| Reihenschaltung |
| \( R \, und \, C \) |
\( R \, und \, L \) |
| Widerstandsdreiecke |
|
|
| Scheinwiderstände |
| $$ Z = \frac{U}{I} $$ |
$$ Z = \frac{U}{I} $$ |
| $$ Z = \sqrt{R^2 + X_C^2} $$ |
$$ Z = \sqrt{R^2 + X_L^2} $$ |
| $$ Z = \frac{X_C}{\sin \varphi} $$ |
$$ Z = \frac{X_L}{\sin \varphi} $$ |
| $$ Z = \frac{R}{\cos \varphi} $$ |
$$ Z = \frac{R}{\cos \varphi} $$ |
| Wirkwiderstände |
| $$ R = \sqrt{Z^2 – X_C^2} $$ |
$$ R = \sqrt{Z^2 – X_L^2} $$ |
| $$ R = Z \cdot \cos \varphi $$ |
$$ R = Z \cdot \cos \varphi $$ |
| $$ R = \frac{X_C}{\tan \varphi} $$ |
$$ R = \frac{X_L}{\tan \varphi} $$ |
| Blindwiderstände |
| $$ X_C = \sqrt{Z^2 – R^2} $$ |
$$ X_L = \sqrt{Z^2 – R^2} $$ |
| $$ X_C = Z \cdot \sin \varphi $$ |
$$ X_L = Z \cdot \sin \varphi $$ |
| $$ X_C = R \cdot \tan \varphi $$ |
$$ X_L = R \cdot \tan \varphi $$ |
