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Modern Physics

Junction Transistor

A junction transistor is a three-terminal semiconductor device formed by sandwiching either a thin layer of p-type semiconductor between two n-type layers (n-p-n) or an n-type layer between two p-type layers (p-n-p). It functions primarily as a current-controlled amplifier or a solid-state switch.

UP TGT ScienceUP PGT PhysicsStudy Notes + Practice

Scope and prerequisites

TGT core

Working principle of n-p-n and p-n-p transistors, biasing conditions for active, cut-off, and saturation regions, transistor current components (I_E = I_B + I_C), and common-base (CB) and common-emitter (CE) current gains (α and β).

PGT extension

Detailed mathematical analysis of common-collector configuration, hybrid equivalent parameters (h-parameters), thermal runaway, stability factor, DC load line analysis, and transistor biasing circuits (voltage divider bias).

Prerequisites

  • Energy bands in solids and Fermi level
  • p-n junction diode forward and reverse biasing characteristics
  • Minority and majority charge carrier dynamics in semiconductors

Structural Regions of a Transistor

  • The Emitter is heavily doped to supply a large number of majority charge carriers into the base region.
  • The Base is extremely thin and lightly doped to minimize the recombination of injected charge carriers before they reach the collector.
  • The Collector is moderately doped and physically larger than the emitter and base to effectively dissipate heat generated by collecting charge carriers.

Transistor Biasing and Operating Regions

  • Active Region: Emitter-base junction is forward-biased and collector-base junction is reverse-biased; used for linear amplification.
  • Saturation Region: Both emitter-base and collector-base junctions are forward-biased; the transistor acts as a closed switch.
  • Cut-off Region: Both emitter-base and collector-base junctions are reverse-biased; the transistor acts as an open switch.

Current Components in a Transistor

  • The total emitter current (I_E) is the sum of hole and electron currents crossing the emitter-base junction.
  • A small fraction of carriers recombine in the base, constituting the base current (I_B).
  • The remaining major portion of injected carriers crosses into the collector, constituting the collector current (I_C).

Transistor Configurations

  • Common-Base (CB) Configuration: Base is common to input (emitter) and output (collector); characterized by low input impedance, high output impedance, and voltage gain with current gain (α) less than unity.
  • Common-Emitter (CE) Configuration: Emitter is common to input (base) and output (collector); characterized by moderate input impedance, moderate output impedance, and high current gain (β) greater than unity.
  • Common-Collector (CC) Configuration: Collector is common to input (base) and output (emitter); characterized by very high input impedance, very low output impedance, and voltage gain close to unity (voltage follower).

Derivations

Relation between Common-Base Current Gain (α) and Common-Emitter Current Gain (β)

Conditions: Active region operation with negligible reverse saturation leakage current (I_CBO)

  • Write the fundamental current relation for any transistor: $I_E = I_B + I_C$.
  • Define the common-base current gain as $\alpha = \Delta I_C / \Delta I_E \approx I_C / I_E$.
  • Define the common-emitter current gain as $\beta = \Delta I_C / \Delta I_B \approx I_C / I_B$.
  • Substitute $I_B = I_E - I_C into the definition of \beta: \beta = \frac{I_C}{I_E - I_C}$.
  • Divide numerator and denominator by I_E: $\beta = \frac{I_C / I_E}{1 - (I_C / I_E)}$.
  • Substitute I_C / $I_E = \alpha into the expression$ to yield the final relation.

Result: $\beta = \frac{\alpha}{1 - \alpha} \quad \text{and} \quad \alpha = \frac{\beta}{1 + \beta}$

Relation including Collector-to-Base Leakage Current (I_CEO)

Conditions: CE configuration accounting for minority carrier reverse saturation current

  • Start with the fundamental CB collector current equation: $I_C = \alpha I_E + I_CBO$.
  • Substitute $I_E = I_B + I_C into the collector current equation: I_C = \alpha (I_B + I_C) + I_CBO$.
  • Rearrange terms to collect I_C on the left side: I_C (1 - \alpha) = \alpha I_B + I_CBO.
  • Divide by (1 - α): $I_C = \frac{\alpha}{1 - \alpha} I_B + \frac{I_CBO}{1 - \alpha}$.
  • Substitute $\beta = \alpha / (1 - \alpha)$ and define $I_CEO = I_CBO / (1 - \alpha)$.

Result: $I_C = \beta I_B + I_CEO$

Formula sheet

Formula / lawEquationVariables and unitsConditions
Total Emitter Current$$I_E = I_B + I_C$$$I_E = Emitter current$, $I_B = Base current$, $I_C = Collector current$
Ampere (A)
Universal Kirchoff's law at transistor nodes
Common-Base Current Gain$$\alpha = \frac{\Delta I_C}{\Delta I_E}$$\Delta $I_C = Change in collector current$, \Delta $I_E = Change in emitter current$
Dimensionless
Constant collector-base voltage V_CB
Common-Emitter Current Gain$$\beta = \frac{\Delta I_C}{\Delta I_B}$$\Delta $I_C = Change in collector current$, \Delta $I_B = Change in base current$
Dimensionless
Constant collector-emitter voltage V_CE
Alpha-Beta Interconversion$$\beta = \frac{\alpha}{1 - \alpha}$$\alpha = CB current gain, \beta = CE current gain
Dimensionless
Active region
Collector Current with Leakage in CE$$I_C = \beta I_B + (1 + \beta) I_CBO$$$I_CBO = Open-circuit collector-base leakage current$
Ampere (A)
Common-emitter configuration
AC Voltage Gain in CE Amplifier$$A_v = \beta \left(\frac{R_L}{r_in}\right)$$$R_L = Load resistance$, $r_in = Input resistance$
Dimensionless
Small-signal low-frequency analysis
AC Power Gain$$A_p = \beta \times A_v$$$A_p = Power gain$, $A_v = Voltage gain$, \beta = Current gain
Dimensionless
CE configuration
Transistor Transconductance$$g_m = \frac{\Delta I_C}{\Delta V_{BE}} \approx \frac{I_C}{V_T}$$$V_T = Thermal voltage (\approx 26 mV at room temp)$
Siemens (S) or \Omega^{-1}
Active region, room temperature

Graphs and experiments

CB Input Characteristics

Draw: Curves of input current (I_E) versus input voltage (V_EB) for various constant values of output voltage (V_CB).

Interpret: Resemble forward-biased p-n junction diode characteristics. A change in V_CB has a negligible effect on the curves.

Exam use: Evaluates understanding of input resistance determination ($r_e = \Delta V_EB / \Delta I_E at constant V_CB)$.

CE Output Characteristics

Draw: Curves of collector current (I_C) versus collector-emitter voltage (V_CE) for different constant base currents (I_B).

Interpret: Shows three regions: active (nearly horizontal flat curves), saturation (steep rise at low V_CE), and cut-off (I_C \approx 0 when $I_B = 0)$.

Exam use: Frequently tested for identifying operating regions, load line plotting, and determining output resistance.

DC Load Line and Q-Point

Draw: A straight load line equation $I_C = -\frac{1}{R_L} V_CE + \frac{V_CC}{R_L} superimposed on the CE output characteristics intersecting the active region at the Quiescent point (Q)$.

Interpret: The Q-point defines the DC operating voltages and currents without any signal input. Proper placement ensures distortion-free amplification.

Exam use: Numerical and conceptual questions on maximum signal handling capacity and thermal stability.

Solved numericals

TGT core

In a transistor, the collector current is 2.4 mA and the base current is 0.1 mA. Find the emitter current and the current amplification factor α.

  • Use the fundamental current relation: $I_E = I_B + I_C$.
  • Substitute the given values: $I_E = 0.1 \text{ mA} + 2.4 \text{ mA} = 2.5 \text{ mA}$.
  • Calculate the current gain $\beta = I_C / I_B = 2.4 / 0.1 = 24$.
  • Calculate α using the relation $\alpha = \beta / (1 + \beta) or \alpha = I_C / I_E = 2.4 / 2.5$.

Answer: Emitter current = 2.5 mA, $\alpha = 0.96$

TGT core

The common-base current gain α of a transistor is 0.98. What is the change in collector current if the emitter current changes by 2 mA?

  • Recall the definition of common-base current gain: $\alpha = \Delta I_C / \Delta I_E$.
  • Rearrange the formula to solve for the change in collector current: \Delta $I_C = \alpha \times \Delta I_E$.
  • Substitute the given values: \Delta $I_C = 0.98 \times 2 \text{ mA}$.
  • Calculate the final product.

Answer: \Delta $I_C = 1.96 \text{ mA}$

PGT extension

A transistor connected in common-emitter mode has a current gain $\beta = 50$. The load resistance R_L is 4 kΩ, and the internal input resistance is 500 \Omega. Calculate the voltage gain and power gain of the amplifier.

  • Use the formula for voltage gain in CE mode: $A_v = \beta \times (R_L / r_{in})$.
  • Substitute the given values: $A_v = 50 \times (4000 \Omega / 500 \Omega)$.
  • Simplify the fraction: 4000 / 500 = 8.
  • Calculate voltage gain: $A_v = 50 \times 8 = 400$.
  • Calculate power gain using $A_p = \beta \times A_v: A_p = 50 \times 400 = 20000$.

Answer: Voltage gain = 400, Power gain = 20,000

Assumptions and limitations

  • Junction transistors operate under low-frequency small-signal approximations unless high-frequency hybrid-π models are employed.
  • Carrier recombination in the base is assumed constant, though it varies slightly with temperature and operating voltage.
  • Transistor parameters are treated as linear over small excursions around the operating point.

Common misconceptions

Common error: The collector current is greater than the emitter current because the collector is larger.

Correct: The emitter current is always the largest current in a transistor ($I_E = I_B + I_C)$.

The emitter supplies all carriers; some are lost in the base, so collector current must be strictly less than emitter current.

Common error: A transistor can step up power passively without an external DC power supply.

Correct: Amplification is a process of transferring a signal from a low-resistance circuit to a high-resistance circuit using DC source energy.

Conservation of energy holds; power gain is achieved by drawing DC power from the bias batteries.

Common error: The base region of a transistor should be heavily doped to facilitate current flow.

Correct: The base region is extremely lightly doped and very thin.

Light doping and small thickness minimize electron-hole recombination in the base, ensuring high collector current.

Quick revision

  • $I_E = I_B + I_C always holds true irrespective of configuration$.
  • Alpha (α) is always less than 1, whereas beta (β) is typically between 20 and 500.
  • Active region requires EB junction forward-biased and CB junction reverse-biased.

Must remember

  • The emitter is heavily doped, the base is extremely thin and lightly doped, and the collector is moderately doped and physically larger.
  • Active Region: Emitter-base junction is forward-biased and collector-base junction is reverse-biased; used for linear amplification.
  • Saturation Region: Both junctions are forward-biased; the transistor acts as a closed switch.
  • Cut-off Region: Both junctions are reverse-biased; the transistor acts as an open switch.
  • Total Emitter Current equation: $I_E = I_B + I_C$.
  • Common-Base current gain $\alpha = \frac{\Delta I_C}{\Delta I_E}$ is always less than unity.
  • Common-Emitter current gain $\beta = \frac{\Delta I_C}{\Delta I_B}$ is greater than unity.
  • Alpha-Beta interconversion formula: $\beta = \frac{\alpha}{1 - \alpha}$.
  • Collector current with leakage in CE configuration: $I_C = \beta I_B + (1 + \beta) I_CBO$.
  • Transistor transconductance in the active region is given by $g_m \approx \frac{I_C}{V_T}$.

Glossary

Emitter ($I_E$)The heavily doped region of a transistor that supplies charge carriers.
Base ($I_B$)The extremely thin and lightly doped middle region of a transistor.
Collector ($I_C$)The moderately doped and larger region that collects charge carriers.
Alpha ($\alpha$)Current gain in Common-Base configuration, defined as $\frac{\Delta I_C}{\Delta I_E}$.
Beta ($\beta$)Current gain in Common-Emitter configuration, defined as $\frac{\Delta I_C}{\Delta I_B}$.
Thermal Voltage ($V_T$)Voltage equivalent of temperature, approximately $26\text{ mV}$ at room temperature.
Transconductance ($g_m$)Ratio of change in collector current to change in base-emitter voltage.

Transistor Configurations Comparison

ParameterCommon-Base (CB)Common-Emitter (CE)Common-Collector (CC)
Input ImpedanceLowModerateVery High
Output ImpedanceHighModerateVery Low
Current GainLess than unity ($\alpha$)High ($\beta$)High ($1+\beta$)
Voltage GainHighHighClose to unity
Phase Shift$0^\circ$$180^\circ$$0^\circ$

Practice Quiz

Choose an option to reveal the explanation.

1. Which region of a junction transistor is heavily doped to supply a large number of majority charge carriers?

Explanation: The emitter is heavily doped specifically to inject a large number of majority charge carriers into the base region.

2. Why is the base region of a transistor made extremely thin and lightly doped?

Explanation: The base is thin and lightly doped so that minimum charge carriers recombine within it before successfully reaching the collector.

3. In the active region of a transistor, what are the biasing conditions for the emitter-base and collector-base junctions?

Explanation: For linear amplification (active region), the emitter-base junction is forward-biased and the collector-base junction is reverse-biased.

4. When a transistor acts as a closed switch, which operating region is it in?

Explanation: In the saturation region, both the emitter-base and collector-base junctions are forward-biased, allowing maximum current flow (closed switch).

5. Which fundamental equation correctly relates the emitter current ($I_E$), base current ($I_B$), and collector current ($I_C$)?

Explanation: By Kirchhoff's current law at transistor nodes, the total emitter current equals the sum of base current and collector current: $I_E = I_B + I_C$.

6. What is the physical significance of the Common-Base current gain $\alpha$?

Explanation: Common-base current gain $\alpha$ is defined as $\frac{\Delta I_C}{\Delta I_E}$ and is strictly less than $1$ because $I_C < I_E$.

7. If the Common-Base current gain $\alpha$ of a transistor is $0.98$, what is its Common-Emitter current gain $\beta$?

Explanation: Using the relation $\beta = \frac{\alpha}{1 - \alpha}$, we get $\beta = \frac{0.98}{1 - 0.98} = \frac{0.98}{0.02} = 49$.

8. Which configuration provides very high input impedance, very low output impedance, and a voltage gain close to unity?

Explanation: The Common-Collector configuration acts as a voltage follower, characterized by very high input impedance, low output impedance, and $A_v \approx 1$.

9. What is the corrected expression for collector current in the common-emitter configuration including leakage current $I_{CBO}$?

Explanation: The complete collector current equation in CE configuration incorporating leakage is $I_C = \beta I_B + (1 + \beta) I_{CBO}$, where $I_{CEO} = (1+\beta)I_{CBO}$.

10. What is the approximate transconductance ($g_m$) of a transistor operating at a collector current of $1\text{ mA}$ at room temperature?

Explanation: Transconductance $g_m \approx \frac{I_C}{V_T}$. With $I_C = 1\text{ mA}$ and $V_T \approx 26\text{ mV}$, $g_m \approx \frac{1\text{ mA}}{26\text{ mV}} \approx 38.46\text{ mS}$.

11. Which statement about the collector region is correct?

Explanation: The collector is moderately doped and physically larger to effectively dissipate the heat generated by collecting charge carriers.

12. When both emitter-base and collector-base junctions are reverse-biased, the transistor operates in the:

Explanation: When both junctions are reverse-biased, almost no current flows, and the transistor acts as an open switch in the cut-off region.

13. In a Common-Emitter amplifier, what is the relationship between the AC voltage gain ($A_v$) and current gain ($\beta$)?

Explanation: The AC voltage gain in a CE amplifier is given by $A_v = \beta \left(\frac{R_L}{r_{in}}\right)$, where $R_L$ is load resistance and $r_{in}$ is input resistance.

14. Which misconception about transistor currents is false?

Explanation: The statement that collector current is greater than emitter current is false; $I_E$ is always the largest current since $I_E = I_B + I_C$.

15. What is the AC power gain ($A_p$) expression in a Common-Emitter configuration?

Explanation: Power gain is the product of current gain and voltage gain, hence $A_p = \beta \times A_v$ for the CE configuration.

PYQ Patterns

These are pattern-based practice questions. Authentic year labels are only used when verified from a source.

1. In a transistor, the collector current is $15\text{ mA}$ and the base current is $1.5\text{ mA}$. What is the emitter current?

Explanation: Using $I_E = I_B + I_C$, we get $I_E = 1.5\text{ mA} + 15\text{ mA} = 16.5\text{ mA}$.

2. If the current gain $\alpha$ of a transistor is $0.96$, the collector current changes by $12\text{ mA}$ when the emitter current changes by:

Explanation: Since $\alpha = \frac{\Delta I_C}{\Delta I_E}$, we have $\Delta I_E = \frac{\Delta I_C}{\alpha} = \frac{12\text{ mA}}{0.96} = 12.5\text{ mA}$.

3. For a transistor circuit, if $\beta = 100$ and base current $I_B = 20\text{ \mu A}$, calculate the approximate collector current ignoring leakage.

Explanation: $I_C = \beta I_B = 100 \times 20\text{ \mu A} = 2000\text{ \mu A} = 2\text{ mA}$.

4. Which of the following configurations is most suitable for impedance matching when connecting a low impedance source to a high impedance load?

Explanation: Common-Collector (emitter follower) has very high input impedance and very low output impedance, making it ideal for impedance matching.

5. In a common-base amplifier circuit, the change in emitter current is $2\text{ mA}$ and the resulting change in collector current is $1.96\text{ mA}$. Calculate the current amplification factor $\alpha$.

Explanation: $\alpha = \frac{\Delta I_C}{\Delta I_E} = \frac{1.96\text{ mA}}{2\text{ mA}} = 0.98$.

6. What happens to the base current if the emitter current increases while collector current remains constant?

Explanation: From $I_B = I_E - I_C$, if $I_E$ increases while $I_C$ is constant, $I_B$ must increase.

Timed Topic Test

Attempt these questions under a ten-minute limit using a separate timer.

1. Which region in a transistor is doped moderately compared to the heavily doped emitter?

Explanation: The collector region is moderately doped, whereas the emitter is heavily doped and the base is lightly doped.

2. In a transistor operating in the active region, the reverse bias on the collector-base junction causes:

Explanation: The reverse bias on the collector-base junction creates a high resistance barrier that sweeps across the injected minority carriers, forming the collector current.

3. If $\alpha = 0.95$, what is the value of the CE current gain $\beta$?

Explanation: $\beta = \frac{\alpha}{1 - \alpha} = \frac{0.95}{1 - 0.95} = \frac{0.95}{0.05} = 19$.

4. The base current $I_B$ in a transistor is generally what percentage of the total emitter current $I_E$?

Explanation: Because the base is thin and lightly doped, only a small fraction ($1\%$ to $5\%$) of carriers recombine, making $I_B$ very small compared to $I_E$.

5. Which transistor configuration exhibits a phase reversal of $180^\circ$ between input signal voltage and output signal voltage?

Explanation: The Common-Emitter configuration inverts the output signal relative to the input, producing a $180^\circ$ phase shift.

6. Why is amplification possible in a transistor despite collector current being slightly less than emitter current?

Explanation: Amplification is achieved by transferring a signal from a low-resistance input circuit to a high-resistance output circuit, multiplying the voltage/power using DC bias energy.

7. If $I_C = 2\text{ mA}$ and $I_B = 40\text{ \mu A}$, find the Common-Emitter current gain $\beta$.

Explanation: $\beta = \frac{I_C}{I_B} = \frac{2\text{ mA}}{40\text{ \mu A}} = \frac{2000\text{ \mu A}}{40\text{ \mu A}} = 50$.

8. What is the primary role of the DC bias batteries in a transistor amplifier circuit?

Explanation: DC biasing establishes the necessary operating point (quiescent point) by properly forward-biasing the emitter-base junction and reverse-biasing the collector-base junction.

9. In the saturation region, what happens to the collector-emitter voltage ($V_{CE}$)?

Explanation: In saturation, both junctions are forward-biased, causing the collector-emitter voltage $V_{CE}$ to drop to a minimum saturation value (typically around $0.2\text{ V}$).i

10. Calculate the transconductance $g_m$ of a transistor operating with a collector current of $2.6\text{ mA}$ at room temperature ($V_T \approx 26\text{ mV}$)?

Explanation: $g_m = \frac{I_C}{V_T} = \frac{2.6\text{ mA}}{26\text{ mV}} = 0.1\text{ S}$ (or $100\text{ mS}$). Wait, let's recheck: $2.6\text{ mA} / 26\text{ mV} = 0.1\text{ S}$ which is $100\text{ mS}$. Let's verify option: $0.1\text{ S}$ is correct.