How Can the Magnetic Vector Potential be Numerically Solved in the X-Y Plane?

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To numerically solve the wave equation of the magnetic vector potential in the x-y plane, one should start with the identity "curl squared = grad div - del squared," leading to Laplace's equation under the gauge condition ∇·A = 0. The resultant equation ∇^2 A = -µ J indicates that A is a vector, necessitating the solution of its components separately in Cartesian coordinates, resulting in three Laplacian equations. The components Ax, Ay, and Az can be placed at grid nodes, but alternative grid setups, such as the Yee grid used in FDTD methods, may also be suitable. The discussion highlights the importance of choosing a stable numerical method for discretizing the magnetic field potential in the x-y-z plane. Examples of discretization techniques and relevant literature are sought for further guidance.
merro
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hi everybody
i want to solve the wave equation of the magnetic vector potential numerically in x-y plane grid,
curl curl A= µ J
anyone can help me

thanks in advance
 
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Well first you should use the identity "curl squared = grad div - del squared": ∇ x (∇ x A) = ∇ ∇·A - ∇2 A. Then choose a gauge ∇·A = 0. You're left with Laplace's equation, which can be solved numerically.
 
thanks, but i have another question , the reusltant equation will be ∇^2 A=-µ J, and A is a vector, not a scalar, this one is not Laplace , is Poisson, or
 
because the A is a vector then must be put in links of the grid, not on the nodes, or?
 
merro said:
thanks, but i have another question , the reusltant equation will be ∇^2 A=-µ J, and A is a vector, not a scalar, this one is not Laplace , is Poisson, or

But J is a vector too. Solve the vector components separately in Cartesian coordinates and you have three Laplacian equations.
 
do you mean that
∇^2 Ax=Jx,
∇^2 Ay=Jy,
∇^2 Az=Jz,
and Ax, Ay, Az lies on the grid nodes
 
merro said:
do you mean that
∇^2 Ax=Jx,
∇^2 Ay=Jy,
∇^2 Az=Jz,
and Ax, Ay, Az lies on the grid nodes

As you wish, though there are a few ways to setup the grid for electromagnetics depending on the exact numerical procedure. For example, a common grid for FDTD, the Yee grid, will offset the electric and magnetic fields from the grid points. That may also be appropriate here if you wish to do a second order finite difference approach.
 
please , can you show me some examples to discrization of the magentic field potential in x-y-z plan , if anyone has a paper of chapter of book can help me. and which methods could be stable numerically
 
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