Part of a single rectangular loop of wire with
dimensions shown in the (Figure 1) is
situated inside a region of uniform magnetic field of
0.470T .
The total resistance of the loop is
0.610? .
. Neglect gravity.
Te motional emf induced in the loop is via the velocity "v" of the back leg "length L" as it is pulled thru the "B" field, and is;
E = LvB
this creates a current "i" in the loop of resistance "R" ,whic from Ohm's law is;
i = E/R = LvB/R
The induced current now interacts with the B-field to produce the force;
P = iLB = vL^2B^2/R
From Lenz' law ,this force will be opposite the pulling force. So you have the general force eq, from Newton's 2nd law;
F - P = ma
For constant velocity the acceleration is zero and you finally have;
F = P = vL^2B^2/R
F = 6.2*0.35^2*0.47^2/0.61 = 0.275 N
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