Question 10.9: Consider a common-gate amplifier with gm = 1.25 mA/V, ro = 2...

Consider a common-gate amplifier with gm = 1.25 mA/V, ro = 20 kΩ, Cgs = 20 fF, Cgd = 5 fF, CL = 25 fF, Rsig = 10 kΩ, and RL = 20 kΩ. Assume that CL includes Cdb. Determine the input resistance, the midband gain, and the upper 3-dB frequency fH.

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Figure 10.27 shows the CG amplifier circuit at midband frequencies. We note that

vo = iRL

vsig = i(Rsig + Rin)

Thus, the overall voltage gain is given by

G_{v} = \frac{v_{o}}{v_{sig}} = \frac{R_{L}}{R_{sig}  +  R_{in}}

The value of Rin is found from Eq. (10.101) as

R_{in} = \frac{r_{o}  +  R_{L}}{1  +  g_{m} r_{o}} \simeq \frac{r_{o}  +  R_{L}}{g_{m} r_{o}}                          (10.101)

R_{in} = \frac{r_{o}  +  R_{L}}{1  +  g_{m} r_{o}}

= \frac{20  +  20}{1  +  (1.25  ×  20)} = 1.54  kΩ

Thus, Gv can now be determined as

G_{v} = \frac{20}{10  +  1.54} = 1.73  V/V

Observe that as expected Gv is very low. This is due to the fact that the CG amplifier draws a large input current, equal, in fact, to the load current i.

To obtain an estimate of the 3-dB frequency fH, we first determine Rgs and Rgd using Eqs. (10.100) and (10.102),

Rgs = Rsig || Rin                  (10.100)

Rgs = Rsig || Rin = 10 || 1.54 = 1.33 kΩ

Rgd = RL || Ro                    (10.102)

where Ro is given by Eq. (10.103),

Ro = ro + Rsig + (gmro)Rsig                                (10.103)

= 20 + 10 + 25 × 10 = 280 kΩ

Thus,

Rgd = 20 || 280 = 18.7 kΩ

Now we can compute the sum of the open-circuit time constants, τH,

τH = CgsRgs + (Cgd + CL) Rgd

τH = 20 × 10−15 × 1.33 × 103 + (5 + 25) × 10−15 × 18.7 × 103

= 26.6 × 10−12 + 561 × 10−12

= 587.6 ps

and the upper 3-dB frequency fH can be obtained as

f_{H} = \frac{1}{2π  τ_{H}} = \frac{1}{2π  ×  587.6  ×  10^{-12}} = 270.9  MHz

Observe that fH is indeed much higher than (about twice) the corresponding value for the CS amplifier found in Example 10.8. Another important observation can be made by examining the two components of τH: The contribution of the input circuit is 26.6 ps, while that of the output circuit is 561 ps; thus the limitation on the high-frequency response is posed by the output circuit.

Figure 10.27

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