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

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Sec. 9] L<strong>in</strong>e Integrals 2S&<br />

D. Applications of the L<strong>in</strong>e Integral<br />

Evaluate the areas of figures bounded by the follow<strong>in</strong>g curves:<br />

2336. The ellipse x = a cos/, y = bs\nt.<br />

2337. The astroid jt = acos 3<br />

/, #-=as<strong>in</strong> 8<br />

/.<br />

2338. The cardioid x = a (2 cos/ cos 2/), y = a (2 s<strong>in</strong>/<br />

s<strong>in</strong> 20-<br />

2339*. A loop of the folium of Descartes x* +if 3zxy = Q<br />

(a>0).<br />

2340. The curve (x + = y)* axy.<br />

2341*. A circle of radius r is roll<strong>in</strong>g without slid<strong>in</strong>g along a<br />

fixed circle of radius R and outside it. Assum<strong>in</strong>g that<br />

n<br />

is an<br />

<strong>in</strong>teger, f<strong>in</strong>d the area bounded by the curve (epicycloid) described<br />

by some po<strong>in</strong>t of the mov<strong>in</strong>g circle. Analyze the particular case<br />

of r R (cardioid).<br />

2342*. A circle of radius r is roll<strong>in</strong>g without slid<strong>in</strong>g along<br />

D<br />

that is an<br />

a fixed circle of radius R and <strong>in</strong>side it. Assum<strong>in</strong>g<br />

<strong>in</strong>teger, f<strong>in</strong>d the area bounded by the curve (hypocycloid) described<br />

by some po<strong>in</strong>t of the mov<strong>in</strong>g circle. Analyze the particular<br />

r><br />

case when r = j (astroid).<br />

2343. A field is generated by a force of constant magnitude F<br />

<strong>in</strong> the positive jt-direelion F<strong>in</strong>d the work that the field does<br />

when a material po<strong>in</strong>t traces clockwise a quarter of the circle<br />

x 2 2<br />

-^-y ^=R ly<strong>in</strong>g <strong>in</strong> the first quadrant.<br />

2344. F<strong>in</strong>d the work done by the force of gravity when<br />

a material po<strong>in</strong>t of mass m is moved ironi position A (JC P // l? zjto<br />

position B (x 2 , // 2 , z 2 ) (the z-axis is directed vertically up-<br />

wards).<br />

2345. F<strong>in</strong>d the work done by an elastic force directed towards<br />

the coord<strong>in</strong>ate orig<strong>in</strong> if the magnitude of the force is proportional<br />

to the distance of the po<strong>in</strong>t fiom the orig<strong>in</strong> and if the po<strong>in</strong>t<br />

of application of the force traces counterclockwise a quarter of<br />

the ellipse ^s4-^i=l ly<strong>in</strong>g <strong>in</strong> the first quadrant.<br />

2346. F<strong>in</strong>d the potential function of a force R {X, Y, Z\<br />

and determ<strong>in</strong>e the work done by the force over a given path if:<br />

a) X = 0, K:=0. Z-=rng (force of gravity) and the mate-<br />

rial po<strong>in</strong>t is moved from position A (x lt y l9 zj to position<br />

B(* Uv *i)'b)<br />

x= ?, K=-^. Z=-* f where jx = const and<br />

r Yx* 4 if -\- f (Newton attractive force) and the material po<strong>in</strong>t<br />

moves from position A (a, b, c) to <strong>in</strong>f<strong>in</strong>ity;

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