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electrical_engineering_2:polyphase_networks [2024/06/18 02:38] – [Excercises] mexleadmin | electrical_engineering_2:polyphase_networks [2025/06/24 00:40] (aktuell) – mexleadmin | ||
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Zeile 362: | Zeile 362: | ||
==== 7.2.2 Three-Phase System ==== | ==== 7.2.2 Three-Phase System ==== | ||
- | See also: [[https:// | + | See also: __ BROKEN-LINK: |
The most commonly used polyphase system is the three-phase system. The three-phase system has advantages over a DC system or single-phase AC system: | The most commonly used polyphase system is the three-phase system. The three-phase system has advantages over a DC system or single-phase AC system: | ||
* Simple three-phase machines can be used for generation. | * Simple three-phase machines can be used for generation. | ||
- | * Rotary field machines (e.g. synchronous | + | * Rotary field machines (e.g., synchronous or induction motors) can also be simply connected to a load, converting electrical energy into mechanical energy. |
* When a symmetrical load can be assumed, the energy flow is constant in time. | * When a symmetrical load can be assumed, the energy flow is constant in time. | ||
* For energy transport, the voltage can be up-transformed and thus the AC current, as well as the associated power loss (= waste heat), can be reduced. | * For energy transport, the voltage can be up-transformed and thus the AC current, as well as the associated power loss (= waste heat), can be reduced. | ||
Zeile 383: | Zeile 383: | ||
=== Three-phase generator === | === Three-phase generator === | ||
- | * The windings of a three-phase generator are called $\rm U$, $\rm V$, $\rm W$; the winding connections are correspondingly called: $\rm U1$, $\rm U2$, $\rm V1$, $\rm V2$, $\rm W1$, $\rm W2$ (see <imgref imageNo10> | + | * The windings of a three-phase generator are called $\rm U$, $\rm V$, $\rm W$. \\ Often they are also colour-coded as red, yellow and blue - and consecutively sometimes also called $\rm R$, $\rm Y$, $\rm B$. |
+ | * The winding connections are correspondingly called: $\rm U1$, $\rm U2$, $\rm V1$, $\rm V2$, $\rm W1$, $\rm W2$ (see <imgref imageNo10> | ||
< | < | ||
- | * The typical **winding connections** | + | * The typical **winding connections** |
< | < | ||
* The **phase voltages** | * The **phase voltages** | ||
Zeile 851: | Zeile 852: | ||
A passive component is fed by a sinusoidal AC voltage with the RMS value $U=230~\rm V$ and $f=50.0~\rm Hz$. The RMS current on this component is $I=5.00~\rm A$ with a phase angle of $\varphi=+60°$. | A passive component is fed by a sinusoidal AC voltage with the RMS value $U=230~\rm V$ and $f=50.0~\rm Hz$. The RMS current on this component is $I=5.00~\rm A$ with a phase angle of $\varphi=+60°$. | ||
- | 1. Draw the equivalent circuits based on a series and on a parallel circuit. \\ | + | 1. Draw the equivalent circuits based on a series and a parallel circuit |
# | # | ||
Zeile 988: | Zeile 989: | ||
A magnetic coil shows at a frequency of $f=50.0 {~\rm Hz}$ the voltage of $U=115{~\rm V}$ and the current $I=2.60{~\rm A}$ with a power factor of $\cos \varphi = 0.30$ | A magnetic coil shows at a frequency of $f=50.0 {~\rm Hz}$ the voltage of $U=115{~\rm V}$ and the current $I=2.60{~\rm A}$ with a power factor of $\cos \varphi = 0.30$ | ||
- | - Calculate the real power, the reactive power, and the apparent power . | + | - Calculate the real power, the reactive power, and the apparent power. |
- Draw the equivalent parallel circuit. Calculate the active and reactive part of the current. | - Draw the equivalent parallel circuit. Calculate the active and reactive part of the current. | ||
- Draw the equivalent series circuit. Calculate the ohmic and inductive impedance and the value of the inductivity. | - Draw the equivalent series circuit. Calculate the ohmic and inductive impedance and the value of the inductivity. | ||
Zeile 1263: | Zeile 1264: | ||
* The phase shift for every string is $25°$ | * The phase shift for every string is $25°$ | ||
- | - The motor shall be in wye configuration. \\ Write down the string voltage, phase voltage, string current, phase current, and active power | + | 1. The motor shall be in wye configuration. \\ |
- | - The motor shall be in delta configuration. \\ Write down the string voltage, phase voltage, string current, phase current, and active power | + | Write down the string voltage, phase voltage, string current, phase current, and active power |
- | - Compare the results | + | |
+ | # | ||
+ | |||
+ | * The **string voltage** \( U_\rm s \) is always the voltage measured on a single coil ($230 ~\rm V$). | ||
+ | * The **string current** \( I_\rm s \) is always the current measured on a single coil ($10 ~\rm A$). | ||
+ | |||
+ | In a **wye** configuration: | ||
+ | * The **phase voltage** \( U_{\rm ph} = U_{\rm 12} = U_{\rm 23} = U_{\rm 31} \) is the **string voltage** \( U_\rm s \) times \( \sqrt{3} \) | ||
+ | * The **phase current** \( I_{\rm ph} \) is just the **string current** \( I_\rm s \) | ||
+ | |||
+ | So, we can compute: | ||
+ | * **Phase voltage** \( U_{\rm ph} = \sqrt{3} \cdot U_{\rm s} = \sqrt{3} \cdot 230 ~\rm V \approx 398.37 ~\rm V \) | ||
+ | * **Active power**: | ||
+ | |||
+ | \begin{align*} | ||
+ | P &= \sqrt{3} \cdot U_{\rm s} \cdot I_{\rm ph} \cdot \cos(\phi) \\ | ||
+ | &= \sqrt{3} \cdot 398.37 \cdot 10 \cdot \cos(25^\circ) \\ | ||
+ | &= 1.732 \cdot 398.37 \cdot 10 \cdot 0.9063 \, \text{W} \\ | ||
+ | & | ||
+ | \end{align*} | ||
+ | |||
+ | # | ||
+ | |||
+ | # | ||
+ | |||
+ | - string voltage \( U_{\rm s} = 230\, \text{V} \) | ||
+ | - phase voltage \( U_{\rm ph} = 398\, \text{V} \) | ||
+ | - string current \( I_{\rm s} = 10\, \text{A} \) | ||
+ | - phase current \( I_{\rm ph} = 10\, \text{A} \) | ||
+ | - and active power \( P = 6254.79\, \text{W} \) | ||
+ | |||
+ | # | ||
+ | |||
+ | 2. The motor shall be in delta configuration. \\ | ||
+ | Write down the string voltage, phase voltage, string current, phase current, and active power | ||
+ | |||
+ | # | ||
+ | |||
+ | * The **string voltage** \( U_\rm s \) is always the voltage measured on a single coil ($230 ~\rm V$). | ||
+ | * The **string current** \( I_\rm s \) is always the current measured on a single coil ($10 ~\rm A$). | ||
+ | |||
+ | In a **delta** configuration: | ||
+ | * The **phase voltage** \( U_{\rm ph} = U_{\rm 12} = U_{\rm 23} = U_{\rm 31} \) is just the **string voltage** \( U_\rm s \) \) | ||
+ | * The **phase current** \( I_{\rm ph} \) is the **string current** \( I_\rm s \) times \( \sqrt{3} | ||
+ | |||
+ | So, we can compute: | ||
+ | * **Phase current** \( I_{\rm ph} = \sqrt{3} \cdot I_{\rm s} = \sqrt{3} \cdot 10 ~\rm V \approx 17.32 ~\rm A \) | ||
+ | * **Active power**: | ||
+ | |||
+ | \begin{align*} | ||
+ | P &= \sqrt{3} \cdot U_{\rm s} \cdot I_{\rm ph} \cdot \cos(\phi) \\ | ||
+ | &= \sqrt{3} \cdot 200 \cdot 17.32 \cdot \cos(25^\circ) \\ | ||
+ | &= 1.732 \cdot 200 \cdot 17.32 \cdot 0.9063 \, \text{W} \\ | ||
+ | & | ||
+ | \end{align*} | ||
+ | |||
+ | # | ||
+ | |||
+ | # | ||
+ | |||
+ | - string voltage \( U_{\rm s} = 230\, \text{V} \) | ||
+ | - phase voltage \( U_{\rm ph} = 230\, \text{V} \) | ||
+ | - string current \( I_{\rm s} = 10\, \text{A} \) | ||
+ | - phase current \( I_{\rm ph} = 17.32\, \text{A} \) | ||
+ | - and active power \( P = 6254.79\, \text{W} \) | ||
+ | |||
+ | # | ||
+ | |||
+ | 3. Compare the results | ||
+ | |||
+ | # | ||
+ | |||
+ | ^ Configuration ^ String Voltage (V) ^ Phase Voltage (V) ^ Line Voltage (V) ^ String Current (A) ^ Phase Current (A) ^ Line Current (A) ^ Power (W) | | ||
+ | | Wye | 230 | 230 | 398.37 | ||
+ | | Delta | 230 | 230 | 230 | 10 | 10 | 17.32 | 6254.79 | ||
+ | |||
+ | **Conclusion: | ||
+ | Both configurations deliver the same active power to the motor. However: | ||
+ | * In **wye**, voltage across each phase is lower, resulting in lower current per line. | ||
+ | * In **delta**, current per line is higher, even though voltage across each phase equals line voltage. | ||
+ | |||
+ | # | ||
+ | |||
+ | # | ||
+ | |||
+ | # | ||
+ | |||
+ | A three-phase heater with given resistors is connected to the $230~\rm V$/$400~\rm V$ three-phase system. The heater shows purely ohmic behavior and can be configured in wye or delta configuration. \\ | ||
+ | |||
+ | 1. The heater is configured in a delta configuration and provides a constant heating power of $6 ~\rm kW$. \\ | ||
+ | 1.a Calculate the resistor value of a single string in the heater. \\ | ||
+ | 1.b Calculate the RMS values of the string currents and phase currents. \\ | ||
+ | |||
+ | # | ||
+ | ===== 1. Delta configuration ===== | ||
+ | The line-to-line (string) voltage in delta is the system line voltage | ||
+ | \[ | ||
+ | U_{\mathrm s, | ||
+ | \] | ||
+ | |||
+ | **(a) Resistor of one string** | ||
+ | |||
+ | Purely ohmic, total power in delta | ||
+ | \[ | ||
+ | P_\Delta = 3\; | ||
+ | \] | ||
+ | |||
+ | Solve for \(R\): | ||
+ | \begin{align*} | ||
+ | R &= 3\frac{U_{\mathrm s, | ||
+ | | ||
+ | | ||
+ | \end{align*} | ||
+ | |||
+ | **(b) Currents** | ||
+ | |||
+ | String (coil) current | ||
+ | \[ | ||
+ | I_{\mathrm s,\Delta}= \frac{U_{\mathrm s, | ||
+ | = \frac{400}{80}=5.00~\mathrm{A}. | ||
+ | \] | ||
+ | |||
+ | In delta the **phase current equals the string current**: | ||
+ | \[ | ||
+ | I_{\mathrm{ph}, | ||
+ | \] | ||
+ | |||
+ | (The line current would be \(I_{\mathrm L,\Delta}= \sqrt3\, | ||
+ | # | ||
+ | |||
+ | # | ||
+ | * resistor of one string \(R = 80~\Omega\) | ||
+ | * string current \(I_{\mathrm s, | ||
+ | * phase current \(I_{\mathrm{ph}, | ||
+ | # | ||
+ | |||
+ | 2. The heater with the same resistors as in 1. is now configured in a wye configuration. \\ | ||
+ | 2.a Calculate the RMS values of the string currents and phase currents. \\ | ||
+ | 2.b Compare the heating power in delta configuration (1.) and wye configuration (2.) \\ | ||
+ | |||
+ | # | ||
+ | ===== 2. Wye configuration (same resistors \(R=80~\Omega\)) ===== | ||
+ | The string (phase-to-neutral) voltage is the system phase voltage | ||
+ | \[ | ||
+ | U_{\mathrm s,\mathrm Y}=U_{\mathrm{PN}}=230~\mathrm{V}. | ||
+ | \] | ||
+ | |||
+ | **(a) Currents** | ||
+ | |||
+ | String current | ||
+ | \[ | ||
+ | I_{\mathrm s,\mathrm Y}= \frac{U_{\mathrm s,\mathrm Y}}{R} | ||
+ | = \frac{230}{80}=2.875~\mathrm{A}. | ||
+ | \] | ||
+ | |||
+ | In wye the **phase current equals the string current**: | ||
+ | \[ | ||
+ | I_{\mathrm{ph}, | ||
+ | \] | ||
+ | |||
+ | **(b) Heating power in wye** | ||
+ | |||
+ | Pure ohmic load: | ||
+ | \begin{align*} | ||
+ | P_{\mathrm Y} &= 3\; | ||
+ | = 3\; | ||
+ | \approx 1.984~\mathrm{kW}. | ||
+ | \end{align*} | ||
+ | |||
+ | --- | ||
+ | |||
+ | ===== Comparison ===== | ||
+ | \[ | ||
+ | \frac{P_{\mathrm Y}}{P_\Delta} = \frac{1.984~\mathrm{kW}}{6.000~\mathrm{kW}} | ||
+ | | ||
+ | \] | ||
+ | |||
+ | The heater delivers only about **33 %** of the delta power when re-wired in wye. | ||
+ | # | ||
+ | |||
+ | # | ||
+ | * string current \(I_{\mathrm s,\mathrm Y}=2.88~\mathrm{A}\) | ||
+ | * phase current \(I_{\mathrm{ph}, | ||
+ | * heating power \(P_{\mathrm Y}\approx1.98~\mathrm{kW}\) | ||
+ | * comparison: \(P_{\mathrm Y} \approx 0.33\, | ||
+ | # | ||
+ | |||
# | # | ||
- | # | + | # |
A three-phase motor is connected to a three-phase system with a phase voltage of $400 ~\rm V$. The phase current is $16 ~\rm A$ and the power factor $0.9$. \\ | A three-phase motor is connected to a three-phase system with a phase voltage of $400 ~\rm V$. The phase current is $16 ~\rm A$ and the power factor $0.9$. \\ | ||
Zeile 1276: | Zeile 1464: | ||
- | # | + | # |
A symmetrical and balanced three-phase motor of a production line shall be configured in a star configuration and provide a power of $17~\rm kW$ with a power factor of $0.75$. The voltage on a single string is measured to be $135 ~\rm V$. \\ | A symmetrical and balanced three-phase motor of a production line shall be configured in a star configuration and provide a power of $17~\rm kW$ with a power factor of $0.75$. The voltage on a single string is measured to be $135 ~\rm V$. \\ |