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Question: A wheel with \(10\) metallic spokes each \(0.5\;{{m}}\) long rotated with a speed of \(120\;{{rpm}}\...

A wheel with 1010 metallic spokes each 0.5  m0.5\;{{m}} long rotated with a speed of 120  rpm120\;{{rpm}} in a plane normal to the horizontal component of earth’s magnetic field Bh{B_h} at a place. If Bh=0.4  G{B_h} = 0.4\;{{G}}at the place. What is the induced emf between the axle and the rim of the wheel? (1  G=104  T1\;{{G = 1}}{{{0}}^{ - 4}}\;{{T}} )
(A) 0  V0\;{{V}}
(B) 0.628  mV0.628\;{{mV}}
(C) 0.628  μV0.628\;{{\mu V}}
(D) 62.8  μV62.8\;{{\mu V}}

Explanation

Solution

The relative motion of the magnet will produce an induced current because of the induced electromotive force. The change of magnetic flux per unit time is the induced emf. Where, the magnetic flux is the product of the magnetic field and the area covered. The change in the magnetic flux only brings the induced emf between the axle and the rim of the wheel.

Complete step by step solution:
Given data:-
Length of the metallic spoke,r=0.5  mr = 0.5\;{{m}}
Linear speed of the wheel, v=120  rev/min=12060rev/s=2  rev/sv = 120\;{{rev/min = }}\dfrac{{120}}{{60}}{{rev/s = 2}}\;{{rev/s}}
Earth’s magnetic field , Bh=0.4  G=0.4×104  T{B_h} = 0.4\;{{G = 0}}{{.4}} \times {{1}}{{{0}}^{ - 4}}\;{{T}}
The area covered by an angle θ\theta , where rr is the radius is given as,
A=πr2θ2π =r22θ  A = \pi {r^2}\dfrac{\theta }{{2\pi }} \\\ = \dfrac{{{r^2}}}{2}\theta \\\
The expression for the induced emf is given as,
E=dϕdtE = \dfrac{{d\phi }}{{dt}}
Where ϕ\phi is the magnetic flux. Magnetic flux is the product of magnetic fields and the area covered.
Therefore, Magnetic flux ϕ=BA\phi = BA
Where B is the magnetic field and A is the area covered.
Substituting above expression for induced emf,
E=dϕdt =d(BA)dt  E = \dfrac{{d\phi }}{{dt}} \\\ = \dfrac{{d(BA)}}{{dt}} \\\
Substituting in the above expression. We get,
E=d(Br22θ)dt =Br22dθdt  E = \dfrac{{d(B\dfrac{{{r^2}}}{2}\theta )}}{{dt}} \\\ = B\dfrac{{{r^2}}}{2}\dfrac{{d\theta }}{{dt}} \\\
The angle covered in unit time is the angular speed ω\omega .
E=Br22ωE = B\dfrac{{{r^2}}}{2}\omega
Therefore the induced emf is given as,
E=12Br2ωE = \dfrac{1}{2}B{r^2}\omega
The angular speed ω=2πv\omega = 2\pi v
Substituting the value of linear speed,
ω=2π×2  rev/s=4π  rev/s\omega = 2\pi \times {{2}}\;{{rev/s}} = 4\pi \;{{rev/s}}
Substituting the values in the above expression,
E=12×0.4×104  T×(0.5  m)2×4π  rev/s =6.28×105  V =0.628  μV  E = \dfrac{1}{2} \times {{0}}{{.4}} \times {{1}}{{{0}}^{ - 4}}\;{{T}} \times {\left( {0.5\;{{m}}} \right)^2} \times 4\pi \;{{rev/s}} \\\ {{ = 6}}{{.28}} \times {{1}}{{{0}}^{ - 5}}\;{{V}} \\\ {{ = 0}}{{.628}}\;{{\mu V}} \\\
Thus the induced emf between the axle and the rim of the wheel is 0.628  μV{{0}}{{.628}}\;{{\mu V}}.

Thus option C is correct.

Note:
We can find the induced emf between the axle and the rim of the wheel by following the method We have the number of spokes ,N=10N = 10 . The length of each spoke ,l=0.5  ml = 0.5\;{{m}} ,magnetic field B=0.4×104  TB = {{0}}{{.4}} \times {{1}}{{{0}}^{ - 4}}\;{{T}}and the linear speed v=2  rev/sv = {{2}}\;{{rev/s}}.