A proof that magnetic forces do no work?

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Discussion Overview

The discussion revolves around the concept of magnetic forces and their work on charged particles, specifically examining a proof from "Introduction to Electrodynamics" by David J. Griffiths that claims magnetic forces do no work. Participants explore the implications of the mathematical substitution used in the proof and the physical interpretations of motion and force in the context of charged particles in magnetic fields.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions the substitution of displacement with velocity in the proof, arguing that the magnetic force should change the direction of the particle's velocity and thus affect the work done.
  • Another participant asserts that while the particle accelerates in the direction of the force, it moves in the direction of its velocity, challenging the initial claim about the direction of motion.
  • There is a discussion about whether a particle can have a component of velocity in the direction of acceleration, with examples provided to illustrate different scenarios.
  • Some participants argue that in circular motion, the force is radial while the velocity is tangential, suggesting that the magnetic force does not cause inward displacement.
  • One participant emphasizes that the proof applies at every instant and that the actual work calculation only considers the actual force and displacement, not hypothetical scenarios.
  • There is a contention regarding the drawing of velocity components and their relation to force, with one participant asserting that the components drawn do not accurately represent the situation.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the proof and the nature of motion under magnetic forces. There is no consensus on whether the magnetic force can cause displacement in its direction or how to interpret the relationship between force, velocity, and work.

Contextual Notes

Participants reference specific examples and scenarios, such as projectile motion and circular orbits, to illustrate their points, but these examples introduce additional complexity without resolving the central debate about the proof and its implications.

  • #31
Adesh said:
What is actual displacement? That \Delta \theta ?
It is the actual path that the object travels. It is a vector, so no, it is not ##\Delta \theta##. It is the vector ##\Delta \vec r## which can be written as ##\Delta \vec r = \Delta x \hat x + \Delta y \hat y = (\Delta x, \Delta y)## in Cartesian coordinates or as ##\Delta \vec r = \Delta r \hat r + \Delta \theta \hat \theta = (\Delta r, \Delta \theta)## in polar coordinates. So in polar coordinates you can write it ##(0,\Delta \theta)## and as ##\Delta t \to 0## we get ##(0,\Delta \theta/\Delta t) \to (0,d\theta/dt)=(0,v_{\theta}) ## which is always perpendicular to the force ##(F_B,0)## and therefore the work is always 0.
 
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  • #32
A.T. said:
Causation doesn't enter the definition of work.
Please explain me a little further, I really want to learn it.
 
  • #33
Dale said:
It is the actual path that the object travels. It is a vector, so no, it is not ##\Delta \theta##. It is the vector ##\Delta \vec r## which can be written as ##\Delta \vec r = \Delta x \hat x + \Delta y \hat y = (\Delta x, \Delta y)## in Cartesian coordinates or as ##\Delta \vec r = \Delta r \hat r + \Delta \theta \hat \theta = (\Delta r, \Delta \theta)## in polar coordinates. So in polar coordinates you can write it ##(0,\Delta \theta)## and as ##\Delta t \to 0## we get ##(0,\Delta \theta/\Delta t) \to (0,d\theta/dt)=(0,v_{\theta}) ## which is always perpendicular to the force ##(F_B,0)## and therefore the work is always 0.
But we want to prove that the displacement is perpendicular to the force not the velocity.
 
  • #34
Adesh said:
But we want to prove that the displacement is perpendicular to the force not the velocity.
The velocity is the instantaneous displacement. You have studied calculus.
 
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  • #35
Adesh said:
Please explain me a little further, I really want to learn it.

Forget about what causes what. To calculate work done by a particular force on a given object, you only need to know what that force is and what the displacement of the object is. It doesn't matter whether "only part of the displacement was caused by the force" or anything of that sort. You look at the force and take the dot product with displacement (both at the same instant).
 
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  • #36
Adesh said:
But we want to prove that the displacement is perpendicular to the force not the velocity.
In one sense there is no instantaneous displacement. There is an instantaneous displacement from the origin, which is the instantaneous position (vector). But, displacement is the difference of two position measurements. As the time increment tends to zero, the displacement over that time increment tends to zero.

The instantaneous quantities must be the time derivative of something. Velocity is the derivative of position and acceleration is the derivative of velocity. Neither of these need tend to zero as the time increment tends to zero.
 
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  • #37
Adesh said:
In this picture, I have drawn the violet arrow which represents the velocity after a time \Delta t from where the + sign has been made. I have drawn the components of violet velocity, the components are in yellow color and there you see we have a component inwards. What has caused this inward component of velocity? I think it is \mathbf{F_{B}} which acted at + sign has caused this, correct me if I'm wrong.
View attachment 254197
I see what you're saying - the displacement is not parallel to the velocity, and we can clearly see that there is a component of the displacement parallel to the force vector, so their dot product clearly isn't zero, so what gives? Well, this would be true if the force were impulsive - occurring over a finite amount of time - so that the force vector was fixed in that direction. But this force arises out of that magnetic field interacting with the particle's motion, perpendicular to them both. The force vector is not static, it's continually changing in lockstep with the particle's position, always perpendicular.
 
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