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Common base

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Title: Common base  
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Subject: Buffer amplifier, Common emitter, Amplifier, Current source, Common collector
Collection: Single-Stage Transistor Amplifiers
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Common base

Figure 1: Basic NPN common base circuit (neglecting biasing details).

In electronics, a common base (also known as grounded-base) amplifier is one of three basic single-stage bipolar junction transistor (BJT) amplifier topologies, typically used as a current buffer or voltage amplifier.

In this circuit the emitter terminal of the transistor serves as the input, the collector the output, and the base is connected to ground, or "common", hence its name. The analogous field-effect transistor circuit is the common gate amplifier.


  • Simplified Operation 1
  • Applications 2
  • Low-frequency characteristics 3
    • Active loads 3.1
  • Overview of characteristics 4
    • Voltage amplifier 4.1
    • Current follower 4.2
  • See also 5
  • References 6
  • External links 7

Simplified Operation

As current is sunk from the emitter this provides potential difference so causing the transistor to conduct.[1] The current conducted via the collector is proportional to the voltage across the base-emitter junction, accounting for the bias, as with other configurations.[2]

Therefore, if no current is sunk at the emitter the transistor does not conduct.


This arrangement is not very common in low-frequency discrete circuits, where it is usually employed for amplifiers that require an unusually low input impedance, for example to act as a preamplifier for moving-coil microphones. However, it is popular in integrated circuits and in high-frequency amplifiers, for example for VHF and UHF, because its input capacitance does not suffer from the Miller effect, which degrades the bandwidth of the common emitter configuration, and because of the relatively high isolation between the input and output. This high isolation means that there is little feedback from the output back to the input, leading to high stability.

This configuration is also useful as a current buffer since it has a current gain of approximately unity (see formulas below). Often a common base is used in this manner, preceded by a common emitter stage. The combination of these two form the cascode configuration, which possesses several of the benefits of each configuration, such as high input impedance and isolation.

Low-frequency characteristics

At low frequencies and under small-signal conditions, the circuit in Figure 1 can be represented by that in Figure 2, where the hybrid-pi model for the BJT has been employed. The input signal is represented by a Thévenin voltage source, vs, with a series resistance Rs and the load is a resistor RL. This circuit can be used to derive the following characteristics of the common base amplifier.

Definition Expression Approximate expression Conditions
Open-circuit voltage gain {A_{v}} = \begin{matrix} {v_\mathrm{o} \over v_\mathrm{i}} \end{matrix} \Big|_{R_{L}=\infty} \begin{matrix} \frac {(g_m r_\mathrm{o}+1)R_C} {R_C+r_o} \end{matrix} \begin{matrix} g_m R_C \end{matrix} r_o \gg R_C
Short-circuit current gain A_{i} = \begin{matrix} {i_\mathrm{o} \over i_\mathrm{i}} \end{matrix} \Big|_{R_{L}=0} \begin{matrix} \frac {r_{ \pi }+ \beta r_o} {r_{ \pi} +( \beta +1)r_o} \end{matrix} \begin{matrix} \end{matrix} 1 \beta \gg 1
Input resistance R_\mathrm{in} = \begin{matrix} \frac{v_{i}}{i_{i}} \end{matrix} \begin{matrix} \frac {(r_o+R_C\|R_L)r_E} {r_o+r_E +\frac {R_C\|R_L} { \beta +1}} \end{matrix} r_e \left( \approx \frac {1}{g_m}\right) r_o \gg R_C\|R_L \ \ \left( \beta \gg 1 \right)
Output resistance R_\mathrm{out} = \begin{matrix} \frac{v_{o}}{-i_{o}} \end{matrix} \Big|_{v_{s}=0} R_C \| \{v_{S}} = \frac {R_L}{R_S} \end{matrix} .
Note for source impedances such that RS >> rE the output impedance approaches Rout = RC || [ gm ( rπ || RS ) rO ].
  • For the special case of very low impedance sources, the common base amplifier does work as a voltage amplifier, one of the examples discussed below. In this case (explained in more detail below), when RS << rE and RL << Rout, the voltage gain becomes:
A_v =\begin{matrix}\frac {v_{out}}{v_{S}} = \frac {R_L}{r_E} \approx g_m R_L\end{matrix} ,
where gm = IC / VT is the transconductance. Notice that for low source impedance, Rout = rO || RC.
  • The inclusion of rO in the hybrid-pi model predicts reverse transmission from the amplifiers output to its input, that is the amplifier is bilateral. One consequence of this is that the input/output impedance is affected by the load/source termination impedance, hence, for example, the output resistance, Rout, may vary over the range rO || RCRout ≤ (β + 1) rO || RC depending on the source resistance, RS. The amplifier can be approximated as unilateral when neglect of rO is accurate (valid for low gains and low to moderate load resistances), simplifying the analysis. This approximation often is made in discrete designs, but may be less accurate in RF circuits, and in integrated circuit designs where active loads normally are used.

Voltage amplifier

Figure 2: Small-signal model for calculating various parameters; Thévenin voltage source as signal.

For the case when the common base circuit is used as a voltage amplifier, the circuit is shown in Figure 2.

The output resistance is large, at least RC || rO, the value which arises with low source impedance (RS << rE). A large output resistance is undesirable in a voltage amplifier, as it leads to poor voltage division at the output. Nonetheless, the voltage gain is appreciable even for small loads: according to the table, with RS = rE the gain is Av = gm RL / 2. For larger source impedances, the gain is determined by the resistor ratio RL / RS, and not by the transistor properties, which can be an advantage where insensitivity to temperature or transistor variations is important.

An alternative to the use of the hybrid-pi model for these calculations is a general technique based upon two-port networks. For example, in an application like this one where voltage is the output, a g-equivalent two-port could be selected for simplicity, as it uses a voltage amplifier in the output port.

For RS values in the vicinity of rE the amplifier is transitional between voltage amplifier and current buffer. For RS >> rE the driver representation as a Thévenin source should be replaced by representation with a Norton source. The common base circuit stops behaving like a voltage amplifier and behaves like a current follower, as discussed next.

Current follower

Figure 3: Common base circuit with Norton driver; RC is omitted because an active load is assumed with infinite small-signal output resistance

Figure 3 shows the common base amplifier used as a current follower. The circuit signal is provided by an AC Norton source (current IS, Norton resistance RS) at the input, and the circuit has a resistor load RL at the output.

As mentioned earlier, this amplifier is bilateral as a consequence of the output resistance rO, which connects the output to the input. In this case the output resistance is large even in the worst case (it is at least rO || RC and can become (β + 1) rO || RC for large RS). Large output resistance is a desirable attribute of a current source because favorable current division sends most of the current to the load. The current gain is very nearly unity as long as RS >> rE.

An alternative analysis technique is based upon two-port networks. For example, in an application like this one where current is the output, an h-equivalent two-port is selected because it uses a current amplifier in the output port.

See also


  1. ^
  2. ^

External links

  • Basic BJT Amplifier Configurations
  • NPN Common Base Amplifier — HyperPhysics
  • ECE 327: Transistor Basics — Gives example common base circuit (i.e., current source) with explanation.
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