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ABSOLUTE MEASUREMENTS OF ELECTRICAL QUANTITIES SOLUTION

electronics



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Absolute measurements of electrical quantities

Solution



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

Question

Basic formulas and ideas used

Analytical results

Marking guideline



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