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Question: An N-P-N transistor in a common emitter mode is used as a simple voltage amplifier with a collector ...

An N-P-N transistor in a common emitter mode is used as a simple voltage amplifier with a collector current of 4mA4mA. The terminal of a 8V8V battery is connected to the collector through a load resistance RL{R_L}, and to the base through a resistance RB{R_B}. The collector emitter voltage VCE=4V{V_{CE}} = 4V, base-emitter voltage VBE=0.6V{V_{BE}} = 0.6V and base current amplification factor βdc=100{\beta _{dc}} = 100. Calculate the values of RL{R_L} and RB{R_B}.

Explanation

Solution

Apply Kirchhoff’s voltage law to calculate the resistances in the given circuit. It states that the algebraic sum of all electromotive forces and voltage drops across all the resistors is zero for a given closed loop circuit.
The base current amplification factor in common emitter mode is the ratio of collector current and base current. i.e., βdc=ICIB{\beta _{dc}} = \dfrac{{{I_C}}}{{{I_B}}}.

Complete step by step answer:
Draw the circuit containing a common-emitter mode N-P-N transistor which is used as a voltage amplifier.

It is given that the potential difference of the battery VCC=8V{V_{CC}} = 8V
The collector emitter voltage VCE=4V{V_{CE}} = 4V
The collector current IC=4mA{I_C} = 4mA
Base-emitter voltage VBE=0.6V{V_{BE}} = 0.6V
Base current amplification factor βdc=100{\beta _{dc}} = 100
Apply the KVL to the loop ABCGA, we got
ICRL+VCE=VCC{I_C}{R_L} + {V_{CE}} = {V_{CC}}
RL=VCCVCEIC\Rightarrow {R_L} = \dfrac{{{V_{CC}} - {V_{CE}}}}{{{I_C}}}
Substituting all the required values in the above equation
RL=8V4V4×103A\Rightarrow {R_L} = \dfrac{{8V - 4V}}{{4 \times {{10}^{ - 3}}A}}
Further calculate.
RL=103Ω\Rightarrow {R_L} = {10^3}\Omega
Or RL=1KΩ{R_L} = 1K\Omega
Now we know that βdc=ICIB{\beta _{dc}} = \dfrac{{{I_C}}}{{{I_B}}}
IB=ICβdc{I_B} = \dfrac{{{I_C}}}{{{\beta _{dc}}}}
Substitute the value of IC{I_C} and βdc{\beta _{dc}} in the above formula of IB{I_B}.
IB=4×103A100{I_B} = \dfrac{{4 \times {{10}^{ - 3}}A}}{{100}}
Or IB=4×105A{I_B} = 4 \times {10^{ - 5}}A
Apply the kVL to the loop CDEFGC, we got
IBRB+VBE=VCC{I_B}{R_B} + {V_{BE}} = {V_{CC}}
Simplify above equation for RB{R_B}.
RB=VCCVBEIB\Rightarrow {R_B} = \dfrac{{{V_{CC}} - {V_{BE}}}}{{{I_B}}}
Substitute all the required values in the above equation for RB{R_B}.
RB=8V0.6V4×105A\Rightarrow {R_B} = \dfrac{{8V - 0.6V}}{{4 \times {{10}^{ - 5}}A}}
RB=1.85×105Ω\Rightarrow {R_B} = 1.85 \times {10^5}\Omega
Or RB=185kΩ{R_B} = 185k\Omega
The values of RL{R_L} and RB{R_B} are 1kΩ1k\Omega and 185kΩ185k\Omega respectively.

Note: It should be noted that the emitter-base junction is forward biased and collector-base is reversed biased. The emitter current is equal to the sum of collector current and base current.