CUET UG Physics Booster Test 3-Motional EMF and Lorentz Force
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QUESTION 1 OF 20
Identify the correct statements regarding the straight conductor in field:
1. The area enclosed by loop PQRS changes strictly linearly if the velocity v is constant.
2. The induced current direction is determined by the decreasing area opposing the magnetic flux change.
3. Φ_B = Blx is valid even if the magnetic field is rapidly varying with time.
4. The induced emf Blv requires the field to be perpendicular to the plane of the system.
QUESTION 2 OF 20
Analyzing the velocity and field interaction in motional emf will find that:
Statements:
1. The velocity vector must be parallel to the magnetic field vector to induce a current.
2. Replacing the constant velocity with acceleration would make the rate of change of flux independent of time.
3. Moving the arm PQ to the left decreases the enclosed area, thus reducing the magnetic flux and inducing a current to oppose this change.
4. The relative motion between the stationary rails and the magnetic field is the only cause of emf.
QUESTION 3 OF 20
If the magnetic flux enclosed by the loop PQRS is Φ_B = Blx, and the arm PQ moves causing x to decrease, the rate of change of flux dΦ_B/dt corresponds to the induced emf. Thus, if the direction of motion is reversed (x increases), the induced current will
QUESTION 4 OF 20
Choose the incorrect statement about the motional EMF equation:
QUESTION 5 OF 20
Match List I with List II for the theoretical basis of Lorentz Force Origin in motional EMF.
| List I | List II |
|---|---|
| (1) Magnetic force on an arbitrary charge q | (a) Towards Q along the rod |
| (2) Moving charge speed | (b) Identical to rod speed v |
| (3) Force direction | (c) Requires moving charges in a magnetic field |
| (4) Basis for the derivation | (d) qvB |
QUESTION 6 OF 20
In a metallic rod moving perpendicular to a magnetic field, the uniform nature of the magnetic force on all charge carriers and the relative magnitude of the force depend on:
QUESTION 7 OF 20
A charge q of 2.0 C is moved from P to Q in a rod of length 0.5 m, moving at 4.0 m/s in a 0.1 T magnetic field. What is the work done on this charge by the magnetic force?
QUESTION 8 OF 20
Choose the correct statements about EMF as Work per Charge:
Statements:
1. ε = W/q implies that work done in moving a unit charge determines the emf.
2. This definition mathematically connects the Lorentz force derivation directly to Faraday's law.
3. It requires the magnetic field to be non-uniform to perform work.
4. The work done is purely due to the q(v × B) component of the Lorentz force.
QUESTION 9 OF 20
While moving charges experience a magnetic force q(v × B), an emf is nevertheless induced in a completely stationary conductor when
QUESTION 10 OF 20
Identify the correct statements regarding induced electric fields:
Statements:
1. They are generated by time-varying magnetic fields.
2. They explain the existence of induced emf when the conductor is stationary.
3. They are identical in property to electric fields produced by static charges.
4. The force on a charge in a stationary conductor is given solely by qE.
QUESTION 11 OF 20
Which of the following statements is incorrect regarding the behavior of a metallic rod rotating about a central pivot in a uniform magnetic field?
QUESTION 12 OF 20
If free electrons move towards the outer end of a rotating rod, a resulting separation of charges produces an emf. Thus, if the rod rotates at a steady state, the potential difference across the ends of the rod will be
QUESTION 13 OF 20
When integrating the segment EMF for a rotating rod, the dependence of velocity on radius r and the resulting EMF expression are:
QUESTION 14 OF 20
Match List I with List II for variables in the Rotational EMF equation.
| List I | List II |
|---|---|
| (1) Angular frequency ω | (a) R²/2 |
| (2) Linear velocity v | (b) 2πν |
| (3) Radius R | (c) Upper limit of integration |
| (4) Integral of r dr from 0 to R | (d) rω |
QUESTION 15 OF 20
The method of finding emf using the rate of change of area evaluates the flux through a closed loop OPQ, demonstrating that
QUESTION 16 OF 20
The area of a sector swept by a rod of length 1 m rotating at 50 rev/s is increasing. If the uniform magnetic field is 1 T, what is the value of d(Area)/dt, and consequently the induced emf?
QUESTION 17 OF 20
When determining the potential between the axle and rim of a metallic wheel with spokes rotating in a magnetic field,
1. the total emf is the sum of the emfs of individual spokes
2. the presence of the rim shorts out the spokes, resulting in zero emf
3. the emf is equivalent to that of a single solid rotating rod of the same radius
4. the emf depends on the thickness of the individual spokes
Choose the correct options:
QUESTION 18 OF 20
Choose the correct statements about the parallel EMF configuration in a wheel:
1. The spokes act as identical emf sources connected in parallel.
2. The potential difference across any individual spoke equals the potential difference of the entire wheel.
3. The number of spokes alters the total internal resistance, but not the theoretical induced emf.
4. Adding more spokes increases the induced emf proportionally.
QUESTION 19 OF 20
Horizontal Component Effects on a rotating wheel statements:
Statements:
1. A wheel rotating in a plane normal to H_E generates an emf proportional to H_E.
2. If the wheel is rotated perfectly parallel to H_E, the induced motional emf across its spokes is maximized.
3. 1 Gauss (G) equals 10⁻⁴ T, which is crucial for converting H_E into standard SI units.
4. Earth's magnetic field is a realistic source of a uniform B field over the area of a small wheel.
QUESTION 20 OF 20
If a wire of length l falls horizontally with a velocity v perpendicular to the horizontal component of the earth's magnetic field B, the motional emf is Blv. Thus, if a 10 m long wire falls at 5.0 m/s and the induced emf is 1.5 × 10⁻³ V, the horizontal component of the earth's magnetic field must be
Test Complete!
Answer Review
1 Identify the correct statements regarding the straight conductor in field:
1. The area enclosed by loop PQRS changes strictly linearly if the velocity v is constant.
2. The induced current direction is determined by the decreasing area opposing the magnetic flux change.
3. Φ_B = Blx is valid even if the magnetic field is rapidly varying with time.
4. The induced emf Blv requires the field to be perpendicular to the plane of the system.
�� Constant velocity gives linear area change. �� Lenz's law determines current direction. �� Standard motional emf assumes uniform time-independent magnetic field.
- Statement 1 is correct because area A = lx changes linearly when x changes uniformly with time. → Statement 2 is correct because the induced current opposes the change in magnetic flux according to Lenz's law. → Statement 3 is incorrect because Φ = Blx in this simple form assumes B is constant. For a time-varying magnetic field, flux becomes time dependent through B(t). → Statement 4 is correct because ε = Blv is derived for the case where the magnetic field is perpendicular to the plane of motion.
- �� Option A → Contains incorrect Statement 3.
- �� Option C → Contains incorrect Statement 3.
- �� Option D → Contains incorrect Statement 3.
Used
- �� Elimination
Application:
- �� Identify the statement inconsistent with the assumptions used in motional emf derivation.
Final Logic:
- �� Statement 3 is false; Statements 1, 2 and 4 are correct.
- "Constant B → Φ = Blx."
2 Analyzing the velocity and field interaction in motional emf will find that:
Statements:
1. The velocity vector must be parallel to the magnetic field vector to induce a current.
2. Replacing the constant velocity with acceleration would make the rate of change of flux independent of time.
3. Moving the arm PQ to the left decreases the enclosed area, thus reducing the magnetic flux and inducing a current to oppose this change.
4. The relative motion between the stationary rails and the magnetic field is the only cause of emf.
�� Area decreases. �� Flux decreases. �� Current opposes the decrease.
- Statement 3 is correct because moving PQ left decreases area and magnetic flux. → According to Lenz's law, induced current opposes the decrease in flux. → Statement 1 is false because maximum motional emf occurs when v is perpendicular to B. → Statement 2 is false because acceleration generally makes flux change time dependent. → Statement 4 is false because emf arises from conductor-field interaction and changing flux.
- �� Option A → Statement 1 is incorrect.
- �� Option B → Statement 2 is incorrect.
- �� Option D → Statement 4 is incorrect.
Used
- �� Elimination
Application:
- �� Test each statement using Faraday's law and Lorentz force concepts.
Final Logic:
- �� Only Statement 3 is correct.
- "Decrease Flux → Oppose Loss."
3 If the magnetic flux enclosed by the loop PQRS is Φ_B = Blx, and the arm PQ moves causing x to decrease, the rate of change of flux dΦ_B/dt corresponds to the induced emf. Thus, if the direction of motion is reversed (x increases), the induced current will
�� Flux change reverses sign. �� Emf reverses sign. �� Current reverses direction.
- Reversing the motion reverses the sign of dΦ/dt. → Since ε = −dΦ/dt, the induced emf changes sign. → Therefore, the induced current flows in the opposite direction.
- �� Option A → Current direction depends on the sign of flux change.
- �� Option C → Flux is still changing, so emf exists.
- �� Option D → No exponential dependence occurs.
Used
- �� Contextual/Tonal Matching
Application:
- �� Follow the sign change in flux variation.
Final Logic:
- �� Reverse motion → Reverse current.
- "Reverse Motion = Reverse Current."
4 Choose the incorrect statement about the motional EMF equation:
�� Motional emf is magnetic in origin. �� Uses Lorentz force and flux change. �� Static-charge electric fields are not involved.
- The motional emf equation ε = Blv is derived using magnetic force on moving charges or via Faraday's law. → It does not explicitly involve electric fields generated by static charges. → Therefore Statement C is incorrect.
- �� Option A → Correct statement.
- �� Option B → Direct consequence of ε = Blv.
- �� Option D → Valid derivation method.
Used
- �� Odd One Out
Application:
- �� Identify the statement unrelated to motional emf derivation.
Final Logic:
- �� Static-charge electric fields are not part of the derivation.
- "Motional EMF → Magnetic Origin."
5 Match List I with List II for the theoretical basis of Lorentz Force Origin in motional EMF.
| List I | List II |
|---|---|
| (1) Magnetic force on an arbitrary charge q | (a) Towards Q along the rod |
| (2) Moving charge speed | (b) Identical to rod speed v |
| (3) Force direction | (c) Requires moving charges in a magnetic field |
| (4) Basis for the derivation | (d) qvB |
�� Magnetic force = qvB. �� Charges move with rod speed. �� Lorentz force requires moving charges.
- 1 → d because magnetic force magnitude is qvB. → 2 → b because charge carriers move with the rod at speed v. → 3 → a because force pushes charges toward Q. → 4 → c because Lorentz force requires moving charges in a magnetic field.
- �� Option B → Force magnitude and speed mismatched.
- �� Option C → Speed and direction mismatched.
- �� Option D → Incorrect assignment of Lorentz force expression.
Used
- �� Option Grouping
Application:
- �� Match each physical quantity with its standard definition.
Final Logic:
- �� Direct Lorentz-force matching gives 1-d, 2-b, 3-a, 4-c.
- "qvB → v → Direction."
6 In a metallic rod moving perpendicular to a magnetic field, the uniform nature of the magnetic force on all charge carriers and the relative magnitude of the force depend on:
�� F = qvB. �� Uniform B gives uniform force. �� Depends on speed.
- The Lorentz force is F = qvB. → In a uniform magnetic field, force is independent of position. → The magnitude depends directly on speed v.
- �� Option A → Force is not proportional to v².
- �� Option C → Force on a charge does not depend on rod length.
- �� Option D → Electric field is not the primary cause.
Used
- �� Elimination
Application:
- �� Apply Lorentz force equation.
Final Logic:
- �� Uniform field + speed determines force.
- "qvB, not qv²B."
7 A charge q of 2.0 C is moved from P to Q in a rod of length 0.5 m, moving at 4.0 m/s in a 0.1 T magnetic field. What is the work done on this charge by the magnetic force?
�� W = qvBl. �� Substitute values. �� Obtain 0.4 J.
- W = qvBl → W = (2)(4)(0.1)(0.5) → W = 0.4 J
- �� Option B → Half the correct value.
- �� Option C → Double the correct value.
- �� Option D → Four times the correct value.
Used
- �� Substitution
Application:
- �� Direct substitution into W = qvBl.
Final Logic:
- �� W = 0.4 J.
- "Work = qvBl."
8 Choose the correct statements about EMF as Work per Charge:
Statements:
1. ε = W/q implies that work done in moving a unit charge determines the emf.
2. This definition mathematically connects the Lorentz force derivation directly to Faraday's law.
3. It requires the magnetic field to be non-uniform to perform work.
4. The work done is purely due to the q(v × B) component of the Lorentz force.
�� EMF = Work/Charge. �� Links Lorentz force to Faraday's law. �� Uniform magnetic field is sufficient.
- Statement 1 is the definition of emf. → Statement 2 correctly connects microscopic and macroscopic descriptions of induction. → Statement 3 is incorrect because a uniform magnetic field can also produce motional emf. → Statement 4 is correct in the standard motional emf derivation.
- �� Option A → Contains incorrect Statement 3.
- �� Option C → Contains incorrect Statement 3.
- �� Option D → Contains incorrect Statement 3.
Used
- �� Elimination
Application:
- �� Identify the false statement.
Final Logic:
- �� Statement 3 is incorrect.
- "EMF = Work ÷ Charge."
9 While moving charges experience a magnetic force q(v × B), an emf is nevertheless induced in a completely stationary conductor when
�� Changing magnetic field creates electric field. �� Stationary conductor can still have emf. �� Faraday's law applies.
- A changing magnetic field generates an induced electric field. → This electric field produces emf even in a stationary conductor.
- �� Option A → Drift velocity is not the cause.
- �� Option B → Static magnetic field alone does not induce emf.
- �� Option D → Circuit connection does not determine emf generation.
Used
- �� Elimination
Application:
- �� Apply Faraday's law.
Final Logic:
- �� Changing B induces emf.
- "Changing B → Induced E."
10 Identify the correct statements regarding induced electric fields:
Statements:
1. They are generated by time-varying magnetic fields.
2. They explain the existence of induced emf when the conductor is stationary.
3. They are identical in property to electric fields produced by static charges.
4. The force on a charge in a stationary conductor is given solely by qE.
�� Induced fields arise from changing B. �� They explain stationary-conductor emf. �� They are non-conservative.
- Statement 1 is correct by Faraday's law. → Statement 2 is correct because induced electric fields explain emf in stationary conductors. → Statement 3 is incorrect because induced electric fields are non-conservative, unlike electrostatic fields. → Statement 4 is correct because for stationary charges magnetic force is zero and electric force qE acts.
- �� Option B → Contains incorrect Statement 3.
- �� Option C → Contains incorrect Statement 3.
- �� Option D → Contains incorrect Statement 3.
Used
- �� Elimination
Application:
- �� Identify the statement inconsistent with induced electric fields.
Final Logic:
- �� Statement 3 is false; 1, 2 and 4 are correct.
- "Induced E forms loops."
11 Which of the following statements is incorrect regarding the behavior of a metallic rod rotating about a central pivot in a uniform magnetic field?
�� Velocity depends on radius. �� Lorentz force depends on velocity. �� Force is not the same everywhere.
- For a rotating rod, linear speed is v = ωr. → At the pivot, r = 0 and hence v = 0, so magnetic force is zero. → At the rim, velocity is maximum and Lorentz force is maximum. → Therefore, the force is not equal at the pivot and rim.
- �� Option A → Correct; electrons are displaced due to Lorentz force.
- �� Option B → Correct; charge separation produces emf.
- �� Option D → Correct; equilibrium is eventually reached.
Used
- �� Elimination
Application:
- �� Use v = ωr to check force variation.
Final Logic:
- �� Since F = qvB and v varies with r, force cannot be equal everywhere.
- "Rim fastest, force greatest."
12 If free electrons move towards the outer end of a rotating rod, a resulting separation of charges produces an emf. Thus, if the rod rotates at a steady state, the potential difference across the ends of the rod will be
�� Charge separation occurs. �� Equilibrium develops. �� Constant emf is produced.
- Rotation continuously produces charge separation. → A balancing electric field develops. → At steady state, the potential difference becomes constant and non-zero.
- �� Option A → Charge separation creates emf.
- �� Option C → Potential does not increase indefinitely.
- �� Option D → Uniform rotation in constant B gives steady emf.
Used
- �� Contextual/Tonal Matching
Application:
- �� Interpret the meaning of "steady state".
Final Logic:
- �� Steady state implies constant potential difference.
- "Steady rotation → Steady emf."
13 When integrating the segment EMF for a rotating rod, the dependence of velocity on radius r and the resulting EMF expression are:
�� v = ωr. �� Velocity varies linearly with r. �� Integration produces R² dependence.
- Linear velocity: v = ωr → Elemental emf: dε = Bωrdr → Integrating from 0 to R: ε = ½BωR² → Therefore velocity varies linearly with r and emf is proportional to R².
- �� Option B → Velocity is not quadratic in r.
- �� Option C → Velocity is not constant.
- �� Option D → Final emf depends on R², not R.
Used
- �� Substitution
Application:
- �� Use v = ωr in emf integration.
Final Logic:
- �� Linear velocity dependence yields quadratic radius dependence.
- "v ∝ r, emf ∝ R²."
14 Match List I with List II for variables in the Rotational EMF equation.
| List I | List II |
|---|---|
| (1) Angular frequency ω | (a) R²/2 |
| (2) Linear velocity v | (b) 2πν |
| (3) Radius R | (c) Upper limit of integration |
| (4) Integral of r dr from 0 to R | (d) rω |
�� ω = 2πν. �� v = rω. �� R is upper integration limit. �� ∫rdr = R²/2.
- 1 → b because ω = 2πν. → 2 → d because linear velocity is v = rω. → 3 → c because R is the upper limit of integration. → 4 → a because: ∫₀ᴿ r dr = R²/2
- �� Option B → Angular frequency and velocity mismatched.
- �� Option C → Integral and velocity mismatched.
- �� Option D → Multiple incorrect pairings.
Used
- �� Option Grouping
Application:
- �� Match standard rotational formulas.
Final Logic:
- �� Direct formula matching gives 1-b, 2-d, 3-c, 4-a.
- "2πν → rω → R → R²/2."
15 The method of finding emf using the rate of change of area evaluates the flux through a closed loop OPQ, demonstrating that
�� ε = B(dA/dt). �� Area sweep changes flux. �� Faraday's law applies.
- Magnetic flux: Φ = BA → Therefore: ε = B(dA/dt) → The induced emf equals magnetic field multiplied by the rate of area swept.
- �� Option B → Resistor presence is irrelevant.
- �� Option C → Area change alone can induce emf.
- �� Option D → θ changes with ω.
Used
- �� Substitution
Application:
- �� Use Faraday's law with changing area.
Final Logic:
- �� Flux change comes from area sweep.
- "Area Sweep = EMF."
16 The area of a sector swept by a rod of length 1 m rotating at 50 rev/s is increasing. If the uniform magnetic field is 1 T, what is the value of d(Area)/dt, and consequently the induced emf?
�� ω = 2πν. �� dA/dt = ½R²ω. �� ε = B(dA/dt).
- ν = 50 rev/s → ω = 2π(50) = 100π rad/s → dA/dt = ½R²ω = ½(1²)(100π) = 50π ≈ 157 m²/s → ε = B(dA/dt) = 1 × 157 = 157 V
- �� Option A → Uses ν instead of ω.
- �� Option C → Double the correct value.
- �� Option D → Incorrect calculation.
Used
- �� Substitution
Application:
- �� Convert frequency to angular speed before calculation.
Final Logic:
- �� dA/dt = 50π ≈ 157.
- "50 rev/s → 100π rad/s."
17 When determining the potential between the axle and rim of a metallic wheel with spokes rotating in a magnetic field,
1. the total emf is the sum of the emfs of individual spokes
2. the presence of the rim shorts out the spokes, resulting in zero emf
3. the emf is equivalent to that of a single solid rotating rod of the same radius
4. the emf depends on the thickness of the individual spokes
Choose the correct options:
�� Each spoke behaves like a rotating rod. �� Spokes are in parallel. �� Same emf as one rod.
- Each spoke generates the same emf. → Since all spokes connect the same axle and rim, they are effectively in parallel. → The wheel behaves like a single rotating rod of radius R.
- �� Option A → Parallel emfs do not add.
- �� Option B → Rim does not eliminate emf.
- �� Option D → Thickness does not determine induced emf.
Used
- �� Elimination
Application:
- �� Analyze spoke connection configuration.
Final Logic:
- �� Wheel acts as one rotating rod.
- "Wheel = One Rod."
18 Choose the correct statements about the parallel EMF configuration in a wheel:
1. The spokes act as identical emf sources connected in parallel.
2. The potential difference across any individual spoke equals the potential difference of the entire wheel.
3. The number of spokes alters the total internal resistance, but not the theoretical induced emf.
4. Adding more spokes increases the induced emf proportionally.
�� Spokes are parallel sources. �� Voltage remains same. �� Internal resistance may change.
- Statement 1 is correct because spokes connect the same axle and rim. → Statement 2 is correct because parallel branches have the same potential difference. → Statement 3 is correct because adding spokes can alter effective resistance but not emf. → Statement 4 is incorrect because parallel emfs do not add.
- �� Option B → Contains incorrect Statement 4.
- �� Option C → Contains incorrect Statement 4.
- �� Option D → Contains incorrect Statement 4.
Used
- �� Elimination
Application:
- �� Identify the incorrect statement about parallel sources.
Final Logic:
- �� Parallel branches keep the same emf.
- "Parallel → Same Voltage."
19 Horizontal Component Effects on a rotating wheel statements:
Statements:
1. A wheel rotating in a plane normal to H_E generates an emf proportional to H_E.
2. If the wheel is rotated perfectly parallel to H_E, the induced motional emf across its spokes is maximized.
3. 1 Gauss (G) equals 10⁻⁴ T, which is crucial for converting H_E into standard SI units.
4. Earth's magnetic field is a realistic source of a uniform B field over the area of a small wheel.
�� Maximum emf requires field normal to rotation plane. �� Unit conversion is correct. �� Earth's field is approximately uniform locally.
- Statement 1 is correct because emf is proportional to magnetic field strength. → Statement 2 is incorrect because emf is maximized when the wheel rotates in a plane normal to the field, not parallel to it. → Statement 3 is correct since 1 G = 10⁻⁴ T. → Statement 4 is correct for small laboratory dimensions.
- �� Option A → Contains incorrect Statement 2.
- �� Option C → Contains incorrect Statement 2.
- �� Option D → Contains incorrect Statement 2.
Used
- �� Elimination
Application:
- �� Identify the false statement regarding field orientation.
Final Logic:
- �� Statement 2 violates the condition for maximum flux cutting.
- "Normal Field → Maximum EMF."
20 If a wire of length l falls horizontally with a velocity v perpendicular to the horizontal component of the earth's magnetic field B, the motional emf is Blv. Thus, if a 10 m long wire falls at 5.0 m/s and the induced emf is 1.5 × 10⁻³ V, the horizontal component of the earth's magnetic field must be
�� ε = Blv. �� Rearrange for B. �� Substitute values.
- B = ε/(lv) → B = (1.5 × 10⁻³)/(10 × 5) → B = 3 × 10⁻⁵ T → B = 0.30 × 10⁻⁴ T
- �� Option B → Ten times larger than actual value.
- �� Option C → Half the correct value.
- �� Option D → Five times larger than actual value.
Used
- �� Substitution
Application:
- �� Rearrange ε = Blv and solve for B.
Final Logic:
- �� B = 0.30 × 10⁻⁴ T.
- "Find B? Divide by lv."
