoretical argument that shows that the work done on a treadmill is the same as on a real hill.

b) the empirical evidence that this is not the case.

Edit: I'll leave this post in, but I don't think we need any such complicated explanation. See my later posts about gravity providing the force in the case of a treadmill, but not in the case of moving uphill.

I think I have the explanation. It's certainly more complicated than it first appeared. When you walk (on the flat or uphill) you tend to bounce up. On a inclined treadmill, it's clear that the force is not constant. You give a very definite push with each foot for a short time and then ease off. This raises your centre of gravity for a short time. The push is vertical, rather than tangential to the treadmill, but it's probably a bit of both. The greater the vertical force, the longer the weight is off your feet and the longer you do not need to apply a force against the treadmill.

By this mechanism, you avoid having to apply the tangential force against the treadmill for all the distance.

On the flat or at slow speeds, this bouncing would be inefficient. But, as the treadmill speed increases, it becomes more economical to adopt this bouncing gait. Certainly, this is what happens with me as the treadmill speeds up. It's a very definite sequence of short sharp pushes with each foot.

It's too late today to look at this, but I'll try to do some basic calculations tomorrow. It's not clear to me whether you do save energy this way, but the evidence of walking uphill suggests it must be so.
 
Last edited:
  • #30
jbriggs444 said:
Let's see you justify the claim of zero work. What force are you considering acting on what body?

Slow down. I was expecting to be contradicted, and rightly. Read my sentence again. I am stating, clearly I think, that my zero-work assumption is wrong.
 
  • Like
Likes phinds
  • #31
harrylentil said:
Slow down. I was expecting to be contradicted, and rightly. Read my sentence again. I am stating, clearly I think, that my zero-work assumption is wrong.
Fair enough. The zero-work assumption is wrong.

@lewando is trying to direct us on a productive course. But rather than replace legs with wheels, I would prefer to idealize things differently and assume for the moment that we are dealing with massless legs. The legs have two external interfaces. One at the hips where they push upward. One at the feet where they push downward. If we wish to compute the net work done by the legs, we should examine both interfaces.

We can make the further simplifying assumption that there are, on average, no horizontal forces. Realistically there would be wind resistance, but we can reasonably neglect this (or put a fan in front of the treadmill to generate a headwind). Realistically, there is energy dissipation in the strike of foot on track. But I do not think that is the effect that that we are trying to concentrate on. So let us ignore that as well. In the absence of horizontal forces, we are concerned entirely with the upward force of leg on hip and the downward force of leg/foot on track. And we are concerned entirely with the vertical motion at those two interfaces.

We have two scenarios to compare.

In one case (climbing a hill), the hips are moving upward at a vertical velocity of +v and the feet, when planted on the ground, are not moving at all. The force at the hip is equal to the weight of the runner's body. Call that mg. The force at the feet is, on average, equal and opposite (recall that we are still under the simplifying assumption of massless legs). Call this scenario A.

In the other case (climbing a treadmill), the hips are stationary and the feet, when planted on the track, are moving downward. Their vertical velocity is -v. The force at the hip is still equal to the weight of the runner's body. The force at the feet is, on average, equal and opposite. Call this scenario B.

Let us tot up the work being done by the legs in scenario A. That's ##mg \cdot v + (-mg) \cdot 0 = mgv##
Let us tot up the work being done by the legs in scenario B. That's ##mg \cdot 0 + (-mg) \cdot (-v) = mgv##

Edit: A concern had been raised earlier that the motor on the treadmill was somehow contributing to the energy balance. However, that concern is misplaced. The work and energy associated with the motor and any friction in the bearings are not relevant. Those forces act between the treadmill's mechanism and its belt. They do not enter into a calculation of work done by the runner.
 
Last edited:
  • Like
Likes harrylentil
  • #32
jbriggs444 said:
Pick a frame of reference and stick with it.

From the ground frame, the treadmill's surface is moving. But it seems that you wish to adopt the belt frame. That's fine. But in that frame, the runner's legs are lifting his body exactly as if he were running up a fixed incline.

No. Because when you are on the treadmill it's gravity that is providing the force. The force on the treadmill is not being generated by the use of your muscles, but by gravity pushing your weight into the treadmill.

When you genuinely move uphill, your weight is supported, but each step you must move your entire mass against gravity by using your muscles.
 
  • #33
jbriggs444 said:
We can make the further simplifying assumption that there are, on average, no horizontal forces. Realistically there would be wind resistance, but we can reasonably neglect this (or put a fan in front of the treadmill to generate a headwind). Realistically, there is energy dissipation in the strike of foot on track. But I do not think that is the effect that that we are trying to concentrate on. So let us ignore that as well. In the absence of horizontal forces, we are concerned entirely with the upward force of leg on hip and the downward force of leg/foot on track. And we are concerned entirely with the vertical motion at those two interfaces.

We have two scenarios to compare.

In one case (climbing a hill), the hips are moving upward at a vertical velocity of +v and the feet, when planted on the ground, are not moving at all. The force at the hip is equal to the weight of the runner's body. Call that mg. The force at the feet is, on average, equal and opposite (recall that we are still under the simplifying assumption of massless legs). Call this scenario A.

In the other case (climbing a treadmill), the hips are stationary and the feet, when planted on the track, are moving downward. Their vertical velocity is -v. The force at the hip is still equal to the weight of the runner's body. The force at the feet is, on average, equal and opposite. Call this scenario B.

Let us tot up the work being done by the legs in scenario A. That's ##mg \cdot v + (-mg) \cdot 0 = mgv##
Let us tot up the work being done by the legs in scenario B. That's ##mg \cdot 0 + (-mg) \cdot (-v) = mgv##

Edit: A concern had been raised earlier that the motor on the treadmill was somehow contributing to the energy balance. However, that concern is misplaced. The work and energy associated with the motor and any friction in the bearings are not relevant. Those forces act between the treadmill's mechanism and its belt. They do not enter into a calculation of work done by the runner.

Let's take scenario C: you are standing on a treadmill that is moving down.

The work being done by the legs is still ##mgv##. It's the same forces as before. You can see the error in this case. The leg muscles are doing no external work, as it's gravity that is providing the force. Your body is simply transmitting that force as it does when you are standing.
 
  • #34
PeroK said:
No. Because when you are on the treadmill it's gravity that is providing the force. The force on the treadmill is not being generated by the use of your muscles, but by gravity pushing your weight into the treadmill.
Again, this is completely irrelevant. The work performed by your muscles is the work performed by your muscles.
 
  • #35
PeroK said:
Let's take scenario C: you are standing on a treadmill that is moving down.

The work being done by the legs is still ##mgv##. It's the same forces as before. You can see the error in this case. The leg muscles are doing no external work, as it's gravity that is providing the force. Your body is simply transmitting that force as it does when you are standing.
Do the math.
 

Similar threads

Replies
20
Views
2K
Replies
23
Views
2K
Replies
35
Views
2K
  • Introductory Physics Homework Help
Replies
4
Views
1K
Replies
6
Views
2K
Replies
5
Views
856
  • Mechanics
Replies
2
Views
1K
  • Introductory Physics Homework Help
Replies
2
Views
474
Replies
15
Views
2K
Back
Top