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BJT NPN: Emitter, Base, Collector 

This tutorial visualizes an NPN Bipolar Junction Transistor (BJT): a thin Base (P) sandwiched between Emitter (N) and Collector (N). In active mode, the Emitter–Base junction is forward-biased and the Base–Collector junction is reverse-biased. A small base current Ib controls a large collector current Ic; most electrons injected from the Emitter are swept across the thin Base into the Collector.

 

Mathematical foundation

1. Structure

Emitter (N): High concentration of electrons. Base (P): Very thin (~10% width), moderate holes. Collector (N): Large region to collect electrons.

2. Active mode

VBE > 0.7 V forward-biases the Emitter–Base junction: electrons enter the Base. VCE > 0 reverse-biases the Base–Collector junction: the field pulls electrons into the Collector. Because the Base is thin, most electrons drift through (collector current Ic); a small fraction recombine (base current Ib).

3. Current gain

Ie = Ib + Ic (Kirchhoff). Ic = β Ib in active mode, with β (beta) the current gain. IcIe when β ≫ 1.

4. Energy bands

Two junctions: a "hill" at Emitter–Base (lowered by VBE) and a steep "cliff" at Base–Collector (driven by VCE) that sweeps electrons into the Collector.

0.70 V
5.00 V
100
0.40 Hz
Ic vs Vce (output characteristics)
Time domain (oscilloscope): Input Vbe [V] / Output Ic [mA]

 

Usage

Use the sliders and Source to explore the NPN BJT:

  1. Source: Choose DC (constant voltages), Sinusoidal, Pulse, or Triangle. The Vbe and Vce sliders set the magnitude (amplitude) for non-DC sources. The readouts show instantaneous voltages.
  2. Wave speed (Hz): For Sinusoidal, Pulse, and Triangle, this sets the frequency. Use a low value (e.g. 0.1–0.4 Hz) to see the BJT respond in slow motion.
  3. Vbe (0–1.2 V): Base–Emitter voltage. Above ~0.7 V the EB junction opens: electrons leave the Emitter and enter the Base. Below 0.5 V little current flows.
  4. Vce (0–10 V): Collector–Emitter voltage. In active mode (Vce > ~0.2 V) the BC junction pulls electrons into the Collector. Arrows show Ie, Ib, Ic (Ie = Ib + Ic).
  5. β (gain): Current gain Ic/Ib. Higher β gives more collector current for the same base current.
  6. Top canvas: Emitter (N, blue), thin Base (P, red), Collector (N, blue). Blue dots = electrons; red circles = holes in Base. Depletion regions at EB and BC. Energy band below: hill at EB, cliff at BC.
  7. Bottom canvas: Ic vs Vce for several Ib. Red dot = operating point. Saturation when Vce is small.
  8. Oscilloscope: Time-domain dual trace. Upper (yellow): Input Vbe. Lower (cyan): Output Ic. With Sinusoidal/Pulse/Triangle sources you see how the BJT amplifies or clips the signal; in Cutoff the output trace flattens.

Comparison: Diode = one PN junction; BJT = two junctions (NP and PN). Small base current controls large collector current; the thin Base lets most electrons cross to the Collector instead of recombining.

Parameters

  • Vbe: Forward bias for Emitter–Base. ~0.7 V to turn on.
  • Vce: Collector–Emitter voltage. Active when Vce > ~0.2 V.
  • β: Current gain; Ic = β Ib in active mode.
  • Energy band: EB hill (lowered by Vbe), BC cliff (Vce) sweeps electrons to Collector.

Lab trials

To help users bridge the gap between the physics animation and real-world electronics, here are four structured lab trials. These are designed to guide a beginner from basic switching logic to high-fidelity amplification.

Lab 1: The "Turn-On" Threshold (DC Analysis)

Objective: Observe the exponential nature of the BJT and find the "knee" of the curve where conduction begins.

Setup:

  • Source: DC
  • Vce: 5.0 V (Fixed)
  • Vbe: Start at 0.0 V and slowly increase.

What to Observe:

  • 0.0 V to 0.6 V: Notice the Energy Band "hill" is very high. No particles move to the Collector. Ic remains at 0.000 mA.
  • 0.65 V to 0.72 V: The blue Energy Band hill drops below the Conduction Threshold. Suddenly, particles start "spilling" into the Base.
  • Physics Insight: A tiny increase in Vbe (e.g., from 0.70 to 0.75) causes a massive explosion in particle flow. This is the Exponential Region.

Lab 2: Phase Inversion & Voltage Gain (Sinusoidal)

Objective: Visualize how a BJT acts as an amplifier and why the output "flips" upside down.

Setup:

  • Source: Sinusoidal
  • Vbe: 0.72 V (The "Bias" point)
  • AC Amplitude: 0.02 V (Small Signal)
  • Vce: 5.0 V

What to Observe:

  • Scope: Look at the relationship between the Yellow (Input) and Cyan (Output) waves.
  • Phase Shift: When the Yellow wave peaks UP, the Cyan wave peaks DOWN. This is the 180° phase inversion of the Common Emitter amplifier.
  • The LED: Notice the LED glows brightest when the Cyan Vout is at its lowest point (because low Vout means maximum Ic current is flowing through the LED/Load).

Lab 3: Finding the "Q-Point" (Biasing Lab)

Objective: Learn how to center a signal to prevent distortion (clipping).

Setup:

  • Source: Sinusoidal
  • AC Amplitude: 0.05 V (Medium Signal)
  • Vbe: Start at 0.60 V.

The Challenge:

  • At 0.60 V, you will see CUTOFF CLIPPING (the bottom of the wave is missing).
  • Slowly increase Vbe. Watch the white Q-Point dot on the oscilloscope.
  • Goal: Adjust Vbe until the Cyan wave is perfectly centered between the "Cutoff Ceiling" and "Saturation Floor."
  • Observation: This "centered" state is called Class A Biasing, providing the cleanest sound/signal.

Lab 4: The Saturation Wall (Power Limit)

Objective: Observe what happens when the collector doesn't have enough "suction" (Voltage) to handle the base current.

Setup:

  • Source: DC or Sinusoidal
  • Vbe: 0.85 V (High drive)
  • Vce: Start at 5.0 V and slowly decrease toward 0.1 V.

What to Observe:

  • Energy Bands: As Vce drops, the "cliff" on the right side of the Energy Band diagram flattens out.
  • Particle Flow: Even though Vbe is high, the particles stop "shooting" into the Collector and start lingering in the Base.
  • Scope: You will see SATURATION CLIPPING. The output wave hits a floor and can't go any lower because the transistor is "fully wide open" but out of supply voltage.

Lab 5: BJT as Switch (Pulse Train)

Objective: See the BJT act as a logic inverter: input high → output low; input low → output high.

Setup (default):

  • Source: Pulse Train
  • AC Amplitude: 0.50 V (large signal)
  • DC Offset: 0.50 V
  • Vbe: 0.00 V (wave provides 0 V low, ~1 V high)
  • Vce: 5.0 V

What to Observe:

  • Scope: Severe clipping on both top and bottom. The wave looks like a square wave, not a sine.
  • Logic: When input is High (1), output is Low (0). When input is Low (0), output is High (1). This is the Logic Inverter behavior.

Summary Table for Students

Vbe Setting Vce Setting Operating Region Use Case
< 0.6 V Any Cutoff Digital "OFF" (Switch)
0.7 – 0.8 V > 1.0 V Active Analog Music/Signal Amp
> 0.8 V < 0.3 V Saturation Digital "ON" (Switch)