Prerequisites
Before studying this topic, make sure you understand:
- Semiconductors - p-type and n-type materials
- p-n Junction - Junction biasing concepts
- Current Electricity - Ohm’s law and circuit analysis
The Hook: What’s Inside Your Smartphone Processor?
Your smartphone processor contains over 15 BILLION transistors in an area smaller than your fingernail! Each transistor:
- Switches ON/OFF billions of times per second
- Acts as a tiny amplifier or digital switch
- Consumes less power than a grain of sand heating up
Mind-blowing scale:
- iPhone 14 Pro chip: 16 billion transistors
- All transistors switching → performing trillion operations/second
- If each transistor was 1 cm, the chip would be size of Manhattan!
How does a simple sandwich of p-n-p or n-p-n semiconductors create the brain of modern civilization? Let’s decode the most important invention of the 20th century!
Interactive Demo
Visualize transistor amplification and switching action:
The Core Concept: What is a Transistor?
Transistor = Transfer Resistor
Name origin:
- Transfer + Resistor = Transistor
- Small current in input transfers to large current in output
- Acts like current-controlled resistor
Two p-n Junctions Back-to-Back
Bipolar Junction Transistor (BJT) has two types:
1. npn Transistor:
C (Collector)
|
n
|
p ←— B (Base)
|
n
|
E (Emitter)
2. pnp Transistor:
C (Collector)
|
p
|
n ←— B (Base)
|
p
|
E (Emitter)
Three regions:
- Emitter (E): Heavily doped, emits charge carriers
- Base (B): Very thin (~1 µm), lightly doped
- Collector (C): Moderately doped, collects carriers
Single p-n junction (diode):
- Current flows one way
- Can’t amplify
Two junctions (transistor):
- Base-Emitter (BE): Forward biased (allows current)
- Base-Collector (BC): Reverse biased (normally blocks)
- Magic: Carriers from emitter cross thin base into collector
- Small base current controls large collector current!
Think of it like:
- Water dam with small control valve (base)
- Tiny adjustment → huge water flow change (collector)
- Current amplification!
Transistor Action (npn)
Biasing for Active Mode
Proper biasing:
- BE junction: Forward biased (VBE ≈ 0.7V)
- BC junction: Reverse biased (VCB > 0)
Current Flow Mechanism
Step 1: Electrons injected from emitter (heavily doped n-type)
Step 2: Enter thin p-type base
- Some recombine with holes → small base current $I_B$
- Most (>95%) continue through thin base
Step 3: Reach reverse-biased BC junction
- Collector electric field pulls them in
- Creates collector current $I_C$
Result:
$$\boxed{I_E = I_B + I_C}$$where:
- $I_E$ = emitter current (largest)
- $I_C$ = collector current (~99% of $I_E$)
- $I_B$ = base current (~1% of $I_E$)
Current Gain Parameters
1. Current Gain (β or $h_{FE}$):
$$\boxed{\beta = \frac{I_C}{I_B}}$$Typical values: β = 50 to 300
This is the amplification factor!
2. Alpha (α):
$$\boxed{\alpha = \frac{I_C}{I_E}}$$Typical: α ≈ 0.95 to 0.99
Relationship:
$$\boxed{\beta = \frac{\alpha}{1-\alpha}}$$ $$\boxed{\alpha = \frac{\beta}{\beta + 1}}$$Example: β = 100
Input: Base current $I_B = 10$ µA (tiny!)
Output: Collector current $I_C = \beta I_B = 100 \times 10 = 1000$ µA = 1 mA
Amplification = 100×!
Power perspective:
- Small base power controls large collector power
- Like tiny steering wheel controlling massive truck
- This is how transistors amplify signals!
In your smartphone:
- Microphone signal: ~millivolts
- After transistor amplification: volts
- You can hear music clearly through speakers!
Transistor Configurations
1. Common Emitter (CE) - Most Important
Circuit:
VCC
|
RC
|
C ──┴── Vout
Input ──┤ npn
│
E ──┬── GND
|
RE
Characteristics:
- Input: Between base and emitter
- Output: Between collector and emitter
- Emitter is common to both
Properties:
| Parameter | Value |
|---|---|
| Current gain | High (β) |
| Voltage gain | High (~100) |
| Power gain | Very high |
| Phase shift | 180° (inverted) |
| Input resistance | Medium (~1 kΩ) |
| Output resistance | High (~50 kΩ) |
Use: Voltage amplifiers (most common!)
2. Common Collector (CC) - Emitter Follower
Properties:
- Voltage gain ≈ 1 (no amplification)
- Current gain = High
- Output follows input (no inversion)
- Low output impedance
Use: Impedance matching, buffer
3. Common Base (CB)
Properties:
- Current gain < 1 (no current amplification)
- Voltage gain = High
- No phase inversion
- Very low input impedance
Use: High-frequency applications, RF amplifiers
For JEE: Focus on Common Emitter - most important and frequently asked!
Common Emitter Amplifier
Circuit Analysis
DC Analysis (Biasing):
Base voltage:
$$V_B = \frac{R_2}{R_1 + R_2} V_{CC}$$Emitter voltage:
$$V_E = V_B - V_{BE}$$where $V_{BE} \approx 0.7$ V for Si
Emitter current:
$$I_E = \frac{V_E}{R_E}$$Collector current:
$$I_C \approx I_E$$(since α ≈ 1)
Collector voltage:
$$V_C = V_{CC} - I_C R_C$$AC Analysis (Small Signal):
Voltage gain:
$$\boxed{A_v = -\frac{R_C}{r_e}}$$where:
- $r_e$ = dynamic emitter resistance ≈ $\frac{26 \text{ mV}}{I_E}$ at 300K
- Negative sign indicates phase inversion
Alternative form:
$$\boxed{A_v = -\frac{\beta R_C}{R_i}}$$Current gain:
$$\boxed{A_i = \beta}$$Power gain:
$$\boxed{A_p = A_v \times A_i = \beta \times \frac{R_C}{r_e}}$$Input and Output Characteristics
Input characteristic (VBE vs IB):
- Similar to diode curve
- Exponential rise after 0.7V
- Controls base current
Output characteristic (VCE vs IC):
- Shows three regions:
1. Cut-off region: $I_B = 0$, $I_C \approx 0$ (OFF)
2. Active region: $I_C = \beta I_B$ (linear amplification)
3. Saturation region: $V_{CE} < 0.2$ V (fully ON)
When you play music on your phone:
Input: Microphone or audio file → tiny AC signal (~mV)
Transistor amplifier:
- Operating point set in active region
- Small input signal varies base current
- Collector current varies by β times
- Output voltage varies across $R_C$
Output: Amplified signal (~V) drives speaker
Multiple stages: Typical phone has 2-3 amplifier stages
- Each stage amplifies by ~100×
- Total gain: $100 \times 100 = 10,000×$!
- Millivolt input → Volt-level output → Audible sound!
Transistor as a Switch
Digital Switching
Transistor can work in two extreme states:
1. OFF State (Cut-off):
- $I_B = 0$
- $I_C = 0$
- $V_{CE} = V_{CC}$ (maximum)
- Acts like open switch
2. ON State (Saturation):
- $I_B$ > minimum value
- $I_C = I_{C,sat} = \frac{V_{CC}}{R_C}$
- $V_{CE,sat} \approx 0.2$ V (minimum)
- Acts like closed switch
Switching Circuit
VCC
|
RC
|
C ──┴── Vout
Input ──┤ npn
│
E ──┴── GND
Operation:
Input LOW (0V):
- $I_B = 0$
- Transistor OFF
- $V_{out} = V_{CC}$ (HIGH)
Input HIGH (5V):
- $I_B > 0$
- Transistor ON (saturated)
- $V_{out} \approx 0$ V (LOW)
Notice: Output is inverted from input!
This is a NOT gate (inverter)!
Calculating Base Resistor
To ensure saturation:
$$I_B > \frac{I_{C,sat}}{\beta}$$Base current:
$$I_B = \frac{V_{in} - V_{BE}}{R_B}$$For saturation:
$$\boxed{R_B < \frac{(V_{in} - V_{BE}) \beta}{I_{C,sat}}}$$Typically choose: $R_B = \frac{(V_{in} - V_{BE}) \beta}{2 I_{C,sat}}$ (provides margin)
Every logic gate in your processor is made of transistors as switches!
NAND gate: 4 transistors NOR gate: 4 transistors Complex CPU: Billions of transistors switching!
Example - Intel Core i9:
- 16 billion transistors
- Each switches billions of times/second
- Switching speed: < 100 picoseconds (10⁻¹⁰ s)!
- All performing binary logic: 0s and 1s
Power consumption:
- Each transistor uses ~femtojoules per switch
- 16 billion × billions of switches/sec = ~100 watts
- This is why CPUs need cooling fans!
From transistors to Instagram: Binary switches → Logic gates → Processors → Smartphones → Your entire digital life!
Important Formulas Summary
Current Relations
$$\boxed{I_E = I_B + I_C}$$ $$\boxed{\beta = \frac{I_C}{I_B}} \quad \text{(50-300)}$$ $$\boxed{\alpha = \frac{I_C}{I_E}} \quad \text{(0.95-0.99)}$$ $$\boxed{\alpha = \frac{\beta}{\beta+1}}$$CE Amplifier
$$\boxed{A_v = -\frac{R_C}{r_e}} \quad \text{where } r_e = \frac{26 \text{ mV}}{I_E}$$ $$\boxed{A_i = \beta}$$ $$\boxed{A_p = A_v \times A_i}$$Switching
$$\boxed{I_{C,sat} = \frac{V_{CC}}{R_C}}$$ $$\boxed{V_{CE,sat} \approx 0.2 \text{ V}}$$Memory Tricks & Patterns
Mnemonic for npn vs pnp
“npn - Not Pointing iN” - Arrow points OUT “pnp - Pointing iN Permanently” - Arrow points IN
(Arrow is on emitter)
Current Relationship
“Every Base and Collector makes Emitter”
$$I_E = I_B + I_C$$Beta Memory
“Beta is Big, Alpha Almost 1”
- β = 50-300 (large)
- α = 0.95-0.99 (close to 1)
CE Amplifier Sign
“CE Causes inversion” - Common Emitter has negative voltage gain (180° phase shift)
Transistor Regions
“Cut-off is Closed, Saturation is Short”
- Cut-off: Like open circuit (no current)
- Saturation: Like short circuit (full current)
- Active: In between (amplification)
Pattern Recognition
Current magnitudes:
$$I_E > I_C >> I_B$$Typical: If $I_B = 10$ µA, then $I_C \approx 1$ mA, $I_E \approx 1.01$ mA
Voltage drops:
- $V_{BE} \approx 0.7$ V (forward-biased junction)
- $V_{CE,sat} \approx 0.2$ V (in saturation)
- $V_{CE,cutoff} \approx V_{CC}$ (in cut-off)
Dynamic resistance:
$$r_e(\Omega) = \frac{26 \text{ mV}}{I_E(\text{mA})}$$At $I_E = 1$ mA: $r_e = 26$ Ω
When to Use This
Transistor as amplifier when:
- Need voltage/current/power gain
- Analog signal processing
- Operating in active region
- Small signal variations around DC operating point
Transistor as switch when:
- Digital circuits (logic gates)
- ON/OFF control (LED, relay)
- Operating in saturation (ON) or cut-off (OFF)
- No intermediate states needed
For problem solving:
Given circuit, find gain: → Identify configuration (CE/CB/CC) → Use appropriate gain formulas
Given switching circuit: → Check if transistor in saturation or cut-off → Calculate currents and voltages accordingly
Current amplification: → Use $\beta = I_C/I_B$
Common Mistakes to Avoid
Wrong: Using npn formulas for pnp circuit
Correct:
- npn: Conventional current flows C→E, base current is positive
- pnp: Conventional current flows E→C, all polarities reversed
Easy identification:
- Arrow on emitter pointing OUT → npn
- Arrow pointing IN → pnp
For JEE: Most problems use npn (standard convention)
Wrong: “If base voltage is 2V, emitter voltage is 2V”
Correct:
$$V_E = V_B - V_{BE} = 2 - 0.7 = 1.3 \text{ V}$$Always subtract 0.7V for Si transistor (0.3V for Ge)
Common JEE error: Calculating emitter current without accounting for $V_{BE}$
Wrong: “In saturation, $I_C = \beta I_B$”
Correct:
- Active region: $I_C = \beta I_B$ ✓
- Saturation: $I_C < \beta I_B$ (limited by $R_C$)
In saturation:
$$I_C = I_{C,sat} = \frac{V_{CC} - V_{CE,sat}}{R_C} \approx \frac{V_{CC}}{R_C}$$Not dependent on β!
JEE trap: “Find IC when transistor is saturated” - don’t use β formula!
Wrong: “All amplifiers invert signal”
Correct:
- CE amplifier: 180° phase shift (inverted)
- CC amplifier: 0° phase shift (no inversion)
- CB amplifier: 0° phase shift (no inversion)
Remember: Only Common Emitter inverts!
Negative sign in formula:
$$A_v = -\frac{R_C}{r_e}$$The minus means inversion!
Practice Problems
Level 1: Foundation (NCERT/Basic)
A transistor has $\beta = 100$. If base current is 50 µA, find: (a) Collector current (b) Emitter current
Solution:
(a) Collector current:
$$I_C = \beta I_B = 100 \times 50 \times 10^{-6}$$ $$I_C = 5 \times 10^{-3} \text{ A} = 5 \text{ mA}$$(b) Emitter current:
$$I_E = I_B + I_C = 0.05 + 5 = 5.05 \text{ mA}$$Answer: (a) 5 mA, (b) 5.05 mA
Insight: Emitter current only slightly larger than collector current!
For the above transistor, find α.
Solution:
$$\alpha = \frac{\beta}{\beta + 1} = \frac{100}{100 + 1} = \frac{100}{101} = 0.99$$Or directly:
$$\alpha = \frac{I_C}{I_E} = \frac{5}{5.05} = 0.99$$Answer: α = 0.99
Insight: α very close to 1 for good transistor!
Level 2: JEE Main
A CE amplifier has $R_C = 2$ kΩ and transistor operating at $I_E = 2$ mA. Find voltage gain.
Solution:
Dynamic emitter resistance:
$$r_e = \frac{26 \text{ mV}}{I_E(\text{mA})} = \frac{26}{2} = 13 \text{ Ω}$$Voltage gain:
$$A_v = -\frac{R_C}{r_e} = -\frac{2000}{13} = -154$$Answer: $A_v = -154$ (magnitude 154, inverted phase)
Insight: Negative sign means 180° phase shift!
A transistor switch has $V_{CC} = 12$V, $R_C = 1$ kΩ. Find: (a) Collector current in saturation (b) Minimum base current needed if β = 80
Solution:
(a) Saturation collector current:
$$I_{C,sat} = \frac{V_{CC}}{R_C} = \frac{12}{1000} = 0.012 \text{ A} = 12 \text{ mA}$$(b) Minimum base current:
For saturation:
$$I_B > \frac{I_{C,sat}}{\beta} = \frac{12}{80} = 0.15 \text{ mA}$$Practical design (2× margin):
$$I_B = \frac{2 \times 12}{80} = 0.3 \text{ mA}$$Answer:
- (a) 12 mA
- (b) Minimum 0.15 mA, recommended 0.3 mA
Insight: Provide extra base current to ensure hard saturation!
In a CE amplifier, $V_{CC} = 12$V, $R_C = 3$ kΩ, $I_C = 2$ mA. Find: (a) $V_C$ (b) $V_{CE}$ if $V_E = 1$V
Solution:
(a) Collector voltage:
$$V_C = V_{CC} - I_C R_C$$ $$V_C = 12 - (2 \times 10^{-3})(3 \times 10^3)$$ $$V_C = 12 - 6 = 6 \text{ V}$$(b) Collector-emitter voltage:
$$V_{CE} = V_C - V_E = 6 - 1 = 5 \text{ V}$$Answer: (a) 6V, (b) 5V
Check: $V_{CE} = 5$V > 0.2V → Transistor in active region ✓
Level 3: JEE Advanced
A CE amplifier has voltage divider bias: $R_1 = 10$ kΩ, $R_2 = 2.2$ kΩ, $R_E = 1$ kΩ, $R_C = 2.2$ kΩ, $V_{CC} = 12$V. Find: (a) Operating point $(I_C, V_{CE})$ (b) Voltage gain
Solution:
(a) DC analysis:
Base voltage:
$$V_B = \frac{R_2}{R_1 + R_2} V_{CC} = \frac{2.2}{10 + 2.2} \times 12$$ $$V_B = \frac{2.2}{12.2} \times 12 = 2.16 \text{ V}$$Emitter voltage:
$$V_E = V_B - V_{BE} = 2.16 - 0.7 = 1.46 \text{ V}$$Emitter current:
$$I_E = \frac{V_E}{R_E} = \frac{1.46}{1000} = 1.46 \text{ mA}$$Collector current:
$$I_C \approx I_E = 1.46 \text{ mA}$$Collector voltage:
$$V_C = V_{CC} - I_C R_C = 12 - (1.46 \times 2.2)$$ $$V_C = 12 - 3.21 = 8.79 \text{ V}$$VCE:
$$V_{CE} = V_C - V_E = 8.79 - 1.46 = 7.33 \text{ V}$$Operating point: $(1.46 \text{ mA}, 7.33 \text{ V})$
(b) AC analysis:
$$r_e = \frac{26}{1.46} = 17.8 \text{ Ω}$$ $$A_v = -\frac{R_C}{r_e} = -\frac{2200}{17.8} = -124$$Answer:
- (a) Q-point: (1.46 mA, 7.33V)
- (b) $A_v = -124$
Insight: Well-designed bias point near middle of load line for maximum swing!
Show that for a transistor, $\beta = \alpha/(1-\alpha)$.
Solution:
Starting from definitions:
$$\alpha = \frac{I_C}{I_E}, \quad \beta = \frac{I_C}{I_B}$$Also: $I_E = I_B + I_C$
$$\alpha = \frac{I_C}{I_B + I_C} = \frac{I_C/I_B}{I_B/I_B + I_C/I_B}$$ $$\alpha = \frac{\beta}{1 + \beta}$$Solving for β:
$$\alpha(1 + \beta) = \beta$$ $$\alpha + \alpha\beta = \beta$$ $$\alpha = \beta - \alpha\beta = \beta(1 - \alpha)$$ $$\boxed{\beta = \frac{\alpha}{1-\alpha}}$$Check: If $\alpha = 0.99$:
$$\beta = \frac{0.99}{1-0.99} = \frac{0.99}{0.01} = 99$$✓
Proved!
Insight: Small change in α causes large change in β!
- α: 0.98 → 0.99 (1% change)
- β: 49 → 99 (100% change!)
This is why β varies widely between transistors!
Quick Revision Box
| Parameter | Formula | Typical Value |
|---|---|---|
| Current gain (β) | $I_C/I_B$ | 50-300 |
| Alpha (α) | $I_C/I_E$ | 0.95-0.99 |
| $V_{BE}$ | - | 0.7V (Si) |
| $V_{CE,sat}$ | - | 0.2V |
| CE voltage gain | $-R_C/r_e$ | -100 to -500 |
| $r_e$ | $26\text{mV}/I_E$ | 10-50Ω |
Key relation: $I_E = I_B + I_C$, $\beta = \alpha/(1-\alpha)$
JEE Strategy: High-Yield Points
Current relations - Most common!
- $I_E = I_B + I_C$
- $\beta = I_C/I_B$
- $\alpha = I_C/I_E$
- Conversion: $\beta = \alpha/(1-\alpha)$
Transistor configurations:
- Identify CE/CB/CC from circuit
- Remember: CE inverts, others don’t
- CE most commonly asked!
DC biasing calculations:
- Always use $V_{BE} = 0.7$V
- $V_E = V_B - 0.7$
- $I_E = V_E/R_E$
- $I_C \approx I_E$
CE amplifier gain:
- $r_e = 26\text{mV}/I_E(\text{mA})$
- $A_v = -R_C/r_e$
- Negative sign = phase inversion
Switching operation:
- Cut-off: $I_B = 0$, $V_{CE} = V_{CC}$
- Saturation: $V_{CE} = 0.2$V, $I_C = V_{CC}/R_C$
- Don’t use $\beta$ in saturation!
Conceptual questions:
- “Why base thin?” → Most carriers reach collector
- “Why emitter heavily doped?” → Inject many carriers
- “Active vs saturation?” → Check $V_{CE}$ value
Time-saving tricks:
- For β = 100: $I_C \approx 100 I_B$
- For $I_E$: $I_E \approx I_C$ (α ≈ 1)
- In saturation: $V_{CE} \approx 0$ (short circuit)
- In cut-off: $I_C \approx 0$ (open circuit)
Related Topics
Within Electronic Devices
- Semiconductors - p-n junction basics
- p-n Junction - Understanding junctions
- Logic Gates - Transistors as digital switches
Connected Chapters
- Current Electricity - Circuit analysis
- Magnetism - Hall effect in semiconductors
Real-world Applications
- Amplifiers - Audio, RF, instrumentation
- Switches - Digital logic, power control
- Oscillators - Signal generation
- Processors - Billions in CPU/GPU
- Memory - RAM, Flash storage
Teacher’s Summary
Transistor = Two p-n junctions back-to-back (npn or pnp)
- Emitter (heavily doped) → Base (thin) → Collector (moderate)
- BE forward biased, BC reverse biased for active operation
Current amplification: $\beta = I_C/I_B$ (typically 50-300)
- Small base current controls large collector current
- $I_E = I_B + I_C$ (Kirchhoff’s law)
- $\alpha = I_C/I_E \approx 0.99$ (most carriers reach collector)
As amplifier (Active region):
- Common Emitter most important
- Voltage gain: $A_v = -R_C/r_e$ where $r_e = 26\text{mV}/I_E$
- Phase inverted (180°)
- Used in audio, RF, instrumentation
As switch (Cut-off/Saturation):
- Cut-off: $I_B = 0$ → transistor OFF → $V_{CE} = V_{CC}$
- Saturation: $I_B$ large → transistor ON → $V_{CE} \approx 0.2$V
- Foundation of digital logic gates
15 billion transistors in your smartphone processor - each a tiny amplifier or switch, working together to create the digital world!
“From a simple sandwich of doped silicon to the brain of civilization - the transistor is humanity’s most important invention after the wheel!”