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

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344 .<br />

ANSWERS AND SOLUTIONS<br />

Fig. 457<br />

Fig. 458<br />

The field created by the current with a density I at an arbitrary po<strong>in</strong>t<br />

of space A is equ<strong>al</strong> to HI=k·2njR (Fig. 456). Here R is the distance from<br />

the axis of the conductor to po<strong>in</strong>t A. (It is assumed that the current flows<br />

toward us.)<br />

At the same po<strong>in</strong>t, the current flow<strong>in</strong>g through the volume. correspond<strong>in</strong>g<br />

to the space, but <strong>in</strong> the reverse direction, <strong>in</strong>duces a field of H 2=k·2njr.<br />

Figure 456 shows that the tot<strong>al</strong> <strong>in</strong>tensity of the field is<br />

Obviously,<br />

H=VH:+H:-2H 1Ht cos ex<br />

Therefore, the <strong>in</strong>tensity H =k·2njd is the same for <strong>al</strong>l the po<strong>in</strong>ts of the<br />

space. .<br />

551. Triangle AOC is similar to triangle BAD (Fig. 456) s<strong>in</strong>ce they have<br />

one equ<strong>al</strong> angle, and the sides conf<strong>in</strong><strong>in</strong>g these angles are proportion<strong>al</strong>.'<br />

Therefore, L AOC=L BAD. But R l..H 1 , and therefore H l..d.<br />

The <strong>in</strong>tensity of the magn<strong>et</strong>ic field at any ro<strong>in</strong>t of the space is perpendicular<br />

to the l<strong>in</strong>e that connects the centres 0 the conductor and the space.<br />

The distribution of the l<strong>in</strong>es is shown <strong>in</strong> Fig. 457.<br />

552. k=..!.., where c is the velocity of light <strong>in</strong> a vacuum.<br />

c<br />

553. No, it will not. Forces of attraction exist b<strong>et</strong>ween the separate elements<br />

of the current. As a result, the density of the current <strong>in</strong>creases somewhat<br />

toward the axis of the conductor. The effect is negligible.<br />

554. When lightn<strong>in</strong>g strikes. a very high current flows for an <strong>in</strong>stant<br />

through the pipe and the separate elements of the current are mutu<strong>al</strong>ly<br />

attracted with a high force. It is this force that converts the pipe <strong>in</strong>to<br />

a rod.

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