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

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388 ANSWERS AND SOLUTIONS<br />

Fig. 500<br />

a<br />

F'<br />

J<br />

I<br />

J<br />

I<br />

I<br />

I<br />

\ I<br />

\ I<br />

\ 0<br />

s<br />

D<br />

If n is odd (n=2i+ 1) it can<br />

easily be seen that the i-th images<br />

lie on the cont<strong>in</strong>uations of<br />

the mirrors and th us co<strong>in</strong>ci de<br />

with the (i + 1) th and <strong>al</strong>l the subsequent<br />

images. For this reason<br />

there will be 2i images, Le.,<br />

n-l as before.<br />

690. Us<strong>in</strong>g the solution of<br />

Problem 689, l<strong>et</strong> us plot consecutively<br />

the first, second, third,<br />

<strong>et</strong>c., images of source S <strong>in</strong> the<br />

mirrors (Fig. 500). All of them<br />

will lie on a circle with a radius<br />

OS and the centre at po<strong>in</strong>to.<br />

If a is an <strong>in</strong>teger, the last i-th<br />

images will either g<strong>et</strong> onto po<strong>in</strong> ts<br />

C and D at which the circle <strong>in</strong>tersects<br />

the cont<strong>in</strong>uations of the<br />

mirrors, or will co<strong>in</strong>cide with<br />

po<strong>in</strong>t<br />

P diam<strong>et</strong>r<strong>al</strong>ly opposite to<br />

the source. In both cases the<br />

. number of images will be a-I.<br />

If a is not an <strong>in</strong>teger, for example a=2i ± ~, where ~ < 1, and i is an<br />

<strong>in</strong>teger, the last i-th images will lie on arc CPD that is beh<strong>in</strong>d both the<br />

first and the second mirrors and there wiII be no more reflections. Thus, the<br />

tot<strong>al</strong> number of images will be 2i.<br />

691. L<strong>et</strong> us plot the image of po<strong>in</strong>t B <strong>in</strong> mirror bd (Fig. 501). L<strong>et</strong> us<br />

then construct image B 1 <strong>in</strong> mirror cd. Also, B 3 is the image of B 2 In mirror<br />

ac and 8 4 is the image of 8 3 <strong>in</strong> mirror abo<br />

L<strong>et</strong> us connect po<strong>in</strong>ts A and B 4 • Po<strong>in</strong>t C is the po<strong>in</strong>t of <strong>in</strong>tersection of ab<br />

with l<strong>in</strong>e AB 4 • L<strong>et</strong> us now draw l<strong>in</strong>e B 3C from B 3 , and connect po<strong>in</strong>t D at<br />

which this l<strong>in</strong>e <strong>in</strong>tersects ac with 8 2 • E with B 1 , and F with B.<br />

It can be stated that broken l<strong>in</strong>e ACDEFB is the sought path of the<br />

beam. Indeed, s<strong>in</strong>ce B 3CB4 is an isosceles triangle, CD is the reflection of<br />

beam AC.

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