A long conducting duct has rectangular cross-section of width (from to ) and height…

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Conductors, capacitance and boundary-value electrostatics · Conductors, capacitance and boundary-value electrostatics

The Boundary-Value Problem, Ch Separation of variables in Cartesian geometry

Problem

A long conducting duct has rectangular cross-section of width aa (from x=0x=0 to x=ax=a) and height bb (from y=0y=0 to y=by=b), with its length along zz. Three walls, x=0x=0, y=0y=0 and y=by=b, are earthed. Thin insulating strips separate them from the fourth wall, x=ax=a, held at potential V0V_0. The duct is long enough that the potential inside depends only on xx and yy, and there is no free charge inside. ((a)) Substitute V(x,y)=X(x)Y(y)V(x,y)=X(x)Y(y) into Laplace's equation ∂2V/∂x2+∂2V/∂y2=0\partial^2V/\partial x^2+\partial^2V/\partial y^2=0 and show that X′′/XX''/X and Y′′/YY''/Y must each be a constant, the two constants equal and opposite. ((b)) Two boundary conditions, Y(0)=0Y(0)=0 and Y(b)=0Y(b)=0, apply on the pair of earthed walls that face each other. By trying both signs for the constant multiplying Y′′/YY''/Y and checking which one admits a solution YY that is not zero everywhere while satisfying both conditions, show that the sign must be such that Y′′=−k2YY''=-k^2Y for some real kk, and find the allowed values of kk. ((c)) Write the function X(x)X(x) that solves the companion equation and vanishes on the earthed wall x=0x=0.

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