Bipolar transistors must be properly biased to operate correctly. In circuits made with individual devices (discrete circuits), biasing networks consisting of resistors are commonly employed. Much more elaborate biasing arrangements are used in integrated circuits, for example, bandgap voltage references and current mirrors. The voltage divider configuration achieves the correct voltages by the use of resistors in certain patterns. By selecting the proper resistor values, stable current levels can be achieved that vary only little over temperature and with transistor properties such as β.

The operating point of a device, also known as bias point, quiescent point, or Q-point, is the point on the output characteristics that shows the DC collector–emitter voltage (V_ce) and the collector current (I_c) with no input signal applied.

Bias circuit requirements

A bias network is selected to stabilize the operating point of the transistor, by reducing the following effects of device variability, temperature, and voltage changes:^[1]

• The gain of a transistor can vary significantly between different batches, which results in widely different operating points for sequential units in serial production or after replacement of a transistor.
• Due to the Early effect, the current gain is affected by the collector–emitter voltage.
• Both gain and base–emitter voltage depend on the temperature.
• The leakage current also increases with temperature.

A bias circuit may be composed of only resistors, or may include elements such as temperature-dependent resistors, diodes, or additional voltage sources, depending on the range of operating conditions expected.

Signal requirements

For analog operation of a class-A amplifier, the Q-point is placed so the transistor stays in active mode (does not shift to operation in the saturation region or cut-off region) across the input signal's range. Often, the Q-point is established near the center of the active region of a transistor characteristic to allow similar signal swings in positive and negative directions.

For digital operation, the Q-point is instead chosen so the transistor switches from the "on" (saturation) to the "off" (cutoff) state.

Thermal considerations

At constant current, the voltage across the emitter–base junction V_BE of a bipolar transistor decreases by 2 mV (silicon) and 1.8 mV (germanium) for each 1 °C rise in temperature (reference being 25 °C). By the Ebers–Moll model, if the base–emitter voltage V_BE is held constant and the temperature rises, the current through the base–emitter junction I_B will increase, and thus the collector current I_C will also increase. Depending on the bias point, the power dissipated in the transistor may also increase, which will further increase its temperature and exacerbate the problem. This deleterious positive feedback results in thermal runaway.^[2] There are several approaches to mitigate bipolar transistor thermal runaway. For example,

• Negative feedback can be built into the biasing circuit so that increased collector current leads to decreased base current. Hence, the increasing collector current throttles its source.
• Heat sinks can be used that carry away extra heat and prevent the base–emitter temperature from rising.
• The transistor can be biased so that its collector is normally less than half of the power supply voltage, which implies that collector–emitter power dissipation is at its maximum value. Runaway is then impossible because increasing collector current leads to a decrease in dissipated power; this notion is known as the half-voltage principle. The circuits below primarily demonstrate the use of negative feedback to prevent thermal runaway.

Types of bias circuit for class-A amplifiers

The following discussion treats five common biasing circuits used with class-A bipolar transistor amplifiers:

1. Fixed bias
2. Collector-to-base bias
3. Fixed bias with emitter resistor
4. Voltage divider bias or potential divider
5. Emitter bias

Fixed bias (base bias)

This form of biasing is also called base bias or fixed resistance biasing.

In the given fixed bias circuit,

$${\displaystyle I_{\text{b))={\frac {V_{\text{cc))-V_{\text{be))}{R_{\text{b))))\,.}$$

The common-emitter current gain of a transistor (specified as a range on its data sheet as h_FE or β), allows us to obtain ${\textstyle I_{\text{c))}$ as well:

$${\displaystyle I_{\text{c))=\beta I_{\text{b))\,.}$$

$${\displaystyle V_{\text{ce))=V_{\text{cc))-{I_{\text{c))R_{\text{c))}\,.}$$

${\textstyle (V_{\text{ce)),\ I_{\text{c)))}$

Advantages:

• The operating point is set by two resistors and the calculation is very simple.

Disadvantages:

• Since the bias is set by the base current, the collector current is directly proportional to β. Therefore, the operating point will vary significantly when transistors are swapped and it is unstable under changes in temperature.
• For small-signal transistors (e.g., not power transistors) with relatively high values of β (i.e., between 100 and 200), this configuration will be prone to thermal runaway. In particular, the stability factor, which is a measure of the change in collector current with changes in reverse saturation current, is approximately β+1. To ensure absolute stability of the amplifier, a stability factor of less than 25 is preferred, and so small-signal transistors have large stability factors.^{[citation needed]}

Usage:

Due to the above inherent drawbacks, fixed bias is rarely used in linear circuits (i.e., those circuits which use the transistor as a current source). Instead, it is often used in circuits where the transistor is used as a switch. However, one application of fixed bias is to achieve crude automatic gain control in the transistor by feeding the base resistor from a DC signal derived from the AC output of a later stage.

Collector feedback bias

This configuration employs negative feedback to prevent thermal runaway and stabilize the operating point. In this form of biasing, the base resistor ${\displaystyle R_{\text{b))}$ is connected to the collector instead of connecting it to ${\displaystyle V_{\text{cc))}$. So any thermal runaway will induce a voltage drop across the ${\displaystyle R_{\text{c))}$ resistor that will throttle the transistor's base current.

From Kirchhoff's voltage law, the voltage ${\displaystyle V_((\text{R))_{\text{b))))$ across the base resistor ${\displaystyle R_{\text{b))}$ is

${\displaystyle V_((\text{R))_{\text{b))}=V_{\text{cc))\,-\,{\mathord {\overbrace {(I_{\text{c))+I_{\text{b)))R_{\text{c))} ^((\text{Voltage drop across ))R_{\text{c))))}\,-\,{\mathord {\overbrace {V_{\text{be))} ^{\text{Voltage at base)))).}$

By the Ebers–Moll model, ${\displaystyle I_{\text{c))=\beta I_{\text{b))}$, and so

${\displaystyle V_((\text{R))_{\text{b))}=V_{\text{cc))-(\overbrace {\beta I_{\text{b))} ^{I_{\text{c))}+I_{\text{b)))R_{\text{c))-V_{\text{be))=V_{\text{cc))-I_{\text{b))(\beta +1)R_{\text{c))-V_{\text{be)).}$

From Ohm's law, the base current ${\displaystyle I_{\text{b))=V_((\text{R))_{\text{b))}/R_{\text{b))}$, and so

${\displaystyle \overbrace {I_{\text{b))R_{\text{b))} ^{V_((\text{R))_{\text{b))))=V_{\text{cc))-I_{\text{b))(\beta +1)R_{\text{c))-V_{\text{be)).}$

Hence, the base current ${\displaystyle I_{\text{b))}$ is

${\displaystyle I_{\text{b))={\frac {V_{\text{cc))-V_{\text{be))}{R_{\text{b))+(\beta +1)R_{\text{c))))}$

If ${\displaystyle V_{\text{be))}$ is held constant and temperature increases, then the collector current ${\displaystyle I_{\text{c))}$ increases. However, a larger ${\displaystyle I_{\text{c))}$ causes the voltage drop across resistor ${\displaystyle R_{\text{c))}$ to increase, which in turn reduces the voltage ${\displaystyle V_((\text{R))_{\text{b))))$ across the base resistor ${\displaystyle R_{\text{b))}$. A lower base-resistor voltage drop reduces the base current ${\displaystyle I_{\text{b))}$, which results in less collector current ${\displaystyle I_{\text{c))}$. Because an increase in collector current with temperature is opposed, the operating point is kept stable.

Advantages:

• Circuit stabilizes the operating point against variations in temperature and β (i.e. replacement of transistor).
• Circuit stabilizes the operating point (as a fraction of ${\displaystyle V_{\text{cc))}$) against variations in ${\displaystyle V_{\text{cc))}$.

Disadvantages:

• Although small changes in β are OK, large changes in β will greatly change the operating point. ${\displaystyle R_{\text{b))}$ must be chosen once β is known fairly accurately (perhaps within ~ 25%), yet the variability of β between "identical" parts is often larger than this.

• In this circuit, to keep ${\displaystyle I_{\text{c))}$ independent of ${\displaystyle \beta }$, the following condition must be met:
  $${\displaystyle I_{\text{c))=\beta I_{\text{b))={\frac {\beta (V_{\text{cc))-V_{\text{be)))}{R_{\text{b))+R_{\text{c))+\beta R_{\text{c))))\approx {\frac {(V_{\text{cc))-V_{\text{be)))}{R_{\text{c))))}$$

  
  which is the case when
  $${\displaystyle \beta R_{\text{c))\gg R_{\text{b)).}$$

  
• As ${\displaystyle \beta }$-value is fixed (and generally unknown) for a given transistor, this relation can be satisfied either by keeping ${\displaystyle R_{\text{c))}$ fairly large or making ${\displaystyle R_{\text{b))}$ very low.

• If ${\displaystyle R_{\text{c))}$ is large, a high ${\displaystyle V_{\text{cc))}$ is necessary, which increases cost as well as precautions necessary while handling.
• If ${\displaystyle R_{\text{b))}$ is low, the reverse bias of the collector–base region is small, which limits the range of collector voltage swing that leaves the transistor in active mode.

• The resistor ${\displaystyle R_{\text{b))}$ causes an AC feedback, reducing the voltage gain of the amplifier. This undesirable effect is a trade-off for greater Q-point stability. However, a T (R-C-R) network can be used to reduce the AC feedback, which however poses a heavier load on the collector than the simple feedback resistor. At higher frequencies a R-L feedback network can be used, however, it will introduce peaking into the frequency response at various points.

Usage: In this configuration, which is known as "voltage-shunt feedback', the output voltage is sensed and the feedback signal (a current) is applied in shunt (i.e., in parallel with the input). This means that the input impedance "looking into the base" is actually reduced. This can easily be verified by application of Miller's Theorem. This situation is similar to that of an inverting op-amp circuit where the input impedance of the amplifier at the virtual earth is near zero and the overall input impedance is determined by the external series resistor. Due to the gain reduction from feedback, this biasing form is used only when the trade-off for stability is warranted. Adding an emitter resistor to this circuit will increase the input impedance

Fixed bias with emitter resistor

The fixed bias circuit is modified by attaching an external resistor to the emitter. This resistor introduces negative feedback that stabilizes the Q-point. From Kirchhoff's voltage law, the voltage across the base resistor is

$${\displaystyle V_{R_{\text{b))}=V_{\text{cc))-I_{\text{e))R_{\text{e))-V_{\text{be))}$$

$${\displaystyle I_{\text{b))={\frac {V_{R_{\text{b)))){R_{\text{b))))}$$

Similarly, if the transistor is replaced by another, there may be a change in I_c (corresponding to change in β-value, for example). By similar process as above, the change is negated and operating point kept stable.

For the given circuit,

$${\displaystyle I_{\text{b))={\frac {V_{\text{cc))-V_{\text{be))}{R_{\text{b))+(\beta +1)R_{\text{e))))}$$

The circuit has the tendency to stabilize operating point against changes in temperature and β-value.

Disadvantages:

• In this circuit, to keep I_c independent of β the following condition must be met:
  $${\displaystyle I_{\text{c))=\beta I_{\text{b))={\frac {\beta (V_{\text{cc))-V_{\text{be)))}{R_{\text{b))+(\beta +1)R_{\text{e))))\approx {\frac {(V_{\text{cc))-V_{\text{be)))}{R_{\text{e))))}$$

  
  which is approximately the case if
  $${\displaystyle (\beta +1)R_{\text{e))\gg R_{\text{b)).}$$

  

• As β-value is fixed for a given transistor, this relation can be satisfied either by keeping R_e very large, or making R_b very low.
  • If R_e is of large value, high V_cc is necessary. This increases cost as well as precautions necessary while handling.
  • If R_b is low, a separate low voltage supply should be used in the base circuit. Using two supplies of different voltages is impractical.
• In addition to the above, R_e causes AC feedback which reduces the voltage gain of the amplifier.

Usage:

The feedback also increases the input impedance of the amplifier when seen from the base, which can be advantageous. Due to the above disadvantages, this type of biasing circuit is used only with careful consideration of the trade-offs involved.

Collector-Stabilized Biasing.

Voltage divider biasing or emitter bias

The voltage divider is formed using external resistors R₁ and R₂. The voltage across R₂ forward biases the emitter junction. By proper selection of resistors R₁ and R₂, the operating point of the transistor can be made independent of β. In this circuit, the voltage divider holds the base voltage fixed (independent of base current), provided the divider current is large compared to the base current. However, even with a fixed base voltage, collector current varies with temperature (for example) so an emitter resistor is added to stabilize the Q-point, similar to the above circuits with emitter resistor. The voltage divider configuration achieves the correct voltages by the use of resistors in certain patterns. By manipulating the resistors in certain ways you can achieve more stable current levels without having β value affect it too much.

In this circuit the base voltage, ${\textstyle V_{\text{b))}$, across ${\displaystyle R_{2}\ }$is given by

$${\displaystyle V_{\text{b))=V_{\text{cc)){\frac {R_{2)){(R_{1}+R_{2})))-I_{\text{b)){\frac {R_{1}R_{2)){(R_{1}+R_{2})))\approx V_{\text{cc)){\frac {R_{2)){(R_{1}+R_{2})))}$$

${\displaystyle I_{\text{b))<<I_{1}=V_{\text{b))/R_{1))$

It is also known that

$${\displaystyle V_{\text{b))=V_{\text{be))+V_{\text{e))=V_{\text{be))+I_{\text{e))R_{\text{e)).}$$

$${\displaystyle I_{\text{b))={\frac ((\frac {V_{\text{cc))}{1+R_{1}/R_{2))}-V_{\text{be))}{(\beta +1)R_{\text{e))+R_{1}\parallel R_{2))))$$

• Operating point is almost independent of β variation.
• Operating point stabilized against shift in temperature.

Disadvantages:

• In this circuit, to keep I_c independent of β the following condition must be met:
  $${\displaystyle I_{\text{c))=\beta I_{\text{b))=\beta {\frac ((\frac {V_{\text{cc))}{1+R_{1}/R_{2))}-V_{\text{be))}{(\beta +1)R_{\text{e))+R_{1}\parallel R_{2))}\approx {\frac ((\frac {V_{\text{cc))}{1+R_{1}/R_{2))}-V_{\text{be))}{R_{\text{e)))),}$$

  
  which is approximately the case if
  $${\displaystyle (\beta +1)R_{\text{e))>>R_{1}\parallel R_{2))$$

  
  where R₁ || R₂ denotes the equivalent resistance of R₁ and R₂ connected in parallel.

• As β-value is fixed for a given transistor, this relation can be satisfied either by keeping R_e fairly large, or making R₁||R₂ very low.
  • If R_e is of large value, high V_cc is necessary. This increases cost as well as precautions necessary while handling.
  • If R₁ || R₂ is low, either R₁ is low, or R₂ is low, or both are low. A low R₁ raises V_b closer to V_c, reducing the available swing in collector voltage, and limiting how large R_c can be made without driving the transistor out of active mode. A low R₂ lowers V_be, reducing the allowed collector current. Lowering both resistor values draws more current from the power supply and lowers the input resistance of the amplifier as seen from the base.
• AC as well as DC feedback is caused by R_e, which reduces the AC voltage gain of the amplifier. A method to avoid AC feedback while retaining DC feedback is discussed below.

Usage:

The circuit's stability and merits as above make it widely used for linear circuits.

Voltage divider with AC bypass capacitor

The standard voltage divider circuit discussed above faces a drawback – AC feedback caused by resistor R_e reduces the gain. This can be avoided by placing a capacitor (C_e) in parallel with R_e, as shown in circuit diagram.

Advantages:

• The result is that the DC operating point is well controlled.

• The AC-gain is much higher (approaching β), rather than the much lower (but predictable) value of ${\displaystyle R_{\text{c))/R_{\text{e))}$ without the capacitor.

Disadvantages:

• Adds an extra component.

Emitter bias

When a split supply (dual power supply) is available, this biasing circuit is the most effective. It provides zero bias voltage at the emitter or collector for load.^{[clarification needed]} The negative supply V_ee is used to forward-bias the emitter junction through R_e. The positive supply V_cc is used to reverse-bias the collector junction.

If R_b is small enough, base voltage will be approximately zero. Therefore, emitter current is,

$${\displaystyle I_{\text{e))={\frac {V_{\text{ee))-V_{\text{be))}{R_{\text{e))))}$$

• The operating point is independent of ${\textstyle \beta }$ if ${\textstyle R_{\text{e))\gg R_{\text{b))/\beta }$.

• Only two resistors are necessary for the common collector configuration. (And four resistors for a common emitter or common base configuration.)

Disadvantages:

• This type can only be used when a split (dual) power supply is available.

Class-B and AB amplifiers

Signal requirements

Class B and AB amplifiers employ 2 active devices to cover the complete 360 deg of input signal flow. Each transistor is therefore biased to perform over approximately 180 deg of the input signal. Class B bias is when the collector current I_c with no signal is just conducting (about 1% of maximum possible value). Class-AB bias is when the collector current I_c is about 1⁄4 of maximum possible value. The class-AB push–pull output amplifier circuit below could be the basis for a moderate-power audio amplifier.

Q3 is a common emitter stage that provides amplification of the signal and the DC bias current through D1 and D2 to generate a bias voltage for the output devices. The output pair are arranged in class-AB push–pull, also called a complementary pair. The diodes D1 and D2 provide a small amount of constant voltage bias for the output pair, just biasing them into the conducting state so that crossover distortion is minimized. That is, the diodes push the output stage into class-AB mode (assuming that the base-emitter drop of the output transistors is reduced by heat dissipation).

This design automatically stabilizes its operating point, since overall feedback internally operates from DC up through the audio range and beyond. The use of fixed diode bias requires the diodes to be both electrically and thermally matched to the output transistors. If the output transistors conduct too much, they can easily overheat and destroy themselves, as the full current from the power supply is not limited at this stage.

A common solution to help stabilize the output device operating point is to include some emitter resistors, typically an ohm or so. Calculating the values of the circuit's resistors and capacitors is done based on the components employed and the intended use of the amplifier.