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After some time t, the normal to the coil plane makes an angle w t with the magnetic field . Then, the magnetic flux through the coil is
where the vector surface is given by
Therefore
The induced electromotive force is
The instantaneous power is e R , therefore
where we used
The total field at the center the coil at the instant t is
where is the magnetic field due to the induced current
with and I = e / R
Therefore
The mean values of its components are
And the mean value of the total magnetic field is
The needle orients along the mean field, therefore
Finally, the resistance of the coil measured by this procedure, in terms of , is
The force on a unit positive charge in a disk is radial and its modulus is
where B is the magnetic field at the center of the coil
Then, the electromotive force (e.m.f.) induced on each disk by the magnetic field B is
Finally, the induced e.m.f. between 1 and 4 is e = eD + e D'
When the reading of G vanishes, and Kirchoff laws give an immediate answer. Then we have
The force per unit length f between two indefinite parallel straight wires separated by a distance h is.
for and length , the force F induced on C2 by the neighbor coils C1 is
In equilibrium
Then
(1)
so that
The balance comes back towards the equilibrium position for a little angular deviation dj if the gravity torques with respect to the fulcrum O are greater than the magnetic torques.
Therefore, using the suggested approximation
Taking into account the equilibrium condition (1), one obtains
Finally, for
T
Th 2 ANSWER SHEET
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