Abid Mir
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Look over to #16 #46 #49
Philip Wood said:A fair point: upward magnetic forces on charge carriers in top wire are balanced by downward electric forces from the rest of the wire due to imbalance in charge distribution, and it is the Newton 3 upward electric force on the rest of the wire which actually lifts the wire. So it's the electric force which does work lifting the wire.
This is doubtless true, but is a bit like saying: I pull a trolley along with a gloved hand, so it's not me but my glove that is doing work on the trolley.
What I do find satisfying is an explanation is in terms of the magnetic force components on each charge carrier parallel to the wire and perpendicular to the wire, as explained in my post 12. I'll show the forces on a diagram, and try and make my case clearly below.View attachment 87798 argument from there.
I don't quite agree with you here. It's not the magnetic field varying with time that induces the back-emf, or, equivalently that causes the 'backward' forces along the wire on the charge carriers. Rather, it's that the wire, and therefore its charge carriers, are moving through a magnetic field, and therefore experiencing a Magnetic Lorentz force, q \mathbf{v} \times \mathbf{B}. This can, if one wishes, be regarded as electromagnetic induction by means of flux cutting, but there's no need to use the terminology of e-m induction: the argument can all be carried through in terms of forces and work, as I did in post 12 and the handwritten continuation.Abid Mir said:As the magnetic field varies with time due to movement of wire upwards , an induced electric field (non conservative) develops inside the wire between the drifting electrons and the protons.
magnetic force to the left?Philip Wood said:Good. And it's good that, according to BvU, Griffiths also attributes the work done to the power supply.
I don't quite agree with you here. It's not the magnetic field varying with time that induces the back-emf, or, equivalently that causes the 'backward' forces along the wire on the charge carriers. Rather, it's that the wire, and therefore its charge carriers, are moving through a magnetic field, and therefore experiencing a Magnetic Lorentz force, q \mathbf{v} \times \mathbf{B}. This can, if one wishes, be regarded as electromagnetic induction by means of flux cutting, but there's no need to use the terminology of e-m induction: the argument can all be carried through in terms of forces and work, as I did in post 12 and the handwritten continuation.
Note that all this is about forces due to the magnetic field. There is also an electric field, which exerts a force to the right on the charge carriers, opposing the magnetic force to the left, and which is set up by the power supply. This ultimately does the work. [Note that the force between electrons and ions is yet another force due to an electric field.]
Yeah k i got it tyPhilip Wood said:Yes, to the left, as in the hand-drawn diagram. This is the component of the magnetic force which arises from the upward motion of the wire. The other (upward) force component arises from the drift velocity of the charge-carriers along the wire.
I assume that "ty" means "Thank you".Abid Mir said:Yeah k i got it ty
That's one of the enigmas of human behavior too difficult for a simple minded physicist to explain. What can be simpler than the statement thatBvU said:Hello Abid, Philip,
How come these threads rant on and on from one misunderstanding to the next misinterpretation, while it's so easy to read on a bit further and get it all handed on a silver platter ? And if at that point something is still unclear, it's easier to post very specific questions that allow much more compact answers !