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

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Sec. 12] Fundamentals of Field Theory 289<br />

which <strong>in</strong> vector form is<br />

ff (\ r\ r*<br />

div a dx dy dz.<br />

5. Circulation of a vector, the work of a Held. The l<strong>in</strong>e <strong>in</strong>tegral of the<br />

vector a along the curve C is def<strong>in</strong>ed by the formula<br />

f a dr= \ a s ds V a x dx -f- a ydy -f a z dz<br />

C C C<br />

and represents the work done by the field a along the curve C (as<br />

is the<br />

projection of the vector a on the tangent to C).<br />

If C is closed, then the l<strong>in</strong>e <strong>in</strong>tegral (1) is called the circulation of the<br />

vector field a around the contour C.<br />

If the closed curve C bounds a two-sided surfaces, then Stokes' formula<br />

holds, which <strong>in</strong> vector form has the form<br />

adr= f f /i rotadS,<br />

where n is the vector of the normal to the surface S; the direction of the<br />

vector should be chosen so that for an observer look<strong>in</strong>g <strong>in</strong> the direction of n<br />

the circulation of the contour C should be counterclockwise <strong>in</strong> a right-handed<br />

coord<strong>in</strong>ate system.<br />

6. Potential and solenoidal fields. The vector iield a(r) is called poten-<br />

tial if<br />

where Uf(r) is a scalar function (the potential of the field).<br />

For the potentiality of a field a, given <strong>in</strong> a simply-connected doma<strong>in</strong>,<br />

it is necessary and sufficient that it be non rotational, that is, rota = 0. In<br />

that case there exists a potential U def<strong>in</strong>ed by the equation<br />

U,<br />

dU ~a x dx-}- a v dy -f- a 2 dz.<br />

If the potential U is a s<strong>in</strong>gle-valued function, then \ a dr U (B) U (A);<br />

AB<br />

<strong>in</strong> particular, the circulation of the vector a is equal to zero: m adr=Q.<br />

A vector field a (r) is called solenoidal if at each po<strong>in</strong>t of the field div<br />

a = 0; <strong>in</strong> this case the flux of the vector through any closed surface is zero.<br />

If the field is at the same time potential and solenoidal, then div (grad U)=.Q<br />

and the potential function U is harmonic; that is, it satisfies the Laplace<br />

or AU=0 where A= isthe<br />

*'=;+>+><br />

"Er++5-. '<br />

Laplacian operator<br />

2371. Determ<strong>in</strong>e the level surfaces of the scalar field<br />

where r \fx*+y*-\-z*. What will the level surfaces be of a field<br />

U = F(Q), where<br />

10-1900<br />

(0

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