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

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96 PROBLEMS<br />

of the vessel is placed <strong>in</strong>to a strong electric field b<strong>et</strong>ween<br />

the plates of a capacitor ow<strong>in</strong>g to which the level of the kerosene<br />

<strong>in</strong> this part is higher than <strong>in</strong> the other. A cha<strong>in</strong> of b<strong>al</strong>ls<br />

is passed over two pulleys.<br />

The specific weight of the materi<strong>al</strong> of the b<strong>al</strong>ls is less than<br />

that of the kerosene.<br />

The lift<strong>in</strong>g force act<strong>in</strong>g on the b<strong>al</strong>ls will be greater <strong>in</strong> the<br />

left-hand part than <strong>in</strong> the right-hand one because more b<strong>al</strong>ls<br />

are immersed <strong>in</strong> the kerosene <strong>in</strong> the left-hand part. For this<br />

reason the <strong>in</strong>ventor believes that the cha<strong>in</strong> should start rotat<strong>in</strong>g<br />

clockwise. Why will there actu<strong>al</strong>ly be no rotation?<br />

453. The space b<strong>et</strong>ween the plates of a plane capacitor is<br />

filled with a dielectric whose permittivity is ere One plate is<br />

given a charge +Q and the other -Q. D<strong>et</strong>erm<strong>in</strong>e the density<br />

of the bound electric charges that appear on the surface of the<br />

dielectric and the forces that are exerted by the field on the<br />

dielectric.<br />

454. The space b<strong>et</strong>ween the plates of a plane capacitor is<br />

filled with a dielectric. Each molecule of the dielectric is assumed<br />

to have the form of a "dumb-bell" with a length I whose<br />

ends carry charges +Q and -Q. The number of molecules <strong>in</strong><br />

a unit of volume (1 ern") is n.<br />

L<strong>et</strong> us assume further that <strong>al</strong>l the molecules have turned <strong>al</strong>ong<br />

the electric field under its action. F<strong>in</strong>d the <strong>in</strong>tensity E of the<br />

field <strong>in</strong>side the capacitor filled with the dielectric if before fill<strong>in</strong>g<br />

it the <strong>in</strong>tensity of the field was Eo.<br />

455. A dielectric consists of molecules each of which can be<br />

represented as two charges +Q and -Q b<strong>et</strong>ween which an<br />

"elastic force" acts. The latter term should be understood to mean<br />

that x (the distance b<strong>et</strong>ween the charges +Q and -Q) can be<br />

found from the equ<strong>al</strong>ity kx= QE, where E is the <strong>in</strong>tensity<br />

of the field act<strong>in</strong>g on the charges, and k is a proportion<strong>al</strong>ity<br />

factor.<br />

Assume that a unit of volume (1 ern") of the dielectric conta<strong>in</strong>s<br />

n molecules. Solve Problem 454, assum<strong>in</strong>g that the space<br />

b<strong>et</strong>ween the plates of the plane capacitor is filled with a dielectric<br />

of this type.<br />

D<strong>et</strong>erm<strong>in</strong>e the permittivity of the dielectric.<br />

456. A capacitor is filled with the dielectric whose properties<br />

are described <strong>in</strong> Problem 455.<br />

F<strong>in</strong>d the energy stored <strong>in</strong> the dielectric ow<strong>in</strong>g to its polarization.<br />

.

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