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| Both sides previous revision Previous revision Next revision | Previous revision | ||
| electrical_engineering_and_electronics_2:block08 [2026/05/12 02:49] – mexleadmin | electrical_engineering_and_electronics_2:block08 [2026/05/19 02:12] (current) – mexleadmin | ||
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| Line 543: | Line 543: | ||
| \end{align*} | \end{align*} | ||
| - | Choose the voltage as reference: | ||
| - | \begin{align*} | ||
| - | \underline{U}=U\angle 0^\circ | ||
| - | \end{align*} | ||
| - | |||
| - | The branch currents are: | ||
| - | \begin{align*} | ||
| - | \underline{I}_R &= \frac{U}{R}\angle 0^\circ \\ | ||
| - | \underline{I}_L &= \frac{U}{X_L}\angle -90^\circ \\ | ||
| - | \underline{I}_C &= \frac{U}{X_C}\angle +90^\circ | ||
| - | \end{align*} | ||
| - | |||
| - | with the reactances | ||
| - | \begin{align*} | ||
| - | X_L &= \omega L \\ | ||
| - | X_C &= \frac{1}{\omega C} | ||
| - | \end{align*} | ||
| - | |||
| - | The source current is the phasor sum: | ||
| - | \begin{align*} | ||
| - | \underline{I} | ||
| - | = \underline{I}_R+\underline{I}_L+\underline{I}_C | ||
| - | \end{align*} | ||
| </ | </ | ||
| # | # | ||
| Line 571: | Line 548: | ||
| <WRAP half column> | <WRAP half column> | ||
| # | # | ||
| + | {{drawio> | ||
| \begin{align*} | \begin{align*} | ||
| \underline{U}_R | \underline{U}_R | ||
| Line 631: | Line 609: | ||
| <WRAP half column> | <WRAP half column> | ||
| # | # | ||
| + | |||
| + | [[https:// | ||
| + | |||
| + | |||
| \begin{align*} | \begin{align*} | ||
| f_0 \approx 3.18~{\rm kHz} | f_0 \approx 3.18~{\rm kHz} | ||
| Line 698: | Line 680: | ||
| # | # | ||
| <WRAP leftalign> | <WRAP leftalign> | ||
| + | Choose the voltage as reference: | ||
| + | \begin{align*} | ||
| + | \underline{U}=U\angle 0^\circ | ||
| + | \end{align*} | ||
| + | |||
| + | The branch currents are: | ||
| + | \begin{align*} | ||
| + | \underline{I}_R &= \frac{U}{R}\angle 0^\circ \\ | ||
| + | \underline{I}_L &= \frac{U}{X_L}\angle -90^\circ \\ | ||
| + | \underline{I}_C &= \frac{U}{X_C}\angle +90^\circ | ||
| + | \end{align*} | ||
| + | |||
| + | with the reactances | ||
| + | \begin{align*} | ||
| + | X_L &= \omega L \\ | ||
| + | X_C &= \frac{1}{\omega C} | ||
| + | \end{align*} | ||
| + | |||
| At $f=f_0$: | At $f=f_0$: | ||
| \begin{align*} | \begin{align*} | ||
| Line 703: | Line 703: | ||
| \end{align*} | \end{align*} | ||
| - | The branch currents are: | + | we get: |
| \begin{align*} | \begin{align*} | ||
| \underline{I}_R | \underline{I}_R | ||
| Line 711: | Line 711: | ||
| \underline{I}_C | \underline{I}_C | ||
| &= 0.24~{\rm A}\angle +90^\circ | &= 0.24~{\rm A}\angle +90^\circ | ||
| + | \end{align*} | ||
| + | |||
| + | |||
| + | The source current is the phasor sum: | ||
| + | \begin{align*} | ||
| + | \underline{I} | ||
| + | = \underline{I}_R+\underline{I}_L+\underline{I}_C | ||
| \end{align*} | \end{align*} | ||
| Line 733: | Line 740: | ||
| \underline{U} &= 12~{\rm V}\angle 0^\circ \\ | \underline{U} &= 12~{\rm V}\angle 0^\circ \\ | ||
| \underline{I}_R &= 1.2~{\rm mA}\angle 0^\circ \\ | \underline{I}_R &= 1.2~{\rm mA}\angle 0^\circ \\ | ||
| - | \underline{I}_L & | + | \underline{I}_L & |
| - | \underline{I}_C & | + | \underline{I}_C & |
| \underline{I} &= 1.2~{\rm mA}\angle 0^\circ | \underline{I} &= 1.2~{\rm mA}\angle 0^\circ | ||
| \end{align*} | \end{align*} | ||
| + | |||
| + | {{drawio> | ||
| + | |||
| # | # | ||
| </ | </ | ||
| Line 758: | Line 768: | ||
| The input reactive power is: | The input reactive power is: | ||
| \begin{align*} | \begin{align*} | ||
| - | Q = 0 | + | Q = 0 ~\rm var |
| \end{align*} | \end{align*} | ||
| Line 779: | Line 789: | ||
| \begin{align*} | \begin{align*} | ||
| P &= 14.4~{\rm mW} \\ | P &= 14.4~{\rm mW} \\ | ||
| - | Q &= 0 \\ | + | Q &= 0 ~{\rm var}\\ |
| S &= 14.4~{\rm mVA} | S &= 14.4~{\rm mVA} | ||
| \end{align*} | \end{align*} | ||
| Line 823: | Line 833: | ||
| \underline{I} | \underline{I} | ||
| &= 1.2~{\rm mA} - j(0.48~{\rm A}-0.12~{\rm A}) \\ | &= 1.2~{\rm mA} - j(0.48~{\rm A}-0.12~{\rm A}) \\ | ||
| - | &= 0.0012 - j0.36~{\rm A} | + | &= 0.0012 - j \cdot 0.36~{\rm A} |
| \end{align*} | \end{align*} | ||
| Line 829: | Line 839: | ||
| \begin{align*} | \begin{align*} | ||
| I & | I & | ||
| - | \varphi_I &\approx | + | \varphi_I &= -89.8 ... ^\circ |
| \end{align*} | \end{align*} | ||
| Line 838: | Line 848: | ||
| <WRAP half column> | <WRAP half column> | ||
| # | # | ||
| + | |||
| + | |||
| \begin{align*} | \begin{align*} | ||
| \underline{U} &= 12~{\rm V}\angle 0^\circ \\ | \underline{U} &= 12~{\rm V}\angle 0^\circ \\ | ||
| \underline{I}_R &= 1.2~{\rm mA}\angle 0^\circ \\ | \underline{I}_R &= 1.2~{\rm mA}\angle 0^\circ \\ | ||
| - | \underline{I}_L & | + | \underline{I}_L & |
| - | \underline{I}_C & | + | \underline{I}_C & |
| - | \underline{I} & | + | \underline{I} & |
| \end{align*} | \end{align*} | ||
| + | |||
| + | {{drawio> | ||
| + | |||
| + | |||
| # | # | ||
| </ | </ | ||
| Line 855: | Line 871: | ||
| # | # | ||
| + | |||
| + | <WRAP right> | ||
| + | |||
| Many power electronic converters generate harmonics of the grid frequency. | Many power electronic converters generate harmonics of the grid frequency. | ||
| Line 876: | Line 895: | ||
| \end{align*} | \end{align*} | ||
| - | 1. Give the complex input impedance of the harmonic trap. | + | 1. Give the formula of the complex input impedance of the harmonic trap. |
| <WRAP group> | <WRAP group> | ||
| <WRAP half column rightalign> | <WRAP half column rightalign> | ||
| Line 913: | Line 932: | ||
| </ | </ | ||
| - | 2. How large must $L_{\rm trap}$ be so that the 5th harmonic is suppressed? | + | 2. How large must $L_{\rm trap}$ be so that the 5th harmonic is suppressed |
| <WRAP group> | <WRAP group> | ||
| <WRAP half column rightalign> | <WRAP half column rightalign> | ||
| Line 963: | Line 982: | ||
| </ | </ | ||
| - | 3. How large is the complex input impedance for the fundamental frequency $\nu=1$? | + | 3. How large is the complex input impedance for the fundamental frequency |
| <WRAP group> | <WRAP group> | ||
| <WRAP half column rightalign> | <WRAP half column rightalign> | ||
| Line 990: | Line 1009: | ||
| Thus: | Thus: | ||
| \begin{align*} | \begin{align*} | ||
| - | \underline{Z}_{\rm | + | \underline{Z}_{\rm |
| &= j(X_L-X_C) \\ | &= j(X_L-X_C) \\ | ||
| &= j(84.9~{\rm \Omega}-2122~{\rm \Omega}) \\ | &= j(84.9~{\rm \Omega}-2122~{\rm \Omega}) \\ | ||
| - | &= -j2037~{\rm \Omega} | + | &= -j \cdot 2037~{\rm \Omega} |
| \end{align*} | \end{align*} | ||
| </ | </ | ||
| Line 1001: | Line 1020: | ||
| # | # | ||
| \begin{align*} | \begin{align*} | ||
| - | \underline{Z}_{\rm | + | \underline{Z}_{\rm |
| - | = -j2037~{\rm \Omega} | + | = -j \cdot 2037~{\rm \Omega} |
| \end{align*} | \end{align*} | ||
| # | # | ||
| Line 1015: | Line 1034: | ||
| At the fundamental frequency, the harmonic trap has the impedance: | At the fundamental frequency, the harmonic trap has the impedance: | ||
| \begin{align*} | \begin{align*} | ||
| - | \underline{Z}_{\rm | + | \underline{Z}_{\rm |
| \end{align*} | \end{align*} | ||
| The current magnitude is: | The current magnitude is: | ||
| \begin{align*} | \begin{align*} | ||
| - | I &= \frac{U}{|Z_{\rm | + | I &= \frac{U}{|Z_{\rm |
| &= \frac{230~{\rm V}}{2037~{\rm \Omega}} \\ | &= \frac{230~{\rm V}}{2037~{\rm \Omega}} \\ | ||
| &= 0.113~{\rm A} | &= 0.113~{\rm A} | ||
| Line 1051: | Line 1070: | ||
| </ | </ | ||
| - | 5. Draw the magnitude of the input impedance $Z$ as a function of the frequency $\omega$. | + | 5. Draw the magnitude of the input impedance $Z$ as a function of the frequency $\omega$. |
| <WRAP group> | <WRAP group> | ||
| <WRAP half column rightalign> | <WRAP half column rightalign> | ||
| Line 1108: | Line 1127: | ||
| f_5=250~{\rm Hz} | f_5=250~{\rm Hz} | ||
| \end{align*} | \end{align*} | ||
| + | |||
| + | {{drawio> | ||
| + | |||
| # | # | ||
| </ | </ | ||