Sliding Bar in a Uniform Magnetic Field

AI Thread Summary
The problem involves a metal bar sliding down frictionless inclined rails in a uniform magnetic field. The effective gravitational force acting on the bar is mg sin φ, while the induced electromotive forces (emfs) in the wire loops formed by the bar are calculated as -BLv and BLv. The current through the bar is derived from these emfs, resulting in I = (2BLv)/R. The force due to the current is balanced by the gravitational component, leading to the equation for terminal speed v = (Rmg tan φ)/(2B²L²). However, the solution provided was marked incorrect by the online homework system, despite yielding correct results for subsequent parts of the problem.
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Homework Statement


A metal bar with length L, mass m, and resistance R is placed on frictionless metal rails that are inclined at an angle \phi above the horizontal. The rails have negligible resistance. A uniform magnetic field of magnitude is directed downward in the figure B. The bar is released from rest and slides down the rails.

(In the diagram it can be seen that the bar divides a rectangle into two smaller rectangles. As the bar slides, one grows, and the other shrinks.)

What is the terminal speed of the bar?

Homework Equations


\cal{E}=IR
\cal{E}=-\frac{d\Phi_m}{dt}

The Attempt at a Solution


Effective gravity has magnitude

mg\sin\phi

The two wire loops formed by the bar have respective emfs

{\cal E}_{1}=-\frac{d\Phi_{1}}{dt}=-BLv
{\cal E}_{2}=-\frac{d\Phi_{2}}{dt}=BLv

Therefore, the current along the bar is

I=\frac{-{\cal E}_{1}+{\cal E}_{2}}{R}=\frac{2BLv}{R}

The negative sign appears because one loop runs clockwise and the other counterclockwise.

This creates a force

F=ILB=\frac{2B^{2}L^{2}}{R}v

and an effective force

\frac{2B^{2}L^{2}}{R}v\cos\phi

The two are in equilibrium when

\frac{2B^{2}L^{2}}{R}v = mg\tan\phi
v = \frac{Rmg\tan\phi}{2B^{2}L^{2}}

The online homework system says this is incorrect, and I can't fiqure out why.
 
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