CUET UG Physics Booster Test 3- Band Theory and Intrinsic Properties
๐ Answers are locked once submitted โ results and explanations appear at the end.
QUESTION 1 OF 20
Match List I with List II regarding solid formation
| List I | List II |
|---|---|
| 1. โ Isolated atom | I. โ 8N available energy states |
| 2. โ Atoms in a solid | II. โ Energy decided by orbit |
| 3. โ Energy variation in band | III. โ Outer orbits overlap |
| 4. โ Continuous band source | IV. โ Continuous |
QUESTION 2 OF 20
The underlying reason that each electron has a different energy level forming a continuous variation is
QUESTION 3 OF 20
Correct statements about the valence band
1. It contains the energy levels of the valence electrons.
2. With no external energy, all valence electrons reside here.
3. At 0 K, it is partially filled in an intrinsic semiconductor.
4. Its top level is designated as EV.
QUESTION 4 OF 20
If the lowest level in the conduction band happens to be lower than the highest level of the valence band,
QUESTION 5 OF 20
At absolute zero, out of the 8N available energy states in a Si crystal, the number of completely unoccupied states in the upper band is:
QUESTION 6 OF 20
Incorrect statement regarding thermal excitation in intrinsic semiconductors
QUESTION 7 OF 20
Band gap comparison statements
1. The energy required to take out an electron is least for Ge, followed by Si, and highest for C.
2. Carbon has a band gap of 5.4 eV.
3. The band gap for Silicon is 0.7 eV.
4. Carbon (diamond) functions as an insulator due to its large gap.
QUESTION 8 OF 20
The energy gap between the top of the valence band and the bottom of the conduction band is essentially a region where
QUESTION 9 OF 20
For metallic conductors, the energy gap between conduction and valence bands and the corresponding electrical conductivity are respectively:
QUESTION 10 OF 20
The typical range of resistivity for a metal is:
QUESTION 11 OF 20
Consider a material with a band gap of 5.4 eV
QUESTION 12 OF 20
Correct statements regarding bound electrons in insulators
1. Electrons in the valence band all remain tightly bound.
2. No free electrons are available in the conduction band.
3. The forbidden gap completely prevents electron transitions at room temperature.
4. At room temperature, some bound electrons cross the gap easily.
QUESTION 13 OF 20
Incorrect statement about semiconducting gaps
QUESTION 14 OF 20
At room temperature, the relation governing the dynamic equilibrium of electron-hole pairs generated intrinsically is:
QUESTION 15 OF 20
The thermal energy effectively ionises only a few atoms in the crystalline lattice, which directly
QUESTION 16 OF 20
Match List I with List II regarding Si/Ge lattice
| List I | List II |
|---|---|
| 1. โ Outermost orbit of Si | I. โ 4 |
| 2. โ Outermost orbit of Ge | II. โ n = 3 |
| 3. โ Number of outer electrons per atom | III. โ Diamond-like |
| 4. โ Lattice structure type | IV. โ n = 4 |
QUESTION 17 OF 20
The mechanism of thermal energy affecting electron pairs in pure semiconductors implies
QUESTION 18 OF 20
Shared electron movement statements
1. Under an applied electric field, free electrons move completely independently as conduction electrons.
2. The electron originally set free is not involved in the process of hole motion.
3. Hole motion happens when an electron from a nearby covalent bond jumps to a vacant site.
4. The apparent movement of the hole is exactly the actual movement of a free electron.
QUESTION 19 OF 20
Suppose an intrinsic semiconductor generates a free electron current Ie of 2 mA and a hole current Ih of 1 mA under an electric field. The total current I will be:
QUESTION 20 OF 20
For an electron breaking free from a covalent bond, the charge of the free electron and the effective charge of the resulting hole are respectively:
Test Complete!
Answer Review
1 Match List I with List II regarding solid formation
| List I | List II |
|---|---|
| 1. โ Isolated atom | I. โ 8N available energy states |
| 2. โ Atoms in a solid | II. โ Energy decided by orbit |
| 3. โ Energy variation in band | III. โ Outer orbits overlap |
| 4. โ Continuous band source | IV. โ Continuous |
Isolated atoms have discrete orbit-based energies. Overlapping outer orbits form bands. Energy becomes continuous in solids.
Correct matching: Isolated atom โ Energy decided by orbit (II) Atoms in a solid โ Outer orbits overlap (III) Energy variation in band โ Continuous (IV) Continuous band source โ 8N available energy states (I)
- Option B โ Reverses isolated atom and solid properties.
- Option C โ Incorrect assignment of energy variation.
- Option D โ Incorrect matching of continuous variation.
Used
- Option Grouping
Application:
- Match fundamental concepts of band formation.
Final Logic:
- Only Option A correctly matches all entries.
"Orbit โ Overlap โ Continuous Band."
2 The underlying reason that each electron has a different energy level forming a continuous variation is
Electron surroundings differ slightly. Energy levels split into many values. Continuous bands are formed.
Inside a crystal, electrons experience slightly different surrounding charge environments. Consequently, their energies differ slightly, resulting in a very large number of closely spaced levels that form energy bands.
- Option B โ Electrons are not distributed in the nucleus.
- Option C โ The Bohr model requires modification for solids.
- Option D โ Does not explain energy-level splitting.
Used
- Direct Concept Application
Application:
- Identify the origin of continuous energy variation.
Final Logic:
- Different charge environments create different energies.
"Different Surroundings โ Different Energies."
3 Correct statements about the valence band
1. It contains the energy levels of the valence electrons.
2. With no external energy, all valence electrons reside here.
3. At 0 K, it is partially filled in an intrinsic semiconductor.
4. Its top level is designated as EV.
Valence electrons occupy the valence band. It is full at absolute zero. EV denotes the top of the valence band.
The valence band contains the energy levels occupied by valence electrons. In an intrinsic semiconductor at 0 K, it is completely filled. The highest energy level of this band is represented by EV. Statement C is incorrect because the valence band is fully occupied at 0 K.
- Option A โ Includes incorrect statement C.
- Option C โ Includes incorrect statement C.
- Option D โ Includes incorrect statement C.
Used
- Option Grouping
Application:
- Evaluate each statement separately.
Final Logic:
- Only A, B, and D are correct.
"VB Full at 0 K."
4 If the lowest level in the conduction band happens to be lower than the highest level of the valence band,
This represents band overlap. Electrons move freely. Metallic conduction becomes possible.
When the conduction band overlaps the valence band, electrons can move easily into available conduction states without requiring additional energy. This leads to high conductivity, characteristic of metals.
- Option A โ Opposite of actual behavior.
- Option B โ Band overlap implies zero or negative effective gap.
- Option C โ Energy states do not reduce this way.
Used
- Conceptual Matching
Application:
- Relate band overlap to conductivity.
Final Logic:
- Band overlap enables free electron movement.
"Overlap = Easy Conduction."
5 At absolute zero, out of the 8N available energy states in a Si crystal, the number of completely unoccupied states in the upper band is:
Total available states = 8N. 4N valence electrons occupy lower band. Upper band contains 4N empty states.
In a silicon crystal, there are 8N available energy states. At 0 K, the 4N valence electrons completely fill the lower band (valence band). Therefore, the upper band (conduction band) remains completely empty with 4N available states.
- Option A โ Upper band is not occupied.
- Option B โ Only half the correct value.
- Option D โ Total states include both bands.
Used
- Substitution
Application:
- Use the relation between available states and valence electrons.
Final Logic:
- 8N states โ 4N occupied states = 4N empty states.
"8N States, 4N Filled, 4N Empty."
6 Incorrect statement regarding thermal excitation in intrinsic semiconductors
At equilibrium, generation equals recombination. Electrons and holes are created together. Conduction band becomes partially occupied.
In thermal equilibrium, the rate of carrier generation equals the rate of recombination. Therefore, statement C is incorrect. If generation exceeded recombination continuously, carrier concentration would increase indefinitely.
- Option A โ Correct.
- Option B โ Correct.
- Option D โ Correct.
Used
- Equilibrium Principle
Application:
- Apply generation-recombination equilibrium.
Final Logic:
- At equilibrium, generation = recombination.
"Equilibrium Means Equal Rates."
7 Band gap comparison statements
1. The energy required to take out an electron is least for Ge, followed by Si, and highest for C.
2. Carbon has a band gap of 5.4 eV.
3. The band gap for Silicon is 0.7 eV.
4. Carbon (diamond) functions as an insulator due to its large gap.
Ge has the smallest gap. Diamond has the largest gap. Silicon has 1.1 eV, not 0.7 eV.
Germanium has the smallest energy gap (~0.7 eV), Silicon has ~1.1 eV, and diamond has ~5.4 eV. The large energy gap of diamond prevents thermal excitation and causes insulating behavior. Statement C is incorrect because 0.7 eV corresponds to Germanium.
- Option B โ Includes incorrect statement C.
- Option C โ Includes incorrect statement C.
- Option D โ Includes incorrect statement C.
Used
- Option Grouping
Application:
- Compare standard energy-gap values.
Final Logic:
- A, B, and D are correct.
"Ge 0.7 โ Si 1.1 โ C 5.4."
8 The energy gap between the top of the valence band and the bottom of the conduction band is essentially a region where
The gap is a forbidden region. No electron states exist there. Electrons must gain sufficient energy to cross it.
The forbidden energy gap is the region between the valence band and conduction band where no allowed electron energy states exist. Electrons must acquire energy equal to or greater than Eg to move across this region.
- Option A โ Describes energy bands.
- Option C โ Describes metals.
- Option D โ Refers to valence-band occupancy.
Used
- Direct Recall
Application:
- Recall the definition of forbidden energy gap.
Final Logic:
- No allowed states exist in the band gap.
"Forbidden Gap = No States."
9 For metallic conductors, the energy gap between conduction and valence bands and the corresponding electrical conductivity are respectively:
Bands overlap in metals. Electrons move freely. Conductivity is extremely high.
Metals have overlapping valence and conduction bands or effectively zero band gap. As a result, a large number of free electrons are available for conduction, giving metals very high conductivity.
- Option A โ Describes insulators.
- Option B โ Describes semiconductors.
- Option D โ Incorrect relationship.
Used
- Conceptual Matching
Application:
- Connect band structure to conductivity.
Final Logic:
- Overlap produces very high conductivity.
"Metal = Overlap = High Conductivity."
10 The typical range of resistivity for a metal is:
Metals have very low resistivity. Free electrons move easily. They are excellent conductors.
Metals possess very low resistivity values, typically ranging from about 10โปโธ ฮฉ m to 10โปยฒ ฮฉ m. This low resistivity results from the availability of numerous free electrons for conduction.
- Option A โ Semiconductor range.
- Option B โ Insulator range.
- Option D โ Not a standard metallic range.
Used
- Direct Recall
Application:
- Recall standard resistivity classifications.
Final Logic:
- Metals exhibit the lowest resistivity values.
"Metal = Lowest Resistivity."
11 Consider a material with a band gap of 5.4 eV
A 5.4 eV gap is extremely large. Thermal energy at room temperature is insufficient. The material behaves as an insulator.
A band gap of 5.4 eV is characteristic of diamond (carbon), which behaves as an insulator. Because the gap is very large, room-temperature thermal energy cannot excite electrons from the valence band to the conduction band.
- Option A โ Semiconductors typically have Eg < 3 eV.
- Option B โ Group IV membership does not automatically make a material metallic.
- Option D โ Such high conductivity is characteristic of good conductors, not insulators.
Used
- Substitution
Application:
- Compare the given band gap with standard material classifications.
Final Logic:
- A 5.4 eV gap prevents thermal excitation and conduction.
"5.4 eV = Diamond Insulator."
12 Correct statements regarding bound electrons in insulators
1. Electrons in the valence band all remain tightly bound.
2. No free electrons are available in the conduction band.
3. The forbidden gap completely prevents electron transitions at room temperature.
4. At room temperature, some bound electrons cross the gap easily.
Valence electrons remain bound. Conduction band remains empty. Large band gap prevents excitation.
Insulators possess a very large forbidden energy gap. As a result, electrons remain tightly bound in the valence band, the conduction band contains essentially no free electrons, and room-temperature thermal energy cannot bridge the gap. Statement D is incorrect because electrons do not cross the gap easily.
- Option B โ Includes incorrect statement D.
- Option C โ Includes incorrect statement D.
- Option D โ Includes incorrect statement D.
Used
- Option Grouping
Application:
- Evaluate each statement using insulating-band theory.
Final Logic:
- A, B, and C are correct; D is incorrect.
"Big Gap, Bound Electrons."
13 Incorrect statement about semiconducting gaps
Thermal excitation promotes electrons upward. Electrons move from valence band to conduction band. Option C reverses the process.
In semiconductors, thermal energy excites electrons from the valence band into the conduction band. Statement C incorrectly describes the direction of excitation. Although recombination can occur, thermal excitation itself is from valence to conduction band.
- Option A โ Correct semiconductor property.
- Option B โ Correct description of carrier generation.
- Option D โ Correct comparison with insulators.
Used
- Direction Check
Application:
- Verify the direction of electron excitation.
Final Logic:
- Thermal excitation occurs from valence band to conduction band.
"Electrons Go Up, Not Down."
14 At room temperature, the relation governing the dynamic equilibrium of electron-hole pairs generated intrinsically is:
Equilibrium requires balance. Carrier concentration remains constant. Generation equals recombination.
In thermal equilibrium, electron-hole pairs are continuously generated and recombined. The carrier concentration remains constant because the rate of generation equals the rate of recombination.
- Option A โ Carrier concentration would continuously increase.
- Option C โ Carrier concentration would continuously decrease.
- Option D โ Thermal generation exists at room temperature.
Used
- Equilibrium Principle
Application:
- Apply equilibrium conditions for intrinsic semiconductors.
Final Logic:
- Generation and recombination rates are equal.
"Equilibrium = Equal Rates."
15 The thermal energy effectively ionises only a few atoms in the crystalline lattice, which directly
Thermal energy breaks some covalent bonds. Free electrons are produced. Corresponding holes are created.
When thermal energy breaks a covalent bond, an electron becomes free to move in the conduction band. The bond vacancy left behind behaves as a hole. Together they form an electron-hole pair.
- Option A โ The crystal structure remains intact.
- Option B โ Band overlap does not occur.
- Option D โ Carrier generation increases conductivity.
Used
- Cause-and-Effect Analysis
Application:
- Determine the direct result of thermal ionisation.
Final Logic:
- Thermal excitation produces free electrons and holes.
"Broken Bond โ Electron + Hole."
16 Match List I with List II regarding Si/Ge lattice
| List I | List II |
|---|---|
| 1. โ Outermost orbit of Si | I. โ 4 |
| 2. โ Outermost orbit of Ge | II. โ n = 3 |
| 3. โ Number of outer electrons per atom | III. โ Diamond-like |
| 4. โ Lattice structure type | IV. โ n = 4 |
Si outer orbit โ n = 3. Ge outer orbit โ n = 4. Both have four valence electrons.
Correct matching: Outermost orbit of Si โ n = 3 (II) Outermost orbit of Ge โ n = 4 (IV) Number of outer electrons โ 4 (I) Structure type โ Diamond-like (III)
- Option B โ Reverses Si and Ge orbit numbers.
- Option C โ Incorrect electron assignment.
- Option D โ Incorrect orbit assignments.
Used
- Option Grouping
Application:
- Match lattice characteristics of Si and Ge.
Final Logic:
- Only Option A correctly matches all entries.
"Si โ 3, Ge โ 4."
17 The mechanism of thermal energy affecting electron pairs in pure semiconductors implies
Increasing temperature breaks some bonds. Electrons become free carriers. Holes are simultaneously produced.
As temperature increases, some covalent bonds acquire enough energy to break. The released electrons enter the conduction band and become mobile charge carriers.
- Option A โ Bonds can break with increasing temperature.
- Option C โ Lattice melting does not occur at room temperature.
- Option D โ Vacancies behave as positive holes.
Used
- Physical Interpretation
Application:
- Analyze the effect of temperature on covalent bonds.
Final Logic:
- Thermal energy frees some valence electrons.
"Heat Frees Electrons."
18 Shared electron movement statements
1. Under an applied electric field, free electrons move completely independently as conduction electrons.
2. The electron originally set free is not involved in the process of hole motion.
3. Hole motion happens when an electron from a nearby covalent bond jumps to a vacant site.
4. The apparent movement of the hole is exactly the actual movement of a free electron.
Free electrons conduct independently. Hole motion occurs through bond-electron shifts. Hole motion is only an apparent movement.
Free electrons move through the conduction band under an electric field. Hole motion occurs when neighboring bond electrons successively fill vacancies. The original free electron is not responsible for hole movement. Statement D is incorrect because hole motion is an apparent movement, not the actual motion of a free conduction electron.
- Option B โ Includes incorrect statement D.
- Option C โ Includes incorrect statement D.
- Option D โ Includes incorrect statement D.
Used
- Option Grouping
Application:
- Distinguish between electron conduction and hole conduction.
Final Logic:
- A, B, and C are correct.
"Hole Moves by Bond Shifting."
19 Suppose an intrinsic semiconductor generates a free electron current Ie of 2 mA and a hole current Ih of 1 mA under an electric field. The total current I will be:
Total current is the sum of both currents. Electron and hole currents contribute together. Add the magnitudes directly.
For an intrinsic semiconductor: \(I=I_{e}+I_{h}\) Given: \(I_{e}=2ย mAI_{h}=1ย mA\) Therefore, \(I=2+1=3ย mA\)
- Option A โ Incorrect sum.
- Option B โ Ignores hole current.
- Option D โ Current is not zero.
Used
- Substitution
Application:
- Apply the current relation directly.
Final Logic:
- Total current = 3 mA.
"Total Current = Electron + Hole."
20 For an electron breaking free from a covalent bond, the charge of the free electron and the effective charge of the resulting hole are respectively:
Electron carries negative charge. Hole behaves as a positive charge carrier. They are generated as a pair.
When an electron leaves a covalent bond, it carries its natural charge of โq. The vacancy left behind behaves as a positively charged hole with effective charge +q.
- Option A โ Hole is not negatively charged.
- Option B โ Electron is not positively charged.
- Option D โ Electron and hole have opposite charges.
Used
- Direct Recall
Application:
- Recall the charges of electrons and holes.
Final Logic:
- Electron = โq, Hole = +q.
"Electron Negative, Hole Positive."
