Electric Field in a BJT MCQ Quiz - Objective Question with Answer for Electric Field in a BJT - Download Free PDF

Last updated on Jun 12, 2025

Latest Electric Field in a BJT MCQ Objective Questions

Electric Field in a BJT Question 1:

Operating Frequency limitation for a Bipolar semi-conductor device is due to

  1. Junction Parasitic
  2. Electron Mobility
  3. both (1) and (2)
  4. None of above

Answer (Detailed Solution Below)

Option 3 : both (1) and (2)

Electric Field in a BJT Question 1 Detailed Solution

The correct answer is: 3) both (1) and (2)

Explanation:

  • Junction Parasitics (like capacitance and resistance at the PN junctions) slow down the switching speed of the device, especially at high frequencies.

  • Electron Mobility affects how quickly charge carriers can move through the semiconductor. Lower mobility results in slower device response, thus limiting high-frequency operation.

Both factors contribute to the frequency limitation of bipolar semiconductor devices.

Electric Field in a BJT Question 2:

Consider the npn transistor shown in figure.

F1 S.B Madhu 26.05.20 D5

Assume that one-half of the base current enters from each side of the emitter strip and flows uniformly to the center of the emitter. Assume the following parameters for the transistor:

NB = 1016 cm-3,  xB = 0.70 μm

μp = 400 cm2/V-s,  S = 8 μm

Emitter length L = 100 μm

The resistance between x = 0 and x = S/2 for the flow of base current (IB) will be ______ Ω.

Answer (Detailed Solution Below) 885 - 900

Electric Field in a BJT Question 2 Detailed Solution

The structure of the base region of the given NPN transistor is redrawn as:

F1 S.B Madhu 26.05.20 D6

The cross-sectional area of the base will be:

A = L × xB

The resistance is given by:

\(R = \frac{{\rho \ell }}{A} = \frac{\ell }{{\sigma A}}\)

σ conducting of the material given as:

σ = e μ N

μ = Mobility of the carriers

N = Number of carrier concentrations

Since the Base is of p-type, the conduction carriers will be holes, i.e.

σ = e μp NB

Now, the resistance between x = 0 to x = S/2 will be:

\(R = \frac{{S/2}}{{e{\mu _p}\;{N_B}\left( {L{x_B}} \right)}}\)

Putting the respective values, we get:

\(R = \frac{{4 \times {{10}^{ - 4}}}}{{\left( {1.6 \times {{10}^{ - 19}}} \right)\left( {400} \right)\left( {{{10}^{16}}} \right)\left( {100 \times {{10}^{ - 4}}} \right)\left( {0.7 \times {{10}^{ - 4}}} \right)}}\)

R = 893 Ω

Electric Field in a BJT Question 3:

In a uniformly doped BJT, assume that NE, NB and NC are the emitter, base and collector doping in atoms/cm3, respectively. If the emitter injection efficiency of the BJT is close to unity, which one of the following conditions is TRUE?

  1. NE = NB = NC
  2. NE ≫ NB and N< NC
  3. NE = NB and N< NC
  4. NE< NB< NC

Answer (Detailed Solution Below)

Option 2 : NE ≫ NB and N< NC

Electric Field in a BJT Question 3 Detailed Solution

The emitter injection efficiency is a measure of how efficient the emitter is in injecting electrons into the base.

It is important because the entire transistor action is due to the electrons injected into the base.

The holes, which are simultaneously injected into the emitter, are useless from this point of view.

In BJT the doping profile are related as-

NE> NC> NB

Now, as emitter injection efficiency of the BJT is close to unity we can say

NE≫ NB

Thus, NE≫ NB and N< NC

Top Electric Field in a BJT MCQ Objective Questions

In a uniformly doped BJT, assume that NE, NB and NC are the emitter, base and collector doping in atoms/cm3, respectively. If the emitter injection efficiency of the BJT is close to unity, which one of the following conditions is TRUE?

  1. NE = NB = NC
  2. NE ≫ NB and N< NC
  3. NE = NB and N< NC
  4. NE< NB< NC

Answer (Detailed Solution Below)

Option 2 : NE ≫ NB and N< NC

Electric Field in a BJT Question 4 Detailed Solution

Download Solution PDF

The emitter injection efficiency is a measure of how efficient the emitter is in injecting electrons into the base.

It is important because the entire transistor action is due to the electrons injected into the base.

The holes, which are simultaneously injected into the emitter, are useless from this point of view.

In BJT the doping profile are related as-

NE> NC> NB

Now, as emitter injection efficiency of the BJT is close to unity we can say

NE≫ NB

Thus, NE≫ NB and N< NC

Operating Frequency limitation for a Bipolar semi-conductor device is due to

  1. Junction Parasitic
  2. Electron Mobility
  3. both (1) and (2)
  4. None of above

Answer (Detailed Solution Below)

Option 3 : both (1) and (2)

Electric Field in a BJT Question 5 Detailed Solution

Download Solution PDF

The correct answer is: 3) both (1) and (2)

Explanation:

  • Junction Parasitics (like capacitance and resistance at the PN junctions) slow down the switching speed of the device, especially at high frequencies.

  • Electron Mobility affects how quickly charge carriers can move through the semiconductor. Lower mobility results in slower device response, thus limiting high-frequency operation.

Both factors contribute to the frequency limitation of bipolar semiconductor devices.

Electric Field in a BJT Question 6:

In a uniformly doped BJT, assume that NE, NB and NC are the emitter, base and collector doping in atoms/cm3, respectively. If the emitter injection efficiency of the BJT is close to unity, which one of the following conditions is TRUE?

  1. NE = NB = NC
  2. NE ≫ NB and N< NC
  3. NE = NB and N< NC
  4. NE< NB< NC

Answer (Detailed Solution Below)

Option 2 : NE ≫ NB and N< NC

Electric Field in a BJT Question 6 Detailed Solution

The emitter injection efficiency is a measure of how efficient the emitter is in injecting electrons into the base.

It is important because the entire transistor action is due to the electrons injected into the base.

The holes, which are simultaneously injected into the emitter, are useless from this point of view.

In BJT the doping profile are related as-

NE> NC> NB

Now, as emitter injection efficiency of the BJT is close to unity we can say

NE≫ NB

Thus, NE≫ NB and N< NC

Electric Field in a BJT Question 7:

Consider the npn transistor shown in figure.

F1 S.B Madhu 26.05.20 D5

Assume that one-half of the base current enters from each side of the emitter strip and flows uniformly to the center of the emitter. Assume the following parameters for the transistor:

NB = 1016 cm-3,  xB = 0.70 μm

μp = 400 cm2/V-s,  S = 8 μm

Emitter length L = 100 μm

The resistance between x = 0 and x = S/2 for the flow of base current (IB) will be ______ Ω.

Answer (Detailed Solution Below) 885 - 900

Electric Field in a BJT Question 7 Detailed Solution

The structure of the base region of the given NPN transistor is redrawn as:

F1 S.B Madhu 26.05.20 D6

The cross-sectional area of the base will be:

A = L × xB

The resistance is given by:

\(R = \frac{{\rho \ell }}{A} = \frac{\ell }{{\sigma A}}\)

σ conducting of the material given as:

σ = e μ N

μ = Mobility of the carriers

N = Number of carrier concentrations

Since the Base is of p-type, the conduction carriers will be holes, i.e.

σ = e μp NB

Now, the resistance between x = 0 to x = S/2 will be:

\(R = \frac{{S/2}}{{e{\mu _p}\;{N_B}\left( {L{x_B}} \right)}}\)

Putting the respective values, we get:

\(R = \frac{{4 \times {{10}^{ - 4}}}}{{\left( {1.6 \times {{10}^{ - 19}}} \right)\left( {400} \right)\left( {{{10}^{16}}} \right)\left( {100 \times {{10}^{ - 4}}} \right)\left( {0.7 \times {{10}^{ - 4}}} \right)}}\)

R = 893 Ω

Electric Field in a BJT Question 8:

Operating Frequency limitation for a Bipolar semi-conductor device is due to

  1. Junction Parasitic
  2. Electron Mobility
  3. both (1) and (2)
  4. None of above

Answer (Detailed Solution Below)

Option 3 : both (1) and (2)

Electric Field in a BJT Question 8 Detailed Solution

The correct answer is: 3) both (1) and (2)

Explanation:

  • Junction Parasitics (like capacitance and resistance at the PN junctions) slow down the switching speed of the device, especially at high frequencies.

  • Electron Mobility affects how quickly charge carriers can move through the semiconductor. Lower mobility results in slower device response, thus limiting high-frequency operation.

Both factors contribute to the frequency limitation of bipolar semiconductor devices.

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