Work and Friction: How Does Fxv Apply?

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Discussion Overview

The discussion revolves around the application of the formula for mechanical power, specifically in the context of friction and relative motion between a block and a floor. Participants explore how power is calculated for both the block and the floor, considering different reference frames and the implications of frictional forces.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant suggests that while the block experiences friction and thus has mechanical power associated with it, the floor does not have motion and therefore does not have mechanical power, despite producing heat.
  • Another participant emphasizes that motion is relative, indicating that both the block and the floor can be seen as moving relative to each other.
  • A participant explains that the mechanical power for the block is negative due to the frictional force acting against its motion, while the power for the floor is zero since it does not move.
  • There is a discussion about a scenario involving a train where a person pushes a mass; participants question whether the mechanical power is zero or based on the velocity of the mass relative to the train.
  • Some participants argue that the mechanical power is zero when the velocity at the point of application of the force is zero, while others point out that this perspective depends on the chosen reference frame.
  • It is noted that mechanical power is not invariant in Newtonian physics and can vary based on the reference frame used for analysis.

Areas of Agreement / Disagreement

Participants express differing views on how to calculate mechanical power in various scenarios, particularly regarding the influence of reference frames. There is no consensus on the implications of these calculations for the floor and the block.

Contextual Notes

Participants highlight that the discussion involves assumptions about reference frames and the nature of motion, which may not be universally applicable. The relationship between heat produced and mechanical power is also noted as complex and dependent on thermodynamic properties.

Who May Find This Useful

This discussion may be useful for those interested in the principles of mechanics, particularly in understanding the effects of friction, relative motion, and reference frames on mechanical power calculations.

leafy
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Suppose you're a point on the floor and a block mass slide pass you. The block mass said " I have friction acting on me during my motion so the mechanical power is friction x my speed". When ask the point on the floor, it said "well, I don't have motion so there is no mechanical power". Yet the floor produce heat.

you can apply Fxv to the block, but how can you apply Fxv to the floor?

{moderator’s note: split from https://www.physicsforums.com/threads/can-static-force-do-work.1010439/#post-6578451 }
 
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Motion is relative. The floor or a block has relative speed v to the other . For the floor, a block moves. For a block, the floor moves.
 
Suppose the block is being pushed in the positive ##x## direction. Then the velocity ##\vec v## (of the block) is in the positive direction and the frictional force ##-\vec F## acting on the block is in the negative direction (with the minus sign reminding us of that fact). Then the mechanical power on the block is ##P_{block}=-\vec F \cdot \vec v<0## with the negative sign indicating that mechanical power is leaving the block.

By Newton’s 3rd law the frictional force ##\vec F## is in the positive direction. Then the mechanical power on the floor is ##P_{floor}=\vec F \cdot 0 = 0##. So no mechanical power enters the floor.

The mechanical power that leaves the block and does not enter the floor is transformed into thermal energy at a rate ##\dot Q=-(P_{floor}+P_{block})=\vec F \cdot \vec v>0##

It is incorrect to assume that all of the heat ##\dot Q## goes into the floor, so ##\vec F \cdot \vec v## is not a relevant quantity for the floor. All that you can say from mechanics is that heat is produced at the interface at a rate ##\dot Q##. Then how much heat goes into the block vs the floor depends on their thermodynamic properties.
 
So there is no different between motion of material or motion of the force here because they're both exactly the same. What about if you're on a train moving right at 1 m/s and pushing a mass left. When the mass reach 1m/s left. What is the mechanical power? Fx1m/s or 0?
 
leafy said:
What about if you're on a train moving right at 1 m/s and pushing a mass left. When the mass reach 1m/s left. What is the mechanical power? Fx1m/s or 0?
The same rule applies always for all mechanical forces. In that case the velocity of the material at the point of application of the force is ##\vec v= 0## so the mechanical power is ##P=\vec F \cdot \vec v=0##.
 
Dale said:
The same rule applies always for all mechanical forces. In that case the velocity of the material at the point of application of the force is ##\vec v= 0## so the mechanical power is ##P=\vec F \cdot \vec v=0##.
I see that you always take the absolute(earth) frame. But to the person on the train, the power is not 0.
 
leafy said:
I see that you always take the absolute(earth) frame. But to the person on the train, the power is not 0.
Correct. Mechanical power depends on the reference frame. It is not an invariant in Newtonian physics.

I took the Earth frame (which is not absolute in any sense) because that is how you described it, but if you use a different frame you apply the same rule and thus get a different value for mechanical power.
 
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