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Problems in Mathematical Analysis.pdf - pwp.net.ipl.pt

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174 Def<strong>in</strong>ite Integrals [Ch. 5<br />

and<br />

Solution. We have:<br />

10<br />

p t*<br />

.-Jo.irt-o.i T = 250 metres<br />

=-=25 m/sec.<br />

2. The work of a force. If a variable force X=f(x) acts <strong>in</strong> the direction<br />

of the x-axis, then the work of this force over an <strong>in</strong>terval [x ly x z ] is<br />

A =<br />

Example 2. What work has to be performed to stretch a spr<strong>in</strong>g 6 cm, if<br />

a force of 1 kgf stretches it 1 by cm?<br />

Solution, Accord<strong>in</strong>g to Hook's law the force X kgf stretch<strong>in</strong>g the spr<strong>in</strong>g<br />

by xm is equal to X = kx, where k is a proportionality constant.<br />

Putt<strong>in</strong>g x = 0.01 m and X = l kgf, we get = 100 and, hence, X = 100v.<br />

Whence the sought-for work is<br />

0.06 0.08<br />

A = j 100 x dx = 50 x 2 = 0. 18 kgm<br />

3. K<strong>in</strong>etic energy. The k<strong>in</strong>etic energy of a material po<strong>in</strong>t of mass m and<br />

velocity v is def<strong>in</strong>ed as<br />

mv*<br />

The k<strong>in</strong>etic energy of a system of n material po<strong>in</strong>ts with masses<br />

mv m 2% ..., m n hav<strong>in</strong>g respective velocities t; lf v 2 , ..., v n , is equal to<br />

To compute the k<strong>in</strong>etic energy of a solid, the latter is appropriately partitioned<br />

<strong>in</strong>to elementary particles (which play the part of material po<strong>in</strong>ts); then<br />

by summ<strong>in</strong>g the k<strong>in</strong>etic energies of these particles we get, <strong>in</strong> the limit, an<br />

<strong>in</strong>tegral <strong>in</strong> place of the sum (1).<br />

Example 3. F<strong>in</strong>d the k<strong>in</strong>etic energy of a homogeneous circular cyl<strong>in</strong>der<br />

of density 6 with base radius R and altitude h rotat<strong>in</strong>g about its axis with<br />

angular velocity CD.<br />

Solution. For the elementary mass dm we take the mass of a hollow<br />

cyl<strong>in</strong>der of altitude h with <strong>in</strong>ner radius r and wall thickness dr (Fig. 60).<br />

We have:<br />

S<strong>in</strong>ce the l<strong>in</strong>ear velocity of the mass dm is equal to t; = /-co, the elementary<br />

k<strong>in</strong>etic energy is

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