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CE / CS Amplifier Bench

Design a common-emitter (BJT) or common-source (FET) amplifier from scratch — set bias resistors, see the Q-point on the load line, and read gain, input/output impedance, and bandwidth at a glance.

Adjust the bias

Vᴄᴄ (V)12.0 V
Rᴄ (kΩ)2.2 kΩ
Rᴇ (kΩ)1.0 kΩ
R₁ (kΩ)33.0 kΩ
R₂ (kΩ)10.0 kΩ
β150.0
Rʟ (kΩ)10.0 kΩ
Vɪɴ (mV)20.0 mV
OFF — degenerated gain
0.01.22.33.54.7I_C (mA)0.03.26.39.512.6V_CE (V)5.3V2.1

Q-point

Vʙ = 2.8 V

Iᴄ = 2.1 mA

Vʙᴇ = 0.7 V

Vᴄᴇ = 5.3 V

gₘ = 83.6 mA/V

rπ = 1.8 kΩ

rₒ = 47.8 kΩ

Amplifier

Aᵥ = -1.7 V/V
Rɪɴ = 1.5
Rₒᴜᴛ = 2.1
VCC=12VR1=33kVB=2.8VR2=10kRC=2.2kRE=1.0kCERL=10k

Vin / Vout waveforms

vinvout

Aᵥ = -1.7 V/V  |  Vin peak = 20 mV  |  Vout peak ≈ 34 mV

Q-point Guide

Vᴄᴇ sweet spot
target ≈ Vᴄᴄ/2 = 6.0 V    actual: 5.3 V
Maximum symmetric output swing.
Vᴇ stability
target ≥ 1.0 V    actual: 2.1 V
Emitter resistor gives bias stability against temperature drift.
Active region
BJT is biased correctly in the active region for amplification.

BJT amplifier configurations

The three BJT amplifier configurations — common-emitter, common-base, and common-collector (emitter follower) — each offer a different combination of voltage gain, current gain, input impedance, and output impedance.

Configuration comparison

  • Common-emitter (CE): high voltage gain (inverting), moderate Rin, moderate Rout. General-purpose amplifier.
  • Common-base (CB): unity current gain, very low Rin, high Rout, non-inverting. Used in RF/microwave; excellent high-frequency response.
  • Common-collector (CC) / emitter follower: unity voltage gain (non-inverting), very high Rin, very low Rout. Used as an impedance buffer between high-impedance sources and low-impedance loads.

Learn more → BJT Amplifier — Learn

Quick experiments

  • Turn a gain into decibels. Set a voltage gain of 10 and read 20 dB. Gain 100 gives 40 dB, gain 1000 gives 60 dB — every ×10 in voltage adds 20 dB, because dB is a logarithmic scale.
  • Drive the amplifier into clipping. With a 12 V supply and a gain of 20, raise the input past 300 mV peak. The required 6 V peak output no longer fits inside the rails and the waveform tops flatten.
  • Trade gain for bandwidth. For a fixed gain-bandwidth product, halving the gain doubles the usable bandwidth. A 1 MHz GBW part gives 1 MHz at unity gain but only 10 kHz at a gain of 100.
  • Stack two stages. Cascade gains of 10 and 20 for an overall 200. In decibels that is 20 dB + 26 dB = 46 dB — gains multiply, but decibels simply add.
  • Check that a gain below 1 is attenuation. Set the gain to 0.5. The result is −6 dB. Negative decibels mean the signal shrank, which is exactly what a divider or a pad does.

Formula reference

Voltage gain
Av=VoutVinA_v = \frac{V_{out}}{V_{in}}

A dimensionless ratio, not yet in decibels.

Voltage gain in decibels
AdB=20log10AvA_{dB} = 20 \log_{10} A_v

×10 → 20 dB, ×2 → about 6 dB, ×1 → 0 dB.

Power gain in decibels
GdB=10log10 ⁣(PoutPin)G_{dB} = 10 \log_{10}\!\left(\frac{P_{out}}{P_{in}}\right)

Uses 10, not 20, because power already varies as voltage squared.

Gain-bandwidth product
GBW=Av×f3dBGBW = A_v \times f_{-3dB}

Roughly constant for a given op-amp, so gain and bandwidth trade directly.

SymbolMeaningUnit
AvA_vVoltage gain as a plain ratio
AdBA_{dB}The same gain in decibelsdB
GBWGBWGain-bandwidth productHz
f3dBf_{-3dB}Bandwidth at the chosen gainHz

Common mistakes

  • Using 10·log for a voltage ratio.

    Voltage and current ratios use 20·log; power ratios use 10·log. Applying the power formula to a voltage gain of 10 gives 10 dB instead of the correct 20 dB.

  • Adding gains from cascaded stages.

    Plain gains multiply — stages of 10 and 20 give 200, not 30. Only the decibel values add, which is precisely why designers work in decibels.

  • Expecting full output swing right up to the rails.

    Most op-amps lose one to two volts at each rail. A 12 V supply may only swing 8–10 V peak-to-peak unless the part is specified rail-to-rail — and even then only lightly loaded.

  • Quoting bandwidth without stating the gain.

    Bandwidth is meaningless on its own. A 1 MHz GBW amplifier has 1 MHz of bandwidth at unity gain but only 10 kHz at a gain of 100.

  • Blaming distortion entirely on clipping.

    Slew-rate limiting distorts fast signals long before the peaks flatten. If a large-amplitude sine turns triangular as frequency rises, the slew rate is the limit, not the supply.

Frequently asked questions

What is the difference between voltage gain and power gain?

Voltage gain is the ratio of output voltage to input voltage. Power gain is the ratio of output power to input power. Because power is proportional to voltage squared into the same load, a voltage gain of 10 corresponds to a power gain of 100.

How do I convert a gain to decibels?

For voltage, dB = 20 times log10 of the voltage ratio. For power, dB = 10 times log10 of the power ratio. A voltage gain of 10 is 20 dB, a gain of 100 is 40 dB, and a gain of 1 is 0 dB.

What causes an amplifier to clip?

Clipping happens when the output tries to swing beyond the supply rails. The peaks get flattened, which adds harmonic distortion. Fix it by lowering the input level, reducing the gain, or raising the supply voltage so the required swing fits inside the rails.

Why does gain fall off at high frequency?

Every amplifier has internal and load capacitance that shunts signal to ground as frequency rises, and a finite gain-bandwidth product. Once the required gain multiplied by the signal frequency exceeds that product, the gain must fall.

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