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Bukhovtsev-et-al-Problems-in-Elementary-Physics

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352 ANSWERS AND SOLUTIONS<br />

the r<strong>in</strong>g is arranged <strong>al</strong>ong the force l<strong>in</strong>es of the field (the <strong>in</strong>duced current is<br />

zero) or when the plane of the r<strong>in</strong>g is strictly perpendicular to the force l<strong>in</strong>es<br />

(the moment of the forces is zero).<br />

Accord<strong>in</strong>g to Lens's law, the first position of the r<strong>in</strong>g will be stable <strong>in</strong> an<br />

<strong>in</strong>creas<strong>in</strong>g magn<strong>et</strong>ic field, and the second unstable.<br />

In a decreas<strong>in</strong>g magn<strong>et</strong>ic field, on the contrary, equilibrium will be stable<br />

when the angle b<strong>et</strong>ween the plane of the r<strong>in</strong>g and. the force l<strong>in</strong>es is a right<br />

one, and unsta ble when the plane of the r<strong>in</strong>g is para lIel to the force l<strong>in</strong>es.<br />

583. L<strong>et</strong> the velocity of the conductor be v at a certa<strong>in</strong> moment of time.<br />

The e. m. f. (<strong>in</strong> volts) at the same moment of time will thus be cC= 10- 8 Hlo,<br />

and the current I=ir x 10- 8 Hlo,<br />

The action of the magn<strong>et</strong>ic field on the<br />

conductor carry<strong>in</strong>g a current will <strong>in</strong>duce a force f that prevents free dropp<strong>in</strong>g<br />

of the conductor:<br />

f= 10-' H~2fJ<br />

be<strong>in</strong>g considered, the acceleration can be de­<br />

Hence, at the moment of time<br />

term<strong>in</strong>ed from the relationship<br />

H 2 l 2U<br />

ma=mg-f=mg-IO-8~<br />

It is easy to see that as the velocity <strong>in</strong>creases, the acceleration a will dlm<strong>in</strong>ish<br />

and become zero at the moment of equ<strong>al</strong>ity of the forces f=mg. From<br />

this moment on, the conductor will move with a constant velocity Vk equ<strong>al</strong> to<br />

mgRXI0 9<br />

Vk H 2l 2<br />

584. "The e. m. f. of <strong>in</strong>duction appear<strong>in</strong>g <strong>in</strong> the conductor (measured <strong>in</strong> volts)<br />

is It= 10- 8 Hlu.<br />

The charge on the plates of the capacitor can be found from the relationship<br />

Q=l1C= 10- 8 HlvC<br />

The current flow<strong>in</strong>g <strong>in</strong> the circuit is<br />

1=~~=10-8 HlC ~~=10-8HICa<br />

where a Is the sought acceleration.<br />

The <strong>in</strong>teraction of this current with the magn<strong>et</strong>ic field will produce a force F l<br />

act<strong>in</strong>g on the mov<strong>in</strong>g conductor. On the basis of Lenz's law, this force will<br />

be directed oppositely tc the force F.<br />

The force F I =kJHI = lo-eHt/laC, if C is measured <strong>in</strong> farads. The sought<br />

acceleration can be found from the equation ma=F-Fl.<br />

Hence,<br />

F<br />

is a constant quantity.

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