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?
Solución de inteligencia artificial de Upstudy
Responder
Solución
Respondido por UpStudy AI y revisado por un tutor profesional


Extra Insights
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
