Chapter 1

Amplifier Models

• These are purely models, and cannot be replicated in a real world environment. They are meant to explain.
• Trans stands for transfer - from voltage to current or visa versa.
• The inputs and outputs can be either current or voltage. This leads to 4 amplifier models.
• You can use any of these models, though some may be easier to work with (if you are given the Thevenin or Norton equivalent)

Amplifier models

Amplifier type Gain parameter Gain equation	Voltage input	Current input
Voltage output	Voltage Open-circuit voltage gain $A_{voc}={\frac {v_{ooc}}{v_{i}}}$	Transresistance Open-circuit transresistance gain $R_{moc}={\frac {v_{ooc}}{i_{i}}}$
Current output	Transconductance Short-circuit transconductance gain $G_{msc}={\frac {i_{osc}}{v_{i}}}$	Current Short-circuit current gain $A_{isc}={\frac {i_{osc}}{i_{i}}}$

Characteristics of ideal amplifiers

Amplifier Type	Input Impedance	Output Impedance	Gain Parameter
Voltage	$\infty$	0	$A_{voc}\,$
Current	0	$\infty$	$A_{isc}\,$
Transconductance	$\infty$	$\infty$	$G_{msc}\,$
Transresistance	0	0	$R_{moc}\,$

Differential Amplifiers

• $V_{o}=A_{d}(v_{i1}-v_{i2})\,$, where $A_{d}\,$ is the differential gain

Definitions

• Input Resistance: $R_{i}$ of an amplifier is the equivalent resistance seen when looking into the input terminals
• Output Resistance:$R_{o}$ is the Thevenin resistance seen when looking back into the output terminals of an amplifier
• Open-circuit voltage gain: the ratio of output amplitude to input amplitude with the output terminals open circuited
• Short-circuit current gain: the current gain with the output terminals of the amplifier short circuited
• Differential input signal: is the difference between the input voltages. $v_{id}=v_{i1}-v_{i2}\,$
• Common-mode input signal: is the average of the input voltages. $v_{icm}={\frac {1}{2}}(v_{i1}+v_{i2})$

Bag of Tricks

• Buffer amplifier
• Inverting amplifier