Feldverhalten an Grenzflächen

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Stetigkeit

an Grenzflächen mit unterschiedlichem $\mu_{r}^{\left(1\right)},$ $\mu_{r}^{\left(2\right)}$

$\displaystyle \vec{n}\left(\vec{B}_{2}-\vec{B}_{1}\right)$	$\displaystyle =$	0
$\displaystyle B_{1n}$	$\displaystyle =$	$\displaystyle B_{2n}$
$\displaystyle H_{1n}\mu_{r}^{\left(1\right)}$	$\displaystyle =$	$\displaystyle H_{2m}\mu_{r}^{\left(2\right)}$

$\displaystyle \left(\vec{t}\times\vec{n}\right)\left(\vec{H}_{2}-\vec{H}_{1}\right)$

$\displaystyle =$

$\displaystyle \vec{j}_{F}\vec{t}$

$\vec{j}_{F}$ Flächenstromdichte. Wenn gilt weiter;

$\displaystyle H_{2t}$ $\displaystyle =$ $\displaystyle H_{1t}$

$\displaystyle B_{2t}\mu_{r}^{\left(1\right)}$ $\displaystyle =$ $\displaystyle B_{1t}\mu_{r}^{\left(2\right)}$

Marco Möller 20:49:26 12.02.2007

$\displaystyle H_{2t}$	$\displaystyle =$	$\displaystyle H_{1t}$
$\displaystyle B_{2t}\mu_{r}^{\left(1\right)}$	$\displaystyle =$	$\displaystyle B_{1t}\mu_{r}^{\left(2\right)}$