Finding the Potential Between Two Coaxial Cylinders Using Laplace's Equation

Click For Summary
SUMMARY

The discussion focuses on solving for the electric potential between two coaxial cylinders with radii {a,b} using Laplace's Equation. The boundary conditions are defined as V(a, φ) = 2 cos φ and V(b, φ) = 12 sin φ. The solution employs the method of separation of variables, leading to the potential function V(r, φ) expressed in terms of a series involving cosine and sine functions. The participants emphasize the necessity of correctly applying the boundary conditions for k=1 to derive nontrivial solutions.

PREREQUISITES
  • Understanding of Laplace's Equation in cylindrical coordinates
  • Familiarity with boundary value problems in electrostatics
  • Knowledge of separation of variables technique
  • Basic concepts of Fourier series in potential theory
NEXT STEPS
  • Study the method of separation of variables in more depth
  • Explore Fourier series applications in solving boundary value problems
  • Investigate the implications of boundary conditions in electrostatics
  • Learn about potential theory in cylindrical geometries
USEFUL FOR

Students and professionals in physics and engineering, particularly those focused on electrostatics, boundary value problems, and mathematical methods in physics.

cscott
Messages
778
Reaction score
1

Homework Statement



Two coaxial cylinders, radii {a,b} where b>a. Find the potential between the two cylinder surfaces.

Boundary conditions:
V(a,\phi) = 2 \cos \phi
V(b,\phi) = 12 \sin \phi

Homework Equations



Solution by separation of variables:
V(r,\phi) = a_0 + b_0 \ln s + \sum_k \left[ r^k(a_k \cos k\phi + b_k \sin k\phi)+r^{-k}(c_k\cos k\phi + d_k \sin k\phi)\right]

The Attempt at a Solution



I don't think I can eliminate the r^{-k} term because the origin isn't between the two cylinders.

I think k=1 is the only term in the summation that is required for the solution.

V(r,\phi) = r(a_1 \cos \phi + b_1 \sin \phi)+\frac{1}{r}(c_1\cos \phi + d_1 \sin \phi)

I don't see how to have the cosines vanish for V(b) and sines vanish for V(a) because of the common k in both.
 
Last edited:
Physics news on Phys.org
You should actually write down the boundary conditions for k=1. There are nontrivial solutions.
 
I made a typo in my boundary conditions

Boundary conditions (in volts):
V(a,\phi) = 2 \cos \phi
V(b,\phi) = 12 \sin \phiTaking V(r,\phi)_{k=1} gives,
V(r,\phi) = r(a_1 \cos \phi + b_1 \sin \phi)+\frac{1}{r}(c_1\cos \phi + d_1 \sin \phi)

I will take a look at this...
 

Similar threads

  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 29 ·
Replies
29
Views
3K
Replies
3
Views
2K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 2 ·
Replies
2
Views
6K
  • · Replies 7 ·
Replies
7
Views
6K
Replies
10
Views
4K