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

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284 ANSWERS AND SOLUTIONS<br />

Fig. 403<br />

mg+4aa. ~ 2 3<br />

x a 2pg -. em<br />

Equilibrium is possible only if F<strong>al</strong>l<br />

is greater than Fcd by an amount<br />

equ<strong>al</strong> to the weight of the section<br />

of the film be<strong>in</strong>g considered.<br />

The difference b<strong>et</strong>ween the forces<br />

of surface tension can be expla<strong>in</strong>ed<br />

by the difference <strong>in</strong> the concentration<br />

of the soap <strong>in</strong> the surface<br />

layers of the film.<br />

354. The force of expulsion b<strong>al</strong>ances<br />

the weight of the cube mg<br />

and the force of surface tension 4aa.<br />

i.e., a 2 xpg = mg+ 4aa , where x is<br />

the sought distance. Therefore,<br />

The forces of surface tension <strong>in</strong>troduce a correction of about 0.1 em.<br />

355. The water rises to a height h = 2a . The potenti<strong>al</strong> energy of the wapgr<br />

ter colurnn is<br />

E = mgh = 2na;2<br />

p 2 pg<br />

4n(£2<br />

The forces of surface tension perform the work W=2nrah=--. One h<strong>al</strong>f<br />

Pi<br />

of this work goes to <strong>in</strong>crease the potenti<strong>al</strong> energy, and the other h<strong>al</strong>f to<br />

evolve heat. Hence,<br />

2na<br />

Q=pg<br />

2<br />

356. The pressure <strong>in</strong>side the liquid at a po<strong>in</strong>t that is at a height h above<br />

a certa<strong>in</strong> level is less than the pressure at this level by pgh. The pressure<br />

is zero at the level of the liquid <strong>in</strong> the vessel. Therefore, the pressure at<br />

the height h is negative (the liquid is str<strong>et</strong>ched) and is equ<strong>al</strong> to p= -pgh.<br />

357. The forces of attraction act<strong>in</strong>g on a molecule <strong>in</strong> the surface layer<br />

from <strong>al</strong>l the other molecules produce a resultant directed downward. The<br />

closest neighbours, however, exert a force of repulsion on the molecule which<br />

is therefore <strong>in</strong> equi librium.<br />

Ow<strong>in</strong>g to the forces of attraction and repulsion, the density of the liquid<br />

is sm<strong>al</strong>ler <strong>in</strong> the surface layer than <strong>in</strong>side. Indeed, molecule / (Fig. 404) is<br />

acted upon by the force of repulsion from molecule 2 and the forces of<br />

attract ion from <strong>al</strong>l the other molecules (3, 4, ...). Molecule 2 is acted upon<br />

by the forces of repulsion from 3 and / and the forces of attraction from the<br />

molecules <strong>in</strong> the deep layers. As a result, distance /-2 should be greater<br />

than 2-3, <strong>et</strong>c.<br />

This course of reason<strong>in</strong>g is quite approximate (therm<strong>al</strong> motion, <strong>et</strong>c., is<br />

disregarded), but nevertheless it gives a qu<strong>al</strong>itatively correct result.<br />

An <strong>in</strong>crease <strong>in</strong> the surface of the liquid causes new sections of the rarefied<br />

surface layer to appear. Here work should be performed aga<strong>in</strong>st the forces<br />

of attraction b<strong>et</strong>ween the molecules. It is this work that constitutes the<br />

surface energy.

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