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dummy [2026/05/18 02:56] mexleadmindummy [2026/05/26 13:48] (current) – removed mexleadmin
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-===== Exercises ===== 
  
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Quick check: ideal transformer voltage and current ratio 
-#@TaskText_HTML@# 
- 
-A transformer has $N_1=1200$ turns and $N_2=300$ turns.   
-The primary RMS voltage is $U_1=230~{\rm V}$.   
-The secondary side supplies a load current $I_2=2.0~{\rm A}$. 
- 
-1. Calculate the turns ratio $n$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2001~@# 
-<WRAP leftalign> 
-The turns ratio of an ideal transformer is defined as: 
-\begin{align*} 
-n=\frac{N_1}{N_2} 
-\end{align*} 
- 
-Insert the given values: 
-\begin{align*} 
-n 
-&= 
-\frac{1200}{300} 
-\\ 
-&= 
-4 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2001~@# 
-\begin{align*} 
-n=4 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate the ideal secondary voltage $U_2$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2002~@# 
-<WRAP leftalign> 
-For an ideal transformer, the voltage ratio follows the turns ratio: 
-\begin{align*} 
-n=\frac{U_1}{U_2} 
-\end{align*} 
- 
-Therefore: 
-\begin{align*} 
-U_2 
-&= 
-\frac{U_1}{n} 
-\\ 
-&= 
-\frac{230~{\rm V}}{4} 
-\\ 
-&= 
-57.5~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2002~@# 
-\begin{align*} 
-U_2=57.5~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate the magnitude of the ideal primary current $I_1$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2003~@# 
-<WRAP leftalign> 
-For the ideal transformer, the current ratio is inverse to the voltage ratio: 
-\begin{align*} 
-I_1=\frac{I_2}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_1 
-&= 
-\frac{2.0~{\rm A}}{4} 
-\\ 
-&= 
-0.50~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2003~@# 
-\begin{align*} 
-I_1=0.50~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. State whether this is a step-up or step-down transformer. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2004~@# 
-<WRAP leftalign> 
-Compare the primary and secondary voltages: 
-\begin{align*} 
-U_1 &= 230~{\rm V} 
-\\ 
-U_2 &= 57.5~{\rm V} 
-\end{align*} 
- 
-Since 
-\begin{align*} 
-U_2<U_1 
-\end{align*} 
- 
-the transformer reduces the voltage. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2004~@# 
-The transformer is a step-down transformer. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Quick check: mutual inductance from reluctance 
-#@TaskText_HTML@# 
- 
-Two coils are wound on the same ideal magnetic core.   
-The main magnetic reluctance is 
- 
-\begin{align*} 
-R_{\rm mH}=2.0\cdot 10^6~\frac{1}{\rm H}. 
-\end{align*} 
- 
-The number of turns is $N_1=500$ and $N_2=100$. 
- 
-1. Calculate $L_{1{\rm H}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2005~@# 
-<WRAP leftalign> 
-The main-flux inductance of coil 1 is: 
-\begin{align*} 
-L_{1{\rm H}} 
-= 
-\frac{N_1^2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-L_{1{\rm H}} 
-&= 
-\frac{500^2}{2.0\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.125~{\rm H} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2005~@# 
-\begin{align*} 
-L_{1{\rm H}}=0.125~{\rm H} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate $L_{2{\rm H}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2006~@# 
-<WRAP leftalign> 
-The main-flux inductance of coil 2 is: 
-\begin{align*} 
-L_{2{\rm H}} 
-= 
-\frac{N_2^2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-L_{2{\rm H}} 
-&= 
-\frac{100^2}{2.0\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.0050~{\rm H} 
-\\ 
-&= 
-5.0~{\rm mH} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2006~@# 
-\begin{align*} 
-L_{2{\rm H}} 
-= 
-0.0050~{\rm H} 
-= 
-5.0~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate $M$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2007~@# 
-<WRAP leftalign> 
-The mutual inductance is: 
-\begin{align*} 
-M 
-= 
-\frac{N_1N_2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-M 
-&= 
-\frac{500\cdot 100}{2.0\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.025~{\rm H} 
-\\ 
-&= 
-25~{\rm mH} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2007~@# 
-\begin{align*} 
-M 
-= 
-0.025~{\rm H} 
-= 
-25~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Check whether the units are correct. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2008~@# 
-<WRAP leftalign> 
-The reluctance is given in: 
-\begin{align*} 
-[R_{\rm mH}]=\frac{1}{\rm H} 
-\end{align*} 
- 
-The number of turns is dimensionless. Therefore: 
-\begin{align*} 
-\left[ 
-\frac{N^2}{R_{\rm mH}} 
-\right] 
-= 
-\frac{1}{1/{\rm H}} 
-= 
-{\rm H} 
-\end{align*} 
- 
-The same argument applies to the mutual inductance: 
-\begin{align*} 
-\left[ 
-\frac{N_1N_2}{R_{\rm mH}} 
-\right] 
-= 
-{\rm H} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2008~@# 
-The unit is correct because 
-\begin{align*} 
-\frac{1}{1/{\rm H}}={\rm H} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Mutual inductance and leakage from a magnetic path 
-#@TaskText_HTML@# 
- 
-Two coils are wound on the same magnetic core. The shared main magnetic path has the reluctance 
- 
-\begin{align*} 
-R_{\rm mH}=1.6\cdot 10^6~\frac{1}{\rm H}. 
-\end{align*} 
- 
-The numbers of turns are 
- 
-\begin{align*} 
-N_1=400, 
-\qquad 
-N_2=100. 
-\end{align*} 
- 
-The leakage inductances are 
- 
-\begin{align*} 
-L_{1\sigma}=4.0~{\rm mH}, 
-\qquad 
-L_{2\sigma}=0.30~{\rm mH}. 
-\end{align*} 
- 
-Calculate: 
- 
-  * $L_{1{\rm H}}$ 
-  * $L_{2{\rm H}}$ 
-  * $M$ 
-  * the total self-inductances $L_1$ and $L_2$ 
-  * the coupling coefficient $k=\frac{M}{\sqrt{L_1L_2}}$ 
- 
-1. Calculate $L_{1{\rm H}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2009~@# 
-<WRAP leftalign> 
-The main-flux self-inductance of coil 1 is: 
-\begin{align*} 
-L_{1{\rm H}} 
-= 
-\frac{N_1^2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-L_{1{\rm H}} 
-&= 
-\frac{400^2}{1.6\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.100~{\rm H} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2009~@# 
-\begin{align*} 
-L_{1{\rm H}}=0.100~{\rm H}=100~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate $L_{2{\rm H}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2010~@# 
-<WRAP leftalign> 
-The main-flux self-inductance of coil 2 is: 
-\begin{align*} 
-L_{2{\rm H}} 
-= 
-\frac{N_2^2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-L_{2{\rm H}} 
-&= 
-\frac{100^2}{1.6\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.00625~{\rm H} 
-\\ 
-&= 
-6.25~{\rm mH} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2010~@# 
-\begin{align*} 
-L_{2{\rm H}} 
-= 
-0.00625~{\rm H} 
-= 
-6.25~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate $M$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2011~@# 
-<WRAP leftalign> 
-The mutual inductance is: 
-\begin{align*} 
-M 
-= 
-\frac{N_1N_2}{R_{\rm mH}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-M 
-&= 
-\frac{400\cdot 100}{1.6\cdot 10^6~1/{\rm H}} 
-\\ 
-&= 
-0.025~{\rm H} 
-\\ 
-&= 
-25~{\rm mH} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2011~@# 
-\begin{align*} 
-M 
-= 
-0.025~{\rm H} 
-= 
-25~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Calculate the total self-inductances $L_1$ and $L_2$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2012~@# 
-<WRAP leftalign> 
-The total self-inductance is the sum of main-flux inductance and leakage inductance. 
- 
-For coil 1: 
-\begin{align*} 
-L_1 
-&= 
-L_{1{\rm H}}+L_{1\sigma} 
-\\ 
-&= 
-100~{\rm mH}+4.0~{\rm mH} 
-\\ 
-&= 
-104~{\rm mH} 
-\end{align*} 
- 
-For coil 2: 
-\begin{align*} 
-L_2 
-&= 
-L_{2{\rm H}}+L_{2\sigma} 
-\\ 
-&= 
-6.25~{\rm mH}+0.30~{\rm mH} 
-\\ 
-&= 
-6.55~{\rm mH} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2012~@# 
-\begin{align*} 
-L_1 &= 104~{\rm mH} 
-\\ 
-L_2 &= 6.55~{\rm mH} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-5. Calculate the coupling coefficient $k=\frac{M}{\sqrt{L_1L_2}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2013~@# 
-<WRAP leftalign> 
-The coupling coefficient is: 
-\begin{align*} 
-k 
-= 
-\frac{M}{\sqrt{L_1L_2}} 
-\end{align*} 
- 
-Insert the values in henry: 
-\begin{align*} 
-k 
-&= 
-\frac{0.025~{\rm H}}{\sqrt{0.104~{\rm H}\cdot 0.00655~{\rm H}}} 
-\\ 
-&\approx 
-0.96 
-\end{align*} 
- 
-The coupling is strong, but not ideal, because leakage inductances are present. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2013~@# 
-\begin{align*} 
-k\approx 0.96 
-\end{align*} 
- 
-The coupling is strong, but not ideal. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Quick check: referring secondary quantities to the primary side 
-#@TaskText_HTML@# 
- 
-A transformer has $n=5$.   
-The secondary winding resistance is $R_2=0.20~\Omega$ and the secondary leakage reactance is $X_{2\sigma}=0.35~\Omega$. 
- 
-Calculate the values $R'_2$ and $X'_{2\sigma}$ referred to the primary side. 
- 
-1. Calculate $R'_2$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2014~@# 
-<WRAP leftalign> 
-When a resistance is referred from the secondary side to the primary side, it is multiplied by $n^2$: 
-\begin{align*} 
-R'_2 
-= 
-n^2R_2 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-R'_2 
-&= 
-5^2\cdot 0.20~\Omega 
-\\ 
-&= 
-25\cdot 0.20~\Omega 
-\\ 
-&= 
-5.0~\Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2014~@# 
-\begin{align*} 
-R'_2=5.0~\Omega 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate $X'_{2\sigma}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2015~@# 
-<WRAP leftalign> 
-The secondary leakage reactance is also referred to the primary side by multiplying with $n^2$: 
-\begin{align*} 
-X'_{2\sigma} 
-= 
-n^2X_{2\sigma} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-X'_{2\sigma} 
-&= 
-5^2\cdot 0.35~\Omega 
-\\ 
-&= 
-25\cdot 0.35~\Omega 
-\\ 
-&= 
-8.75~\Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2015~@# 
-\begin{align*} 
-X'_{2\sigma}=8.75~\Omega 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Check the unit. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2016~@# 
-<WRAP leftalign> 
-The turns ratio $n$ is dimensionless: 
-\begin{align*} 
-[n]=1 
-\end{align*} 
- 
-Therefore, multiplying by $n^2$ does not change the unit: 
-\begin{align*} 
-[R'_2] &= \Omega 
-\\ 
-[X'_{2\sigma}] &= \Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2016~@# 
-The unit remains $\Omega$, because $n$ is dimensionless. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Quick check: short-circuit voltage and fault current 
-#@TaskText_HTML@# 
- 
-A transformer has a rated primary current $I_{1{\rm N}}=10~{\rm A}$ and a short-circuit voltage $u_{\rm k}=5~\%$. 
- 
-1. Calculate the continuous short-circuit current $I_{1{\rm k}}$ when rated primary voltage is applied. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2017~@# 
-<WRAP leftalign> 
-The short-circuit current can be estimated from the rated current and the relative short-circuit voltage: 
-\begin{align*} 
-I_{1{\rm k}} 
-= 
-I_{1{\rm N}}\cdot \frac{100~\%}{u_{\rm k}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_{1{\rm k}} 
-&= 
-10~{\rm A}\cdot \frac{100~\%}{5~\%} 
-\\ 
-&= 
-200~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2017~@# 
-\begin{align*} 
-I_{1{\rm k}}=200~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Estimate the initial peak short-circuit current $i_{\rm p}$ using $i_{\rm p}\approx 2.54 I_{1{\rm k}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2018~@# 
-<WRAP leftalign> 
-The initial peak current is estimated by: 
-\begin{align*} 
-i_{\rm p} 
-\approx 
-2.54\cdot I_{1{\rm k}} 
-\end{align*} 
- 
-Insert the continuous short-circuit current: 
-\begin{align*} 
-i_{\rm p} 
-&\approx 
-2.54\cdot 200~{\rm A} 
-\\ 
-&= 
-508~{\rm A} 
-\end{align*} 
- 
-The short-circuit current is much larger than the rated current. Protection devices must be selected accordingly. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2018~@# 
-\begin{align*} 
-i_{\rm p}\approx 508~{\rm A} 
-\end{align*} 
- 
-Protection devices must be selected accordingly. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Longer exercise: transformer equivalent circuit for an actuator supply 
-#@TaskText_HTML@# 
- 
-A single-phase transformer supplies an actuator driver.   
-Rated data and equivalent circuit data are: 
- 
-\begin{align*} 
-U_{1{\rm N}}&=230~{\rm V}, 
-& 
-U_{2{\rm N}}&=23~{\rm V}, 
-& 
-I_{2{\rm N}}&=5.0~{\rm A}, 
-\\ 
-R_1&=1.2~\Omega, 
-& 
-X_{1\sigma}&=1.8~\Omega, 
-\\ 
-R_2&=0.012~\Omega, 
-& 
-X_{2\sigma}&=0.018~\Omega. 
-\end{align*} 
- 
-Assume $n=\frac{U_{1{\rm N}}}{U_{2{\rm N}}}$. The magnetizing branch is neglected for the loaded operating point. 
- 
-1. Calculate $n$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2019~@# 
-<WRAP leftalign> 
-The turns ratio is estimated from the rated voltages: 
-\begin{align*} 
-n 
-= 
-\frac{U_{1{\rm N}}}{U_{2{\rm N}}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-n 
-&= 
-\frac{230~{\rm V}}{23~{\rm V}} 
-\\ 
-&= 
-10 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2019~@# 
-\begin{align*} 
-n=10 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Refer $R_2$ and $X_{2\sigma}$ to the primary side. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2020~@# 
-<WRAP leftalign> 
-Secondary quantities are referred to the primary side by multiplying them with $n^2$: 
-\begin{align*} 
-R'_2 &= n^2R_2 
-\\ 
-X'_{2\sigma} &= n^2X_{2\sigma} 
-\end{align*} 
- 
-With $n=10$: 
-\begin{align*} 
-R'_2 
-&= 
-10^2\cdot 0.012~\Omega 
-\\ 
-&= 
-1.2~\Omega 
-\\[4pt] 
-X'_{2\sigma} 
-&= 
-10^2\cdot 0.018~\Omega 
-\\ 
-&= 
-1.8~\Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2020~@# 
-\begin{align*} 
-R'_2 &= 1.2~\Omega 
-\\ 
-X'_{2\sigma} &= 1.8~\Omega 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate $R_{\rm k}$ and $X_{\rm k}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2021~@# 
-<WRAP leftalign> 
-The short-circuit equivalent values are the sums of the primary quantities and the referred secondary quantities: 
-\begin{align*} 
-R_{\rm k} 
-&= 
-R_1+R'_2 
-\\ 
-X_{\rm k} 
-&= 
-X_{1\sigma}+X'_{2\sigma} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-R_{\rm k} 
-&= 
-1.2~\Omega+1.2~\Omega 
-\\ 
-&= 
-2.4~\Omega 
-\\[4pt] 
-X_{\rm k} 
-&= 
-1.8~\Omega+1.8~\Omega 
-\\ 
-&= 
-3.6~\Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2021~@# 
-\begin{align*} 
-R_{\rm k} &= 2.4~\Omega 
-\\ 
-X_{\rm k} &= 3.6~\Omega 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Calculate the primary rated current magnitude $I_{1{\rm N}}$ using the ideal current ratio. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2022~@# 
-<WRAP leftalign> 
-For an ideal transformer, the primary current magnitude is: 
-\begin{align*} 
-I_{1{\rm N}} 
-= 
-\frac{I_{2{\rm N}}}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_{1{\rm N}} 
-&= 
-\frac{5.0~{\rm A}}{10} 
-\\ 
-&= 
-0.50~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2022~@# 
-\begin{align*} 
-I_{1{\rm N}}=0.50~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-5. Estimate the magnitude of the internal voltage drop $U_{\rm k}\approx |\underline{Z}_{\rm k}|I_{1{\rm N}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2023~@# 
-<WRAP leftalign> 
-First calculate the magnitude of the short-circuit impedance: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-= 
-\sqrt{R_{\rm k}^2+X_{\rm k}^2} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-&= 
-\sqrt{(2.4~\Omega)^2+(3.6~\Omega)^2} 
-\\ 
-&= 
-4.33~\Omega 
-\end{align*} 
- 
-Now calculate the internal voltage drop: 
-\begin{align*} 
-U_{\rm k} 
-&\approx 
-|\underline{Z}_{\rm k}|I_{1{\rm N}} 
-\\ 
-&= 
-4.33~\Omega\cdot 0.50~{\rm A} 
-\\ 
-&= 
-2.17~{\rm V} 
-\end{align*} 
- 
-This is a primary-side voltage drop. On the secondary side: 
-\begin{align*} 
-\frac{2.17~{\rm V}}{10} 
-= 
-0.217~{\rm V} 
-\end{align*} 
- 
-For a $23~{\rm V}$ actuator supply this is small but not zero. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2023~@# 
-\begin{align*} 
-|\underline{Z}_{\rm k}| &= 4.33~\Omega 
-\\ 
-U_{\rm k} &\approx 2.17~{\rm V} 
-\end{align*} 
- 
-Secondary-side equivalent: 
-\begin{align*} 
-U_{\rm k,2}\approx 0.217~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Short-circuit voltage from the transformer impedance 
-#@TaskText_HTML@# 
- 
-A transformer has the rated primary data 
- 
-\begin{align*} 
-U_{1{\rm N}}=230~{\rm V}, 
-\qquad 
-I_{1{\rm N}}=2.0~{\rm A}. 
-\end{align*} 
- 
-The short-circuit equivalent impedance referred to the primary side is 
- 
-\begin{align*} 
-R_{\rm k}=1.5~\Omega, 
-\qquad 
-X_{\rm k}=4.0~\Omega. 
-\end{align*} 
- 
-Calculate: 
- 
-  * $|\underline{Z}_{\rm k}|$ 
-  * the rated short-circuit voltage $U_{1{\rm k}}$ 
-  * the relative short-circuit voltage $u_{\rm k}$ 
-  * the prospective continuous short-circuit current $I_{1{\rm k}}$ for rated primary voltage 
-  * the approximate first peak current $i_{\rm peak}\approx 2.54 I_{1{\rm k}}$ 
- 
-1. Calculate $|\underline{Z}_{\rm k}|$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2024~@# 
-<WRAP leftalign> 
-The short-circuit impedance magnitude is: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-= 
-\sqrt{R_{\rm k}^2+X_{\rm k}^2} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-&= 
-\sqrt{(1.5~\Omega)^2+(4.0~\Omega)^2} 
-\\ 
-&= 
-4.27~\Omega 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2024~@# 
-\begin{align*} 
-|\underline{Z}_{\rm k}|=4.27~\Omega 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate the rated short-circuit voltage $U_{1{\rm k}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2025~@# 
-<WRAP leftalign> 
-The primary voltage required to drive rated current through the short-circuited transformer is: 
-\begin{align*} 
-U_{1{\rm k}} 
-= 
-|\underline{Z}_{\rm k}|I_{1{\rm N}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-U_{1{\rm k}} 
-&= 
-4.27~\Omega\cdot 2.0~{\rm A} 
-\\ 
-&= 
-8.54~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2025~@# 
-\begin{align*} 
-U_{1{\rm k}}=8.54~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate the relative short-circuit voltage $u_{\rm k}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2026~@# 
-<WRAP leftalign> 
-The relative short-circuit voltage is: 
-\begin{align*} 
-u_{\rm k} 
-= 
-\frac{U_{1{\rm k}}}{U_{1{\rm N}}}\cdot 100~\% 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-u_{\rm k} 
-&= 
-\frac{8.54~{\rm V}}{230~{\rm V}}\cdot 100~\% 
-\\ 
-&= 
-3.71~\% 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2026~@# 
-\begin{align*} 
-u_{\rm k}=3.71~\% 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Calculate the prospective continuous short-circuit current $I_{1{\rm k}}$ for rated primary voltage. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2027~@# 
-<WRAP leftalign> 
-The prospective continuous short-circuit current is: 
-\begin{align*} 
-I_{1{\rm k}} 
-= 
-I_{1{\rm N}}\cdot \frac{100~\%}{u_{\rm k}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_{1{\rm k}} 
-&= 
-2.0~{\rm A}\cdot \frac{100}{3.71} 
-\\ 
-&= 
-53.9~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2027~@# 
-\begin{align*} 
-I_{1{\rm k}}=53.9~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-5. Calculate the approximate first peak current $i_{\rm peak}\approx 2.54 I_{1{\rm k}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2028~@# 
-<WRAP leftalign> 
-The approximate first peak current is: 
-\begin{align*} 
-i_{\rm peak} 
-\approx 
-2.54 I_{1{\rm k}} 
-\end{align*} 
- 
-Insert the short-circuit current: 
-\begin{align*} 
-i_{\rm peak} 
-&\approx 
-2.54\cdot 53.9~{\rm A} 
-\\ 
-&= 
-137~{\rm A} 
-\end{align*} 
- 
-Even though the rated current is only $2.0~{\rm A}$, a short-circuit fault could lead to a much larger current until protection reacts. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2028~@# 
-\begin{align*} 
-i_{\rm peak}\approx 137~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Voltage drop under load using the Kapp approximation 
-#@TaskText_HTML@# 
- 
-A transformer has the turns ratio 
- 
-\begin{align*} 
-n=10. 
-\end{align*} 
- 
-The short-circuit equivalent parameters referred to the primary side are 
- 
-\begin{align*} 
-R_{\rm k}=2.4~\Omega, 
-\qquad 
-X_{\rm k}=3.6~\Omega. 
-\end{align*} 
- 
-The secondary load current is 
- 
-\begin{align*} 
-I_2=4.0~{\rm A}. 
-\end{align*} 
- 
-The load has the power factor 
- 
-\begin{align*} 
-\cos\varphi=0.8 
-\end{align*} 
- 
-and is inductive. 
- 
-Estimate the voltage drop on the secondary side using 
- 
-\begin{align*} 
-\Delta U_1 
-\approx 
-I_1\left(R_{\rm k}\cos\varphi+X_{\rm k}\sin\varphi\right) 
-\end{align*} 
- 
-and 
- 
-\begin{align*} 
-\Delta U_2\approx \frac{\Delta U_1}{n}. 
-\end{align*} 
- 
-1. Calculate the primary current magnitude $I_1$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2029~@# 
-<WRAP leftalign> 
-The primary current magnitude is approximately: 
-\begin{align*} 
-I_1 
-= 
-\frac{I_2}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_1 
-&= 
-\frac{4.0~{\rm A}}{10} 
-\\ 
-&= 
-0.40~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2029~@# 
-\begin{align*} 
-I_1=0.40~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Determine $\sin\varphi$ for the inductive load. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2030~@# 
-<WRAP leftalign> 
-For an inductive load with $\cos\varphi=0.8$: 
-\begin{align*} 
-\sin\varphi 
-= 
-\sqrt{1-\cos^2\varphi} 
-\end{align*} 
- 
-Insert the value: 
-\begin{align*} 
-\sin\varphi 
-&= 
-\sqrt{1-0.8^2} 
-\\ 
-&= 
-0.6 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2030~@# 
-\begin{align*} 
-\sin\varphi=0.6 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Estimate the primary-side voltage drop $\Delta U_1$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2031~@# 
-<WRAP leftalign> 
-Use the Kapp approximation: 
-\begin{align*} 
-\Delta U_1 
-&\approx 
-I_1\left(R_{\rm k}\cos\varphi+X_{\rm k}\sin\varphi\right) 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-\Delta U_1 
-&\approx 
-0.40~{\rm A} 
-\left( 
-2.4~\Omega\cdot 0.8 
-+ 
-3.6~\Omega\cdot 0.6 
-\right) 
-\\ 
-&= 
-0.40~{\rm A} 
-\left( 
-1.92~\Omega+2.16~\Omega 
-\right) 
-\\ 
-&= 
-1.63~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2031~@# 
-\begin{align*} 
-\Delta U_1\approx 1.63~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Estimate the secondary-side voltage drop $\Delta U_2$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2032~@# 
-<WRAP leftalign> 
-The secondary-side voltage drop is: 
-\begin{align*} 
-\Delta U_2 
-\approx 
-\frac{\Delta U_1}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-\Delta U_2 
-&\approx 
-\frac{1.63~{\rm V}}{10} 
-\\ 
-&= 
-0.163~{\rm V} 
-\end{align*} 
- 
-The secondary voltage decreases by approximately $0.16~{\rm V}$ for this operating point. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2032~@# 
-\begin{align*} 
-\Delta U_2\approx 0.163~{\rm V} 
-\end{align*} 
- 
-The secondary voltage decreases by approximately $0.16~{\rm V}$. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Why the magnetizing branch can be neglected in the short-circuit test 
-#@TaskText_HTML@# 
- 
-A transformer has the rated primary voltage 
- 
-\begin{align*} 
-U_{1{\rm N}}=230~{\rm V}. 
-\end{align*} 
- 
-Its rated primary current is 
- 
-\begin{align*} 
-I_{1{\rm N}}=3.0~{\rm A}. 
-\end{align*} 
- 
-At rated voltage and no-load operation, the magnetizing current is approximately 
- 
-\begin{align*} 
-I_{\rm m,N}=0.12~{\rm A}. 
-\end{align*} 
- 
-The short-circuit voltage is 
- 
-\begin{align*} 
-u_{\rm k}=6.0~\%. 
-\end{align*} 
- 
-Assume that the magnetizing current is approximately proportional to the applied voltage. 
- 
-1. Calculate the short-circuit test voltage $U_{1{\rm k}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2033~@# 
-<WRAP leftalign> 
-The short-circuit test voltage is: 
-\begin{align*} 
-U_{1{\rm k}} 
-= 
-\frac{u_{\rm k}}{100~\%}\cdot U_{1{\rm N}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-U_{1{\rm k}} 
-&= 
-0.06\cdot 230~{\rm V} 
-\\ 
-&= 
-13.8~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2033~@# 
-\begin{align*} 
-U_{1{\rm k}}=13.8~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Estimate the magnetizing current $I_{\rm m,k}$ during the short-circuit test. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2034~@# 
-<WRAP leftalign> 
-The magnetizing current is assumed to be proportional to the voltage: 
-\begin{align*} 
-I_{\rm m,k} 
-= 
-I_{\rm m,N}\cdot \frac{U_{1{\rm k}}}{U_{1{\rm N}}} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I_{\rm m,k} 
-&= 
-0.12~{\rm A}\cdot \frac{13.8~{\rm V}}{230~{\rm V}} 
-\\ 
-&= 
-0.0072~{\rm A} 
-\\ 
-&= 
-7.2~{\rm mA} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2034~@# 
-\begin{align*} 
-I_{\rm m,k} 
-= 
-0.0072~{\rm A} 
-= 
-7.2~{\rm mA} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Compare $I_{\rm m,k}$ with $I_{1{\rm N}}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2035~@# 
-<WRAP leftalign> 
-Compare the short-circuit magnetizing current with the rated current: 
-\begin{align*} 
-\frac{I_{\rm m,k}}{I_{1{\rm N}}} 
-= 
-\frac{0.0072~{\rm A}}{3.0~{\rm A}} 
-\end{align*} 
- 
-Calculate the ratio: 
-\begin{align*} 
-\frac{I_{\rm m,k}}{I_{1{\rm N}}} 
-&= 
-0.0024 
-\\ 
-&= 
-0.24~\% 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2035~@# 
-\begin{align*} 
-\frac{I_{\rm m,k}}{I_{1{\rm N}}} 
-= 
-0.24~\% 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Explain why the magnetizing branch can be neglected. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2036~@# 
-<WRAP leftalign> 
-During the short-circuit test, the applied voltage is much smaller than the rated voltage: 
-\begin{align*} 
-U_{1{\rm k}} \ll U_{1{\rm N}} 
-\end{align*} 
- 
-Since the magnetizing current is assumed to be approximately proportional to the applied voltage, the magnetizing current is also very small: 
-\begin{align*} 
-I_{\rm m,k}=7.2~{\rm mA} 
-\end{align*} 
- 
-Compared with the rated current: 
-\begin{align*} 
-I_{1{\rm N}}=3.0~{\rm A} 
-\end{align*} 
- 
-the magnetizing current is only $0.24~\%$. 
- 
-So during the short-circuit test, almost all current flows through the short-circuit path consisting of $R_{\rm k}$ and $X_{\rm k}$. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2036~@# 
-The magnetizing branch $R_{\rm Fe}\parallel jX_{1{\rm H}}$ can usually be neglected in the short-circuit test. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Why the short-circuit equivalent circuit is often sufficient under load 
-#@TaskText_HTML@# 
- 
-A transformer has the turns ratio $n=10$. The short-circuit equivalent parameters referred to the primary side are $R_{\rm k}=2.0~\Omega$, $X_{\rm k}=4.0~\Omega$. 
- 
-The secondary load current is $I_2=5.0~{\rm A}$. The load is ohmic-inductive with $\cos\varphi=0.8$. 
- 
-The no-load current on the primary side is approximately $I_{10}=0.03~{\rm A}$. 
-\\ \\  
-1. Calculate the load-related primary current $I'_2$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2037~@# 
-<WRAP leftalign> 
-The load-related primary current is: 
-\begin{align*} 
-I'_2 
-= 
-\frac{I_2}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I'_2 
-&= 
-\frac{5.0~{\rm A}}{10} 
-\\ 
-&= 
-0.50~{\rm A} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2037~@# 
-\begin{align*} 
-I'_2=0.50~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Estimate the primary-side voltage drop. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2038~@# 
-<WRAP leftalign> 
-The voltage drop is estimated with: 
-\begin{align*} 
-\Delta U_1 
-\approx 
-I'_2 
-\left( 
-R_{\rm k}\cos\varphi 
-+ 
-X_{\rm k}\sin\varphi 
-\right) 
-\end{align*} 
- 
-For $\cos\varphi=0.8$: 
-\begin{align*} 
-\sin\varphi 
-&= 
-\sqrt{1-\cos^2\varphi} 
-\\ 
-&= 
-\sqrt{1-0.8^2} 
-\\ 
-&= 
-0.6 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-\Delta U_1 
-&\approx 
-0.50~{\rm A} 
-\left( 
-2.0~\Omega\cdot 0.8 
-+ 
-4.0~\Omega\cdot 0.6 
-\right) 
-\\ 
-&= 
-0.50~{\rm A} 
-\left( 
-1.6~\Omega+2.4~\Omega 
-\right) 
-\\ 
-&= 
-2.0~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2038~@# 
-\begin{align*} 
-\Delta U_1\approx 2.0~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Calculate the secondary-side voltage drop $\Delta U_2\approx \frac{\Delta U_1}{n}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2039~@# 
-<WRAP leftalign> 
-The secondary-side voltage drop is: 
-\begin{align*} 
-\Delta U_2 
-\approx 
-\frac{\Delta U_1}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-\Delta U_2 
-&\approx 
-\frac{2.0~{\rm V}}{10} 
-\\ 
-&= 
-0.20~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2039~@# 
-\begin{align*} 
-\Delta U_2\approx 0.20~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Estimate an upper bound for the neglected voltage drop caused by $I_{10}$. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2040~@# 
-<WRAP leftalign> 
-First calculate the magnitude of the short-circuit impedance: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-= 
-\sqrt{R_{\rm k}^2+X_{\rm k}^2} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-|\underline{Z}_{\rm k}| 
-&= 
-\sqrt{(2.0~\Omega)^2+(4.0~\Omega)^2} 
-\\ 
-&= 
-4.47~\Omega 
-\end{align*} 
- 
-The upper bound for the voltage drop caused by the no-load current is: 
-\begin{align*} 
-\Delta U_{1,10} 
-&\leq 
-|\underline{Z}_{\rm k}|I_{10} 
-\\ 
-&= 
-4.47~\Omega\cdot 0.03~{\rm A} 
-\\ 
-&= 
-0.134~{\rm V} 
-\end{align*} 
- 
-On the secondary side: 
-\begin{align*} 
-\Delta U_{2,10} 
-&\leq 
-\frac{0.134~{\rm V}}{10} 
-\\ 
-&= 
-0.0134~{\rm V} 
-\end{align*} 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2040~@# 
-\begin{align*} 
-|\underline{Z}_{\rm k}| &= 4.47~\Omega 
-\\ 
-\Delta U_{1,10} &\leq 0.134~{\rm V} 
-\\ 
-\Delta U_{2,10} &\leq 0.0134~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-5. Decide whether the short-circuit equivalent circuit is sufficient for this load estimate. 
-<WRAP group> 
-<WRAP half column rightalign> 
-#@PathBegin_HTML~2041~@# 
-<WRAP leftalign> 
-The load-related secondary-side voltage drop is: 
-\begin{align*} 
-\Delta U_2\approx 0.20~{\rm V} 
-\end{align*} 
- 
-The estimated neglected secondary-side voltage drop caused by the no-load current is at most: 
-\begin{align*} 
-\Delta U_{2,10}\leq 0.0134~{\rm V} 
-\end{align*} 
- 
-This is small compared with the load-related drop of $0.20~{\rm V}$. 
-</WRAP> 
-#@PathEnd_HTML@# 
-</WRAP> 
-<WRAP half column> 
-#@ResultBegin_HTML~2041~@# 
-For this engineering estimate, the short-circuit equivalent circuit is sufficient. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-#@TaskEnd_HTML@# 
- 
- 
-#@TaskTitle_HTML@##@Lvl_HTML@#~~#@ee2_taskctr#~~  Ideal transformer versus real transformer 
-#@TaskText_HTML@# 
- 
-A transformer has the rated primary voltage of $U_1=230~{\rm V}$ and and the turns ratio $n=10$. A resistive load draws $I_2=4.0~{\rm A}$. \\ 
-For the real transformer, the short-circuit equivalent parameters referred to the primary side are $R_{\rm k}=2.4~\Omega$, $X_{\rm k}=3.2~\Omega$. \\ 
-The iron loss is approximately $P_{\rm Fe}=1.5~{\rm W}$. \\ 
-Assume a resistive load with $\cos\varphi=1$. 
-\\ \\  
-1. Calculate the ideal secondary voltage $U_{2,\rm ideal}$. 
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-For the ideal transformer: 
-\begin{align*} 
-U_{2,\rm ideal} 
-= 
-\frac{U_1}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-U_{2,\rm ideal} 
-&= 
-\frac{230~{\rm V}}{10} 
-\\ 
-&= 
-23.0~{\rm V} 
-\end{align*} 
-</WRAP> 
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-</WRAP> 
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-\begin{align*} 
-U_{2,\rm ideal}=23.0~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-2. Calculate the load-related primary current $I'_2$. 
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-The load-related primary current is: 
-\begin{align*} 
-I'_2 
-= 
-\frac{I_2}{n} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-I'_2 
-&= 
-\frac{4.0~{\rm A}}{10} 
-\\ 
-&= 
-0.40~{\rm A} 
-\end{align*} 
-</WRAP> 
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-</WRAP> 
-<WRAP half column> 
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-\begin{align*} 
-I'_2=0.40~{\rm A} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-3. Estimate the real secondary voltage. 
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-For a resistive load, the approximate primary-side voltage drop is: 
-\begin{align*} 
-\Delta U_1 
-\approx 
-I'_2R_{\rm k} 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-\Delta U_1 
-&\approx 
-0.40~{\rm A}\cdot 2.4~\Omega 
-\\ 
-&= 
-0.96~{\rm V} 
-\end{align*} 
- 
-The corresponding secondary-side voltage drop is: 
-\begin{align*} 
-\Delta U_2 
-&\approx 
-\frac{\Delta U_1}{n} 
-\\ 
-&= 
-\frac{0.96~{\rm V}}{10} 
-\\ 
-&= 
-0.096~{\rm V} 
-\end{align*} 
- 
-Thus the real secondary voltage is approximately: 
-\begin{align*} 
-U_{2,\rm real} 
-&\approx 
-23.0~{\rm V}-0.096~{\rm V} 
-\\ 
-&= 
-22.90~{\rm V} 
-\end{align*} 
-</WRAP> 
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-</WRAP> 
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-\begin{align*} 
-\Delta U_1 &\approx 0.96~{\rm V} 
-\\ 
-\Delta U_2 &\approx 0.096~{\rm V} 
-\\ 
-U_{2,\rm real} &\approx 22.90~{\rm V} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-4. Estimate the copper losses. 
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-The copper losses are: 
-\begin{align*} 
-P_{\rm Cu} 
-\approx 
-R_{\rm k}(I'_2)^2 
-\end{align*} 
- 
-Insert the values: 
-\begin{align*} 
-P_{\rm Cu} 
-&\approx 
-2.4~\Omega\cdot (0.40~{\rm A})^2 
-\\ 
-&= 
-0.384~{\rm W} 
-\end{align*} 
- 
-The real transformer also has iron losses: 
-\begin{align*} 
-P_{\rm Fe}=1.5~{\rm W} 
-\end{align*} 
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-</WRAP> 
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-\begin{align*} 
-P_{\rm Cu}\approx 0.384~{\rm W} 
-\end{align*} 
- 
-Additionally: 
-\begin{align*} 
-P_{\rm Fe}=1.5~{\rm W} 
-\end{align*} 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
-5. Compare ideal and real transformer behavior. 
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-<WRAP leftalign> 
-For the ideal transformer: 
-\begin{align*} 
-U_{2,\rm ideal}=23.0~{\rm V} 
-\end{align*} 
- 
-For the real transformer: 
-\begin{align*} 
-U_{2,\rm real}\approx 22.90~{\rm V} 
-\end{align*} 
- 
-The real transformer has copper losses and iron losses: 
-\begin{align*} 
-P_{\rm Cu}&\approx 0.384~{\rm W} 
-\\ 
-P_{\rm Fe}&=1.5~{\rm W} 
-\end{align*} 
- 
-So the main differences are: 
- 
-  * the ideal transformer has exactly $U_2=23.0~{\rm V}$, the real transformer has a slightly lower voltage, 
-  * the ideal transformer has no losses, the real transformer has copper and iron losses, 
-  * the ideal transformer has no leakage voltage drop, the real transformer has a load-dependent voltage drop. 
- 
-For this operating point the transformer is close to ideal, but not exactly ideal. 
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-</WRAP> 
-<WRAP half column> 
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-The real transformer differs from the ideal transformer by: 
- 
-  * a slightly lower secondary voltage, 
-  * copper and iron losses, 
-  * a load-dependent voltage drop. 
- 
-For this operating point it is close to ideal, but not exactly ideal. 
-#@ResultEnd_HTML@# 
-</WRAP> 
-</WRAP> 
- 
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