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Electronics Principles & Applications Fifth Edition Chapter 7 More About Small-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler
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Amplifier Coupling Voltage Gain FET Amplifier Negative Feedback Frequency Response INTRODUCTION
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V CC These two points are at different dc voltages. Capacitive coupling is convenient in cascade ac amplifiers.
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V CC Direct coupling is required for dc gain.
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V CC The darlington is a popular dc arrangement.
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V CC P S 10:1 10 Z RATIO = T RATIO 2 = 10 2 = 100 Z COLLECTOR = 100 x 10 = 1000 Transformer coupling offers the advantage of impedance matching.
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V CC Transformer coupling can be used in bandpass amplifiers to achieve selectivity. fRfR Gain
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Amplifier coupling quiz Capacitive coupling is not useful for _________ amplifiers. dc Dc frequency response requires ________ coupling. direct Transformer coupling offers the advantage of _________ matching. impedance Tuned transformer coupling provides frequency _____________. selectivity A darlington amplifier is an example of _________ coupling. direct
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R B1 E B C RLRL V CC R B2 RERE = 12 V 2.7 k 22 k = 2.2 k More about solving the practical circuit for its ac conditions: = 220 Z in = ?
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R B1 E B C RLRL V CC R B2 RERE = 12 V 2.7 k 22 k = 2.2 k Z in is a combination of R B1, R B2, and r in of the transistor. = 220 r in = (R E + r E ) r in = (220 + 9.03 ) r in = 34.4 k Note: r in = r E when R E is bypassed. Determine r in first:
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R B1 E B C RLRL V CC R B2 RERE = 12 V 2.7 k 22 k = 2.2 k = 220 Z in = 1 R B2 1 r in 1 + R B1 1 +++ Z in = 1 2.7 k 1 34.4 k 1 22 k 1 Z in = 2.25 k R B1, R B2, and r in act in parallel to load the input signal.
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R B1 V CC R B2 RERE = 12 V 2.7 k 22 k RLRL = 2.2 k = 220 Load = 2.2 k What happens when an amplifier is loaded? R L and the Load act in parallel. R P = 1.1 k
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R B1 R B2 RERE V CC = 12 V 2.7 k 22 k RLRL = 2.2 k = 220 Load = 2.2 k There are two saturation currents for a loaded amplifier. R P = 1.1 k I SAT(DC) = V CC R L + R E = 4.96 mA I SAT(AC) = V CC R P + R E = 9.09 mA
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0 24 6 8 1012 14 16 18 2 4 6 8 10 12 14 V CE in Volts I C in mA 20 A 0 A 100 A 80 A 60 A 40 A There are three load lines for a loaded amplifier. DC TEMPORARY AC The DC load line connects V CC and I SAT(DC). The temporary AC load line connects V CC and I SAT(AC).
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0 24 6 8 1012 14 16 18 2 4 6 8 10 12 14 V CE in Volts I C in mA 20 A 0 A 100 A 80 A 60 A 40 A 5.3 V DC AC TEMP. AC The quiescent V CE is projected to the DC load line to establish the Q-point. The AC load line is drawn through the Q-point, parallel to the temporary AC load line.
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0 24 6 8 1012 14 16 18 2 4 6 8 10 12 14 V CE in Volts I C in mA 20 A 0 A 100 A 80 A 60 A 40 A 5.3 V AC The AC load line shows the limits for V CE and if the Q-point is properly located. With loaded amplifiers, the Q-point is often closer to saturation.
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R B1 R B2 RERE V CC = 12 V 2.7 k 22 k RLRL = 2.2 k = 220 Load = 2.2 k What about voltage gain for a loaded amplifier? R P = 1.1 k A V = RPRP R E + r E A V = 1.1 k 220 9.03 = 4.8
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V CC Z in of the 2nd stage loads the 1st stage. When analyzing cascade amplifiers, remember: 2nd 1st
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Amplifier ac conditions quiz Emitter bypassing _________ an amplifier’s input impedance. decreases Loading at the output of an amplifier ________ its voltage gain. decreases A loaded amplifier has two load lines: dc and ___________. ac The clipping points of a loaded amplifier are set by its _______ load line. ac In a cascade amplifier, the Z in of a stage _______ the prior stage. loads
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Drain Source Gate V DD = 20 V V GS = 1.5 V RGRG C R L = 5 k Input signal Common-source JFET amplifier. Fixed bias I SAT = 20 V 5 k = 4 mA Phase-inverted output
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0 2 4 1 V DS in Volts I D in mA 5 10 15 20 25 3 -2.5 -2.0 -1.5 -0.5 0 N-channel JFET characteristic curves V GS in Volts Load line The q-point is set by the fixed bias. 8 V P-P 1 V P-P A V = 8
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0 2 4 1 V DS in Volts I D in mA 5 10 15 20 25 3 -2.5 -2.0 -1.5 -0.5 0 Determining forward transfer admittance: Y fs = IDID V GS V GS in Volts V DS 1.6 mA = 1.6 mS
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D S G V DD = 20 V V GS = 1.5 V RGRG C R L = 5 k When the forward transfer admittance is known, the voltage gain can be determined using: A V = Y fs x R L = 1.6 mS x 5 k = 8 This agrees with the graphic solution.
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D S G V DD V GS = I D x R S RGRG C RLRL RSRS Source bias eliminates the need for a separate V GS supply. I S = I D This resistor also provides ac negative feedback which decreases the voltage gain.
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V in - BV out A(V in - BV out ) BV out A = open loop gain Summing junction V in V out A B Feedback A negative feedback model B = feedback ratio V out = A(V in - BV out ) V out = AV in - ABV out AV in V out 1 = - AB AV in V out AB +1 = V in V out AB +1 A = V in V out AB +1 A = A V in V out A simplified model
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D S G V DD RGRG C RLRL RSRS = 5 k = 800 The feedback ratio (B) for this circuit is easy to determine since the source and drain currents are the same. B = 800 5 k = 0.16
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AB +1 A V in V out Use the simplified model: A (WITH NEG. FEEDBACK) = 8 (8)(0.16) + 1 = 3.51
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CSCS D G V DD RGRG C RLRL RSRS The source bypass capacitor will eliminate the ac negative feedback and restore the voltage gain.
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JFET amplifier quiz In a common-source amplifier, the input signal goes to the _______. gate In a common-source amplifier, the input to output phase relationship is ____. 180 o The voltage gain of a C-S amplifier is equal to Y fs x _________. load resistance Source bias is produced by current flow through the _______ resistor. source An unbypassed source resistor _______ the voltage gain of a C-S amp. decreases
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Amplifier Negative Feedback DC reduces sensitivity to device parameters DC stabilizes operating point DC reduces sensitivity to temperature change AC reduces gain AC increases bandwidth AC reduces signal distortion and noise AC may change input and output impedances
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0.707 A max A f The frequency response curve of an ac amplifier Bandwidth The gain is maximum in the midband. A max Midband The bandwidth spans the -3 dB points which are called the break frequencies. -3dB
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Amplifier frequency response The lower break frequency is partly determined by coupling capacitors. It is also influenced by emitter bypass capacitors. The upper break frequency is partly determined by transistor internal capacitance. Both break frequencies can be influenced by negative feedback.
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REVIEW Amplifier Coupling Voltage Gain FET Amplifier Negative Feedback Frequency Response
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