B-Fields: Deriving Faraday's Law & Why No Work?

[ChanceLiterature]

This statement has always confused me. Now my confusion is coming home to roast while we cover EMF.

If we consider work mathematically as ∫f.dl and require integral to be path independent then of course the B-field does no work.

However, it seems like there is a deeper meaning to B-fields do no work. Is there?

Tied into this is faradays law. Faraday's Law can be "derived" from emf (it's in quotes because I understand faradays is first principles). In this derivation emf force is stated to be closed integral ∫E.dl. I do not understand why this why emf or this induced force around the loop is necessarily due to an E-field as opposed to to B-field.

 

[anuttarasammyak]

For some clarification I think you are saying that B-field do no work to charges. B-field do work to magnetic dipoles as we see two magnets attract and collide.

In this derivation emf force is stated to be closed integral ∫E.dl.

it equals to
-\int_A\frac{\partial \mathbf{B}}{\partial t} \cdot d\mathbf{A}
using B.

 

[ChanceLiterature]

For some clarification I think you are saying that B-field do no work to charges. B-field do work to magnetic dipoles as we see two magnets attract and collide.

it equals to
-\int_A\frac{\partial \mathbf{B}}{\partial t} \cdot d\mathbf{A}
using B.

Yes, I'm trying to highlight two points of confusion. You're right I was not clear enough. I hope this helps.

1) I am asking why B-fields do no work on a point charge when the path integral of a charge on a B-field is non-zero? Did we define work as path integral only over conservative fields? Is this why we say B-fields do no work?

2) I am not sure why the closed line integral of B is necessarily zero (if I still had my copy of Boas' Mathematics in the physical sciences, I might know why/if this holds). Additionally, if it is not necessarily zero, I am not sure why the resulting the emf is defined as closed E.dl.

My confusion with Faraday's law in the original question derives from not understanding emf I suspect. Thus, I think ironing out point of confusion 2 will help

 

[anuttarasammyak]

A familiar reply to 1) is to see the formula of Lorentz force the part originated from B of which is
q \mathbf{v} \times \mathbf{B}
and is always perpendicular to velocity of charge q point, $\mathbf{v}$, thus no work done on the charge.

 

[ChanceLiterature]

Thanks. I realized 1 was very dumb after remembering what conservative and close integral meant.

Additionally, even I'm not sure what I'm asking or saying for 2

 

[ChanceLiterature]

Thanks for the help

 

[anuttarasammyak]

2) I am not sure why the closed line integral of B is necessarily zero

Zero we see as for B is
\nabla \cdot \mathbf{B} =0
and thus
\int_S \mathbf{B} \cdot d\mathbf{S}=0
for a closed surface S. Not line integral.