Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
Beide Seiten der vorigen Revision Vorhergehende Überarbeitung Nächste Überarbeitung | Vorhergehende Überarbeitung Nächste Überarbeitung Beide Seiten der Revision | ||
electrical_engineering_1:dc_circuit_transients [2023/12/02 00:50] mexleadmin [Exercises] |
electrical_engineering_1:dc_circuit_transients [2023/12/02 00:55] mexleadmin [Exercises] |
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Zeile 483: | Zeile 483: | ||
* $R_3 = 3 \rm k\Omega$ | * $R_3 = 3 \rm k\Omega$ | ||
* $C = 1 \rm \mu F$ | * $C = 1 \rm \mu F$ | ||
- | * $S_1$ and $S_2$ are opened (open-circuit) | + | * $S_1$ and $S_2$ are opened |
{{drawio> | {{drawio> | ||
Zeile 569: | Zeile 569: | ||
Again the time constant $\tau$ is given as: $\tau= R\cdot C$. \\ | Again the time constant $\tau$ is given as: $\tau= R\cdot C$. \\ | ||
Again, we try to determine which $R$ and $C$ must be used here. \\ | Again, we try to determine which $R$ and $C$ must be used here. \\ | ||
- | To find this out, we have to look at the circuit when both $S_1$ and $S_2$ are closed. | + | To find this out, we have to look at the circuit when both $S_1$ and $S_2$ are closed. \\ |
+ | In this case, we can " | ||
{{drawio> | {{drawio> | ||
Zeile 578: | Zeile 579: | ||
\tau_2 &= R\cdot C \\ | \tau_2 &= R\cdot C \\ | ||
& | & | ||
- | & | + | & |
\end{align*} | \end{align*} | ||