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

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MECHANICS<br />

183<br />

Fig. 294<br />

Fig. 295<br />

(see Problem 34). Hence,<br />

at<br />

a 2<br />

4ml m3- 3m2m3+ ml m2<br />

g<br />

4ml m3+m 2m3+mtm t<br />

mlm2-4mlm3+m2m3<br />

g<br />

4m1m 3+ m2mS+ m 1m2<br />

4mlmS-3mlm2+m2m3<br />

as= 4mlmS+m2mS+mlm2 g<br />

69. The second monkey will be at the same height as the first.<br />

If the mass of the pulley and the weight of the rope are disregarded,<br />

the force T tension<strong>in</strong>g both ends of the rope will be the same and, therefore,<br />

the forces act<strong>in</strong>g on each monkey will equ<strong>al</strong> F=T-mg. Both monkeys have<br />

the same accelerations <strong>in</strong> magnitude and direction and will reach the pul..<br />

ley at the same time.<br />

70. S<strong>in</strong>ce the mass of the pulleys and the str<strong>in</strong>g is negligibly sm<strong>al</strong>l, the<br />

tension of the thread is the same everywhere.<br />

Therefore,<br />

mlg-T=m1a1<br />

mgg- 2T= m 2a2<br />

2T-T=O<br />

Hence, T=O and a1=a2= g.<br />

Both weights f<strong>al</strong>l freely with an acceleration g. Pulleys Band C rotate<br />

counterclockwise and pulley A clockwise.<br />

71. (1) The forces act<strong>in</strong>g on the table and the weight are shown <strong>in</strong> Fig. 295.<br />

The equations of horizont<strong>al</strong> motion have the follow<strong>in</strong>g form:<br />

for the table with the pulley<br />

and for' {h'c weight<br />

0 1<br />

F-F+F/r=-a t g

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