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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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