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

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(1<br />

A6000-"""'------------..li.....-<br />

1<br />

Accord<strong>in</strong>g to the cos<strong>in</strong>e rule,<br />

F=V F~+F:-2FIF2 cos p=<br />

Fig. 976<br />

4 .. /~R~8---r6---2""!!!'R..... 8r-S-c-o-s-=p<br />

=3"nymp V zr+(12-d 2) 2 11(lI-d 2) ~5.8XIO-t gf<br />

233. The sought force of attraction is the geom<strong>et</strong>ric<strong>al</strong> sum of the forces<br />

created by separate elements of the sphere. The sm<strong>al</strong>l elements 01 and 0'2<br />

(Fig. 377) are cut out of the sphere as cones with vertices at po<strong>in</strong>t A obta<strong>in</strong>ed<br />

when the generatrix Be revolves around axis 8 182 • The areas of the elements<br />

( AS )2ro (AS )1ro (AS )2 rop<br />

are 1 and 2 respectively and their masses are _ .....1_~<br />

cos (Xl cos (X2 " cos (Xl<br />

and (AS 2 )2 rop , where (J) is the solid angle at which both elements can be<br />

cos (Xl<br />

seen from po<strong>in</strong>t A; p is the surface density of the sphere (the mass<br />

per unit<br />

of surface); L. (Xl= L. (X2' s<strong>in</strong>ce StOSI is an isosceles triangle. The forces of<br />

attraction created by the elements are equ<strong>al</strong>, respectively, to:<br />

and<br />

m (AS 1 )2

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