Amplifier design with three stages
Your electronics class has probably taught you the hybrid-pi model and given you some complex (yet accurate) formulas for gain, input resistance, and output resistance of the various amplifier topologies. It might help your understanding to have some simpler, approximate formulas. These come from the always-helpful Art of Electronics by Horowitz and Hill.







simulate this circuit &ndash; Schematic created using CircuitLab

$$Current\ gain = \frac{I_C}{I_B} = h_{FE} = \beta$$

$$Input\ resistance\ of\ the\ base: \beta R_E$$

$$Output\ resistance\ of\ the\ emitter: \frac{R_S}{\beta} || R_E$$

$$Output\ resistance\ of\ the\ collector: R_C$$

$$Voltage\ gain = \frac{V_C}{V_{in}} = -\frac{R_C}{R_E}$$

These formulas are based on the following assumptions, some of which may be interchangeable:


\$\beta\$ is large
\$R_E &gt;&gt; r_e\$
The voltage drop across the base-emitter junction is constant
The collector current is not too large


As \$R_E\$ gets smaller, the inherent emitter resistance starts to have a bigger effect on your gain. As the collector current gets larger, the transistor starts acting less like an ideal current source. This is where the \$r_\pi\$ and \$r_o\$ terms from the hybrid-pi model come in. In particular, the common case of a bypassed emitter resistor (which gives you the high gain you need) requires the hybrid-pi model.

As you can see, using series resistors to directly control the input resistance is not necessary. The emitter resistor's value gets multiplied at the base. Just make sure your biasing resistors are large, and you should be fine. As you suspected, a common collector amplifier will give you the output resistance you need.