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transistor bias

Transistor Biasing

Transistor Biasing is the process of setting a transistors DC operating voltage or current conditions to the correct level so that any AC input signal can be amplified correctly by the transistor.

A transistors steady state of operation depends a great deal on its base current, collector voltage, and collector current and therefore, if a transistor is to operate as a linear amplifier, it must be properly biased to have a suitable operating point.

Establishing the correct operating point requires the proper selection of bias resistors and load resistors to provide the appropriate input current and collector voltage conditions. The correct biasing point for a bipolar transistor, either NPN or PNP, generally lies somewhere between the two extremes of operation with respect to it being either “fully-ON” or “fully-OFF” along its load line. This central operating point is called the “Quiescent Operating Point”, or Q-point for short.

When a bipolar transistor is biased so that the Q-point is near the middle of its operating range, that is approximately halfway between cut-off and saturation, it is said to be operating as a Class-A amplifier. This mode of operation allows the output current to increase and decrease around the amplifiers Q-point without distortion as the input signal swings through a complete cycle. In other words, the output current flows for the full 360o of the input cycle.

So how do we set this Q-point biasing of a transistor? – The correct biasing of the transistor is achieved using a process know commonly as Base Bias.

The function of the “DC Bias level” or “no input signal level” is to correctly set the transistors Q-point by setting its Collector current ( IC ) to a constant and steady state value without an input signal applied to the transistors Base.

This steady-state or DC operating point is set by the values of the circuits DC supply voltage ( Vcc ) and the value of the biasing resistors connected the transistors Base terminal.

Related Products: Current Regulator

Since the transistors Base bias currents are steady-state DC currents, the appropriate use of coupling and bypass capacitors will help block bias current setup for one transistor stage affecting the bias conditions of the next. Base bias networks can be used for Common-base (CB), common-collector (CC) or common-emitter (CE) transistor configurations. In this simple transistor biasing tutorial we will look at the different biasing arrangements available for a Common Emitter Amplifier.

Base Biasing a Common Emitter Amplifier

One of the most frequently used biasing circuits for a transistor circuit is with the self-bias of the emitter-bias circuit where one or more biasing resistors are used to set up the initial DC values of transistor currents, ( IB ), ( IC ) and ( IE ).

The two most common forms of transistor biasing are: Beta Dependent and Beta Independent. Transistor bias voltages are largely dependent on transistor beta, ( β ) so the biasing set up for one transistor may not necessarily be the same for another transistor. Transistor biasing can be achieved either by using a single feed back resistor or by using a simple voltage divider network to provide the required biasing voltage.

The following are five examples of transistor Base bias configurations from a single supply ( Vcc ).

Fixed Base Biasing a Transistor

fixed base biasing of transistor

The circuit shown is called as a “fixed base bias circuit”, because the transistors base current, IB remains constant for given values of Vcc, and therefore the transistors operating point must also remain fixed. This two resistor biasing network is used to establish the initial operating region of the transistor using a fixed current bias.

This type of transistor biasing arrangement is also beta dependent biasing as the steady-state condition of operation is a function of the transistors beta β value, so the biasing point will vary over a wide range for transistors of the same type as the characteristics of the transistors will not be exactly the same.

The emitter diode of the transistor is forward biased by applying the required positive base bias voltage via the current limiting resistor RB. Assuming a standard bipolar transistor, the forward base-emitter voltage drop will be 0.7V. Then the value of RB is simply: (VCC – VBE)/IB where IB is defined as IC.

With this single resistor type of biasing method the biasing voltages and currents do not remain stable during transistor operation and can vary enormously. Also the temperature of the transistor can adversely effect the operating point.

Collector Feedback Biasing a Transistor

collector feedback biasing of transistor

This self biasing collector feedback configuration is another beta dependent biasing method that requires only two resistors to provide the necessary DC bias for the transistor. The collector to base feedback configuration ensures that the transistor is always biased in the active region regardless of the value of Beta (β) as the DC base bias voltage is derived from the collector voltage, VC providing good stability.

In this circuit, the base bias resistor, RB is connected to the transistors collector C, instead of to the supply voltage rail, Vcc. Now if the collector current increases, the collector voltage drops, reducing the base drive and thereby automatically reducing the collector current to keep the transistors Q-point fixed. Then this method of collector feedback biasing produces negative feedback as there is feedback from the output to the input through resistor, RB.

The biasing voltage is derived from the voltage drop across the load resistor, RL. So if the load current increases there will be a larger voltage drop across RL, and a corresponding reduced collector voltage, VC which will cause a corresponding drop in the base current, IB which in turn, brings IC back to normal.

The opposite reaction will also occur when transistors collector current becomes less. Then this method of biasing is called self-biasing with the transistors stability using this type of feedback bias network being generally good for most amplifier designs.

Dual Feedback Transistor Biasing

dual feedback transistor biasing

Adding an additional resistor to the base bias network of the previous configuration improves stability even more with respect to variations in Beta, ( β ) by increasing the current flowing through the base bias resistors.

The current flowing through RB1 is generally set at a value equal to about 10% of collector current, IC. Obviously it must also be greater than the base current required for the minimum value of Beta, β.

One of the advantages of this type of self biasing configuration is that the resistors provide both automatic biasing and Rf feedback at the same time.

Transistor Biasing with Emitter Feedback

transistor biasing with emitter feedback

This type of transistor biasing configuration, often called self-emitter biasing, uses both emitter and collector-base feedback to stabilize the collector current even more as resistors RB and RE as well as the emitter-base junction of the transistor are all effectively connected in series with the supply voltage, VCC.

The downside of this emitter feedback configuration is that the output has reduced gain because of the base resistor connection as the collector voltage determines the current flowing through the feedback resistor, RB producing what is called “degenerative feedback”.

The current flowing from the emitter, IE (which is a combination of IC + :IB) causes a voltage drop to appear across RE in such a direction, that it forward biases the emitter-base junction.

So if the emitter current increases, voltage drop IRE also increases. Since the polarity of this voltage reverse biases the emitter-base junction, IB automatically decrease. Therefore the emitter current increase less than it would have done had there been no self biasing resistor.

Resistor values are generally set so that the voltage drop across emitter resistor RE is approximately 10% of VCC and the current flowing through resistor RB1 is 10% of the collector current IC.

This type of transistor biasing configuration works best at relatively low power supply voltages.

Voltage Divider Transistor Biasing

voltage divider transistor biasing

The common emitter transistor is biased using a voltage divider network to increase stability. The name of this biasing configuration comes from the fact that the two resistors RB1 and RB2 form a voltage or potential divider network with their center point connecting the transistors base terminal directly across the supply.

This voltage divider configuration is the most widely used transistor biasing method, as the emitter diode of the transistor is forward biased by the voltage dropped across resistor RB2. Also, voltage divider network biasing makes the transistor circuit independent of changes in beta as the voltages at the transistors base, emitter, and collector are dependant on external circuit values.

To calculate the voltage developed across resistor RB2 and therefore the voltage applied to the base terminal we simply use the voltage divider formula for resistors in series.

Generally the voltage drop across resistor RB2 is much less than for resistor RB1. Then clearly the transistors base voltage VB with respect to ground, will be equal to the voltage across RB2.

The current flowing through resistor RB2 is generally set at 10 times the value of the required base current IB so that it has no effect on the voltage divider current or changes in Beta.

The goal of Transistor Biasing is to establish a known Q-point in order for the transistor to work efficiently and produce an undistorted output signal. Correct biasing of the transistor also establishes its initial AC operating region with practical biasing circuits using either a two or four-resistor bias network.

In bipolar transistor circuits, the Q-point is represented by ( VCE, IC ) for the NPN transistors or ( VEC, IC ) for PNP transistors. The stability of the base bias network and therefore the Q-point is generally assessed by considering the collector current as a function of both Beta (β) and temperature.

Here we have looked briefly at five different configurations for “biasing a transistor” using resistive networks. But we can also bias a transistor using either silicon diodes, zener diodes or active networks all connected to the base terminal of the transistor or by biasing the transistor from a dual power supply.

48 Comments

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  • k
    kidane

    the Best Note!!!

  • S
    S

    Thank you! I’m slogging through the ARRL License Manual for the Am Extra exam and this explanation is vastly more clear.

  • E
    Erratum Report

    You said ‘diode’ but I think meant “electrode.”

    Where? Third paragraph of heading ‘Fixed Base Biasing a Transistor.’

    • Wayne Storr

      No its correct. The pn-junction between the Base and Emitter forms a diode with a forward bias voltage drop of 0.6-to-0.7V for silicon.

      • R
        Robert Sumner

        I see now. Yes, I recall that a transistor can be used as a diode. Neat how you included that in your coverage!

  • v
    vasanth

    l want full information about transistor and its uses as amplifier

  • k
    kebier

    Whay the Q point is given by (VCE, Ic) and not (Vout,Ic)

  • T
    Todd

    Your equations for the base bias circuit are incorrect. The real equation is Vce = Vcc – IcRc

    You are stating that that Vce = Vcc – Vc and that Vc = Vcc – IcRc. This completely false. Your equation in reality comes out to Vce = Vcc – Vce. That is impossible. Looks like you need to go back to school, better yet, go back to Jr High math.

    • A
      Andreas

      Todd, I’m afraid Wayne is right. You see, the transistor’s emitter is grounded, so Ve=0. Therefore Vc=Vce and according to KVL, Vcc=IcRc+Vc.

      Wayne nowhere says that Vce = Vcc – Vc.

    • Wayne Storr

      Sarcasm is a display of ignorance, and so too is your understanding of maths. The application of Kirchoff’s Voltage Law, (KVL) shows that the voltage level at point Vc = Vcc minus the IR voltage drop across the load resistor, then: Vc = Vcc – IcRc
      The voltage across the collector-emitter terminals of the transistor: Vce = Vc – Ve as stated.
      As the emitter terminal is grounded in this configuration at 0v, Vce = Vc – 0 or Vce = Vc
      Thanks.

      • T
        Todd

        Vc does equal Vcc- IcRc. Clearly you don’t understand the failure you have posted on your site. You are stating that Vc = Vcc – Vce. However, Vc = Vce. For example, lets just say that Vce= 0.5V and that Vcc=10V. Therefore IcRc=9.5V (KVL). Vc = Vce, or 0.5V=0.5V. Now lets use your equation. Vc = Vcc – Vce. 0.5V = 10V – 0.5V….whoops, doesn’t work now does it? This is the problem with novices trying to teach. You screw everyone over. Maybe you made a typo in the equation list for the base bias circuit. But you are making yourself look foolish by not correcting your error.

  • G
    Ganga

    A great difference between classA,B,AB

  • G
    Ganga

    Good explained

  • s
    sony

    wat is base drive?

  • d
    dinesh devireddy

    conceptual oriented !

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