Fig. 6.16 Analysis of the current mirror taking into account the finite of the BJTs.

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Fig. 6.2 Different modes of operation of the differential pair: (a) The differential pair with a common-mode input signal v CM . (b) The differential pair with a “large” differential input signal. (c) The differential pair with a large input signal of polarity opposite to that in (b). (d) The differential pair with a small differential input signal v i .

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Transcript of Fig. 6.16 Analysis of the current mirror taking into account the finite of the BJTs.

Page 1: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.2 Different modes of operation of the differential pair: (a) The differential pair with a common-mode input signal vCM. (b)

The differential pair with a “large” differential input signal. (c) The differential pair with a large input signal of polarity opposite to that in (b). (d) The differential pair with a small differential input signal vi.

Page 2: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.3 Transfer characteristics of the BJT differential pair of Fig. 6.2 = 1 assuming 1.

Page 3: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.4 The current an voltages in the differential amplifier when a small difference signal vd is applied.

Page 4: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.5 A simple technique for determining the signal currents in a differential amplifier excited by a differential voltage signal vd;

dc quantities are not shown.

Page 5: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.6 A differential amplifier with emitter existence. Only signal quantities are shown (on color).

Page 6: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.7 Equivalence of the differential amplifier (a) to the two common-emitter amplifiers in (b). This equivalence applies only for differential input signals. Either of the two common-emitter amplifiers in (b) can be used to evaluate the differential gain, input differential resistance, frequency response, and so on, of the differential amplifier.

Page 7: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.10 (a) The differential amplifier fed by a common-mode voltage signal. (b) Equivalent “half-circuits” for the common-mode calculations.

Page 8: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.16 Analysis of the current mirror taking into account the finite of the BJTs.

Page 9: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.18 Generation of a number of cross currents.

Page 10: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.19 A current mirror with base-current compensation.

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Fig. 6.20 The Wilson current mirror.

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Fig. 6.21 The Widlar current source.

Page 13: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.24 Circuit for Example 6.3.

Page 14: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.25 A differential amplifier with an active load.

Page 15: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.26 Small-signal model of the differential amplifier of Fig. 6.25.

Page 16: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.27 (a) The differential form of the cascode amplifier, and (b) its differential half circuit.

Page 17: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.28 A cascode differential amplifier with a Wilson current-mirror active load.

Page 18: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.29 The MOSFET differential pair.

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Fig. 6.30 Normalized plots of the currents in a MOSFET differential pair. Note that VGS is the gate-to-source voltage when the drain

current is equal to the dc bias current (I/2).

Page 20: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.32 MOS current mirrors: (a) basic, (b) cascode, (c) Wilson, (d) modified Wilson.

Page 21: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.35 basic active-loaded amplifier stages; (a) bipolar; (b) MOS; (c) BiCMOS obtained by cascoding Q1 with a BJT, Q2; (d)

BiCMOS double cascode.

Page 22: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.36 Voltage gain of the active-loaded common-source amplifier versus the bias current ID. Outside the subthreshold region, this is a plot of Eq. (6.121) for the case nCox = 20 A/V2, = 0.05 V-1, L = 2 m and W = 20 m.

Page 23: Fig.  6.16   Analysis of the current mirror taking into account the finite    of the BJTs.

Fig. 6.46 A multistage amplifier circuit (Example 6.4).