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

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348 ANSWERS AND SOLUTIONS<br />

cord<strong>in</strong>g to Lens's law, the tot<strong>al</strong> current <strong>in</strong> the coil decreases when the rod<br />

enters it, and <strong>in</strong>creases when the rod leaves it.<br />

A diagram of the change <strong>in</strong> the current is shown <strong>in</strong> Fig. 463.<br />

571. The magn<strong>et</strong>ic flux changes at a constant rate, and therefore the e. m. f.<br />

of <strong>in</strong>duction <strong>in</strong> the second coil will <strong>al</strong>so be constant. If the coil is connected<br />

to a closed circuit, it will carry a direct current, which will s<strong>et</strong> In not at<br />

once, but depend<strong>in</strong>g on the coefficient of self..<strong>in</strong>duction of the second coil and<br />

its resistance.<br />

572. Yes, it will. The e.m.f. of <strong>in</strong>duction is proportion<strong>al</strong> to the rate of<br />

change of the magn<strong>et</strong>ic flux, while the magnitude of the magn<strong>et</strong>ic flux <strong>in</strong><br />

the iron core does not change directly with the current. The relationship will<br />

be more complicated.<br />

573. Accord<strong>in</strong>g to Faraday's law,<br />

A«D<br />

cCi= 10- S AT= 10- 8 kA<br />

The e.m.f, of <strong>in</strong>duction is numeric<strong>al</strong>ly equ<strong>al</strong> to the work performed by<br />

the electric field when a s<strong>in</strong>gle positive charge moves <strong>in</strong> the turn, i.e.,<br />

cCi=2nrE. Hence E= 2 8 ; .<br />

nr<br />

Thus, we f<strong>in</strong><strong>al</strong>ly obta<strong>in</strong>:<br />

E= 10_skn,r 2 =lO-skr<br />

2nf 2<br />

It should be noted that this electric field is <strong>in</strong>duced not by the electric<br />

charges, but by 8 magn<strong>et</strong>ic field vary<strong>in</strong>g with time. L<strong>et</strong> us rec<strong>al</strong>l that when<br />

an electric charge moves <strong>in</strong> a closed circuit <strong>in</strong> an electrostatic field the work<br />

is <strong>al</strong>ways equ<strong>al</strong> to zero. By an electrostatic field is meant an electric field<br />

<strong>in</strong>duced by electric charges.<br />

574. L<strong>et</strong> us divide the r<strong>in</strong>g <strong>in</strong>to n=b 6 a sm<strong>al</strong>l r<strong>in</strong>gs each with a width 6.<br />

L<strong>et</strong> us consider a r<strong>in</strong>g with a height h whose <strong>in</strong>tern<strong>al</strong> radius is x and extern<strong>al</strong><br />

radius is x+6. If 6 is sm<strong>al</strong>l as compared with x, the resistance of such a<br />

r<strong>in</strong>g can be expressed by the formula<br />

2nx<br />

R=p?;ji<br />

The e. m. f. of <strong>in</strong>duction act<strong>in</strong>g <strong>in</strong> this r<strong>in</strong>g (if 6 ~ x) is equ<strong>al</strong> to<br />

L\(!)<br />

8=10- 8 AT= 10-snx'k<br />

The <strong>in</strong>tensity of the current flow<strong>in</strong>g <strong>in</strong> such a r<strong>in</strong>g is<br />

Al =

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