Acceleration From Rest Under Constant Power

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Discussion Overview

The discussion revolves around the concept of acceleration from rest under constant power, exploring the implications of the equations governing this motion. Participants examine the physicality of infinite acceleration at the initial moment and the validity of applying constant power at low speeds, considering both theoretical and practical perspectives.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that the equation for motion under constant power leads to infinite acceleration at time zero, suggesting this is non-physical.
  • Others argue that the situation of infinite acceleration only lasts for an instant, prompting questions about how far an object travels in that instant.
  • There is a contention regarding whether the model used is an approximation, with some asserting that the premise of applying constant power is false at low speeds.
  • Some participants challenge the idea that infinite acceleration is unphysical, suggesting that it can be interpreted as very high acceleration instead.
  • There is a discussion about the implications of applying force to a non-moving object, where power is zero, and how this affects initial acceleration.
  • Some participants express uncertainty about the reality of infinite acceleration, questioning how it aligns with physical principles and the nature of singularities in models.

Areas of Agreement / Disagreement

Participants generally do not reach consensus, with multiple competing views on the physical implications of infinite acceleration, the validity of applying constant power at low speeds, and the interpretation of singularities in the context of physical reality.

Contextual Notes

The discussion highlights limitations in the models used, particularly regarding the assumptions about applying constant power and the behavior of objects at low speeds. There are unresolved mathematical steps and dependencies on definitions that contribute to the ongoing debate.

erobz
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Impossible?!?

By my estimation the equation that describes this motion is given by:

$$Pt = \frac{1}{2}m{ \dot x}^2$$

or

$$\dot{x} = \sqrt{\frac{2P}{m}} \sqrt{t}$$

but this implies:

$$\ddot{x} = \sqrt{\frac{2P}{m}} \frac{1}{\sqrt{t}}$$

So, no matter how small we make the power, we appear to get an infinite acceleration at ##t=0##( or in the case of ##P=0, t= 0##) an indeterminate form ##\frac{0}{\infty}##.

Conclusion: Acceleration from rest under constant power is non-physical. However, with any non-zero initial velocity things seem to be ok with the following:

$$\ddot{x} = \frac{P}{m} \frac{1}{\sqrt{ \frac{2P}{m}t + v_o^2}}$$

Anything interesting here, something I'm missing?
 
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erobz said:
Acceleration from rest under constant power is non-physical.
Correct. However, this situation only lasts for an instant,
 
Vanadium 50 said:
Correct. However, this situation only lasts for an instant.
Well, how far does it travel in that instant?
 
Look at your own equations. Simply because things go to zero and we can can choose to divide by them does not make the world unphysical.
 
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hutchphd said:
Look at your own equations. Simply because things go to zero and we can can choose to divide by them does not make the world unphysical.
I didn't say the world was unphysical. I'm saying the model I'm choosing for the "world" here yields an unphysical result at the initial conditions. I don't think those two things are equivalent.
 
Your model is an approximation. In the jargon it is integrable. To be blunt your point is true but not interesting
 
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erobz said:
Well, how far does it travel in that instant?
I see that apparently the displacement is indifferent to this:

$$x = \frac{2}{3} \sqrt{ \frac{2P}{m}} \sqrt[3]{t} $$
 
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hutchphd said:
Your model is an approximation. In the jargon it is integrable. To be blunt your point is true but not interesting
What about it is an approximation though? Its CoE.
 
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erobz said:
What about it is an approximation though?
The premise that you can apply constant power is false at low speed, for the obvious reason you discovered.
 
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  • #10
In application and in theory. No body is perfectly rigid. Even then no influence tops the speed of light. Science, by its very incarnation, deals with the testable.
As long as the theory conforms to test, a few incidental singularities is not dispositive.
 
  • #11
russ_watters said:
he assumption that you can apply constant power is false at low speed
Exactly. P = Fv. As v →0, for constant P, F →∞.

Approximations break down when approximations break down.
 
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  • #12
russ_watters said:
The premise that you can apply constant power is false at low speed, for the obvious reason you discovered.
$$\ddot{x} = \frac{P}{m} \frac{1}{\sqrt{ \frac{2P}{m}t + v_o^2}}$$

I disagree. At low speeds applying constant power is completely fine. The singularity vanishes. ##\ddot x## may be arbitrarily large or small depending on ##P## but none the less finite when ##v_o > 0##.

It is when we have no initial speed ##v_o = 0## the any applied power ##P>0## yeilds the singularity. So it seems more like its impossible to apply power at zero velocity, not that you can't apply constant power at low speed. The sticky part is how does anything begin to move if we can't apply any power without visiting ##\infty##?
 
  • #13
erobz said:
$$\ddot{x} = \frac{P}{m} \frac{1}{\sqrt{ \frac{2P}{m}t + v_o^2}}$$

I disagree. At low speeds applying constant power is completely fine. The singularity vanishes.
So again, that's math, not reality. In reality there are reasons (some already specified) why it doesn't work that way. It is, as @hutchphd said, the difference between the theory and the application (reality).
 
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  • #14
russ_watters said:
that's math, not reality. In reality
This.
erobz said:
The sticky part is how does anything begin to move if we can't apply any power without visiting infinity?
You have rediscovered a variant of Zeno's paradox.
 
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  • #15
russ_watters said:
So again, that's math, not reality. In reality there are reasons (some already specified) why it doesn't work that way. It is, as @hutchphd said, the difference between the theory and the application (reality).
Yes, but is it not the supposition in Physics that reality is perfect, and when we encounter these singularities in our models of it, it is due to an imperfect model. We naturally should wonder what fixes the model so the singularity yields?
 
  • #16
erobz said:
Yes, but is it not the supposition in Physics that reality is perfect, and when we encounter these singularities in our models of it, it is due to an imperfect model. We naturally should wonder what fixes the C.o.E. so the singularity yields?
What? I think you've forgotten the pont of physics.

And by the way there are actually scenarios where the singularity you noticed is not a problem. Elastic collisions for example.
 
  • #17
erobz said:
Yes, but is it not the supposition in Physics that reality is perfect, and when we encounter these singularities in our models of it, it is due to an imperfect model. We naturally should wonder what fixes the model so the singularity yields?
The results for your "model" are not nonsensical results in case your "power supply" is able to supply an infinite high force for a moment. It's theory taken at face value.
To be realistic, replace the word “infinite acceleration” with “very high acceleration".
 
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  • #18
Where, in your theory, are you not allowed to have infinities? Its your theory and infinite acceleration is up to you. When you apply it to actual reality you will see that there are ameliorating factors and you make a note.
 
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  • #19
erobz said:
...
So, no matter how small we make the power, we appear to get an infinite acceleration at ##t=0##.

Anything interesting here, something I'm missing?
Perhaps the lack of agreement or consistency comes from the concept that we can make power.
We can only transfer mechanical energy at certain rate, via application of a finite amount of force or torque.

Consider, for example, how slowly a space rocket starts moving upwards at the launch pad.
 
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  • #20
erobz said:
I disagree. At low speeds applying constant power is completely fine.
But not at zero exactly.

If you apply a force to a non-moving object, the power is zero (##P=Fv##). So the initial acceleration is known based on ##F=ma##. Once the object starts moving, then you have power. You can then alter your force input such that the power stays constant as the velocity grows.

Even if you had a wheel rotating freely with a certain power input and you lowered it to the ground, as soon as you touched the ground, the power would be zero with respect to the ground. If we assume no slipping, the wheel will decelerate to zero and a certain initial force (in this case determined by the mechanism of friction) would be applied that would set the initial forward acceleration of the wheel. And as soon as it instantly began to move forward, the force would adapt itself to the velocity to respect the constant power input.

Your equation is just not valid at ##t=0##, assuming ##v=0##, because you will always get:
$$\ddot{x} = \sqrt{\frac{2(0)}{m}} \frac{1}{\sqrt{(0)}}$$
You must use another equation which is simply ##a=\frac{F}{m}##.
 
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  • #21
Lnewqban said:
Perhaps the lack of agreement or consistency comes from the concept that we can make power.
We can only transfer mechanical energy at certain rate, via application of a finite amount of force or torque.

Consider, for example, how slowly a space rocket starts moving upwards at the launch pad.
I agree, the problem must come from the idea we can “supply” power. We can supply energy
hutchphd said:
Where, in your theory, are you not allowed to have infinities? Its your theory and infinite acceleration is up to you. When you apply it to actual reality you will see that there are ameliorating factors and you make a note.
Maybe infinite acceleration is fine. I don’t know. The displacement (which is what can be directly measured) is indifferent to the initial infinity…so I don’t know. Like you said. It’s integrable.
 
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  • #22
russ_watters said:
What? I think you've forgotten the point of physics.
I'm not an expert, its arguable I never knew the point. Care to expand on it, because I don't know what the point is if it not to examine what you think you know?
 
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  • #23
erobz said:
I'm not an expert, its arguable I never knew the point. Care to expand on it, because I don't know what the point is if it not to examine what you think you know?
The point of physics is to accurately understand/describe physical reality.
erobz said:
Maybe infinite acceleration is fine. I don’t know.
Infinite acceleration is not possible in the real world, however in some cases it is ok to assume it happens/ignore it for the sake of modeling.
 
  • #24
Lnewqban said:
Perhaps the lack of agreement or consistency comes from the concept that we can make power.
We can only transfer mechanical energy at certain rate, via application of a finite amount of force or torque.
Those two sentences appear to contradict each other, to me.
 
  • #25
erobz said:
I'm not an expert, its arguable I never knew the point. Care to expand on it, because I don't know what the point is if it not to examine what you think you know?
But do not "throw out the baby with the bath water". I agree that an unexamined theory is a bad idea, but unless the theory is completely universal there will be approximations required, because connections to the other degrees of freedom in the world will invoke suppositions. The concept of infinite supplied power is not prohibited by your theory nor would one expect it to be. Other parts of the Physical world conspire to make it not available.
I am again reminded of Feynman's Law of everything. $$U=0$$ The devil is always in the detail
 
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  • #26
hutchphd said:
But do not "throw out the baby with the bath water". I agree that an unexamined theory is a bad idea, but unless the theory is completely universal there will be approximations required, because connections to the other degrees of freedom in the world will invoke suppositions. The concept of infinite supplied power is not prohibited by your theory nor would one expect it to be. Other parts of the Physical world conspire to make it not available.
I am again reminded of Feynman's Law of everything. $$U=0$$ The devil is always in the detail
Just a clarification. Not infinite power, but infinite force - constant power. That is what I find interesting though, any supplied power ##P>0## causes this seemingly paradoxical result. What are the interventions in the physical world that would prevent it from actually happening? The displacement and velocity are indifferent to it, so is that in itself sufficient to say the infinite force isn't a big deal here? In other cases, infinite forces certainly raise eyebrows. I find it interesting that this happens in something as benign as Conservation of Energy, and constant power application. You say it's a bore. That difference must be between what you have experienced, and I have not.
 
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  • #27
I haven't follow the entire thread in detail, but I think it's simplest to just solve the equation of motion than some debates with many words. We always have Newton's equation of motion
$$m \ddot{x}=F.$$
Here we don't know ##F## but have given that the power is constant during the motion, i.e.,
$$P=F v=F \dot{x}=\text{const} \; \Rightarrow \; F=\frac{P}{\dot{x}}.$$
Plugging this into the equation of motion yields
$$m \dot{x} \ddot{x}=P=\text{const}.$$
This you can write as
$$\frac{m}{2} \mathrm{d}_t (\dot{x}^2)=P \; \Rightarrow \; \dot{x}^2=\frac{2 P}{m} t+C.$$
The initial condition says ##v(0)=0##, i.e., ##C=0##. That means
$$\dot{x}=\sqrt{2 P t/m}$$
Integrating this once more you get
$$x(t)=\frac{2}{3} \sqrt{\frac{2 P}{m}} t^{3/2},$$
where I assumed that the position at ##t=0## is ##x(0)=0##.
 
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  • #28
vanhees71 said:
I haven't follow the entire thread in detail, but I think it's simplest to just solve the equation of motion than some debates with many words. We always have Newton's equation of motion
$$m \ddot{x}=F.$$
Here we don't know ##F## but have given that the power is constant during the motion, i.e.,
$$P=F v=F \dot{x}=\text{const} \; \Rightarrow \; F=\frac{P}{\dot{x}}.$$
Plugging this into the equation of motion yields
$$m \dot{x} \ddot{x}=P=\text{const}.$$
This you can write as
$$\frac{m}{2} \mathrm{d}_t (\dot{x}^2)=P \; \Rightarrow \; \dot{x}^2=\frac{2 P}{m} t+C.$$
The initial condition says ##v(0)=0##, i.e., ##C=0##. That means
$$\dot{x}=\sqrt{2 P t/m}$$
Integrating this once more you get
$$x(t)=\frac{2}{3} \sqrt{\frac{2 P}{m}} t^{3/2},$$
where I assumed that the position at ##t=0## is ##x(0)=0##.
Thats not the problem I'm having. The problem is ## \lim_{t \to 0} \ddot x \rightarrow \infty## for all ##P > 0##.
 
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  • #29
Yes, but acceleration with ##P=\text{const}## is a pretty artificial situation to begin with ;-)).
 
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  • #30
vanhees71 said:
Yes, but acceleration with ##P=\text{const}## is a pretty artificial situation to begin with ;-)).
Yeah, why exactly though? You can't even say ##P=0## at ##t=0## to start the motion. If ##P=0## there is no motion. The very moment ##P>0## we have a singularity. It's seeming to be a twist on Zenos's Paradox.
 
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