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NEET PHYSICSMedium

In the circuit shown in the figure, the input voltage ViV_i is 20 V, VBE=0V_{BE} = 0, and VCE=0V_{CE} = 0. The values of IBI_B, ICI_C and β\beta are given by:

A

IB=40 μA,IC=10 mA,β=250I_B = 40 \text{ } \mu\text{A}, I_C = 10 \text{ mA}, \beta = 250

B

IB=25 μA,IC=5 mA,β=200I_B = 25 \text{ } \mu\text{A}, I_C = 5 \text{ mA}, \beta = 200

C

IB=20 μA,IC=5 mA,β=250I_B = 20 \text{ } \mu\text{A}, I_C = 5 \text{ mA}, \beta = 250

D

IB=40 μA,IC=5 mA,β=125I_B = 40 \text{ } \mu\text{A}, I_C = 5 \text{ mA}, \beta = 125

Step-by-Step Solution

Since the exact circuit diagram is missing from the question text, we use the standard values associated with this specific NEET 2018 question: base resistance RB=500 kΩR_B = 500 \text{ k}\Omega, collector resistance RC=4 kΩR_C = 4 \text{ k}\Omega, and supply voltage VCC=20 VV_{CC} = 20 \text{ V}.

  1. For the input (base) loop: Applying Kirchhoff's voltage law: ViIBRBVBE=0V_i - I_B R_B - V_{BE} = 0 IB=ViVBERB=200500×103 ΩI_B = \frac{V_i - V_{BE}}{R_B} = \frac{20 - 0}{500 \times 10^3 \text{ } \Omega} IB=40×106 A=40 μAI_B = 40 \times 10^{-6} \text{ A} = 40 \text{ } \mu\text{A}

  2. For the output (collector) loop: Applying Kirchhoff's voltage law: VCCICRCVCE=0V_{CC} - I_C R_C - V_{CE} = 0 Assuming VCC=Vi=20 VV_{CC} = V_i = 20 \text{ V} (as per standard configurations for this problem): IC=VCCVCERC=2004×103 ΩI_C = \frac{V_{CC} - V_{CE}}{R_C} = \frac{20 - 0}{4 \times 10^3 \text{ } \Omega} IC=5×103 A=5 mAI_C = 5 \times 10^{-3} \text{ A} = 5 \text{ mA}

  3. Current Gain (β\beta): The common-emitter current gain β\beta is the ratio of collector current to base current: β=ICIB=5×103 A40×106 A\beta = \frac{I_C}{I_B} = \frac{5 \times 10^{-3} \text{ A}}{40 \times 10^{-6} \text{ A}} β=500040=125\beta = \frac{5000}{40} = 125

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