BJT Cascode Amplifier Calculator

This BJT Amplifier calculator calculates bias voltages and currents, gains, and frequency responses for the Cascode amplifier. Enter values of Cascode amplifier and hit the “Compute” button to use this online calculator for computing bias voltage and current levels, gain and frequency response for the Cascode amplifier.

BJT Cascode Amplifier Calculator

R1
(K ohms)
VC1 (Collector Voltage)
(V)
R2
(K ohms)
VE1 (Emitter Voltage)
(V)
R3
(K ohms)
VB1 (Base Voltage)
(V)
RC (Collector resistor)
(K ohms)
VC2 (Collector Voltage)
(V)
RE1 (Emitter resistor, AC bypassed)
(K ohms)
VE2 (Emitter Voltage)
(V)
RE2 (Emitter resistor, gain control)
(ohms)
VB2 (Base Voltage)
(V)
VP (Supply Voltage)
(V)
IC (Collector Voltage)
(mA)
Beta (DC Current Gain)
IB (Base Voltage)
(mA)
VBE (Base to emitter drop)
(V)
gm (Transconductance)
Rs (Source Resistance):
(ohms)
rπ(Input Resistance of BJT at low freq)
(ohms)
RL (Load resistor)
(ohms)
RIN (Input Resistance of Amp)
(K ohms)
fT (Current Gain BW Product):
(MHz)
A (Amplifier Voltage Gain)
CCB (Cu Collector-Base Cap.):
(pF)
f1
(MHz)
CBE (Cπ, Base-Emitter Cap.): Optional
(pF)
f2
(MHz)
BW
(MHz)

Equations

VB1= R3/(R1+R2+R3)

VB2= (R2+R3)/(R1+R2+R3)

VE1= VB1-VBE

VE2= VB2-VBE

VC1= VE2

VC2= VP - IC*RC

RB1= R3*(R1+R2)/ (R1+R2+R3)

IB*RB1 + IB*Beta*RE+VBE=VB1

IB= (VB1-VBE)/(RB1+Beta*RE)

IC= Beta*IB

gm = Ic/25mA

rπ=Beta/gm

If RE2 is zero ohms:

A= -gm*((RL||RC)*(R2||R3))/(R23+RS)*(rπ/(rπ+Rx+(R2||R3||RS)),

else

A= -(RL||RC)/RE2

Rx is typically10-30 ohms, we use 20 in the calculator.

fT= gm/(2π*(CBE+CBC))

f1= 1/(Rin*(Cbe+ 2*Ccb))/(2*π);

f2= 1/(RL*Ccb)/(2*π);

The lower pole is dominate:

BW= f1;

Introduction

DC Analysis of Cascode Amplifier (BJT) video lecture from Multistage Amplifier chapter of Electronic Devices and Circuits Subject for all engineering students.

Cascode Amplifier (BJT) - DC Analysis - Multistage Amplifier - Electronic Devices and Circuits

BJT Cascode Amplifier Calculator Overview

The BJT Cascode Amplifier Calculator helps estimate the bias voltages, currents, small-signal gain, and frequency-response indicators of a BJT cascode amplifier. It is intended for early circuit design and quick checking before you confirm the circuit with transistor datasheets, simulation, PCB layout review, and bench measurement.

A BJT cascode amplifier combines a common-emitter input transistor with a common-base transistor above it. The lower transistor converts the input voltage into signal current, while the upper transistor holds the lower transistor's collector voltage more nearly constant. This reduces the Miller-effect multiplication of collector-base capacitance and helps the circuit keep useful gain at higher frequencies than a simple common-emitter stage.

BJT cascode amplifier circuit diagram

What Is a BJT Cascode Amplifier?

A cascode amplifier is a two-transistor amplifier structure. In a BJT version, the input device usually works as a common-emitter stage, and the second device works as a common-base stage. The common-base device acts as a current buffer and reduces the voltage swing at the collector of the input transistor.

This arrangement is useful because the collector-base capacitance of a common-emitter transistor can appear much larger at the input due to the Miller effect. By keeping the lower transistor's collector node from moving very much, the cascode structure reduces this feedback path and improves high-frequency performance.

What This Calculator Can Help Estimate

Calculated ItemMeaningWhy It Matters
Bias currentThe DC operating current through the cascode transistor stack.Sets transconductance, small-signal gain, noise behavior, and power dissipation.
Bias voltagesThe base, emitter, and collector voltages needed to keep both BJTs in the active region.Prevents saturation or cutoff and preserves output swing.
Voltage gainThe approximate small-signal voltage gain of the cascode stage.Checks whether the selected collector load and emitter degeneration meet the gain target.
Input and output resistanceThe approximate impedance seen at the signal input and output nodes.Helps match the amplifier to the previous and next circuit stages.
Frequency responseThe estimated change in gain as frequency increases.Helps check whether the amplifier has enough bandwidth for RF, IF, video, or fast analog signals.

Common Input Parameters

InputMeaningTypical Unit
VCCPositive supply voltage for the cascode stage.V
RCCollector resistor or equivalent load resistance.Ω or kΩ
REEmitter resistance or emitter degeneration resistance in the lower transistor stage.Ω
VB1Base bias voltage for the input transistor.V
VB2Base bias voltage for the common-base cascode transistor.V
βTransistor DC current gain used for estimating base current.unitless
fTTransition frequency of the selected transistor.MHz or GHz
Load capacitanceCapacitance at the output node, including device, PCB, cable, and probe capacitance.pF

Core Cascode Amplifier Formulas

For a simplified BJT small-signal estimate at room temperature, the intrinsic emitter resistance can be approximated as:

re ≈ 26 mV / IE

where IE is the emitter current in amperes. With emitter degeneration, a simplified midband voltage gain estimate is:

Av ≈ -RC / (re + RE)

If the emitter degeneration is bypassed for AC, the midband gain becomes closer to:

Av ≈ -RC / re

These formulas are first-order estimates. Real gain depends on transistor output resistance, load resistance, bias point, device capacitances, wiring parasitics, and the impedance of the following stage.

Why the Cascode Improves Bandwidth

In a simple common-emitter amplifier, the base-collector capacitance is multiplied by voltage gain at the input. This Miller effect increases the effective input capacitance and reduces high-frequency response.

In a cascode amplifier, the common-base transistor keeps the collector of the common-emitter transistor at a nearly fixed AC voltage. Because the collector voltage moves less, the feedback through collector-base capacitance is reduced. The result is usually wider bandwidth and better isolation between input and output.

Example Calculation

Suppose a BJT cascode stage uses RC = 2.2 kΩ, IE = 2 mA, and RE = 100 Ω.

re ≈ 26 mV / 0.002 A = 13 Ω

Av ≈ -2200 Ω / (13 Ω + 100 Ω) ≈ -19.5 V/V

If the emitter resistance is bypassed for AC, the gain estimate becomes much higher:

Av ≈ -2200 Ω / 13 Ω ≈ -169 V/V

The higher calculated gain does not automatically mean the practical circuit will work better. It can reduce linearity, increase sensitivity to transistor variation, and place more demand on bandwidth, output swing, and stability.

Biasing Checklist

CheckWhat to Confirm
Lower transistor active regionThe input transistor should have enough collector-emitter voltage to avoid saturation during the full signal swing.
Upper transistor active regionThe common-base transistor also needs enough collector-emitter voltage for the desired output swing.
Base bias stabilityBias dividers or references should be stiff enough that signal current and base current do not shift the operating point too much.
Emitter currentThe selected current should support the gain and bandwidth target without exceeding power or thermal limits.
Output swingThe output node should remain inside the usable voltage range under expected signal conditions.

Advantages and Limits of Cascode Amplifiers

AdvantagePractical Meaning
Reduced Miller effectImproves high-frequency response compared with a high-gain common-emitter stage.
Good input-output isolationReduces reverse signal coupling from output to input.
High output resistanceUseful for current-source loads and high-gain analog stages.
Better wideband behaviorMakes the topology useful in RF, IF, video, and fast analog circuits.
LimitDesign Impact
More voltage headroom requiredTwo stacked transistors need enough supply voltage to keep both devices in the active region.
More biasing complexityThe upper base bias must be chosen carefully for signal swing and device operation.
Layout sensitivityAt high frequency, long leads, high-impedance nodes, and probe capacitance can dominate the result.
Not automatically stableParasitics, load capacitance, and poor decoupling can still cause peaking or oscillation.

BJT Basics for This Calculator

A bipolar junction transistor is a current-controlled semiconductor device with three terminals: base, collector, and emitter. In amplifier operation, a small base-emitter signal controls a larger collector current. The two main BJT polarities are NPN and PNP.

PNP transistor symbol

NPN transistor symbol

ItemNPN BJTPNP BJT
Usual current directionConventional collector current flows from collector to emitter.Conventional emitter current flows from emitter to collector.
Base-emitter bias for conductionBase is more positive than emitter.Base is more negative than emitter.
Emitter arrowArrow points out.Arrow points in.
Use in cascode stagesCommon in positive-supply amplifier examples.Used in complementary or negative-supply versions.

Applications of BJT Cascode Amplifiers

BJT cascode amplifiers are commonly used where a single common-emitter stage does not provide enough high-frequency performance. Typical applications include RF front ends, IF amplifiers, video amplifiers, high-speed analog stages, current-buffered gain stages, and internal gain stages of analog ICs.

How to Use This Calculator Safely

Use the calculator to estimate a starting point, then check the design against the selected transistor datasheet. Confirm maximum collector-emitter voltage, collector current, power dissipation, transition frequency, capacitances, noise requirements, and package thermal limits. For RF or fast analog circuits, include the PCB layout and measurement setup in your verification plan.

Oscilloscope probes, cables, breadboards, and long test leads can add enough capacitance and inductance to change the measured bandwidth. For high-frequency measurements, use proper probing, short grounds, controlled impedance where needed, and an output buffer if the next stage or instrument load would disturb the amplifier.

Common Mistakes to Avoid

MistakeConsequence
Using gain formulas without checking headroomThe amplifier may clip because the two stacked transistors do not have enough voltage margin.
Ignoring transistor capacitancesThe real bandwidth may be much lower than the simple resistor-based estimate.
Driving a heavy capacitive load directlyThe output may show peaking, slow response, or oscillation.
Building high-frequency prototypes on a breadboardParasitic capacitance and inductance can dominate the circuit behavior.
Forgetting temperature variationVBE, β, leakage, and bias current can shift with temperature.

FAQ

Is a cascode amplifier the same as a cascade amplifier?

No. A cascade amplifier simply connects amplifier stages in sequence. A cascode amplifier is a specific topology that combines a common-emitter or common-source stage with a common-base or common-gate stage.

Why does a cascode amplifier need more supply voltage?

The two transistors are stacked vertically in the signal path. Each transistor needs enough voltage across it to stay in the active region, so the circuit usually needs more headroom than a single-transistor common-emitter amplifier.

Can this calculator predict exact RF performance?

No. It gives useful first-order estimates, but exact RF performance depends on transistor models, PCB parasitics, layout, source and load impedance, decoupling, and measurement setup.

When should I add an output buffer?

Add a buffer when the following stage, cable, probe, or load resistance would significantly reduce gain or bandwidth. A buffer can isolate the high-impedance cascode output node from external loading.

Related Online Calculation Tools

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Op-Amp Voltage and Gain Calculator - calculates output voltage and gain for inverting and non-inverting op-amp circuits.

Ohm's Law Calculator - calculates voltage, current, resistance, and power.

Frequently Asked Questions

What parameters does the BJT Cascode Amplifier Calculator compute?

The calculator computes bias voltages (VB1/VB2/VE1/VC1/VC2), currents (IB/IC), transconductance (gm), input resistance (rπ), voltage gain (A), and frequency responses (f1/f2/BW). It uses resistor values, Beta, VBE, and capacitance inputs to determine these parameters via predefined equations .

How is the voltage gain (A) calculated when RE2 is non-zero?

If RE2 (gain control resistor) is not zero, the voltage gain is calculated as A = -(RL || RC) / RE2. This simplifies gain control by directly relating it to the ratio of load/collector resistance and RE2 .

Why is a buffer stage recommended for frequencies above 2MHz?

At frequencies >2MHz, parasitic capacitance (e.g., from scope probes) can degrade bandwidth. A buffer stage (like an emitter follower) isolates the output, preventing loading effects and maintaining frequency response accuracy during measurements .

How does the calculator account for transistor parameters like Beta and VBE?

Beta (DC current gain) and VBE (base-emitter voltage drop) are user-input values. Beta influences base current (IB = (VB1 - VBE)/(RB1 + Beta*RE)), while VBE adjusts emitter voltages (VE1 = VB1 - VBE / VE2 = VB2 - VBE) .

What design choices maximize the amplifier’s bandwidth?

Bandwidth (BW ≈ f1) is maximized by increasing the sum of RE1 and RE2. This reduces the lower pole frequency (f1 = 1/(Rin*(Cbe + 2*Ccb))/(2π)), extending the usable frequency range
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