CSM: ideal solenoid magnet - Analytical expression #21
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Description of the example
In this example, we consider a solenoid conductor with finite thickness and infinite length.
This allow us to ignore the z components in our equations.
We admit that there is only a radial expansion.
Geometry
The conductor$\Omega$ consists in a rectangular cross section torus.$\mathbf{R}^3/\Omega$ .
The geometry also contains an external domain which is an approximation of
Input parameters
current density:$\textbf{j}$ in $A/m^2$ .$\textbf{b}$ in $T$ .
magnetic field:
Model & Toolbox
From the momentum conservation equation, we have:
$j_{\theta}$ :
[
div\sigma+\textbf{j}\times\textbf{b}=0
]
With the hypothesys specified in introduction, this equation may be rewritten :
[
-\sigma_{\theta}+\frac{\partial}{\partial r}(r\sigma_{r})=-rj_{\theta}b_{z}
]
For a solenoid conductor with finite thickness and infinite length, we have for a constant current density
[
b_{z} = ...
]
With these hypothesys, we can show that (see [REF002]):
[
u_{r} = ...
]
toolbox: elasticity
Materials
|Name |Description | Value | Unit |
|$E$ |Young modulus||$128.10^{9}$|$Pa=kg.m^{-1} .s^{-2}$|
|$\nu$|Poisson's ratio|0.33|- |
Boundary conditions
Outputs
The output is describe the output set of the example
Fields
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Measures
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Benchmark
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[X] Verification
[] Validation
[] Performance
The computed values of the displacements on r-axis in the solenoidal mid-plane are compared
with the analytical expression given by Montgomery.
References (articles, papers, reports...)
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