Lecture (10) Power Amplifiers (2)

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Lecture (10) Power Amplifiers (2) By: Dr. Ahmed ElShafee ١ Class B/AB Power the ideal maximum peak output current for both dual supply and single supply push pull amplifiers is approximately Ic(sat), and the maximum peak output voltage is approximately VCEQ. Substituting VCC>2 for VCEQ, the maximum average output power is ٢

DC Input Power The dc input power comes from the VCC supply and is Since each transistor draws current for a half cycle, the current is a half wave signal with an average value of ٣ Efficiency An advantage of push pull class B and class AB amplifiers over class A is a much higher efficiency. Recall that the maximum efficiency for class A is 0.25 (25 ٤ percent).

Example 01 Find the maximum ac output power and the dc input power of the amplifier in Figure ٥ ٦

Input Resistance class B/class AB amplifiers Since RE RL ٧ Example 02 ٨

this will have an effect on the preamp driver stage. The output resistance of the preamp stage and the input resistance of the power amp effectively form a voltage divider ٩ Darlington Class AB Amplifier push pull amplifiers can present a quite low input resistance to the preceding amplifier that drives it. Depending on the output resistance of the preceding amplifier, the low pushpull input resistance can load it severely and significantly reduce the voltage gain. ١٠

١١ Darlington/Complementary Darlington Class AB Amplifier The complementary Darlington, also known as the Sziklai pair, ١٢

Class C amplifiers A class C amplifier is normally operated with a resonant circuit load ١٣ It is biased below cutoff with the negative VBB supply. The ac source voltage has a peak value that is slightly greater than VBB +VBE ١٤

١٥ Power Dissipation The power dissipation of the transistor in a class C amplifier is low because it is on for only a small percentage of the input cycle. The collector current and the collector voltage during the on time of the transistor are shown in Figure To avoid complex mathematics, we will assume ideal pulse approximations ١٦

١٧ the maximum current amplitude is Ic(sat) and the minimum voltage amplitude is Vce(sat) during the time the transistor is on. The power dissipation during the on time is, The transistor is on for a short time, ton, and off for the rest of the input cycle. Therefore, assuming the entire load line is used, the power dissipation averaged over the entire cycle is ١٨

Example 03 ١٩ ٢٠

Tuned Operation Because the collector voltage (output) is not a replica of the input, the resistively loaded class C amplifier alone is of no value in linear applications. It is to use a class C amplifier with a parallel resonant circuit (tank), ٢١ The current pulse charges the capacitor to approximately VCC, ٢٢

After the pulse, the capacitor quickly discharges, thus charging the inductor. Then, after the capacitor completely discharges, the inductor s magnetic field collapses and then quickly recharges C to near VCC in a direction opposite to the previous charge. This completes one half cycle of the oscillation ٢٣ Next, the capacitor discharges again, increasing the inductor s magnetic field The inductor then quickly recharges the capacitor back to a positive peak slightly less than the previous one, due to energy loss in the winding resistance. This completes one full cycle, ٢٤

The amplitude of each successive cycle of the oscillation will be less than that of the previous cycle because of energy loss in the resistance of the tank circuit, as shown in Figure However, the regular recurrences of the collector current pulse re energizes the resonant circuit and sustains the oscillations at a constant amplitude. ٢٥ When the tank circuit is tuned to the frequency of the input signal (fundamental), reenergizing occurs on each cycle of the tank voltage, Vr ٢٦

When the tank circuit is tuned to the second harmonic of the input signal, re energizing occurs on alternate cycles as shown in Figure ٢٧ In this case, a class C amplifier operates as a frequency multiplier By tuning the resonant tank circuit to higher harmonics, further frequency multiplication factors are achieved. ٢٨

Maximum Output Power Since the voltage developed across the tank circuit has a peak to peak value of approximately 2VCC, the maximum output power can be expressed. ٢٩ Rc is the equivalent parallel resistance of the collector tank circuit at resonance and represents the parallel combination of the coil resistance and the load resistance. It usually has a low value. ٣٠

Clamper Bias for a Class C Amplifier The base emitter junction functions as a diode. When the input signal goes positive, capacitor C1 is charged to the peak value with the polarity This action produces an average voltage at the base of approximately Vp This places the transistor in cutoff except at the positive peaks, when the transistor conducts for a short interval. For good clamping action, the R1C1 time constant of the clamping circuit must be much greater than the period of the input signal ٣١ During the time up to the positive peak of the input (t0 to t1), the capacitor charges to Vp 0.7 ٣٢

During the time from t1 to t2, as shown in part (c), the capacitor discharges very little because of the large RC time constant. The capacitor, therefore, maintains an average charge slightly less than Vp 0.7 ٣٣ Since the dc value of the input signal is zero ( positive side of C1), the dc voltage at the base (negative side of C1) is slightly more positive than (Vp 0.7) ٣٤

Near the positive peaks of the input voltage, the base voltage goes slightly above 0.7 V and causes the transistor to conduct for a short time, ٣٥ the capacitor couples the ac input signal through to the base so that the voltage at the transistor s base is the ac signal riding on a dc level slightly more positive than (Vp 0.7) ٣٦

Example 04 Determine the voltage at the base of the transistor, the resonant frequency, and the peakto peak value of the output signal voltage for the class C amplifier in Figure ٣٧ ٣٨

٣٩ Thanks,.. Wish you the best of luck ٤٠