Line integral in polar/spherical system?

AI Thread Summary
A vector field can indeed exist in polar and spherical coordinate systems, and it is possible to define line integrals in these systems. The discussion explores the formulation of a vector field in polar coordinates, exemplified by A(r, φ) = r^3, and the corresponding line integral from (r1, φ1) to (r2, φ2). The calculations involve transforming the differential elements into polar and spherical coordinates, leading to expressions for arc length in both systems. The thread emphasizes the importance of correctly applying these transformations to compute line integrals effectively. Understanding these concepts is crucial for tackling problems in vector calculus involving polar and spherical coordinates.
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Hello, sorry for my English;D

Homework Statement


Can a vector field exist in polar/spherical system? is it possible to define line integral in these systems? does it make any sense a vector field defined in polar system, ex. \vec A\left(r,\varphi\right)=r^3? and a line integral from r_1,\varphi_1 to r_2,\varphi_2 like this \int\limits_L\vec A\left(r,\varphi\right)\mbox{d}r+r\vec A\left(r,\varphi\right)\mbox{d}\varphi, where L is a line defined by r\left(\phi\right) equation or r=r(t),\quad\phi=\phi(t)
and for spherical system \int\limits_L\vec A\left(r,\varphi,\phi\right)\mbox{d}r+r\vec A\left(r,\varphi,\phi\right)\mbox{d}\varphi+r\vec A\left(r,\varphi,\phi\right)\mbox{d}\phi?
thanks!
 
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In polar coordinates, x= r cos(\phi) so dx= cos(\phi)dr- r sin(\phi)d\phi. y= r sin(\phi) so dy= sin(\phi)dr+ r cos(\phi)d\phi.

dx^2= cos^2(\phi)dr^2- 2r cos(\phi)sin(\phi)drd\phi+ r^2 sin^2(\phi)d\phi^2
dy^2= sin^2(\theat)dr^2+ 2r cos(\phi)sin(\phi)drd\phi+ r^2cos^2(\phi)d\phi^2

so dx^2+ dy^2= dr^2+ r^2 d\phi^2 so the "differential of arc length", ds, is given by ds= \sqrt{dr^2+ r^2d\phi^2}.

If r and \phi are given in terms of a parameter, t, then
ds= \sqrt{\left(\frac{dr}{dt}\right)^2+ r^2\left(\frac{d\phi}{dt}\right)^2}dt

In spherical coordinates:

Since x= \rho cos(\theta)sin(\phi), dx= cos(\theta)sin(\phi)d\rho- \rho sin(\theta)sin(\phi)d\phi+ \rho cos(\theta)cos(\phi)d\phi.

Since y= \rho sin(\theta)sin(\phi), dx= sin(\theta)sin(\phi)d\rho+ \rho cos(\theta)sin(\phi)d\phi+ \rho sin(\theta)cos(\phi)d\phi.

Since z= \rho cos(\phi), dz= cos(\phi)d\rho- \rho sin(\phi)d\phi.

The "differential of areclength", ds, is given by ds= \sqrt{dx^2+ dy^2+ dz^2}. Use the above equations to write that in terms of d\rho, d\theta, and d\phi. it starts out messy but there is a lot of cancelling at the end.
 
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