13.5. Shunt – Series Cascade Amplifier

The cascading of two common-source amplifier stages will now be explored. This will expand the discussion on feedback amplifiers to include the shunt – series (current) amplifier. As shown in Fig. 13.5, the current Io is sensed, with the feedback network consisting of RS2 and Rf, and a fraction of Io is summed at the gate input node along with the input source current. Gate resistor RG1 provides for an addition bias design variable but otherwise is simply combined with the source resistance, Rs, in the amplifier performance analysis or design.

Figure 13.5. Shunt-series feedback amplifier. This is a current amplifier with feedback amplifier gain, Ai = Io/Ii.


13.5.1. DC Design

For the design, assume that a choice has been made for ID1 and ID2 and VG2 = VD1. The latter must be such that VG2 > VGS1 + VGS2. Then, for RD1, use

Equation 13.10


As will be indicated below, the ideal current gain is

Equation 13.11


Use this, based on the feedback-amplifier design current gain goal, to obtain a relation between Rf and RS2. This gives

Equation 13.12


Now determine the value of RS2 which statisfies the design value of ID2. This is obtaned from

Equation 13.13


where 13.12 has been used for Rf and where VS2 = VG1 – VGS2 and

Equation 13.14


and

Equation 13.15


Finally, select RG1 to satisfy the VGS1 requirement from

Equation 13.16


13.5.2. DC Stability

The feedback network provides significant bias stabilization and the effect can be assessed by the same formulation as for the opamp. In Unit 11.4, it was shown that the output voltage for a given offset voltage is [(11.16)]


As applied to our shunt – series circuit (by equivalency), AVNI = 1 + Rf/RG1, and avo is the voltage-gain magnitude (minus terminal equivalent) from the gate, Vg1, to the source Vs2, that is, the gain of the case of a common-source stage (M1) and a source-follower stage (M2). Also, for this case, ΔVo ≡ ΔVS2. Note that for this case, ΔVo is a bias-voltage change, whereas for the opamp, it is the output voltage (different from zero volts).

Suppose that the dc (bias) is at a set state. Then the bias is altered such as by a change of a transitor parameter (either by temperature change or substituting one transistor for a new one). For example, a change in Vtno of M1 is equivalent to installing an offset voltage, and [(11.16)] can be applied directly to this case. Make RG1 = Rf for AVNI = 2. Also assume a typical avo = 40 (common-source stage). For a change of δVtno ≡ –Voff = –0.1 V, ΔVO ≈ 2 · 0.1 V = 0.2 V. Note that based on avo = 40, with no feedback stabilzation, the change in output would be approximately avoδVtno = 4 V.

13.5.3. Signal Current Gain

We first compute the open-loop transconductance and then the open-loop current gain. This is done, for a good approximation, by disconnecting the right side of Rf from the souce of M2 and connecting it to ground. (This disables the shunt – series feedback and otherwise alters the circuit only slightly.) The result is

Equation 13.17


where Ri = Rs||RG1||Rf. (This assumes that Rf >> RS2 which is consistent with AiI >> 1.) Transconductance Gm is for the complete cascade circuit (open loop), that is,

Equation 13.18


Note that the series – series feedback effect is retained in the open-loop computation and that RS2 has been used as an approximation for RS2||Rf. This once again assumes that Rf >> RS2. The loop gain is

Equation 13.19


Following the discussion in Unit 11, which led to (11.3), the current gain with feedback is then

Equation 13.20


where (ideal current gain of the feedback amplifier)

Equation 13.21


As a design example, suppose the design goal is AiI = 10. Assume that the transistors have Vtno = 1 V, kn1 = 1000 μA/V2, and kn2 = 2000 μA/V2. We select ID1 = 100 μA, ID2 = 200 μA, VDD = 10 V, and VG2 = 3.5 V. From (13.12) and (13.13) we obtain RS2 = 11.4 kΩ and Rf = 103 kΩ. Based on (13.16), the value of RG1 is RG1 = 156 kΩ. To satisfy the drain voltage requirements, RD1 = 65 kΩ and RD2 = 25 kΩ. The latter is based on VD2 = VDD/2. Also, we assume that Rs = 100 kΩ.

The open-loop transconductance is Gm = 3372 μA/V and Ri = 38 kΩ for ai = 129. Loop gain T = 12.9 such that Ai = 9.28. We note that since Ai ≈ AiI = 10, the current gain is very predictable, despite bias and parameter variations.

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