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Session 44; 1/6 Sample Exam Solution Problem 1: You are given a single phase diode rectifier, as shown below. Do the following: L d I s v (t) s L s C d V d Load : 310V Xs : 0.4ohm at 400 Hz Vspk : 360V Vs : Vspk 2 ω : 2 400Hz Xs Ls : Ls 0.2 mh ω A. Assume that L d 0 and C d is large. Plot the ac current versus time for one 400 Hz cycle. Determine the angles at which conduction begins in degrees. Also determine the peak dc current. Since the capacitor voltage is fixed at 310 V, there will be no decrease in due to the voltage drop across Ls, and since no current flows prior to diode turn on in this case, we can find θb from Vs*sin(θb). Note that we are already given the peak voltage θb : asin θb 59.4 deg 2 Vs Note: This exam was originally assigned as a take home exam, so solving for θ f in order to plot the waveform was not a time issue. In the final in this class you won't need to do so.

Session 44; 2/6 Now solve for θf, using the equation for the current. θf1 : 150deg Given θf ( ( ) cos( θf1) ) ( ) 2 Vs cos θb θf1 θb 0 : Find( θf1) θf 152 deg θb2 : θb + θb2 239.4 deg θf2 : θf + θf2 332 deg Expression for current (conditional so it doesn't reverse) t1 : 0, 0.00005sec.. 0.0025sec vs1( t1) : 2 Vs sin( ω t1) ia( t1) : 1 ω ( Ls) 2 Vs ( cos( θb) cos( ω t1) ) ( ω t1 θb) if θb ω t1 θf 1 ω ( Ls) 2 Vs ( cos( θb2) cos( ω t1) ) + ( ω t1 θb2) if θb2 ω t1 0 otherwise θf2 360 ia( t1) vs1( t1) 0 146.67 0 6.25. 10 4 0.00125 0.00187 0.0025 t1

Session 44; 3/6 Find angle of peak current and peak current: θp : + θb θp 120.6 deg 2 2 Convert to seconds: tpeak θp : tpeak 8.4 10 4 s ω ia( tpeak) 88.5A (b) In many cases it is desirable to have continuous conduction. Describe potential benefits to having continuous conduction. How would the circuit need to be modified from the conditions of part A to achieve continuous conduction? Would the voltages need to change? 1. If it is continuous conduction, the peak current will be lower (if the average current is the same). Also the harmonic content of the waveform may improve somewhat. 2. We would want to add enough inductance on the dc side of the circuit to bring it to continuous conduction. Adding additional inductance on the ac side can help somewhat too, but the dc side inductance has the larger impact. 3. There would be commutation overlap due to the ac side inductance, so the average dc voltage wou be somewhat lower. Problem 2: For the converter shown below, determine the following: (a) What type of converter is it? Buck-Boost V d S L C - V o D +

Session 44; 4/6 (b) Duty cycle : 25V L : 0.2mH Rout : 3.25ohm : 18V fs : 5kHz Ts : 1 fs Solve the equation: D1 1 D1 for D: D : + D 0.4 Is it in continuous conduction? Iob : ( 1 D) 2 fs 2L Iob 3A Io : Rout Io 5.5 A Since Io > Iob, continuous conduction So the result for D above is correct. c. We want to limit V o to 0.5% of the output voltage. Determine the necessary capacitance. Io D Ts C : 0.5% 0.1 V Therefore we can solve for C: C : Io D Ts C 5152.1 µf What would happen if a smaller capacitor was used? If the size of the capacitor is decreased, the peak to peak ripple voltage would increase, and the current to the load would also show more ripple.

Session 44; 5/6 Problem 3 A. You are given a boost converter. You measure the input voltage to be 15 V from a 100W source and have an output current of 4 A. Assuming no power losses determine: input current, output voltage, duty ratio. The filter inductance is 100 µh and the switching frequency is 10 khz. : 15V L : 100µH Pin : 100W fs : 10kHz Iout : 4A Pout : Pin ut : Pout Iout ut 25 V Iin : Pin Iin 6.7 A D : ut ut D 0.4 Check continuous: Iob : ut D ( 1 D) 2 2L fs Iob 1.8 A This is smaller than the load current, so it is in continuous conduction. B Given a diode rectifier with a large dc filter capacitor, how does the average dc voltage normally relate to the RMS ac voltage if there is now ac side inductance. o 2 2 Vs where v s () t 2Vs sin( ω t) 2 2 0.9 or simplifying: o 0.9 Vs If the ac side inductance is called Ls:

Session 44; 6/6 o ω Ls Idave If Ls is 0, then: 0.9 Vs Problem 4: Answer the following questions. (a) What does the commutation overlap angle represent? The commutation overlap angle (µ or u) represents the impact of the ac side inductance on the transition (or commutation) from one pair of diode to the next in the cycle. If the circuit is in contiuous conduction, the current through the ac side inductor will not be zero when the trans occurs. As a result, the current in the inductor will need to go to zero. At the same time the current in the other inductor will be ringing up. µ 1,2 3,4 I dc (b) What must be present in the circuit for commutation overlap to occur? AC side inductance and enough dc side inductance to bring the circuit nearly to continuous conduction. (c) Will there be commutation overlap if the diode current goes to zero before θ 180deg? Explain No. Commutation overlap only occurs when there current through the diode needs to be forced to zero (along with the inductor current) at the voltage zero crossing. (d) How does commutation overlap impact the dc voltage? Explain The dc voltage is reduced as follows: o 0.9 Vs o ω Ls Idave