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| electrical_engineering_2:task_1.9.3_with_calculation [2023/03/10 11:33] – mexleadmin | electrical_engineering_2:task_1.9.3_with_calculation [Unbekanntes Datum] (aktuell) – gelöscht - Externe Bearbeitung (Unbekanntes Datum) 127.0.0.1 | ||
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| - | <panel type=" | ||
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| - | <WRAP right> | ||
| - | {{elektrotechnik_1: | ||
| - | </ | ||
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| - | Determine the capacitance $C$ for the plate capacitor drawn on the right with the following data: | ||
| - | * rectangular electrodes with edge length of $6 ~cm$ and $8 ~cm$. | ||
| - | * distance between the plates: $2 ~mm$ | ||
| - | * dielectric A: | ||
| - | * $\varepsilon_{r, | ||
| - | * thickness $d_A = 1.5 ~mm$ | ||
| - | * Dielectric B: | ||
| - | * $\varepsilon_{r, | ||
| - | * thickness $d_B = 0.5 ~mm$ | ||
| - | |||
| - | $\varepsilon_{0} = 8.854 \cdot 10^{-12} | ||
| - | |||
| - | <button size=" | ||
| - | * Which circuit can be used to replace a layered structure with different dielectrics? | ||
| - | </ | ||
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| - | <button size=" | ||
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| - | The total capacitance $C$ can be divided into a partial capacitance $C_A$ and a $C_B$. These are connected in series. \\ | ||
| - | This results in: $C = \frac{C_A \cdot C_B}{C_A + C_B}$ \\ \\ | ||
| - | |||
| - | The partial capacitance $C_A$ can be calculated by | ||
| - | \begin{align*} | ||
| - | C_A &= \varepsilon_{0} \varepsilon_{r, | ||
| - | C_A &= 8.854 \cdot 10^{-12} | ||
| - | C_A &= 28.33 \cdot 10^{-12} ~F \\ | ||
| - | \end{align*} | ||
| - | |||
| - | The partial capacitance $C_B$ can be calculated by | ||
| - | \begin{align*} | ||
| - | C_B &= \varepsilon_{0} \varepsilon_{r, | ||
| - | C_B &= 100 \cdot 8.854 \cdot 10^{-12} | ||
| - | C_B &= 8.500 \cdot 10^{-9} ~F \\ | ||
| - | \end{align*} | ||
| - | |||
| - | </ | ||
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| - | <button size=" | ||
| - | \begin{align*} | ||
| - | C = 28.24 \cdot 10^{-12} ~F \rightarrow 28~pF | ||
| - | \end{align*} | ||
| - | \\ | ||
| - | </ | ||
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| - | </ | ||