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

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MECHANICS 49<br />

the rod. F<strong>in</strong>d the distance I from po<strong>in</strong>t 0 at which the bead<br />

will be <strong>in</strong> equilibrium if the coefficient of friction b<strong>et</strong>ween the<br />

bead and the rod is k.<br />

198. A weight with a mass m is attached to the end of<br />

a str<strong>in</strong>g with a length I fastened to a vertic<strong>al</strong> rod rotat<strong>in</strong>g<br />

with an angular velocity ID. Another str<strong>in</strong>g of the same length<br />

as the first and carry<strong>in</strong>g on its end another weight with a mass<br />

m is secured to the first weight.<br />

Prove that dur<strong>in</strong>g rotation the angle b<strong>et</strong>ween the first str<strong>in</strong>g<br />

and the vertic<strong>al</strong> will be sm<strong>al</strong>ler than the angle b<strong>et</strong>ween the<br />

vertic<strong>al</strong> and the second str<strong>in</strong>g. Disregard the weight of the<br />

str<strong>in</strong>g.<br />

199. A weightless rod carries two weights of mass m and JW.<br />

The rod is h<strong>in</strong>ge-jo<strong>in</strong>ted to vertic<strong>al</strong> axis 00' (Fig. 81), which<br />

rotates with an angular velocity ID. D<strong>et</strong>erm<strong>in</strong>e the angle cp formed<br />

by the rod and the vertic<strong>al</strong>.<br />

200. A horizont<strong>al</strong> straight bar rotates with a constant angular<br />

velocity around a vertic<strong>al</strong> axis. A body can move without friction<br />

over the bar. Initi<strong>al</strong>ly, the body is r<strong>et</strong>a<strong>in</strong>ed <strong>in</strong> equilibrium by<br />

a spr<strong>in</strong>g (Fig. 82). What will happen to the body if an <strong>in</strong>iti<strong>al</strong><br />

velocity is imparted to it <strong>al</strong>ong the bar? The length of the spr<strong>in</strong>g<br />

<strong>in</strong> an unstr<strong>et</strong>ehed state can be neglected. .<br />

201. A m<strong>et</strong><strong>al</strong>lic cha<strong>in</strong> with a length of 1=62.8 em and whose<br />

ends are jo<strong>in</strong>ed tog<strong>et</strong>her is fitted onto a wooden disk (Fig. 83).<br />

The disk rotates with a speed of n = 60 rps. F<strong>in</strong>d the tension<br />

of the cha<strong>in</strong> T if its mass is m = 40 g.<br />

202. Water flows with a velocity v <strong>al</strong>ong a rubber tube hav<strong>in</strong>g<br />

the form of a r<strong>in</strong>g (Fig. 84). The radius of the r<strong>in</strong>g is Rand<br />

the diam<strong>et</strong>er of the tube d~R. What force is the rubber tube<br />

str<strong>et</strong>ched with?<br />

203. A homogeneous rod with a length I and a mass m rotates<br />

with an angular velocity (J) <strong>in</strong> a horizont<strong>al</strong> plane around an axis<br />

pass<strong>in</strong>g through its end. F<strong>in</strong>d the tension of the rod at a distance x<br />

from its axis of rotation.<br />

204. A b<strong>al</strong>l with the mass m secured on a weightless rod rotates<br />

with a constant velocity v <strong>in</strong> a horizont<strong>al</strong> plane (Fig. 85).<br />

Its k<strong>in</strong><strong>et</strong>ic energy <strong>in</strong> a coord<strong>in</strong>ate system that is stationary with<br />

respect to the axis of rotation is constant and equ<strong>al</strong> to mv'/2.<br />

The k<strong>in</strong><strong>et</strong>ic energy changes with time from zero to 4mv"/2 with<br />

respect to a read<strong>in</strong>g system that moves rectil<strong>in</strong>early <strong>in</strong> a horizont<strong>al</strong><br />

plane with a velocity v relative to the axis. What is the<br />

reasIn for this change <strong>in</strong> the energy?<br />

4-2042

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