Lecture 14 Transistors and Operational Amplifiers ECE 205

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Lecture 14 Transistors and Operational Amplifiers ECE 205 Prof. Ali Keyhani

Lecture 14 Transistors and Operational Amplifiers ECE 205 Prof. Ali Keyhani

Transistor • A semiconductor device that can be modeled with dependent sources • Transistor

Transistor • A semiconductor device that can be modeled with dependent sources • Transistor types: – Bipolar Junction Transistor (BJT) – Field Effect Transistor (FET) • A transistor has different operating modes with different i-v characteristics

Bipolar Junction Transistor (BJT) • BJTs are made up of alternating layers of n

Bipolar Junction Transistor (BJT) • BJTs are made up of alternating layers of n and p semiconductor materials joined metallurgically • Two types of BJTs: – pnp-type: Principal conduction by positive holes – npn-type: Principal conduction by negative electrons

Bipolar Junction Transistor (BJT) • BJT is a three terminal device: – Emitter (E)

Bipolar Junction Transistor (BJT) • BJT is a three terminal device: – Emitter (E) – Collector (C) – Base (B)

Bipolar Junction Transistor (BJT) • Applying KCL to BJT: – Finding two currents can

Bipolar Junction Transistor (BJT) • Applying KCL to BJT: – Finding two currents can yield the third one • Three operating modes of the BJT transistors: – Active mode – Cutoff mode – Saturation mode

Active Mode • In active mode collector current is controlled by base current and

Active Mode • In active mode collector current is controlled by base current and base-emitter voltage is constant:

Active Mode Circuit model in active mode:

Active Mode Circuit model in active mode:

Cutoff mode • The device acts like an open circuit between collector and emitter:

Cutoff mode • The device acts like an open circuit between collector and emitter: • Circuit model:

Saturation Mode • The device acts like a short circuit between the collector and

Saturation Mode • The device acts like a short circuit between the collector and emitter • Circuit model:

Operating Bounds Active Mode: Cutoff Mode: Saturation Mode:

Operating Bounds Active Mode: Cutoff Mode: Saturation Mode:

BJT Common Emitter Circuit • Assuming the circuit operates in active mode:

BJT Common Emitter Circuit • Assuming the circuit operates in active mode:

Output Response of BJT Circuit

Output Response of BJT Circuit

Operational Amplifier (OP AMP) • A five terminal device : two inputs, one output

Operational Amplifier (OP AMP) • A five terminal device : two inputs, one output and positive and negative supply voltages • OP AMPS are high gain dc amplifiers that perform mathematical operation • The positive and negative power supplies determine the upper and lower limits on the output voltage.

OP AMP packaging:

OP AMP packaging:

 • OP AMP Voltage and current definitions: • The input currents are negligible

• OP AMP Voltage and current definitions: • The input currents are negligible and ideally zero

Transfer Characteristics • Provides the relationship between the noninverting input v. P and inverting

Transfer Characteristics • Provides the relationship between the noninverting input v. P and inverting input v. N and the output voltage v. O • Has three Operating modes: § Linear § + Saturation § - Saturation

Transfer Characteristics Linear Mode: A is the voltage gain which is usually very large

Transfer Characteristics Linear Mode: A is the voltage gain which is usually very large + Saturation Mode: - Saturation Mode:

Ideal OP AMP Model • Based on the equation of the OP AMP operating

Ideal OP AMP Model • Based on the equation of the OP AMP operating in the linear region the dependent source model of the OP AMP is derived: – High Input resistance – Low output resistance – High voltage gain

Ideal OP AMP Model For an Op AMP operating in linear mode: In an

Ideal OP AMP Model For an Op AMP operating in linear mode: In an ideal OP AMP A ∞ therefore : In an ideal OP AMP RI is large hence:

Ideal OP AMP Model

Ideal OP AMP Model

Noninverting OP AMP Since there is no input current voltage division can be used

Noninverting OP AMP Since there is no input current voltage division can be used to find the voltage at inverting input: