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A \( 210 \mathrm{~V}, 1200 \) RPM, 10 A separately excited DC motor is controlled by a \( 1- \) phase fully controlled converter with an AC source voltage of \( 230 \mathrm{~V}, 50 \mathrm{~Hz} \). Assume that sufficient inductance is present in the armature circuit to make the motor current continuous and ripple free for any torque greater than \( 25 \% \) of rated torque. Ra \( =1.5 \Omega \) (a) What should be the value of the firing angle to get the rated torque at 800 rpm? (b) Compute the firing angle for the rated braking torque at - 1200 rpm. (c) Calculate the motor-speed at the rated torque and \( \alpha= \) \( 165^{\circ} \) for the regenerative braking in the second quadrant?

Ask by Tucker Bush. in Tanzania
Mar 09,2025

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**(a) Firing Angle for Rated Torque at 800 rpm:** To achieve the rated torque at 800 rpm, the firing angle \(\alpha\) should be approximately \(165^\circ\). **(b) Firing Angle for Rated Braking Torque at -1200 rpm:** For the rated braking torque at -1200 rpm, the firing angle \(\alpha\) is approximately \(15^\circ\). **(c) Motor Speed at Rated Torque with \(\alpha = 165^\circ\) for Regenerative Braking:** At a firing angle of \(165^\circ\), the motor speed is approximately 800 rpm during regenerative braking in the second quadrant.

Solution

We wish to control a DC motor by means of a fully‐controlled, single–phase AC converter. The converter “develops” an average DC voltage approximately given by \[ V_{d}=\frac{2V_{m}}{\pi}\cos\alpha \] where • \( V_{m} \) is the peak value of the AC supply voltage, and • \(\alpha\) is the firing angle. The AC supply has an rms value of 230 V so that \[ V_{m}=\sqrt{2}\,(230)\approx325.3\;{\rm V} \] which gives \[ V_{d}\approx\frac{2(325.3)}{\pi} \cos\alpha\approx \frac{650.6}{\pi}\cos\alpha\approx207.2\cos\alpha\quad({\rm volts}). \] The DC motor is rated at 210 V, 1200 rpm and 10 A. (The motor is separately excited so that the field remains constant.) When running at its rated point the armature voltage \(210\,{\rm V}\) is “used” to drop voltage across the armature resistance and to “build” the back emf. In other words, the motor “voltage‐equation” is \[ V_{d}=E+I_{a}R_{a} \] In the rated motoring condition the current is 10 A so that \[ E_{\rm rated}=210-10\times 1.5=210-15=195\;{\rm V}. \] Since the back emf is proportional to the speed, \[ E=K\omega\quad \Longrightarrow \quad K=\frac{E_{\rm rated}}{\omega_{\rm rated}}, \] we first convert 1200 rpm to radians per second: \[ \omega_{\rm rated}=1200\frac{2\pi}{60}=40\pi\approx125.66\;{\rm rad/s} \] so that \[ K=\frac{195}{125.66}\approx1.5515\;{\rm V/(rad/s)}. \] Now we solve the three parts. --- **(a) Find the firing angle \(\alpha\) required to have the rated torque (10 A) at 800 rpm** At 800 rpm the motor’s angular speed in rad/s is \[ \omega=800\frac{2\pi}{60}\approx83.78\;{\rm rad/s}. \] Thus the back emf is \[ E=K\omega\approx1.5515\times83.78\approx129.87\;{\rm V}. \] For the same rated (motoring) current (10 A) the voltage drop in the armature is \[ I_{a}R_{a}=10\times1.5=15\;{\rm V}. \] Thus the converter must “supply” a DC voltage of

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To solve the given problems for the separately excited DC motor controlled by a fully controlled converter, let's break down each part systematically. ### (a) Firing angle for rated torque at 800 RPM First, we need to find the back EMF (E) at 800 RPM. The relation between speed and back EMF is given by: \[ E = \left( \frac{P \cdot \phi \cdot N \cdot Z}{60 \cdot A} \right) \] For simplicity, we can use the equation \( E = K \phi N \), where K is a constant. For the rated speed of 1200 RPM, \( E_{1200} \) is approximately 210 V. Since speed is directly proportional to EMF, we can lay out the equations as ratios. To find the required back EMF at 800 RPM: \[ \frac{E_{800}}{E_{1200}} = \frac{800}{1200} \Rightarrow E_{800} = \frac{800}{1200} \cdot 210 = 140 \text{ V} \] Next, we calculate the DC link voltage \( V_d \): Using the formula for voltage in the motor circuit: \[ V_d = E + I_a \cdot R_a = E + (10A \cdot 1.5\Omega) = 140 + 15 = 155 \text{ V} \] Now, for a fully controlled converter with firing angle \( \alpha \): \[ V_d = \frac{2\sqrt{2}V_{s}}{\pi} \cdot \cos(\alpha) \] Where \( V_s = 230 V \): \[ 155 = \frac{2\sqrt{2} \cdot 230}{\pi} \cdot \cos(\alpha) \] Calculating \( \frac{2\sqrt{2} \cdot 230}{\pi} \): \[ \frac{2 \cdot 1.414 \cdot 230}{3.14} \approx 218.77 \text{ V} \] Substituting back to find \( \cos(\alpha) \): \[ 155 = 218.77 \cdot \cos(\alpha) \Rightarrow \cos(\alpha) \approx \frac{155}{218.77} \approx 0.710 \] \[ \alpha \approx \cos^{-1}(0.710) \approx 44.42^{\circ} \] ### (b) Firing angle for rated braking torque at -1200 RPM For braking torque, the EMF would be negative, so the equation becomes: \[ E_{-1200} = -E_{1200} = -210 \text{ V} \] Now using the same equation for the converter voltage: \[ V_d = E + I_a R_a = -210 + (10A \cdot 1.5\Omega) = -210 + 15 = -195 \text{ V} \] Using the converter voltage equation: \[ -195 = \frac{2\sqrt{2} \cdot 230}{\pi} \cdot \cos(\alpha) \] Solving for cos(α), we need to be careful with the signs here since we're dealing with a negative voltage: \[ -195 = 218.77 \cdot \cos(\alpha) \Rightarrow \cos(\alpha) = \frac{-195}{218.77} \approx -0.891 \] \[ \alpha \approx \cos^{-1}(-0.891) \approx 150.96^{\circ} \] ### (c) Motor speed at rated torque and \( \alpha = 165^{\circ} \) For \( \alpha = 165^{\circ} \), calculate the voltage: \[ V_d = \frac{2\sqrt{2} \cdot 230}{\pi} \cdot \cos(165^{\circ}) \approx -218.77 \cdot \cos(165^{\circ}) \] Given that \( \cos(165^{\circ}) \approx -0.2588\): \[ V_d \approx 218.77 \cdot (-0.2588) \approx -56.66 \text{ V} \] Using \( V_d = E + I_a R_a \): \[ -56.66 = E + (10 \cdot 1.5) \Rightarrow E = -56.66 - 15 = -71.66 \text{ V} \] Now, we can find speed (N): \[ \frac

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