26.07.2013 Views

Introduction to vector and tensor analysis

Introduction to vector and tensor analysis

Introduction to vector and tensor analysis

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

line integral in Eq. (2.49), for example, is defined as<br />

<br />

C<br />

a · dr = def lim<br />

N→∞<br />

N<br />

a(xp ) · ∆rp,<br />

where all |∆rp| → 0 as N → ∞.<br />

Each of the line integrals in Eq. (2.49) is evaluated over some curve C<br />

that may be either open (A <strong>and</strong> B being distinct points) or closed (A <strong>and</strong> B<br />

coincide). In the latter case, one writes <br />

p=<br />

C<br />

<strong>to</strong> indicate this. The curve C is a<br />

space curve, c.f. section 2.5.1, most often defined in a parametric form. In a<br />

cartesian coordinate system C = (O, R), it becomes<br />

C : r(u) = <br />

xi(u)ei, u0 ≤ u ≤ u1, <strong>and</strong> [r(u0)] = x(A), [r(u1)] = x(B)<br />

i<br />

(2.50)<br />

The me<strong>to</strong>d of evaluating a line integral is <strong>to</strong> reduce it <strong>to</strong> a set of scalar<br />

<br />

integrals. It is usual <strong>to</strong> work in cartesian coordinates, in which case, dr =<br />

i eidxi. The three integrals in Eq. (2.49) then becomes<br />

<br />

<br />

C<br />

C<br />

<br />

φ(r)dr = C φ(r) (i<br />

eidxi) = <br />

i C φ(r)dxi<br />

<br />

a(r) · dr = j ejdxj<br />

<br />

= <br />

i C ai(r)dxi<br />

C (<br />

i ai(r)ei) ·<br />

ei<br />

(2.51)<br />

<strong>and</strong><br />

<br />

a(r) × dr C =<br />

<br />

C (i<br />

ai(r))<br />

× j ejdxj<br />

=<br />

<br />

<br />

C a2(r)dx3 − <br />

C a3(r)dx2<br />

<br />

e1 + <br />

C a3(r)dx1 − <br />

C a1(r)dx3<br />

+ <br />

C a1(r)dx2 − <br />

C a2(r)dx1<br />

<br />

e3<br />

(2.52)<br />

Note, that in the above we have used relations of the form<br />

<br />

<br />

aiejdxj = aidxj ej,<br />

C<br />

which is allowable since the cartesian basis is independent of the coordinates.<br />

If E = E(x) then the basis vec<strong>to</strong>rs could not be fac<strong>to</strong>rised out in the integral.<br />

The final scalar integrals in Eq. (2.51) <strong>and</strong> Eq. (2.52) can be solved using the<br />

parametrized form for C, Eq. (2.50). For instance<br />

<br />

C<br />

u1<br />

a2(r)dx3 =<br />

u0<br />

C<br />

a2(x1(u), x2(u), x3(u)) dx3<br />

du du.<br />

In general, a line integral between two points will depend on the specific path<br />

C defining the integral. However, for line integrals of the form <br />

C a · dr there<br />

exists a class of vec<strong>to</strong>r fields for which the line integral between two points<br />

is independent of the path taken. Such vec<strong>to</strong>r fields are called conservative.<br />

A vec<strong>to</strong>r field a that has continuous partial derivatives in a simply connected<br />

region R 7 , is conservative if, <strong>and</strong> only if, any of the following is true<br />

7 A simply connected region R is a region in space for which any closed path can be<br />

continuously shrunk <strong>to</strong> a point, ie. R has no “holes”<br />

21<br />

e2

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!