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Common-Emitter Transistor Amplifier Design

Key Takeaways

  • Due to its high efficiency and positive gain greater than unity, the most commonly used transistor amplifier is the common-emitter transistor amplifier.

  • When a common-emitter transistor amplifier without emitter degeneration is designed, the value of resistor RC is chosen to match the amplifier gain requirements. The gain of this amplifier is directly proportional to the resistor  RC  value.

  • The merit of a common-emitter degeneration amplifier with a bypassed emitter resistor with a parallel resistor design is that the DC biasing of the amplifier is not dependent on the RE1 value, so the designer can set the RE1 value once the DC bias is fixed.  

Amplifiers

Amplifiers are critical to electronic circuits

Transistor amplifiers are circuits that are used to amplify weak audio, DC, or AC signals, and have a wide range of applications. When amplifying AC signals using a transistor amplifier, both voltage and current can be amplified simultaneously. 

There are three configurations of transistor amplifiers:

  1. Common-base amplifiers

  2. Common-emitter amplifiers

  3. Common-collector amplifiers

If the aim is to increase the amplitude of an AC signal, a common-emitter transistor circuit is designed. Common-emitter configurations are the most widely used type of transistor amplifier, due to their high-efficiency and positive gain greater than unity.

Let’s take a closer look at common-emitter transistor amplifiers and discuss some things designers should consider during the common-emitter transistor amplifier design process.

Common-Emitter Transistor Amplifier Design Criteria

Before discussing how to design a common-emitter transistor amplifier, it is important to understand the types of common-emitter amplifiers available. Irrespective of the configuration, an input signal is given to the base and output is collected from the collector terminal in all types of common-emitter amplifiers. The emitter terminal remains common to base and collector.

In a common-emitter without emitter degeneration, the bypass capacitor CB1 makes the ground connection of the emitter, so this configuration can also be called a grounded emitter. When this transistor amplifier is designed, the value of resistor RC is chosen to match the amplifier gain requirements. The gain of this amplifier is directly proportional to the resistor  RC  value. 

In common-emitter configurations without a bypass capacitor, the bias stability and gain of the amplifier depend on resistor RE. This transistor amplifier design gives more importance to the  RC  and  RE  values, as the gain can be controlled using them. 

A common-emitter degeneration amplifier with a bypassed emitter resistor with series emitter resistor has a bypass capacitor that connects the resistor  RE1  to the ground for high-frequency signals and bias stability. Even though the gain of the amplifier is dependent on  RC  and  RE1, designers usually keep RC constant and RE1 as a variable for gain control. 

In a common-emitter degeneration amplifier with a bypassed emitter resistor with a parallel resistor, the RE1 value is considerably smaller than RE, making the low impedance path for high-frequency signals through the bypass capacitor. In this configuration, the gain is controlled by keeping RC constant and varying RE1. The merit of this design is that the DC biasing of the amplifier is not dependent on the RE1 value, so the designer can set the RE1 value once the DC bias is fixed.  

The Steps Required for Common-Emitter Transistor Amplifier Design 

Let’s examine the steps involved in designing a common-emitter transistor amplifier without emitter degeneration. In this transistor amplifier specification, some parameters such as bias voltage, collector current, input resistance, the input AC signal, load resistance, gain, and output voltage can be given according to how the amplifier is designed. Next, let’s consider the given values: bias voltage VCC,  collector current IC, input resistance Rin, and load resistance RL

Step 1: Determine RC 

To calculate the value of RC, we can use equation (1), below. The values of VCC and IC are known. For symmetrical output, the maximum possible value of voltage VCE is 0.5VCC. So, by substituting these known values and rearranging the equation, we can obtain equation (2), allowing us to calculate RC.

Input Resistance calculation equation

Step 2: Determine the ‘Q’ Point

Once the values of VCE and IC are obtained, the Q point can be found from the output characteristics of the transistor. From the output characteristics of the transistor, find the base current curve on which the coordinate (0.5VCC, IC) lies. The base current required for this bias point is obtained. 

Step 3: Determine RE

The emitter resistor RE is usually set as 10% of the resistor RC:

Emitter Resistance calculation equation

Step 4: Determine Emitter Voltage VE

Using the IB and IC values, the emitter current IE can be calculated with the following equation:

Emitter Voltage calculation equation

Step 5: Determine Base Voltage VB

Base Voltage calculation equation

Step 6: Determine RB1 and RB2

The resistors RB1 and RB2 should be designed so that the base current IB flowing in the circuit corresponds to that of the Q-point base current. The Thevenin equivalent circuit of the voltage divider is formed by RB1 and RB2. VBB is the Thevenin equivalent voltage, RB is the Thevenin equivalent resistance, and Rib is the input resistance looking into the base of the transistor. 

Thevenin equivalent resistance Resistor Voltage equation

Step 7: Calculate Thevenin Resistance RB 

The input resistance Rin can be written as equation (9). The resistance Rib can be calculated using equation (10). From the known values of Rin and Rib, the resistance RB can be derived from equation (9).

Thevenin Resistance calculation equation

The base voltage can be given as: 

Base Voltage calculation equation

Step 8:  Calculate RB1 and RB2

From equations (7), (8), and (11), the resistors RB1 and RB2 can be calculated.

The bypass capacitor CE1 is selected so that it obeys equation (12), where XCE is the reactance of the bypass capacitor CE1:

Resistor calculation equation

Step 9: Determine CC1 and CC2

The coupling capacitors can be calculated using the following equations:

Coupling capacitor calculation equation

The variants of common-emitter transistor amplifiers with or without degeneration can be employed to satisfy amplifier requirements in electronic applications. Basic common-emitter transistor amplifier design can be carried out by following steps 1 through 9,  provided the values of VCC, IC, Rin, and RL are known. Depending on the parameters given in amplifier specifications, various equations are derived from the amplifier circuit diagram, which supports the design of the amplifier components.

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