CUET UG Physics Booster Test 3-Dipole Dynamics and Electrostatic Analogs
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QUESTION 1 OF 20
Identify the correct statements regarding the vector product dynamics of a magnetic dipole in a uniform magnetic field.
Statements:
1. The magnitude of torque is maximized when the dipole is perpendicular to the field.
2. The vector product m × B ensures the torque is perpendicular to both m and B.
3. The restoring torque drives the dipole toward the θ = 180° position.
4. If the uniform field B increases, the maximum possible torque increases proportionally.
QUESTION 2 OF 20
A bar magnet of magnetic moment 1.5 J T⁻¹ lies aligned with the direction of a uniform magnetic field of 0.22 T. What is the amount of work required by an external torque to turn the magnet so as to align its magnetic moment opposite to the field direction?
QUESTION 3 OF 20
Incorrect step in the conceptual derivation of magnetic potential energy.
QUESTION 4 OF 20
The scalar product representation of potential energy (-m·B) specifically establishes that
QUESTION 5 OF 20
Regarding the conditions for stable equilibrium of a magnetic dipole
QUESTION 6 OF 20
Match List I (Energy Values) with List II (Equilibrium Characteristics).
| List I | List II |
|---|---|
| 1. U = −mB | a. Arbitrary non-equilibrium state, θ = 120° |
| 2. U = +mB | b. Most stable position, θ = 0° |
| 3. U = 0 | c. Most unstable position, θ = 180° |
| 4. U = mB/2 | d. Neither maximum nor minimum, θ = 90° |
QUESTION 7 OF 20
By utilizing the mathematical replacements from electrostatics (E → B, p → m, 1/ε₀ → μ₀), the analogous equation for the electrostatic torque p × E translates perfectly to:
QUESTION 8 OF 20
Identify the correct statements regarding the conversion of constants between electrostatic and magnetic dipole analogies.
Statements:
1. The free space permittivity term 1/ε₀ is completely replaced by μ₀.
2. The 4π factor found in the denominator of electrostatic field equations remains in the denominator for magnetic field equations.
3. The relative magnetic permeability replaces the dielectric constant perfectly.
4. These replacements are strictly valid only for extremely short dipoles at very large distances (r >> l).
QUESTION 9 OF 20
The dependence on distance (r) for the far axial field of a short magnetic dipole and the electric field of a short electric dipole are respectively:
QUESTION 10 OF 20
Identify the correct statements regarding the vector form of the axial field equation.
Statements:
1. The vector BA is proportional to the magnetic moment vector m.
2. The direction of the axial field is exactly parallel to the dipole moment.
3. The magnitude falls off as the inverse cube of the distance r.
4. The formula assumes that the distance r is much less than the magnet's length l.
QUESTION 11 OF 20
A short bar magnet has an axial magnetic field magnitude of 9.6 × 10⁻⁵ T at a distance of 10 cm. If you move to a point 10 cm away on the equatorial line, the magnitude of the field BE will be:
QUESTION 12 OF 20
Incorrect statement regarding the directional relationship to the magnetic moment.
QUESTION 13 OF 20
According to the dipole analogy table, the formula for the external field torque:
QUESTION 14 OF 20
Based on the comparison of external field energy in the dipole analogy table, the energy values at 0°, 90°, and 180°:
QUESTION 15 OF 20
Match List I (Configurations of needle Q relative to dipole P) with List II (Equilibrium Status).
| List I | List II |
|---|---|
| 1. Q on normal bisector, mQ parallel to BP | a. Unstable, highest potential energy on axis |
| 2. Q on normal bisector, mQ anti-parallel to BP | b. Stable, lowest potential energy on axis |
| 3. Q on axis, mQ parallel to BP | c. Stable, lowest potential energy on bisector |
| 4. Q on axis, mQ anti-parallel to BP | d. Unstable, highest potential energy on bisector A.1-d, 2-c, 3-a, 4-b |
QUESTION 16 OF 20
Identify the correct statements concerning dipole interaction and determination of stable needle orientations.
Statements:
1. The system's potential energy relies on one dipole interacting with the magnetic field produced by the other dipole.
2. Equilibrium is unstable when the secondary dipole aligns anti-parallel to the local magnetic field of the primary dipole.
3. The lowest potential energy configuration among planar orientations occurs when the dipoles are collinear and parallel.
4. The magnetic field on the normal bisector acts exactly parallel to the primary dipole's magnetic moment.
QUESTION 17 OF 20
Identify the correct statement regarding the dynamics of a dipole in a non-uniform magnetic field.
QUESTION 18 OF 20
Why does an iron nail near a bar magnet experience an attractive net force?
QUESTION 19 OF 20
The alignment of a small compass needle is used to visualize the magnetic field. The alignment and the net field direction are:
QUESTION 20 OF 20
Regarding self-torque and internal forces in a current-carrying wire:
Test Complete!
Answer Review
1 Identify the correct statements regarding the vector product dynamics of a magnetic dipole in a uniform magnetic field.
Statements:
1. The magnitude of torque is maximized when the dipole is perpendicular to the field.
2. The vector product m × B ensures the torque is perpendicular to both m and B.
3. The restoring torque drives the dipole toward the θ = 180° position.
4. If the uniform field B increases, the maximum possible torque increases proportionally.
�� Torque on a magnetic dipole is τ = mB sinθ. �� Maximum torque occurs at θ = 90°. �� Torque is perpendicular to both m and B.
A magnetic dipole placed in a uniform magnetic field experiences a torque given by τ = m × B and its magnitude is τ = mB sinθ where θ is the angle between the magnetic moment and the magnetic field. Since sin90° = 1, the torque becomes maximum when the dipole is perpendicular to the magnetic field. The cross-product nature of the equation ensures that the torque vector is perpendicular to both the magnetic moment and the magnetic field. The purpose of this torque is to rotate the dipole toward the stable equilibrium position where the magnetic moment becomes parallel to the magnetic field (θ = 0°), not toward θ = 180°. Since the maximum torque is proportional to both m and B, increasing the magnetic field strength increases the maximum torque proportionally.
- �� Option B → Statement 3 is incorrect because stable equilibrium occurs at θ = 0°.
- �� Option C → Statement 3 is incorrect.
- �� Option D → Statement 3 is incorrect.
Used – Concept Application
- Application
- Use τ = mB sinθ and analyze the angular dependence of torque.
- Final Logic
- Statements 1, 2 and 4 follow directly from the torque equation, while Statement 3 is false.
"Perpendicular Gives Peak Torque."
2 A bar magnet of magnetic moment 1.5 J T⁻¹ lies aligned with the direction of a uniform magnetic field of 0.22 T. What is the amount of work required by an external torque to turn the magnet so as to align its magnetic moment opposite to the field direction?
�� Use magnetic potential energy. �� Initial angle θ = 0°. �� Final angle θ = 180°.
The potential energy of a magnetic dipole in a uniform magnetic field is U = -mB cosθ Initially, the dipole is aligned with the field: θ₁ = 0° Therefore, U₁ = -mB = -(1.5)(0.22) = -0.33 J Finally, the dipole is opposite to the field: θ₂ = 180° Therefore, U₂ = +mB = +(1.5)(0.22) = +0.33 J The work done by the external torque equals the increase in potential energy: W = U₂ - U₁ = 0.33 - (-0.33) = 0.66 J Thus, the required work is 0.66 J.
- �� Option A → Represents only mB, not the total energy change.
- �� Option C → The potential energy changes significantly.
- �� Option D → External work is positive because energy increases.
Used – Formula Application
- Application
- Apply U = -mB cosθ for initial and final orientations.
- Final Logic
- Work required equals the increase in magnetic potential energy, which is 0.66 J.
"Flip the Magnet → Energy Changes by 2mB."
3 Incorrect step in the conceptual derivation of magnetic potential energy.
�� Potential energy is derived from torque. �� Integration introduces a constant. �� The correct expression is U = -mB cosθ.
The torque acting on a magnetic dipole is τ = mB sinθ To rotate the dipole slowly, an external torque equal and opposite to the magnetic torque is applied. The work done by this external torque is stored as magnetic potential energy. Therefore, dU = mB sinθ dθ Integrating, U = -mB cosθ + C where C is the integration constant. By choosing the reference level of potential energy to be zero at θ = 90°, the constant becomes zero. The resulting expression is U = -mB cosθ = -m·B Thus, the integration does not give +mB cosθ. The negative sign is essential because the energy must be minimum when the dipole aligns with the magnetic field.
- �� Option A → Correct expression for magnetic torque.
- �� Option B → Correct interpretation of external work.
- �� Option C → Correct method for choosing the reference energy.
Used – Derivation Analysis
- Application
- Follow the integration process used to derive magnetic potential energy.
- Final Logic
- The correct integral yields -mB cosθ, not +mB cosθ.
"Energy Minus, Torque Plus."
4 The scalar product representation of potential energy (-m·B) specifically establishes that
�� U = -mB cosθ. �� Minimum energy occurs at θ = 0°. �� Stable equilibrium corresponds to minimum energy.
The magnetic potential energy of a dipole in a uniform magnetic field is U = -m·B = -mB cosθ When the magnetic moment is aligned with the magnetic field (θ = 0°), U = -mB which is the minimum possible value. This corresponds to stable equilibrium. When the dipole is opposite to the field (θ = 180°), U = +mB which is the maximum possible value and corresponds to unstable equilibrium. At θ = 90°, the potential energy is zero. The scalar product form therefore directly shows that the most stable configuration occurs when the dipole moment and magnetic field are parallel.
- �� Option A → At θ = 90°, potential energy is zero, not maximum.
- �� Option B → Potential energy depends on the scalar product m·B.
- �� Option D → Conservation of energy is not restricted to θ = 90°.
Used – Concept Application
- Application
- Analyze the expression U = -mB cosθ for different angular positions.
- Final Logic
- The most negative energy occurs when θ = 0°, meaning perfect alignment.
"Aligned Means Lowest Energy."
5 Regarding the conditions for stable equilibrium of a magnetic dipole
�� Stable equilibrium corresponds to minimum potential energy. �� The magnetic moment becomes parallel to the field. �� Torque becomes zero at equilibrium.
A magnetic dipole in a uniform magnetic field experiences a torque that tends to align its magnetic moment with the field. The magnetic potential energy is U = -mB cosθ The minimum value of U occurs when θ = 0°, meaning the magnetic moment is parallel to the magnetic field. This configuration corresponds to stable equilibrium because any small angular displacement increases the potential energy and produces a restoring torque that brings the dipole back to its equilibrium position. At equilibrium, the torque itself is zero because sin0° = 0. Thus, stable equilibrium is determined by minimum potential energy rather than maximum torque.
- �� Option A → Orthogonal orientation gives U = 0, not minimum energy.
- �� Option B → Zero energy does not necessarily imply stability.
- �� Option D → Torque is zero at stable equilibrium, not maximum.
Used – Concept Application
- Application
- Use the relationship between potential energy, torque and equilibrium.
- Final Logic
- Stable equilibrium occurs when U is minimum and the dipole is parallel to the field.
"Parallel is Peaceful."
6 Match List I (Energy Values) with List II (Equilibrium Characteristics).
| List I | List II |
|---|---|
| 1. U = −mB | a. Arbitrary non-equilibrium state, θ = 120° |
| 2. U = +mB | b. Most stable position, θ = 0° |
| 3. U = 0 | c. Most unstable position, θ = 180° |
| 4. U = mB/2 | d. Neither maximum nor minimum, θ = 90° |
�� Potential energy depends on orientation. �� Minimum energy corresponds to stable equilibrium. �� Maximum energy corresponds to unstable equilibrium.
The potential energy of a magnetic dipole in a uniform magnetic field is: U=-mBcosθ For θ = 0°: U=-mB which is the minimum potential energy and represents the most stable equilibrium position. For θ = 180°: U=+mB which is the maximum potential energy and represents the most unstable equilibrium position. For θ = 90°: U=0 This corresponds to neither a maximum nor a minimum value of potential energy. For θ = 120°: U=-mBcos120^∘U=-mB(, 1/2)U=mB/2 This corresponds to an arbitrary non-equilibrium state. Hence: 1 → b 2 → c 3 → d 4 → a Therefore, Option A is correct.
- �� Option B → Stable and unstable positions are interchanged.
- �� Option C → U = +mB is incorrectly matched.
- �� Option D → Multiple energy-state correspondences are incorrect.
Concept Application
- Application
- Use U=-mBcosθfor each given angle and identify the corresponding equilibrium state.
- Final Logic
- Minimum energy → Stable, Maximum energy → Unstable, Zero energy → Intermediate state.
- One Eighty Degree → Maximum
7 By utilizing the mathematical replacements from electrostatics (E → B, p → m, 1/ε₀ → μ₀), the analogous equation for the electrostatic torque p × E translates perfectly to:
�� Electric and magnetic dipoles have analogous torque equations. �� Torque is represented by a cross product. �� Direct substitution gives the magnetic form.
The torque acting on an electric dipole in an external electric field is: τ=p×E NCERT discusses the close analogy between electric dipoles and magnetic dipoles. Using the standard replacements: p→mE→B the corresponding magnetic torque expression becomes: τ=m×B This equation gives both the magnitude and direction of the torque experienced by a magnetic dipole in a uniform magnetic field. The magnitude is: τ=mBsinθ and the direction is determined using the right-hand rule. Therefore, the correct magnetic analogue of p × E is m × B.
- �� Option A → Reversing the order changes the direction of the vector.
- �� Option C → Dot product represents energy, not torque.
- �� Option D → μ₀ is not part of the torque expression.
NCERT Recall
- Application
- Recall the standard electrostatic-to-magnetic substitutions.
- Final Logic
- Replace p by m and E by B directly.
- Cross Means Torque
8 Identify the correct statements regarding the conversion of constants between electrostatic and magnetic dipole analogies.
Statements:
1. The free space permittivity term 1/ε₀ is completely replaced by μ₀.
2. The 4π factor found in the denominator of electrostatic field equations remains in the denominator for magnetic field equations.
3. The relative magnetic permeability replaces the dielectric constant perfectly.
4. These replacements are strictly valid only for extremely short dipoles at very large distances (r >> l).
�� Electric and magnetic dipole equations have similar forms. �� Constants transform systematically. �� The analogy is based on short-dipole approximations.
NCERT develops a mathematical analogy between electric dipoles and magnetic dipoles for points located far from the dipole. The substitutions are: E↔Bp↔m1/ε_0↔μ_0 and 1/4πε_0↔μ_0/4π Notice that the factor 4π remains unchanged in the denominator. Similarly, dielectric behavior in electrostatics corresponds conceptually to magnetic permeability in magnetism. The analogy is valid for short dipoles observed at distances much larger than the dipole length (r≫l), where dipole approximations are applicable. Therefore, all four statements are correct.
- �� Option A → Statement 2 is also correct.
- �� Option B → Statement 4 is also correct.
- �� Option C → Statement 1 is correct.
NCERT Recall
- Application
- Recall the complete correspondence table used in dipole analogies.
- Final Logic
- All listed replacements follow directly from NCERT dipole analogies.
- Epsilon → Mu
9 The dependence on distance (r) for the far axial field of a short magnetic dipole and the electric field of a short electric dipole are respectively:
�� Both are dipole fields. �� Both decrease rapidly with distance. �� Both follow inverse-cube dependence.
For a short magnetic dipole, the far axial magnetic field is: B_A=μ_0/4π2m/r^3 Similarly, the far axial electric field of a short electric dipole is: E_A=1/4πε_02p/r^3 In both cases, the field strength decreases as the inverse cube of the distance from the dipole. This inverse-cube dependence is a characteristic feature of dipole fields and distinguishes them from the inverse-square dependence observed for isolated charges and monopole-like sources. Therefore, both fields vary as: 1/r^3
- �� Option A → Magnetic dipole fields do not vary as 1/r².
- �� Option C → Neither field follows inverse-square dependence.
- �� Option D → Electric dipole fields also vary as 1/r³.
NCERT Recall
- Application
- Recall the axial field expressions for electric and magnetic dipoles.
- Final Logic
- Both dipole fields have inverse-cube dependence.
- Monopole Means Square
10 Identify the correct statements regarding the vector form of the axial field equation.
Statements:
1. The vector BA is proportional to the magnetic moment vector m.
2. The direction of the axial field is exactly parallel to the dipole moment.
3. The magnitude falls off as the inverse cube of the distance r.
4. The formula assumes that the distance r is much less than the magnet's length l.
�� Axial field is proportional to m. �� Direction is along the magnetic moment. �� The dipole approximation requires r >> l.
The axial magnetic field of a short magnetic dipole is: B_A=μ_0/4π2m/r^3 This expression shows that the field vector is directly proportional to the magnetic moment vector. Therefore, the direction of the axial field is parallel to the magnetic moment. The magnitude decreases as: 1/r^3 which is characteristic of dipole fields. The equation is derived under the short-dipole approximation: r≫l where r is the observation distance and l is the dipole length. Therefore, Statements 1, 2 and 3 are correct, while Statement 4 is incorrect.
- �� Option B → Statement 4 is incorrect.
- �� Option C → Statements 2 and 3 are also correct.
- �� Option D → Statement 4 is incorrect.
NCERT Recall
- Application
- Recall the vector form of the axial magnetic field equation.
- Final Logic
- Axial field ∝ m and decreases as 1/r³ for r >> l.
- Cube Law for Dipoles
11 A short bar magnet has an axial magnetic field magnitude of 9.6 × 10⁻⁵ T at a distance of 10 cm. If you move to a point 10 cm away on the equatorial line, the magnitude of the field BE will be:
�� Axial field is twice the equatorial field. �� Both measurements are taken at the same distance. �� Use the ratio BA = 2BE.
For a short magnetic dipole, the magnetic fields at the axial and equatorial positions are: B_A=μ_0/4π2m/r^3B_E=μ_0/4πm/r^3 Thus, B_A=2B_E Given: B_A=9.6×10^(-5) T Therefore, B_E=B_A/2B_E=9.6×10^(-5)/2B_E=4.8×10^(-5) T Hence, the magnetic field at the equatorial position is 4.8 × 10⁻⁵ T. Unit Verification The ratio is dimensionless, so the unit remains Tesla.
- �� Option A → Axial and equatorial fields are not equal.
- �� Option B → Twice the axial field value.
- �� Option C → Half of the correct equatorial field.
Substitution
- Application
- Use the standard NCERT relation between axial and equatorial magnetic fields.
- Final Logic
- B_E=B_A/2
- Equatorial Half
12 Incorrect statement regarding the directional relationship to the magnetic moment.
�� Equatorial field opposes m. �� Axial field aligns with m. �� Statement C incorrectly describes field-line behavior.
The magnetic field on the equatorial line of a short magnetic dipole is: B_E=-μ_0/4πm/r^3 The negative sign indicates that the equatorial magnetic field is opposite to the magnetic moment vector. Hence Statements A and B are correct. The axial magnetic field is: B_A=μ_0/4π2m/r^3 Therefore, the axial field points in the same direction as the magnetic moment, making Statement D correct. Statement C is incorrect because magnetic field lines outside a magnet emerge from the north pole and enter the south pole. Inside the magnet, they travel from south to north. The equatorial plane itself is not described as a region where field lines "travel from south pole back to north pole internally." Hence the statement is not a correct description of the equatorial field.
- �� Option A → Correct property of the equatorial field.
- �� Option B → Negative sign denotes opposite direction.
- �� Option D → Axial field is parallel to m.
NCERT Recall
- Application
- Recall the vector forms of axial and equatorial magnetic fields.
- Final Logic
- Equatorial field opposes m while axial field aligns with m.
- Equatorial Opposes m
13 According to the dipole analogy table, the formula for the external field torque:
�� Torque is represented by a cross product. �� Electric and magnetic dipoles show mathematical analogy. �� Cross products determine rotational effects.
For an electric dipole in an external electric field: τ=p×E For a magnetic dipole in an external magnetic field: τ=m×B Both expressions involve vector cross products. The magnitude of torque depends on the sine of the angle between the dipole moment and the external field: τ=pEsinθ or τ=mBsinθ The cross product nature of these equations shows that torque is fundamentally a rotational effect. It acts to align the dipole moment with the external field and determines the direction of rotation according to the right-hand rule. Therefore, the dipole analogy clearly demonstrates that cross products govern torque interactions in both electrostatic and magnetic systems.
- �� Option A → Dipoles tend to align parallel, not perpendicular.
- �� Option B → Torque depends on a cross product, not a scalar product.
- �� Option D → Torque is rotational, not attractive or repulsive.
NCERT Recall
- Application
- Recall the torque expressions for electric and magnetic dipoles.
- Final Logic
- Torque equations use vector cross products.
- Dot Means Energy
14 Based on the comparison of external field energy in the dipole analogy table, the energy values at 0°, 90°, and 180°:
�� Energy depends on cosθ. �� Parallel alignment gives minimum energy. �� Anti-parallel alignment gives maximum energy.
The potential energy of a dipole in an external field is: U=-pEcosθ for electric dipoles and U=-mBcosθ for magnetic dipoles. At: θ=0^∘U=-pEor-mB which is the minimum energy. At: θ=90^∘U=0 At: θ=180^∘U=+pEor+mB which is the maximum energy. Thus, both electric and magnetic dipoles exhibit identical energy behavior due to the mathematical analogy.
- �� Option B → The energy at 0° is minimum, not zero.
- �� Option C → Intermediate angles are not necessarily unstable.
- �� Option D → Energy depends on dipole moment and field, not mass.
Concept Application
- Application
- Substitute the given angles into the energy equation.
- Final Logic
- 0° → Minimum, 90° → Zero, 180° → Maximum.
- Anti-parallel = Maximum
15 Match List I (Configurations of needle Q relative to dipole P) with List II (Equilibrium Status).
| List I | List II |
|---|---|
| 1. Q on normal bisector, mQ parallel to BP | a. Unstable, highest potential energy on axis |
| 2. Q on normal bisector, mQ anti-parallel to BP | b. Stable, lowest potential energy on axis |
| 3. Q on axis, mQ parallel to BP | c. Stable, lowest potential energy on bisector |
| 4. Q on axis, mQ anti-parallel to BP | d. Unstable, highest potential energy on bisector A.1-d, 2-c, 3-a, 4-b |
�� Stable equilibrium occurs when the dipole aligns with the local field. �� Anti-parallel alignment gives unstable equilibrium. �� Axis and bisector fields have different directions.
The stability of a magnetic dipole depends on its orientation relative to the local magnetic field produced by another dipole. On the axis of dipole P, the magnetic field is directed along the magnetic moment of P. Therefore, when Q is placed on the axis and its magnetic moment is parallel to the local field, the configuration has minimum potential energy and is stable. The anti-parallel orientation corresponds to maximum potential energy and unstable equilibrium. On the normal bisector, the magnetic field is opposite to the magnetic moment of P. Consequently, a dipole aligned parallel to the local field achieves minimum potential energy and stable equilibrium, while an anti-parallel orientation gives unstable equilibrium. Thus: 1 → c 2 → d 3 → b 4 → a
- �� Option B → Axis and bisector configurations are incorrectly interchanged.
- �� Option C → Unstable bisector condition is mismatched.
- �� Option D → Stable and unstable states are reversed.
Concept Application
- Application
- Determine the local magnetic field direction first, then apply the condition for stable equilibrium.
- Final Logic
- Parallel to local field → Stable; Anti-parallel to local field → Unstable.
- Anti-parallel Local Field = Unstable
16 Identify the correct statements concerning dipole interaction and determination of stable needle orientations.
Statements:
1. The system's potential energy relies on one dipole interacting with the magnetic field produced by the other dipole.
2. Equilibrium is unstable when the secondary dipole aligns anti-parallel to the local magnetic field of the primary dipole.
3. The lowest potential energy configuration among planar orientations occurs when the dipoles are collinear and parallel.
4. The magnetic field on the normal bisector acts exactly parallel to the primary dipole's magnetic moment.
�� Dipole interaction energy depends on the local magnetic field. �� Anti-parallel alignment gives unstable equilibrium. �� Collinear parallel dipoles correspond to minimum energy.
The potential energy of a dipole system arises because one magnetic dipole experiences the magnetic field produced by the other dipole. Thus, the interaction energy is determined by: U=-m⋅B Stable equilibrium occurs when the magnetic moment aligns parallel to the local magnetic field, producing minimum potential energy. If the dipole is oriented anti-parallel to the local field, the potential energy becomes maximum and the equilibrium becomes unstable. Among common planar configurations, the lowest energy state occurs when the dipoles are arranged collinearly with their magnetic moments parallel. In this arrangement, the interaction is most favorable energetically. On the normal bisector of a dipole, however, the magnetic field is directed opposite to the magnetic moment of the primary dipole. Therefore Statement 4 is incorrect.
- �� Option B → Statement 4 is incorrect.
- �� Option C → Statement 4 is incorrect.
- �� Option D → Statement 4 is incorrect.
Concept Application
- Application
- Determine the local magnetic field direction and apply the condition for minimum potential energy.
- Final Logic
- Parallel to local field gives stable equilibrium; anti-parallel gives unstable equilibrium.
- Anti-parallel → Unstable
17 Identify the correct statement regarding the dynamics of a dipole in a non-uniform magnetic field.
�� Non-uniform fields produce unequal pole forces. �� Unequal forces create a net force. �� Torque may also be present.
In a non-uniform magnetic field, the magnetic field strength is different at different positions. Consequently, the north and south poles of a magnetic dipole experience forces of unequal magnitudes. Since the forces acting on the two poles are not equal, they do not completely cancel. As a result, the dipole experiences a net force directed toward the region of stronger magnetic field. Additionally, if the dipole is not aligned with the magnetic field, a torque may also act on it. Therefore, a dipole placed in a non-uniform magnetic field can simultaneously experience both force and torque. This behavior differs from that in a uniform magnetic field, where equal and opposite pole forces cancel, leaving only torque.
- �� Option A → This is true only for a perfectly uniform magnetic field.
- �� Option C → Unlike poles attract each other.
- �� Option D → Non-uniform fields can produce torque as well as force.
NCERT Recall
- Application
- Compare the behavior of a dipole in uniform and non-uniform magnetic fields.
- Final Logic
- Unequal magnetic field strengths at the poles produce a net force.
- Non-uniform → Force + Torque
18 Why does an iron nail near a bar magnet experience an attractive net force?
�� Iron becomes magnetized by induction. �� Opposite poles are induced near the magnet. �� The closer attractive force dominates.
When an iron nail is brought near a bar magnet, the magnetic field of the magnet induces magnetization in the nail. The end of the nail nearest the magnet develops a magnetic pole opposite to the nearby pole of the magnet. Since the magnetic field around the magnet is non-uniform, the attractive force on the nearer induced pole is stronger than any force acting on the farther end of the nail. As magnetic force decreases rapidly with distance, the attraction at the near end dominates. Consequently, the nail experiences a net attractive force toward the magnet. This effect explains why iron objects are drawn toward permanent magnets even though they may initially be unmagnetized.
- �� Option A → Iron is not behaving as a perfect diamagnetic material.
- �� Option B → Magnetic monopoles have not been observed.
- �� Option C → Torque and force arise from different physical effects.
Concept Application
- Application
- Analyze induced magnetization and the effect of distance-dependent magnetic forces.
- Final Logic
- The closer induced opposite pole experiences the stronger attraction.
- Induced Pole Nearer → Stronger Attraction
19 The alignment of a small compass needle is used to visualize the magnetic field. The alignment and the net field direction are:
�� A compass aligns along the magnetic field. �� The needle indicates local field direction. �� Field-line mapping uses this principle.
A magnetic compass consists of a small magnetic dipole free to rotate. When placed in a magnetic field, it experiences a torque that aligns its magnetic moment along the local magnetic field direction. Therefore, the direction of the compass needle becomes identical to the direction of the magnetic field at that point. By placing the compass at various positions, one can determine the direction of the magnetic field throughout the surrounding space. This method forms the basis for constructing magnetic field-line diagrams around magnets, current-carrying conductors and solenoids. Hence, both the alignment of the compass needle and the net magnetic field direction are identical.
- �� Option B → The needle does not align opposite to the field.
- �� Option C → The needle is not perpendicular to the field.
- �� Option D → Alignment follows the field direction.
NCERT Recall
- Application
- Recall how magnetic field lines are experimentally mapped.
- Final Logic
- Compass direction equals local magnetic field direction.
- Compass Shows Field
20 Regarding self-torque and internal forces in a current-carrying wire:
�� A current element does not act on itself. �� Self-torque is absent. �� Different elements of the wire can interact.
A current element cannot exert a magnetic force or torque on itself. Therefore, self-force and self-torque are absent for an individual element of a current-carrying conductor. However, different elements of the same conductor can exert magnetic forces on one another. These internal magnetic interactions are real and contribute to the mechanical behavior of current-carrying conductors. Thus, while self-torque is absent, internal forces between different parts of the wire are present. This distinction is important in understanding the magnetic forces acting within loops, coils and other current-carrying structures. Therefore, the correct combination is: • Self-torque → Absent • Internal forces → Present
- �� Option A → Self-torque is absent.
- �� Option C → Internal forces do exist.
- �� Option D → Internal magnetic forces are present.
NCERT Recall
- Application
- Distinguish between self-action and interaction between different current elements.
- Final Logic
- An element cannot act on itself, but different wire elements can interact magnetically.
- Internal Yes
