The Wideband Differential Amplifier Calculator computes bias voltages, current levels, voltage gain, and frequency response for wideband differential amplifier circuits. Enter the amplifier parameters to quickly analyze and design differential amplifiers with accurate performance predictions.
VB = VP*R2/(R1+R2)
VE = VB - VBE
IE = VE/RE
Alpha = Beta/(Beta+1);
IC = Alpha*IE
VC = VP - IC*RC/2
IB = IC/Beta
gm = Ic/25mA
re = Alpha/gm
rπ = Beta/gm
A = Alpha*rπ*RC/(Rs+2*rπ)/re
fP1 = 1/(2*π*(Rs||2*rπ)*(CBE/2+CBC))
fP2 = 1/(2*π*RC*CBC)
fT = gm/(2π*(CBE+CBC))
The lower pole is dominant.

Introduction
This tool is designed to calculate critical performance metrics for wideband differential amplifiers, including current levels, bias voltage, gain, and frequency response.
A Wideband Differential Amplifier is an amplifier designed to maintain a precise amplification factor over a wide frequency range while providing high gain.
By using a specific configuration—tying the collector of the first transistor () to the base of the second () to signal ground—it is possible to overcome the limitations. The resulting gain-bandwidth product is orders of magnitude greater than that of standard common-emitter amplifiers.
A Differential Amplifier (or difference amplifier) is a circuit that amplifies the difference between two input signals while rejecting any signals that are common to both inputs. It is the fundamental building block of the Operational Amplifier (Op-Amp).
The Formula: The basic output equation is:
Where:
Ideally, if , the output is zero. The amplifier focuses purely on the gap between the two voltages.
Differential amplifiers are primarily used to suppress Noise.
The calculator determines critical parameters for designing wide-band differential amplifiers/ including current levels (IC/ IE/ IB)/ bias voltages (VB/ VE/ VC)/ voltage gain (A)/ and frequency response (fP1/ fP2). It also calculates transconductance (gm)/ input resistance (rπ)/ and other key metrics using user-provided resistor values/ supply voltage/ and transistor specifications.
The design ties the collector of Q1 and the base of Q2 to signal ground/ bypassing the Miller effect. This configuration significantly improves gain-bandwidth compared to common-emitter amplifiers/ enabling high-frequency performance without stability issues.
Inputs include resistor values (R1/ R2/ RC/ RE)/ supply voltage (VP)/ transistor Beta (β)/ base-emitter voltage (VBE)/ current gain-bandwidth product (fT)/ and parasitic capacitances (CBC/ optional CBE). Source resistance (Rs) and load resistance (RL) are also needed for accurate gain and frequency calculations.
Beta affects DC current gain/ directly impacting collector current (IC = β*IB) and input resistance (rπ = β/gm). Higher Beta increases voltage gain and input impedance but requires careful thermal and stability management to avoid drift or distortion.
The lower pole fP1 dominates because it arises from the input stage’s RC network (Rs || 2rπ interacting with CBE/2 and CBC). This pole defines the amplifier’s -3dB bandwidth/ while fP2 (from the output RC network) typically lies at higher frequencies due to smaller RC time constants.
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