CUET UG Physics Booster Test 2- Band Theory and Intrinsic Properties
π Answers are locked once submitted β results and explanations appear at the end.
QUESTION 1 OF 20
The formation of energy bands in solids instead of discrete energy levels
QUESTION 2 OF 20
Each electron in a crystal has a unique position and surrounding charge pattern,
QUESTION 3 OF 20
Valence band characteristics statements
Valence band characteristics statements
A. It includes the energy levels of the valence electrons.
B. It is completely occupied at absolute zero temperature.
C. It is always partially empty in insulators.
D. Its highest energy level is denoted as EV.
QUESTION 4 OF 20
Incorrect statement about the conduction band
QUESTION 5 OF 20
If N is the number of atoms in a Si crystal, the total number of outer electrons occupying the lower band at absolute zero is:
QUESTION 6 OF 20
With thermal excitation, electrons move to the conduction band and create vacancies in the valence band. The conduction particles are respectively:
QUESTION 7 OF 20
What is the respective energy gap value for Silicon and Germanium?
QUESTION 8 OF 20
Match List I (Gap Description) with List II (Condition)
| List I | List II |
|---|---|
| 1. Eg > 3 eV | I. Metal (Sn) |
| 2. Eg = 0 | II. Silicon |
| 3. Eg β 1.1 eV | III. Germanium |
| 4. Eg β 0.7 eV | IV. Insulator |
QUESTION 9 OF 20
Correct statements about metalsCorrect statements about metals
A. Conduction band is partially filled.
B. Valence band is partially empty.
C. Conduction and valence bands may overlap.
D. Thermal excitation is required to create an overlap.
QUESTION 10 OF 20
The resistance of metallic materials is low because
A. the energy gap is strictly larger than 3 eV
B. electrons from the valence band can easily move into the conduction band due to overlap
C. thermal excitation ionises all the core atoms
D. holes move freely in the conduction band
QUESTION 11 OF 20
In insulators, the energy gap is large. Consequently
QUESTION 12 OF 20
Insulator conduction statements
Insulator conduction statements
A. There are no electrons in the conduction band.
B. No electrical conduction is possible.
C. Energy gap is so large that thermal excitation cannot bridge it.
D. Holes provide high conductivity in insulators.
QUESTION 13 OF 20
The approximate energy gap for Silicon is:
QUESTION 14 OF 20
Incorrect statement about semiconductors at room temperature
QUESTION 15 OF 20
Match List I (Symbol) with List II (Meaning) in intrinsic semiconductors
| List I | List II |
|---|---|
| 1. ne | I. Total current |
| 2. nh | II. Intrinsic carrier concentration |
| 3. ni | III. Free electron concentration |
| 4. I | IV. Hole concentration |
QUESTION 16 OF 20
In the diamond-like structure of pure Silicon, the number of valence electrons per atom and the number of nearest neighbours are respectively:
QUESTION 17 OF 20
The two shared electrons in a covalent bond can be assumed to
QUESTION 18 OF 20
Correct statements about covalent bonds in Si/Ge
Correct statements about covalent bonds in Si/Ge
A. At low temperatures, an idealised picture shows all bonds intact.
B. As temperature increases, no bonds can be broken.
C. Shared electrons form a valence bond.
D. Each atom takes a share of one electron from each of its four neighbours.
QUESTION 19 OF 20
What is the effective charge of the vacancy (hole) created when an electron breaks away from a covalent bond?
QUESTION 20 OF 20
The total current I in an intrinsic semiconductor is given by the sum of electron current (Ie) and hole current (Ih) as:
Test Complete!
Answer Review
1 The formation of energy bands in solids instead of discrete energy levels
Atoms in solids are closely packed. Outer electron orbits overlap. Energy levels split into bands.
In a solid, atoms are packed very closely together. As a result, the outer electron orbits of neighboring atoms overlap. This overlap causes the discrete energy levels of isolated atoms to split into a very large number of closely spaced energy levels, forming energy bands.
- Option A β Atoms in solids are not far apart.
- Option C β Electrons experience different surrounding charge patterns.
- Option D β Electron motion in solids differs from isolated atoms.
Used
- Contextual/Tonal Matching
Application:
- Identify the physical cause of energy-band formation.
Final Logic:
- Overlapping outer orbits produce energy bands.
"Orbit Overlap β Energy Bands."
2 Each electron in a crystal has a unique position and surrounding charge pattern,
Electrons experience different surroundings. Energy levels split slightly. Continuous bands are formed.
Inside a crystal, no two electrons experience exactly the same surrounding charge distribution. Consequently, their energies differ slightly. These numerous closely spaced energy levels merge into continuous energy bands.
- Option A β Many energy levels are formed.
- Option B β Energy levels do not disappear.
- Option D β Inner core levels do not overlap with the valence band.
Used
- Direct Concept Application
Application:
- Relate electron surroundings to energy-level splitting.
Final Logic:
- Different environments create different energy levels.
"Different Charges β Different Energies."
3 Valence band characteristics statements
Valence band characteristics statements
A. It includes the energy levels of the valence electrons.
B. It is completely occupied at absolute zero temperature.
C. It is always partially empty in insulators.
D. Its highest energy level is denoted as EV.
Valence electrons occupy the valence band. It is full at 0 K. EV denotes the top of the valence band.
The valence band contains the energy levels occupied by valence electrons. At absolute zero temperature, it is completely filled. The highest energy level of the valence band is represented by EV. Statement C is incorrect because in insulators the valence band is completely filled, not partially empty.
- Option A β Includes incorrect statement C.
- Option C β Includes incorrect statement C.
- Option D β Includes incorrect statement C.
Used
- Option Grouping
Application:
- Evaluate each statement individually.
Final Logic:
- Only A, B, and D are correct.
"Valence Band: Full at 0 K."
4 Incorrect statement about the conduction band
Conduction band is above the valence band. It is empty at 0 K in semiconductors. EC denotes its lower edge.
For semiconductors at absolute zero, the conduction band is empty because no electrons possess enough energy to enter it. Therefore, stating that it is completely filled is incorrect.
- Option A β Correct definition.
- Option C β EC denotes the conduction-band minimum.
- Option D β Band overlap enables conduction in metals.
Used
- Elimination
Application:
- Identify the statement inconsistent with band occupancy.
Final Logic:
- The conduction band is empty at 0 K.
"0 K β Empty Conduction Band."
5 If N is the number of atoms in a Si crystal, the total number of outer electrons occupying the lower band at absolute zero is:
Each Si atom contributes 4 valence electrons. At 0 K all remain in the valence band. Total electrons = 4N.
A silicon atom possesses four valence electrons. Therefore, N silicon atoms contribute 4N valence electrons. At absolute zero, all of these electrons occupy the lower energy band (valence band).
- Option A β Too few electrons.
- Option B β Does not match silicon valency.
- Option D β Represents available states, not electrons.
Used
- Substitution
Application:
- Multiply the number of atoms by four valence electrons.
Final Logic:
- N atoms Γ 4 valence electrons = 4N.
"Si Has Four Valence Electrons."
6 With thermal excitation, electrons move to the conduction band and create vacancies in the valence band. The conduction particles are respectively:
Thermal energy creates electron-hole pairs. Electrons become mobile. Holes act as positive carriers.
When a valence electron gains thermal energy, it moves to the conduction band and becomes a free electron. The vacancy left behind behaves like a positively charged particle called a hole.
- Option B β Holes are not produced first.
- Option C β Core ions do not participate in conduction.
- Option D β Bound electrons cannot conduct.
Used
- Direct Recall
Application:
- Apply the concept of electron-hole pair generation.
Final Logic:
- Thermal excitation creates free electrons and holes.
"Electron Up β Hole Left."
7 What is the respective energy gap value for Silicon and Germanium?
Silicon has a larger gap than Germanium. Both are semiconductors. Standard NCERT values are 1.1 eV and 0.7 eV.
The energy gap of Silicon is approximately 1.1 eV, while that of Germanium is approximately 0.7 eV. These values explain why both materials behave as semiconductors.
- Option A β 5.4 eV corresponds to diamond.
- Option C β Values are reversed.
- Option D β Incorrect values.
Used
- Direct Recall
Application:
- Recall standard semiconductor energy gaps.
Final Logic:
- Si = 1.1 eV; Ge = 0.7 eV.
"Si-1.1, Ge-0.7."
8 Match List I (Gap Description) with List II (Condition)
| List I | List II |
|---|---|
| 1. Eg > 3 eV | I. Metal (Sn) |
| 2. Eg = 0 | II. Silicon |
| 3. Eg β 1.1 eV | III. Germanium |
| 4. Eg β 0.7 eV | IV. Insulator |
Large gap β Insulator. Zero gap β Metal. Silicon β 1.1 eV. Germanium β 0.7 eV.
Correct matching: Eg > 3 eV β Insulator Eg = 0 β Metal Eg β 1.1 eV β Silicon Eg β 0.7 eV β Germanium
- Option B β Incorrectly reverses assignments.
- Option C β Incorrect metal assignment.
- Option D β Incorrect insulator assignment.
Used
- Option Grouping
Application:
- Match standard energy-gap values with materials.
Final Logic:
- Only Option A correctly matches all pairs.
"0βMetal, 0.7βGe, 1.1βSi, >3βInsulator."
9 Correct statements about metalsCorrect statements about metals
A. Conduction band is partially filled.
B. Valence band is partially empty.
C. Conduction and valence bands may overlap.
D. Thermal excitation is required to create an overlap.
Metals possess free electrons. Bands may overlap. Thermal excitation is unnecessary.
Metals conduct electricity because the conduction band may be partially filled, the valence band may be partially empty, or both bands may overlap. These conditions already exist naturally and do not require thermal excitation.
- Option B β Includes incorrect statement D.
- Option C β Includes incorrect statement D.
- Option D β Includes incorrect statement D.
Used
- Option Grouping
Application:
- Identify the actual causes of metallic conductivity.
Final Logic:
- A, B, and C are correct; D is incorrect.
"Metal = Overlap and Free Electrons."
10 The resistance of metallic materials is low because
A. the energy gap is strictly larger than 3 eV
B. electrons from the valence band can easily move into the conduction band due to overlap
C. thermal excitation ionises all the core atoms
D. holes move freely in the conduction band
Band overlap provides free electrons. Electrons move with little energy. Conductivity becomes very high.
In metals, the conduction band and valence band overlap or the conduction band is partially filled. Therefore, electrons can move easily under an applied electric field, resulting in low resistance and high conductivity.
- Option A β Describes insulators.
- Option C β Core atoms are not ionized.
- Option D β Conduction is mainly due to free electrons.
Used
- Contextual/Tonal Matching
Application:
- Relate metallic conductivity to band overlap.
Final Logic:
- Band overlap allows easy electron movement.
"Overlap = Low Resistance."
11 In insulators, the energy gap is large. Consequently
Insulators have very large band gaps. Thermal energy cannot excite electrons easily. Electrons remain bound in the valence band.
In insulators, the energy gap is typically greater than 3 eV. The thermal energy available at room temperature is insufficient to move electrons from the valence band to the conduction band. Therefore, electrons remain tightly bound and conduction does not occur.
- Option A β Thermal excitation is insufficient.
- Option C β Conduction band is essentially empty.
- Option D β This resistivity range belongs to metals.
Used
- Elimination
Application:
- Identify the consequence of a large energy band gap.
Final Logic:
- Large gaps keep electrons bound in the valence band.
"Large Gap = Bound Electrons."
12 Insulator conduction statements
Insulator conduction statements
A. There are no electrons in the conduction band.
B. No electrical conduction is possible.
C. Energy gap is so large that thermal excitation cannot bridge it.
D. Holes provide high conductivity in insulators.
Conduction band is empty. Large band gap prevents excitation. Electrical conduction is negligible.
Insulators possess a large forbidden energy gap. Electrons cannot acquire sufficient thermal energy to reach the conduction band, leaving it effectively empty. Hence, electrical conduction is practically impossible. Statement D is incorrect because holes do not provide high conductivity in insulators.
- Option B β Includes incorrect statement D.
- Option C β Includes incorrect statement D.
- Option D β Includes incorrect statement D.
Used
- Option Grouping
Application:
- Evaluate each statement using insulator band theory.
Final Logic:
- A, B, and C are correct; D is incorrect.
"Empty CB + Big Gap = Insulator."
13 The approximate energy gap for Silicon is:
Silicon is a semiconductor. It has a moderate energy gap. Standard value is 1.1 eV.
Silicon possesses an energy band gap of approximately 1.1 eV. This value is large enough to prevent excessive conduction yet small enough to allow controlled carrier generation at room temperature.
- Option A β Corresponds to metals.
- Option B β Approximate value for Germanium.
- Option D β Approximate value for diamond.
Used
- Direct Recall
Application:
- Recall standard energy-gap values.
Final Logic:
- Silicon β 1.1 eV.
"Si = 1.1 eV."
14 Incorrect statement about semiconductors at room temperature
Semiconductors have moderate resistance. Some electrons are thermally excited. Conductivity is greater than in insulators.
At room temperature, thermal energy excites some electrons into the conduction band. Therefore, semiconductors conduct electricity better than insulators and have much lower resistance than insulating materials.
- Option A β Correct statement.
- Option C β Correct characteristic.
- Option D β Conduction electrons move in the conduction band.
Used
- Odd One Out
Application:
- Identify the statement inconsistent with semiconductor behavior.
Final Logic:
- Semiconductor resistance is lower than insulator resistance.
"Semiconductor β Insulator."
15 Match List I (Symbol) with List II (Meaning) in intrinsic semiconductors
| List I | List II |
|---|---|
| 1. ne | I. Total current |
| 2. nh | II. Intrinsic carrier concentration |
| 3. ni | III. Free electron concentration |
| 4. I | IV. Hole concentration |
ne β electron concentration. nh β hole concentration. ni β intrinsic carrier concentration.
Correct matching: ne β Free electron concentration nh β Hole concentration ni β Intrinsic carrier concentration I β Total current Hence Option A is correct.
- Option B β Interchanges ne and nh.
- Option C β Incorrect assignment of ni.
- Option D β Incorrect assignment of nh.
Used
- Option Grouping
Application:
- Match standard semiconductor symbols with meanings.
Final Logic:
- Only Option A matches all definitions correctly.
"e = Electron, h = Hole, i = Intrinsic."
16 In the diamond-like structure of pure Silicon, the number of valence electrons per atom and the number of nearest neighbours are respectively:
Silicon is tetravalent. Each atom has four neighbours. Four covalent bonds are formed.
Each silicon atom possesses four valence electrons and forms covalent bonds with four nearest neighbouring atoms arranged tetrahedrally.
- Option A β Nearest neighbours are not eight.
- Option B β Silicon does not have eight valence electrons.
- Option D β Silicon is not divalent.
Used
- Direct Recall
Application:
- Recall the diamond crystal structure.
Final Logic:
- Silicon β 4 valence electrons and 4 neighbours.
"Silicon = 4 and 4."
17 The two shared electrons in a covalent bond can be assumed to
Covalent bonds involve electron sharing. Shared electrons bind neighbouring atoms. They are not permanently transferred.
In a covalent bond, the shared electron pair is common to both atoms and effectively moves between them, providing the attractive force that holds the crystal structure together.
- Option A β Describes ionic bonding.
- Option B β Electrons remain bound at 0 K.
- Option D β Bond electrons belong to the valence structure.
Used
- Conceptual Matching
Application:
- Identify the nature of covalent bonding.
Final Logic:
- Shared electrons strengthen the bond between atoms.
"Shared Electrons Hold Atoms Together."
18 Correct statements about covalent bonds in Si/Ge
Correct statements about covalent bonds in Si/Ge
A. At low temperatures, an idealised picture shows all bonds intact.
B. As temperature increases, no bonds can be broken.
C. Shared electrons form a valence bond.
D. Each atom takes a share of one electron from each of its four neighbours.
Covalent bonds exist between neighbours. Shared electrons form valence bonds. Thermal energy can break some bonds.
At low temperatures, nearly all covalent bonds remain intact. Shared electrons form valence bonds, and each atom shares electrons with four neighbouring atoms. As temperature rises, some bonds can break due to thermal excitation. Statement B is incorrect because thermal energy can break covalent bonds.
- Option B β Includes incorrect statement B.
- Option C β Includes incorrect statement B.
- Option D β Includes incorrect statement B.
Used
- Option Grouping
Application:
- Evaluate each bonding statement independently.
Final Logic:
- A, C, and D are correct; B is incorrect.
"Heat Breaks Some Bonds."
19 What is the effective charge of the vacancy (hole) created when an electron breaks away from a covalent bond?
A missing electron leaves a positive vacancy. The vacancy behaves like a charge carrier. This carrier is called a hole.
When an electron leaves a covalent bond, a vacancy is created. Since a negative charge is missing, the vacancy behaves as an effective positive charge of magnitude +q.
- Option A β Electron charge is βq.
- Option C β Hole carries effective charge.
- Option D β Hole charge is not doubled.
Used
- Direct Recall
Application:
- Recall the definition of a hole.
Final Logic:
- A hole behaves as a positive charge carrier.
"Missing Electron = Positive Hole."
20 The total current I in an intrinsic semiconductor is given by the sum of electron current (Ie) and hole current (Ih) as:
Both electrons and holes conduct. Their currents add together. Total current is their sum.
In an intrinsic semiconductor, electrical conduction occurs through both electrons and holes. Therefore, the total current is the sum of the electron current and the hole current: I=I_e+I_h
- Option A β Currents do not subtract.
- Option B β Current is not a product.
- Option D β No such relation exists.
Used
- Formula Recall
Application:
- Apply the total-current relation for intrinsic semiconductors.
Final Logic:
- Total current equals electron current plus hole current.
"Electron Current + Hole Current = Total Current."
