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Question: For a CE-transistor amplifier, the audio signal voltage across the collector resistance of \[2{\text...

For a CE-transistor amplifier, the audio signal voltage across the collector resistance of 2 kΩ2{\text{ k}}\Omega is 2 V2{\text{ V}}. Suppose the current amplification factor of the transistor is 100100, find the input signal voltage and base current, if the base resistance is 1 kΩ1{\text{ k}}\Omega .

Explanation

Solution

A transistor is an arrangement in which a thin layer of one type of semiconductor is placed between two thick layers of another type of semiconductor. A device used for increasing the amplitude of variation of alternating voltage or current or power is called an amplifier. A transistor can be used as an amplifier.
In a CE-transistor amplifier, the current amplification factor is given by β=ΔIcΔIb\beta = \dfrac{{\Delta {I_c}}}{{\Delta {I_b}}} where ΔIc\Delta {I_c} is change in collector current and ΔIb\Delta {I_b} is change in base current. In a CE-transistor, the input voltage is given in base and output is received at the collector.

Complete step by step answer:
Let us first discuss transistors and an amplifier.
A transistor is an arrangement in which a thin layer of one type of semiconductor is placed between two thick layers of another type of semiconductor. A device used for increasing the amplitude of variation of alternating voltage or current or power is called an amplifier. A transistor can be used as an amplifier.
Given:
Collector resistance, Rc=2 kΩ{R_c} = 2{\text{ k}}\Omega
Base resistance, Rb=1 kΩ{R_b} = 1{\text{ k}}\Omega
Audio signal voltage across collector resistance, Vc=2 V{V_c} = 2{\text{ V}}
Current amplification factor of the transistor, β=100\beta = 100
We know that in a CE-transistor amplifier, the current amplification factor is given by β=ΔIcΔIb\beta = \dfrac{{\Delta {I_c}}}{{\Delta {I_b}}} where ΔIc\Delta {I_c} is change in collector current and ΔIb\Delta {I_b} is change in base current. In a CE-transistor, the input voltage is given in base and output is received at the collector.
Therefore the current amplification factor can be written as
β=Vc/RcVi/Rb\beta = \dfrac{{{V_c}/{R_c}}}{{{V_i}/{R_b}}} where Vi{V_i} is the input signal voltage.
On rearranging the expression we have
VcVi=βRcRb\dfrac{{{V_c}}}{{{V_i}}} = \beta \dfrac{{{R_c}}}{{{R_b}}}
On substituting the values we have
2Vi=100×21\dfrac{2}{{{V_i}}} = 100 \times \dfrac{2}{1}
So, Vi=0.01 V{V_i} = 0.01{\text{ V}}
Now, we know that
Ib=ViRb{I_b} = \dfrac{{{V_i}}}{{{R_b}}}
Substituting the values we have
Ib=0.011×103=10×106 A=10 μA{I_b} = \dfrac{{0.01}}{{1 \times {{10}^3}}} = 10 \times {10^{ - 6}}{\text{ A}} = 10{\text{ }}\mu {\text{A}}
Hence, the input signal voltage is 0.01 V0.01{\text{ V}} and the base current is 10 μA10{\text{ }}\mu {\text{A}} .

Note: A transistor acts as an amplifier as it raises the strength of a weak signal. Apart from common emitter transistors, common base transistors can also be used as an amplifier. The configuration remains in forward biased condition as the DC bias voltage is applied to the emitter base junction. But maximum amplification is done by the common emitter transistor amplifier.