CUET UG Physics Booster Test 2-Junction Formation and Physics
π Answers are locked once submitted β results and explanations appear at the end.
QUESTION 1 OF 20
Incorrect statement about the wafer conversion process
QUESTION 2 OF 20
Correct statements about the metallurgical junction
1. It acts as a discontinuity for flowing charge carriers if formed by physically pressing slabs together.
2. The inter-atomic crystal spacing is roughly 2 to 3 Γ
.
3. Physical roughness prevents continuous contact at the atomic level in physically joined slabs.
4. A highly efficient p-n junction can be formed by smoothly pressing an n-slab to a p-slab.
QUESTION 3 OF 20
The concentration gradient during p-n junction formation
1. is higher for free electrons in the p-type semiconductor.
2. drives holes from the p-side to the n-side.
3. drives electrons from the n-side to the p-side.
4. ceases to exist the exact moment the depletion region is fully formed.
QUESTION 4 OF 20
Match List I with List II regarding currents in a p-n junction
| List I | List II |
|---|---|
| I. Initial state | P. Concentration gradient |
| II. Equilibrium state | Q. Diffusion current is large, drift is small |
| III. Diffusion current driver | R. Electric field |
| IV. Drift current driver | S. Net current is zero |
QUESTION 5 OF 20
If the strength of the electric field in the depletion region is E, and the thickness of the region is d, the potential difference Vβ is roughly modeled as
QUESTION 6 OF 20
In a p-n junction under equilibrium
QUESTION 7 OF 20
When an electron diffuses from n to p, the ionised donor left behind is ____, creating a layer of ____ charge on the n-side.
QUESTION 8 OF 20
Space-charge region formation statements
1. Diffusing holes leave behind ionized acceptors.
2. Ionized acceptors represent a positive space-charge.
3. Ionized acceptors are immobile due to bonding with surrounding atoms.
4. The negative space-charge region forms on the p-side.
QUESTION 9 OF 20
If a semiconductor diode has an initial uniform free electron concentration of \(5\times {10}^{21}βm^{-3}\), and the depletion process completely removes these from a small volume of \(2\times {10}^{-15}βm^{3}\), what will be the total number of free electrons depleted?
QUESTION 10 OF 20
Incorrect statement about the depletion region thickness
QUESTION 11 OF 20
The polarity of the barrier potential
QUESTION 12 OF 20
The n-material in a p-n junction at equilibrium
1. has lost electrons
2. has acquired holes
3. is negative relative to the p-material
4. is positive relative to the p-material
QUESTION 13 OF 20
When a small external voltage is applied under forward bias, the barrier potential is reduced ____, and only a ____ number of carriers possess enough energy to cross the junction.
QUESTION 14 OF 20
Voltage drop statements in a biased diode
1. The applied voltage mostly drops across the depletion region.
2. The voltage drop across the p-side and n-side is negligible.
3. The depletion region has very low resistance.
4. The depletion region is highly resistive due to no free charges.
QUESTION 15 OF 20
Match List I with List II regarding forward bias
| List I | List II |
|---|---|
| I. p-side connection | P. Mostly across depletion region |
| II. n-side connection | Q. Decreases |
| III. Depletion width | R. Positive terminal |
| IV. Applied voltage drop | S. Negative terminal |
QUESTION 16 OF 20
Correct statements about the barrier height under forward bias
1. The direction of the applied voltage opposes the built-in potential Vβ.
2. The effective barrier height becomes (Vβ β V).
3. Increasing the applied voltage significantly increases the barrier height.
4. A reduced barrier height allows more carriers to have the required energy to cross.
QUESTION 17 OF 20
If the initial barrier height is Vβ, and a reverse bias voltage Vβ and an additional series reverse bias Vβ are applied, the total effective barrier height will be
QUESTION 18 OF 20
If a diode has a barrier potential of \(V_{0}=0.6Β V\), and experiences a reverse drift current of \(2.5β\mu A\), what will be the total charge passing through the junction in 4 seconds strictly due to this drift current?
QUESTION 19 OF 20
Incorrect statement regarding minority carrier injection
QUESTION 20 OF 20
The total diode forward current
Test Complete!
Answer Review
1 Incorrect statement about the wafer conversion process
Only a small region is converted into n-type. The remaining portion stays p-type. This creates a p-n junction.
During p-n junction fabrication, only a selected portion of the p-type silicon wafer is doped with pentavalent impurities. This creates an n-region while the rest remains p-type.
- Option A β Correct fabrication process.
- Option C β Correct result of wafer conversion.
- Option D β Correct advantage over joining separate slabs.
Used
- Conceptual Elimination
Application:
- Identify the statement inconsistent with p-n junction fabrication.
Final Logic:
- Only part of the wafer is converted to n-type.
"One Wafer, Two Regions."
2 Correct statements about the metallurgical junction
1. It acts as a discontinuity for flowing charge carriers if formed by physically pressing slabs together.
2. The inter-atomic crystal spacing is roughly 2 to 3 Γ
.
3. Physical roughness prevents continuous contact at the atomic level in physically joined slabs.
4. A highly efficient p-n junction can be formed by smoothly pressing an n-slab to a p-slab.
Atomic-scale continuity is essential. Physically joined slabs cannot provide a proper junction. Crystal spacing is extremely small.
Statements A, B, and C are correct. Physical roughness prevents perfect atomic contact, making simple pressing of p-type and n-type slabs ineffective for producing a high-quality p-n junction.
- Statement D β Physically pressing slabs does not create an efficient junction.
Used
- Statement Analysis
Application:
- Evaluate each statement regarding junction formation.
Final Logic:
- A, B, and C are correct.
"Atomic Continuity Required."
3 The concentration gradient during p-n junction formation
1. is higher for free electrons in the p-type semiconductor.
2. drives holes from the p-side to the n-side.
3. drives electrons from the n-side to the p-side.
4. ceases to exist the exact moment the depletion region is fully formed.
Holes diffuse from p to n. Electrons diffuse from n to p. Diffusion is driven by concentration differences.
The p-side contains many holes while the n-side contains many electrons. Therefore: Holes diffuse from p-side to n-side. Electrons diffuse from n-side to p-side.
- Statement A β Electron concentration is higher in n-type material.
- Statement D β Concentration gradient still exists at equilibrium; it is balanced by drift.
Used
- Carrier Diffusion Analysis
Application:
- Determine diffusion directions.
Final Logic:
- Only B and C are correct.
"Holes: pβn, Electrons: nβp."
4 Match List I with List II regarding currents in a p-n junction
| List I | List II |
|---|---|
| I. Initial state | P. Concentration gradient |
| II. Equilibrium state | Q. Diffusion current is large, drift is small |
| III. Diffusion current driver | R. Electric field |
| IV. Drift current driver | S. Net current is zero |
Diffusion dominates initially. Net current becomes zero at equilibrium. Diffusion is driven by concentration gradient. Drift is driven by electric field.
Correct matching: I β Q II β S III β P IV β R
- Incorrect matching of diffusion and drift mechanisms.
Used
- Matching Concepts
Application:
- Associate current mechanisms with their causes.
Final Logic:
- Only Option A is correct.
"Gradient β Diffusion, Field β Drift."
5 If the strength of the electric field in the depletion region is E, and the thickness of the region is d, the potential difference Vβ is roughly modeled as
For a uniform electric field: \(V=E\times d\)
The potential difference across a region of thickness \(d\) subjected to electric field \(E\) is approximately: \(V_{0}=Ed\)
- B β Incorrect sign convention.
- C β Incorrect dimensions.
- D β Incorrect dimensions.
Used
- Formula Recall
Application:
- Use the electric fieldβpotential relation.
Final Logic:
- Potential difference equals field Γ distance.
"Voltage = Field Γ Distance."
6 In a p-n junction under equilibrium
Diffusion and drift both exist. Their magnitudes are equal. Net current becomes zero.
At equilibrium: \(I_{drift}=I_{diffusion}\) but in opposite directions. Hence, the total current is zero.
- A β Both currents exist.
- B β Currents are equal.
- D β Drift current exists even without external bias.
Used
- Equilibrium Condition
Application:
- Apply the equilibrium current condition.
Final Logic:
- Opposing currents balance each other.
"Drift = Diffusion at Equilibrium."
7 When an electron diffuses from n to p, the ionised donor left behind is ____, creating a layer of ____ charge on the n-side.
Donor atom loses an electron. Positive ion remains fixed in lattice.
After electron diffusion, donor atoms become positively charged ions. Since they are bonded within the crystal lattice, they remain immobile.
- A β Ion is not mobile.
- B β Donor ions are positive.
- C β Incorrect charge and mobility.
Used
- Charge Analysis
Application:
- Determine donor-ion characteristics.
Final Logic:
- Ionized donor = immobile positive ion.
"Donor Loses Electron β Positive Ion."
8 Space-charge region formation statements
1. Diffusing holes leave behind ionized acceptors.
2. Ionized acceptors represent a positive space-charge.
3. Ionized acceptors are immobile due to bonding with surrounding atoms.
4. The negative space-charge region forms on the p-side.
Hole diffusion exposes acceptor ions. Acceptor ions are negative and immobile. Negative space charge forms on p-side.
Statements A, C, and D are correct. Ionized acceptors possess negative charge, so statement B is incorrect.
- Statement B β Acceptor ions create negative space charge.
Used
- Space-Charge Analysis
Application:
- Determine the nature of acceptor ions.
Final Logic:
- A, C, and D are correct.
"Acceptor Ion = Negative Fixed Charge."
9 If a semiconductor diode has an initial uniform free electron concentration of \(5\times {10}^{21}βm^{-3}\), and the depletion process completely removes these from a small volume of \(2\times {10}^{-15}βm^{3}\), what will be the total number of free electrons depleted?
\(N=nV\)
\(N=(5\times {10}^{21})(2\times {10}^{-15})=10\times {10}^{6}=1.0\times {10}^{7}\)
- Obtained from incorrect multiplication.
Used
- Direct Calculation
Application:
- Multiply concentration by volume.
Final Logic:
- \(N=1.0\times {10}^{7}\)
"Number = Concentration Γ Volume."
10 Incorrect statement about the depletion region thickness
Drift current is not halted. Drift and diffusion currents balance at equilibrium.
The depletion region grows until the electric field becomes strong enough to produce a drift current equal and opposite to the diffusion current. Drift current continues to exist at equilibrium.
- A β Correct order of magnitude.
- B β Correct behavior before equilibrium.
- D β Correct definition.
Used
- Equilibrium Analysis
Application:
- Understand depletion-layer growth.
Final Logic:
- Drift current persists at equilibrium.
"Equilibrium Means Balance, Not Zero Drift."
11 The polarity of the barrier potential
Barrier potential develops naturally in a p-n junction. It opposes further diffusion of majority carriers. This establishes equilibrium.
The built-in electric field and barrier potential oppose the diffusion of majority carriers across the junction. Equilibrium is reached when drift current balances diffusion current.
- Option A β Barrier potential opposes, not supports, carrier flow.
- Option C β Actual polarity is positive on n-side and negative on p-side.
- Option D β Barrier potential is an internal property of the junction.
Used
- Conceptual Understanding
Application:
- Identify the function of the barrier potential.
Final Logic:
- Barrier potential prevents continuous majority-carrier diffusion.
"Barrier Builds Balance."
12 The n-material in a p-n junction at equilibrium
1. has lost electrons
2. has acquired holes
3. is negative relative to the p-material
4. is positive relative to the p-material
Electrons diffuse from n-side to p-side. Positive donor ions remain behind. n-side becomes positive.
The n-region loses some electrons due to diffusion. The uncovered donor ions create a positive space charge, making the n-region positive relative to the p-region.
- Statement B β Holes do not accumulate in the n-region.
- Statement C β n-region becomes positive, not negative.
Used
- Charge Distribution Analysis
Application:
- Analyze charge formation near the junction.
Final Logic:
- Loss of electrons leaves the n-region positively charged.
"Lose Electrons β Become Positive."
13 When a small external voltage is applied under forward bias, the barrier potential is reduced ____, and only a ____ number of carriers possess enough energy to cross the junction.
Small forward bias slightly lowers the barrier. Only a limited number of carriers can cross initially.
For a small forward bias, the barrier potential decreases only slightly. Consequently, only a small fraction of majority carriers gain sufficient energy to cross the junction.
- B & C β Large carrier flow occurs only at higher forward voltages.
- D β Contradictory statement.
Used
- Physical Interpretation
Application:
- Relate small forward bias to carrier transport.
Final Logic:
- Small voltage β small barrier reduction β small carrier crossing.
"Small Bias, Small Crossing."
14 Voltage drop statements in a biased diode
1. The applied voltage mostly drops across the depletion region.
2. The voltage drop across the p-side and n-side is negligible.
3. The depletion region has very low resistance.
4. The depletion region is highly resistive due to no free charges.
Depletion region contains almost no mobile carriers. Its resistance is very high. Most applied voltage appears across it.
Statements A, B, and D are correct. The depletion layer is highly resistive because it lacks free carriers. Therefore, almost the entire applied voltage appears across it.
- Statement C β Depletion region does not have low resistance.
Used
- Region Resistance Analysis
Application:
- Determine where voltage drops in a diode.
Final Logic:
- High resistance causes most voltage to drop across the depletion region.
"No Carriers β High Resistance."
15 Match List I with List II regarding forward bias
| List I | List II |
|---|---|
| I. p-side connection | P. Mostly across depletion region |
| II. n-side connection | Q. Decreases |
| III. Depletion width | R. Positive terminal |
| IV. Applied voltage drop | S. Negative terminal |
p-side β positive terminal. n-side β negative terminal. Depletion width decreases. Voltage drops mainly across depletion layer.
Correct matching: I β R II β S III β Q IV β P
- Incorrect matching of battery connections and depletion width behavior.
Used
- Matching Concepts
Application:
- Associate forward-bias characteristics.
Final Logic:
- Only Option B correctly matches all items.
"Forward Bias: P to Positive."
16 Correct statements about the barrier height under forward bias
1. The direction of the applied voltage opposes the built-in potential Vβ.
2. The effective barrier height becomes (Vβ β V).
3. Increasing the applied voltage significantly increases the barrier height.
4. A reduced barrier height allows more carriers to have the required energy to cross.
Forward bias opposes the barrier. Barrier height decreases. Carrier flow increases.
Forward bias reduces the effective barrier height: \(V_{effective}=V_{0}-V\) As the barrier decreases, more carriers can cross the junction.
- Statement C β Forward bias reduces, not increases, barrier height.
Used
- Formula-Based Reasoning
Application:
- Analyze forward-bias effects.
Final Logic:
- A, B, and D are correct.
"Forward Bias Lowers the Barrier."
17 If the initial barrier height is Vβ, and a reverse bias voltage Vβ and an additional series reverse bias Vβ are applied, the total effective barrier height will be
Reverse bias adds to the barrier potential. Additional reverse voltages further increase it.
Under reverse bias: \(V_{effective}=V_{0}+V_{1}+V_{2}\) because all reverse-bias voltages reinforce the built-in barrier.
- Do not correctly represent reverse-bias addition.
Used
- Formula Recall
Application:
- Apply reverse-bias barrier relation.
Final Logic:
- Reverse voltages add to the built-in potential.
"Reverse Bias = Add the Barriers."
18 If a diode has a barrier potential of \(V_{0}=0.6Β V\), and experiences a reverse drift current of \(2.5β\mu A\), what will be the total charge passing through the junction in 4 seconds strictly due to this drift current?
Use: \(Q=It\)
\(I=2.5\times {10}^{-6}βAt=4βsQ=ItQ=(2.5\times {10}^{-6})(4)Q=1.0\times {10}^{-5}βC\)
- Obtained from incorrect multiplication.
Used
- Direct Numerical Calculation
Application:
- Use the current-charge relationship.
Final Logic:
- \(Q=1.0\times {10}^{-5}βC\)
"Charge = Current Γ Time."
19 Incorrect statement regarding minority carrier injection
Forward bias injects carriers across the junction. Minority carrier concentration becomes highest near the junction.
Injected carriers accumulate near the depletion-region boundaries, causing the minority carrier concentration near the junction edge to increase significantly.
- A β Correct.
- B β Correct electron injection process.
- C β Correct hole injection process.
Used
- Carrier Injection Analysis
Application:
- Understand carrier distribution near the junction.
Final Logic:
- Minority carrier concentration increases near the junction.
"Injection Raises Boundary Concentration."
20 The total diode forward current
Forward current mainly arises from diffusion. Both electrons and holes contribute.
Under forward bias, majority carriers cross the junction and diffuse into the opposite region. The total forward current is the sum of: Hole diffusion current Electron diffusion current
- A β Not solely drift current.
- C β Forward current is predominantly diffusion current.
- D β Forward-biased diode conducts significantly.
Used
- Current Component Analysis
Application:
- Identify contributions to forward current.
Final Logic:
- Forward current = electron diffusion current + hole diffusion current.
"Forward Current = Electron + Hole Diffusion."
