ROUTERA


Semiconductor Electronics, Materials, Devices and Simple Circuits

Class 12th Physics Chapter HOTs


1. Question:

Derive the expression for the current in a forward-biased diode using Shockley’s diode equation.

Solution: The Shockley diode equation gives the current through a diode as a function of the applied voltage VV and the intrinsic properties of the diode:

I=I0(eqVkT1)I = I_0 \left( e^{\frac{qV}{kT}} - 1 \right)

Where:

  • II is the current through the diode,
  • I0I_0 is the saturation current,
  • qq is the charge of an electron,
  • VV is the applied voltage,
  • kk is the Boltzmann constant,
  • TT is the absolute temperature.

For forward bias, V>0V > 0 , and since eqVkT1e^{\frac{qV}{kT}} \gg 1 , the equation simplifies to:

II0eqVkTI \approx I_0 e^{\frac{qV}{kT}}

This represents the current in a forward-biased diode.


2. Question:

What is the significance of the energy band gap in semiconductors? Explain how it affects the conductivity of the material.

Solution: The energy band gap (EgE_g ) is the energy difference between the valence band and the conduction band of a semiconductor. In a pure semiconductor, electrons in the valence band cannot conduct electricity because they need to gain energy to jump into the conduction band.

Effect on conductivity:

  • In intrinsic semiconductors: The conductivity increases with temperature because more electrons gain enough energy to jump to the conduction band, where they can move freely and contribute to electrical conduction.
  • In extrinsic semiconductors: Doping introduces energy levels near the conduction band (in n-type) or near the valence band (in p-type), making it easier for electrons (or holes) to move.

The smaller the band gap, the higher the conductivity because less energy is required for electrons to move into the conduction band.


3. Question:

Calculate the resistance of a semiconductor diode under a forward bias of 0.7 V if the saturation current is 101210^{-12} A.

Solution: Given:

  • Forward voltage V=0.7VV = 0.7 \, \text{V} ,
  • Saturation current I0=1012AI_0 = 10^{-12} \, \text{A} ,
  • Thermal voltage VT=kTq26mVV_T = \frac{kT}{q} \approx 26 \, \text{mV} at room temperature.

Using Shockley’s diode equation:

I=I0(eVVT1)I = I_0 \left( e^{\frac{V}{V_T}} - 1 \right)

Substituting values:

I=1012(e0.70.0261)I = 10^{-12} \left( e^{\frac{0.7}{0.026}} - 1 \right)

Calculating:

I=1012(e26.921)1012×5.5×1011=5.5×101AI = 10^{-12} \left( e^{26.92} - 1 \right) \approx 10^{-12} \times 5.5 \times 10^{11} = 5.5 \times 10^{-1} \, \text{A}

The resistance RR is given by Ohm's law:

R=VI=0.70.551.27ΩR = \frac{V}{I} = \frac{0.7}{0.55} \approx 1.27 \, \Omega

4. Question:

Explain the working of a transistor as an amplifier with the help of input and output characteristics.

Solution: A transistor amplifier works by amplifying the small input signal in the base-emitter region to produce a larger output signal at the collector-emitter region.

Working:

  • In an NPN transistor, when a small AC signal is applied to the base-emitter junction, the base current (IBI_B ) causes a larger current in the collector-emitter region (ICI_C ).
  • The input characteristics show the relationship between the base-emitter voltage (VBEV_{BE} ) and the base current (IBI_B ).
  • The output characteristics show the relationship between the collector-emitter voltage (VCEV_{CE} ) and the collector current (ICI_C ).

Amplification: The current gain (β\beta ) of the transistor determines how much the input current is amplified. The output current is IC=βIBI_C = \beta I_B , and the voltage amplification depends on the load resistor and the transistor’s gain.


5. Question:

Derive the relation for the current gain of a transistor in common-emitter configuration.

Solution: The current gain (β\beta ) of a transistor in the common-emitter configuration is the ratio of the collector current ICI_C to the base current IBI_B :

β=ICIB\beta = \frac{I_C}{I_B}

Derivation:

  • In a common-emitter configuration, the total current entering the base is IBI_B , and the current leaving the collector is ICI_C .
  • The emitter current IEI_E is the sum of the collector and base currents:
IE=IC+IBI_E = I_C + I_B
  • The current gain β\beta is given by:
β=ICIB\beta = \frac{I_C}{I_B}

It is a measure of the transistor’s amplification capacity.


6. Question:

How does the depletion region in a pn-junction diode affect its behavior under reverse bias?

Solution: Under reverse bias, the external voltage pushes the electrons in the n-region and holes in the p-region away from the junction. This causes the depletion region to widen, making it more difficult for charge carriers to cross the junction. As a result, only a very small leakage current (called the reverse saturation current I0I_0 ) flows through the diode.

The depletion region essentially acts as an insulator under reverse bias, and the diode does not conduct current until the reverse voltage exceeds the breakdown voltage.


7. Question:

A p-n junction diode has a forward saturation current of 101210^{-12} A. Calculate the current through the diode when the forward voltage is 0.6 V at room temperature.

Solution: Given:

  • I0=1012AI_0 = 10^{-12} \, \text{A} ,
  • Forward voltage V=0.6VV = 0.6 \, \text{V} ,
  • Thermal voltage VT=26mVV_T = 26 \, \text{mV} .

Using the Shockley diode equation:

I=I0(eVVT1)I = I_0 \left( e^{\frac{V}{V_T}} - 1 \right)

Substituting values:

I=1012(e0.60.0261)I = 10^{-12} \left( e^{\frac{0.6}{0.026}} - 1 \right)

Calculating:

I=1012(e23.081)1012×9.56×109=9.56×103AI = 10^{-12} \left( e^{23.08} - 1 \right) \approx 10^{-12} \times 9.56 \times 10^{9} = 9.56 \times 10^{-3} \, \text{A}

8. Question:

Explain how the rectifier circuit works with a half-wave rectifier and give its efficiency.

Solution: A half-wave rectifier allows current to pass only during one half of the AC cycle. It uses a single diode to rectify the input AC voltage, converting it into pulsating DC.

Working:

  • During the positive half-cycle of the input AC voltage, the diode conducts and allows current to pass.
  • During the negative half-cycle, the diode is reverse-biased and does not conduct.

Efficiency: The efficiency (η\eta ) of a half-wave rectifier is given by:

η=PDCPAC=IDC2RIAC2R=12\eta = \frac{P_{\text{DC}}}{P_{\text{AC}}} = \frac{I_{\text{DC}}^2 R}{I_{\text{AC}}^2 R} = \frac{1}{2}

Hence, the efficiency of a half-wave rectifier is 40.6%.


9. Question:

Calculate the input resistance of a common-emitter transistor amplifier.

Solution: The input resistance of a common-emitter amplifier is the resistance seen by the signal source connected to the base of the transistor. It is given by:

Rin=(β+1β)RER_{\text{in}} = \left( \frac{\beta + 1}{\beta} \right) R_E

Where:

  • RER_E is the resistance connected in the emitter circuit,
  • β\beta is the current gain of the transistor.

The larger the value of β\beta , the higher the input resistance, as β+1β\beta + 1 \approx \beta .


10. Question:

What is the difference between intrinsic and extrinsic semiconductors?

Solution:

  • Intrinsic semiconductors: These are pure semiconductors with no impurity atoms added. The number of free charge carriers is determined solely by the properties of the material itself. Examples include silicon and germanium.
  • Extrinsic semiconductors: These are semiconductors that have been doped with impurities to increase the number of charge carriers. There are two types:
    • n-type: Doped with donor impurities that provide extra electrons.
    • p-type: Doped with acceptor impurities that create holes (missing electrons).

11. Question:

Calculate the output voltage across the load resistor in a transistor amplifier if the input signal is 2mV2 \, \text{mV} and the transistor has a current gain of 100.

Solution: Given:

  • Input signal Vin=2mVV_{\text{in}} = 2 \, \text{mV} ,
  • Current gain β=100\beta = 100 .

The output voltage VoutV_{\text{out}} is related to the input signal by the current gain:

Vout=βVin=100×2mV=200mVV_{\text{out}} = \beta V_{\text{in}} = 100 \times 2 \, \text{mV} = 200 \, \text{mV}

12. Question:

What is the principle of operation of a Zener diode in reverse bias? Explain its use as a voltage regulator.

Solution: A Zener diode is designed to operate in reverse bias. When the reverse voltage exceeds the breakdown voltage (Zener voltage), the diode conducts a significant current without damaging itself.

Voltage Regulation: Zener diodes are used as voltage regulators because they maintain a constant voltage across them. When the input voltage increases, the diode conducts and limits the output voltage to the Zener voltage. If the input voltage decreases, the diode stops conducting, maintaining a stable output.


13. Question:

Explain the formation of energy bands in solids and the difference between conductors, insulators, and semiconductors based on these bands.

Solution: The formation of energy bands in solids results from the overlapping of atomic orbitals in a crystal lattice.

  • Conductors: In conductors (like metals), the conduction band overlaps with the valence band, or the conduction band is partially filled, allowing electrons to move freely and conduct electricity.
  • Insulators: In insulators, the energy gap between the valence band and conduction band is large, so electrons cannot jump to the conduction band at room temperature.
  • Semiconductors: In semiconductors, the energy gap is small enough that at higher temperatures or with doping, electrons can move to the conduction band, allowing for conduction.

14. Question:

What is the significance of the pn-junction in semiconductor devices?

Solution: The pn-junction is the fundamental building block of many semiconductor devices, including diodes, transistors, and solar cells. It forms due to the contact between p-type and n-type materials, creating a depletion region that acts as a barrier for charge carriers.

Significance:

  • Diodes: The pn-junction allows current to flow in one direction (forward bias) and blocks it in the reverse direction (reverse bias).
  • Transistors: The pn-junctions in transistors act as switches or amplifiers depending on the configuration.
  • Solar cells: The pn-junction creates an electric field that helps separate charge carriers generated by incident light.

15. Question:

Explain the working of an LED (Light Emitting Diode).

Solution: An LED is a diode that emits light when current flows through it in the forward direction. The process is called electroluminescence.

Working:

  • When a forward bias is applied, electrons from the n-type material combine with holes in the p-type material.
  • When the electron recombines with the hole, energy is released in the form of photons, which is emitted as light.
  • The energy of the emitted photons depends on the band gap of the semiconductor material, which determines the color of the light.

16. Question:

What is the significance of doping in semiconductors?

Solution: Doping introduces impurity atoms into a semiconductor to change its electrical properties. It is the process that turns an intrinsic semiconductor into an extrinsic one.

Significance:

  • n-type doping: Donor atoms (e.g., phosphorus in silicon) provide extra electrons, making the material more conductive.
  • p-type doping: Acceptor atoms (e.g., boron in silicon) create holes, allowing the flow of charge in the opposite direction. Doping allows for the control of the carrier concentration and electrical conductivity, enabling the creation of diodes, transistors, and other semiconductor devices.

17. Question:

What is the working principle of a solar cell?

Solution: A solar cell works on the principle of the photovoltaic effect, where light energy is converted into electrical energy.

Working:

  • When sunlight strikes the surface of the solar cell, photons are absorbed by the semiconductor material (usually silicon).
  • This energy excites electrons, freeing them from atoms and generating electron-hole pairs.
  • The electric field at the pn-junction causes the electrons to move toward the n-type side and the holes toward the p-type side, creating a flow of current.

18. Question:

Discuss the working of a bipolar junction transistor (BJT) as a switch.

Solution: A bipolar junction transistor can work as a switch by applying appropriate biasing to the base-emitter and collector-emitter junctions.

Working:

  • For the transistor to be "on" (saturated): The base-emitter junction must be forward-biased, and the collector-emitter junction must be forward-biased. The transistor conducts a large current from the collector to the emitter, allowing current to pass through the load.
  • For the transistor to be "off" (cut-off): The base-emitter junction is reverse-biased, and the transistor does not conduct, effectively acting as an open switch.

19. Question:

Calculate the power dissipated in a resistor of 100Ω100 \, \Omega connected to a 12V battery.

Solution: Given:

  • Resistance R=100ΩR = 100 \, \Omega ,
  • Voltage V=12VV = 12 \, \text{V} .

Using the formula for power dissipated in a resistor:

P=V2R=122100=144100=1.44WP = \frac{V^2}{R} = \frac{12^2}{100} = \frac{144}{100} = 1.44 \, \text{W}

20. Question:

Explain the working of a photodiode.

Solution: A photodiode is a semiconductor device that converts light into electrical current. It operates in reverse bias.

Working:

  • When light strikes the photodiode, photons are absorbed by the semiconductor, generating electron-hole pairs.
  • These charge carriers are separated by the electric field at the pn-junction, generating a photocurrent.
  • The photocurrent depends on the intensity of the incident light. The reverse bias ensures that the diode does not conduct under normal conditions, except when exposed to light.

21. Question:

What is a thermistor? How does its resistance vary with temperature?

Solution: A thermistor is a type of resistor whose resistance changes significantly with temperature.

  • NTC thermistor (Negative Temperature Coefficient): As temperature increases, the resistance decreases.
  • PTC thermistor (Positive Temperature Coefficient): As temperature increases, the resistance increases.

Working: Thermistors are used in temperature sensing and temperature compensation applications.


22. Question:

Explain the behavior of an ideal diode in forward and reverse bias.

Solution:

  • Forward bias: When a diode is forward-biased (anode positive), it conducts current with minimal voltage drop (approximately 0.7V for silicon diodes).
  • Reverse bias: When a diode is reverse-biased (cathode positive), no current flows except for a small leakage current. If the reverse voltage exceeds a critical value (breakdown voltage), the diode may break down and conduct.

23. Question:

Calculate the energy band gap of a material if the current at a given temperature is 0.01 A when the applied voltage is 1 V across a p-n junction with a saturation current of 1012A10^{-12} \, \text{A} .

Solution: Using the Shockley diode equation:

I=I0(eVVT1)I = I_0 \left( e^{\frac{V}{V_T}} - 1 \right)

Solving for VTV_T using the value of current:

0.01=1012(e1VT1)0.01 = 10^{-12} \left( e^{\frac{1}{V_T}} - 1 \right)

After solving for the energy band gap (E), this yields 1.1eV1.1 \, \text{eV} .


24. Question:

Explain the working of a photoresistor and its applications.

Solution: A photoresistor (LDR) is a resistor whose resistance decreases with increasing light intensity.

Working:

  • In the presence of light, the resistance of the LDR decreases, allowing more current to pass through.
  • In the absence of light, its resistance increases, limiting the current flow.

Applications:

  • Used in light-sensitive devices such as automatic streetlights, light meters, and alarm systems.

25. Question:

Calculate the output current of a transistor amplifier if the input signal is 5mA5 \, \text{mA} and the transistor's current gain is 50.

Solution: Given:

  • Input current Iin=5mAI_{\text{in}} = 5 \, \text{mA} ,
  • Current gain β=50\beta = 50 .

The output current IoutI_{\text{out}} is:

Iout=βIin=50×5mA=250mAI_{\text{out}} = \beta I_{\text{in}} = 50 \times 5 \, \text{mA} = 250 \, \text{mA}

26. Question:

Describe the working of a junction transistor as an amplifier.

Solution: A junction transistor works as an amplifier by amplifying the current input at the base, which results in a larger output current at the collector. The relationship is given by the current gain β\beta . The transistor operates in the active region, where the base-emitter junction is forward-biased, and the collector-base junction is reverse-biased. The input signal modulates the base current, which in turn controls the larger collector current, producing an amplified output.


27. Question:

What are the advantages of using silicon over germanium in semiconductor devices?

Solution:

  • Silicon has a larger energy band gap (1.1 eV) compared to germanium (0.66 eV), which makes silicon devices more thermally stable.
  • Silicon is less sensitive to temperature changes, making it more reliable.
  • Silicon is more abundant and cheaper than germanium, making it the preferred material for semiconductor devices.

28. Question:

How does the operation of a diode in forward bias differ from reverse bias?

Solution:

  • Forward bias: In forward bias, the diode conducts current with a small voltage drop (approximately 0.7V for silicon). The current increases exponentially with voltage.
  • Reverse bias: In reverse bias, the diode blocks current, and only a small reverse saturation current flows, which is negligible unless the breakdown voltage is reached.

29. Question:

What is the role of a biasing resistor in a transistor circuit?

Solution: The biasing resistor is used to set the operating point of the transistor in a transistor amplifier or switch. It ensures that the transistor remains in the desired region of operation (active, cutoff, or saturation) and stabilizes the current flowing through the transistor to ensure proper amplification or switching performance.


30. Question:

Explain the concept of recombination in semiconductors.

Solution: Recombination occurs when an electron from the conduction band loses energy and falls back into a hole in the valence band, releasing energy in the form of heat or light. This process reduces the number of charge carriers available for conduction and is crucial in the operation of devices like LEDs and solar cells, where controlled recombination is used for light emission.