Solution:
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As the conducting disk is rotating with angular velocity
,
the free charge carriers inside the disk will rotate with the disk and with
respect to the laboratory observer acquire tangential velocity which will depend
linearly on the distance of the charge from the centre of the disk. Therefore,
the speed of a charge carrier at a distance r from the centre of the disk
will be
.
![](images/pic2473.gif)
Because of the magnetic field
, which is
normal to the velocity of the carrier, the charge carrier (charge e) will
experience Lorentz force of magnitude
.
If at an instant we consider a charge carrier located at a distance r
along the line OA, its velocity will be
. As
shown in the diagram magnetic field on the disk is
.
Therefore,
.
Therefore, if the charge carriers are electrons having charge
,
the Lorentz force will be along the direction
.
Electrons will drift toward the circumference of the disk and an electric
field will come into being (like in Hall effect) that at equilibrium will
balance the force
.
The electric field will therefore be
![](images/pic2482.gif)
The potential difference between the points A and O will
therefore be
![](images/pic2483.gif)
If the output current is
, the
power dissipated in the rotor will be
.
Therefore, a torque,
, must be
provided by the motor for keeping the rotor spinning at frequency
.
The magnitude of
can now
be determined by equating the power of the motor with the rate of dissipation of
internal energy in the rotor. That is
![](images/pic2487.gif)
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