Boundary conditions for charged cylinder

AI Thread Summary
The discussion focuses on finding the potential inside and outside a charged infinite cylinder with a specific charge density, σ(φ) = k sin 5φ. The potential is expressed using Bessel functions, with the general form involving coefficients that depend on the charge density. Boundary conditions require continuity of potential at the cylinder's surface, specifically that the potential approaches a defined value as the radial coordinate approaches the cylinder's radius. The charge density influences the coefficients of the Bessel functions but does not dictate the radial dependence of the potential. Understanding these aspects is crucial for solving the problem accurately.
bigplanet401
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Hello,

Charge density \sigma(\phi) = k \sin 5\phi (where k is a constant is glued over the surface of an infinite cylinder of radius R with axis along the z-direction. Find the potential inside and outside the cylinder.

Two things I'm having trouble with:

1. Is the potential of an infinite cylinder
<br /> \begin{equation}<br /> V(\rho^\prime, \phi) = \sum_{m = 0}^{\infty} \, [A_m J_m (k\rho^\prime) + B_m N_m (k\rho^\prime)] [C_m \sin m\phi + D_m \cos m\phi] \; ?<br /> \end{equation}<br />

Do you need to include Neuman functions in the full solution?

2. Whatare the boundary conditions for this problem? Not knowing the potential at rho^prime = R made me confused. How many conditions do you need? And does the charge density tell you in any way about the radial dependence of the potential?
 
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Thank you for your help. The potential of an infinite cylinder is given by the solution to Laplace's equation in cylindrical coordinates: \begin{equation}V(\rho^\prime, \phi) = \sum_{m = 0}^{\infty} \, [A_m J_m (k\rho^\prime) + B_m Y_m (k\rho^\prime)] [C_m \sin m\phi + D_m \cos m\phi]\end{equation}where $J_m$ and $Y_m$ are the Bessel functions of the first and second kind, respectively, $k$ is the wavenumber of the charge density, $\rho^\prime$ is the radial coordinate, and $\phi$ is the angular coordinate.The boundary conditions for this problem depend on the form of the charge density. For the case of a charge density with a constant component, such as $\sigma(\phi) = k \sin 5\phi$, the boundary conditions are that the potential is continuous at the surface of the cylinder, which means that $\lim_{\rho^\prime \rightarrow R} V(\rho^\prime, \phi) = V_0$. Here, $V_0$ is the potential at the surface of the cylinder.The charge density does not tell you about the radial dependence of the potential, but it does constrain the coefficients of the Bessel functions. The coefficients $A_m$ and $B_m$ can be found by integrating the charge density over the surface of the cylinder and applying the boundary condition. Hope this helps.
 
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