Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| electrical_engineering_and_electronics_2:block02 [2026/03/05 02:40] – angelegt mexleadmin | electrical_engineering_and_electronics_2:block02 [2026/03/05 03:09] (aktuell) – mexleadmin | ||
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| Zeile 167: | Zeile 167: | ||
| \end{align*} | \end{align*} | ||
| </ | </ | ||
| - | |||
| - | <panel type=" | ||
| - | |||
| - | Calculate the rectified value of rectangular and triangular signals! Use similar symmetry simplifications as shown for AC signals. Compare it to the values shown in <imgref imageNo5> | ||
| - | |||
| - | </ | ||
| == The RMS Value == | == The RMS Value == | ||
| Zeile 227: | Zeile 221: | ||
| </ | </ | ||
| - | |||
| - | <panel type=" | ||
| - | |||
| - | Calculate the RMS value of rectangular and triangular signals! Use similar symmetry simplifications as shown for AC signals. | ||
| - | Compare it to the values shown in <imgref imageNo5> | ||
| - | |||
| - | </ | ||
| == Comparison of the different Averages == | == Comparison of the different Averages == | ||
| Zeile 403: | Zeile 390: | ||
| ===== Exercises ===== | ===== Exercises ===== | ||
| + | |||
| + | <panel type=" | ||
| + | |||
| + | Calculate the rectified value of rectangular and triangular signals! Use similar symmetry simplifications as shown for AC signals. Compare it to the values shown in <imgref imageNo5> | ||
| + | |||
| + | </ | ||
| + | |||
| + | <panel type=" | ||
| + | |||
| + | Calculate the RMS value of rectangular and triangular signals! Use similar symmetry simplifications as shown for AC signals. | ||
| + | Compare it to the values shown in <imgref imageNo5> | ||
| + | |||
| + | </ | ||
| + | |||
| + | |||
| + | <panel type=" | ||
| + | A coil has a impedance of $80~\Omega$ at a frequency of $500 ~\rm Hz$. At which frequencies the impedance will have the following values? | ||
| + | - $85 ~\Omega$ | ||
| + | - $120 ~\Omega$ | ||
| + | - $44 ~\Omega$ | ||
| + | |||
| + | <button size=" | ||
| + | When the frequency changes the reactance changes but the inductance is constant. Therefore, the inductance is needed. \\ | ||
| + | It can be calculated by the given reactance for $f_0 = 500 ~\rm Hz$. | ||
| + | \begin{align*} | ||
| + | X_{L0}& | ||
| + | L & | ||
| + | \end{align*} | ||
| + | |||
| + | On the other hand, one can also use the rule of proportion here, and circumvent the calculation of inductance.\\ | ||
| + | It is possible to calculate the reactance at other frequencies with the given reactance. | ||
| + | \begin{align*} | ||
| + | X_L& | ||
| + | f & | ||
| + | & | ||
| + | \end{align*} | ||
| + | |||
| + | With the values given: | ||
| + | \begin{equation*} | ||
| + | f_1 = \frac{85 ~\Omega}{80~\Omega}\cdot500~{\rm Hz}\qquad | ||
| + | f_2 = \frac{120~\Omega}{80~\Omega}\cdot500~{\rm Hz}\qquad | ||
| + | f_3 = \frac{44 ~\Omega}{80~\Omega}\cdot500~{\rm Hz} | ||
| + | \end{equation*} | ||
| + | |||
| + | </ | ||
| + | \begin{equation*} | ||
| + | f_1=531.25~{\rm Hz}\qquad f_2=750~{\rm Hz}\qquad f_3=275~{\rm Hz} | ||
| + | \end{equation*} | ||
| + | </ | ||
| + | </ | ||
| + | |||
| + | <panel type=" | ||
| + | A capacitor with $5 ~{\rm µF}$ is connected to a voltage source which generates $U_\sim = 200 ~{\rm V}$. At which frequencies the following currents can be measured? | ||
| + | - $0.5 ~\rm A$ | ||
| + | - $0.8 ~\rm A$ | ||
| + | - $1.3 ~\rm A$ | ||
| + | </ | ||
| + | |||
| + | <panel type=" | ||
| + | A capacitor shall have a capacity of $4.7 ~{\rm µF} \pm 10~\%$. This capacitor shall be used with an AC voltage of $400~\rm V$ and $50~\rm Hz$. | ||
| + | What is the possible current range which could be found on this component? | ||
| + | </ | ||
| + | |||
| + | |||
| + | |||
| ==== Worked examples ==== | ==== Worked examples ==== | ||