# 2D formulation for Electrostatic Problems

From KratosWiki

(Difference between revisions)

Line 11: | Line 11: | ||

\left . \hat n \vec{D} - \bar D_n = 0 \right |_{\Gamma_{q}} & in ~ \Gamma_{q} \\ | \left . \hat n \vec{D} - \bar D_n = 0 \right |_{\Gamma_{q}} & in ~ \Gamma_{q} \\ | ||

\, \\ | \, \\ | ||

− | \left . \displaystyle \frac{\partial V}{\partial r} \right |_{\Gamma_{\infty}} \approx - \frac{V}{r^{exp}} & in ~ \Gamma_{\infty} | + | \left . \displaystyle \frac{\partial V}{\partial r} \right |_{\Gamma_{\infty}} |

+ | \approx \displaystyle - \frac{V}{r^{exp}} & in ~ \Gamma_{\infty} | ||

\end{cases} | \end{cases} | ||

</math> | </math> |

## Revision as of 19:21, 11 November 2009

The 2D Electrostatic Poisson's equation given by the governing PDE and its boundary conditions:

can be written as (see the General formulation for Electrostatic Problems):

with (* n* is the number of nodes of the element):

## 2D formulation for Triangular Elements