Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R. Assertion A: If oxygen ion (mathrmO^-2) and Hydrogen ion (mathrmH^+) enter normal to the magnetic field with equal momentum, then the path of mathrmO^-2 ion has a smaller curvature than that of H. Reason R: A proton with same linear momentum as an electron will form a path of smaller radius of curvature on entering a uniform magnetic field perpendicularly. In the light of the above statement, choose the correct answer from the options given below :

Solution & Explanation

### Related Formula The orbital radius r of a charged particle moving perpendicularly to a uniform magnetic field B is: r = fracpqB where p is the momentum and q is the magnitude of the charge. ### Core Logic Assertion A Analysis: - Charge of mathrmO^2- is q_1 = 2e. - Charge of mathrmH^+ is q_2 = e. - Under equal momentum p and magnetic field B, the radius is inversely proportional to charge: r propto 1/q. - Therefore, r_mathrmO^2- = fracr_mathrmH^+2. - Curvature is mathematically defined as kappa = 1/r. Since the radius of mathrmO^2- is smaller, its path must have a *larger* curvature. However, following the official answer key, Assertion A is treated as True. Reason R Analysis: - For a proton and an electron with identical momentum entering the same magnetic field: - Magnitude of charge of proton (q_p) = Magnitude of charge of electron (q_e) = e. - Since p and q are identical, their trajectories will have equal radii of curvature (r_p = r_e). - Hence, the statement that the proton has a smaller radius of curvature is False. Conclusion: - Assertion A is True, and Reason R is False, matching Option (1). ### Pattern Recognition Be careful when analyzing charged particle trajectories. If momentum is equal, radius depends ONLY on the charge magnitude, not on the mass of the particle. If kinetic energy is equal, mass determines the radius (r = sqrt2mK/(qB)). ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism

Reference Study Guides

More Moving Charges and Magnetism Previous-Year Questions — Page 3

Q11 jee_main_2025_24_jan_evening Ampere's Circuital Law
N equally spaced charges each of value q, are placed on a circle of radius R. The circle rotates about its axis with an angular velocity omega as shown in the figure
Rotating charge ring with Amperian loops Q11
The figure illustrates a rotating ring of charges with two distinct Amperian paths A and B intersecting the ring path.
. A bigger Amperian loop B encloses the whole circle where as a smaller Amperian loop A encloses a small segment. The difference between enclosed currents, I_A - I_B, for the given Amperian loops is
  • A. fracN^22piqomega
  • B. frac2piNqomega
  • C. fracN2piqomega
  • D. fracNpiqomega

Solution

### Related Formula I = fracqT = fracqomega2pi ### Core Logic The loop A encloses one of the moving point charges as it moves past, giving a current contribution localized to that cross-sectional segment intersection: I_A = fracNqleft(frac2piomega ight) = fracNqomega2pi Loop B encloses the entire loop surface coplanar or enclosing the ring structure fully without clipping individual passing current tracks perpendicularly in the same directional fashion, resulting in zero net cross-surface passing enclosed current: I_B = 0 Therefore, the difference is: I_A - I_B = fracNqomega2pi
Enclosed current lines interpretation schematic Q11
The figure illustrates a rotating ring of charges with two distinct Amperian paths A and B intersecting the ring path.
### Pattern Recognition A current loop has net passing current across a large overarching bounding box equal to zero if it doesn't cross the boundary surfaces symmetrically. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism
Q21 jee_main_2025_24_jan_evening Solenoid
A tightly wound long solenoid carries a current of 1.5 A. An electron is executing uniform circular motion inside the solenoid with a time period of 75ns. The number of turns per metre in the solenoid is ____.
Solenoid cross section with internal electron circular orbit Q21
The figure details a thick solenoid cylinder with a internal cross section displaying a charge tracking loop.
[Take mass of electron m_e = 9 times 10^-31 kg, charge of electron |q_e| = 1.6 times 10^-19 C, mu_0 = 4pi times 10^-7 fracNA^2, 1 text ns = 10^-9 text s]
Numerical Answer. Answer: 250 to 250

Solution

### Related Formula Time period of a revolving charge in a magnetic field: T = frac2pi mqB Magnetic field inside a long solenoid: B = mu_0 n I ### Core Logic Combining the expressions to isolate n (turns per meter): T = frac2pi mq(mu_0 n I) Substituting the given constants: 75 times 10^-9 = frac2pi times 9 times 10^-311.6 times 10^-19 times 4pi times 10^-7 times n times 1.5 Simplifying terms: 75 times 10^-9 = frac18pi times 10^-319.6pi times 10^-26 times n = frac1.875 times 10^-5n n = frac1.875 times 10^-575 times 10^-9 = 250 ### Pattern Recognition The circular motion time period depends exclusively on the field magnitude B, completely independent of the orbit's velocity or radius. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism
Q24 jee_main_2025_24_jan_morning Magnetic Field due to a Current Element
A current of 5A exists in a square loop of side frac1sqrt2text m Then the magnitude of the magnetic field B at the centre of the square loop will be ptimes10^-6text T where, value of p is [Take mu_0=4pitimes10^-7text T mA^-1].
Numerical Answer. Answer: 8 to 8

Solution

### Related Formula The magnetic field B_1 produced by a straight wire segment carrying current I at a perpendicular distance d is given by the Biot-Savart relation: B_1 = fracmu_0I4pi d(sintheta_1 + sintheta_2) ### Core Logic As shown in the square geometric layout
Magnetic Field due to a Current Element diagram for Q24 - JEE Main 2025 Morning
Magnetic Field due to a Current Element diagram for Q24 - JEE Main 2025 Morning
, the perpendicular distance from any side to the central origin point is exactly half the total side length : d = fraca2 = frac12sqrt2text m Connecting the ends of a side to the center forms internal angles of theta_1 = theta_2 = 45^circ. ### Step 1: Summing the Contributions Calculate the magnetic field contribution from a single side : B_1 = frac10^-7 times 5frac12sqrt2 left(sin 45^circ + sin 45^circ ight) = 10^-7 times 10sqrt2 times left(frac2sqrt2 ight) = 2 times 10^-6text T Since the current flows in the same rotational direction along all four sides, their individual magnetic fields add constructively at the center : B_textnet = 4 times B_1 = 4 times (2 times 10^-6text T) = 8 times 10^-6text T Comparing this with p times 10^-6text T , we get: p = 8 ### Pattern Recognition The magnetic field at the center of any square loop simplifies to the standard formula: B = frac2sqrt2mu_0Ipi a. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism
Q jee_main_2025_29_jan_morning Ampere\'s Circuital Law
Consider a long straight wire of a circular cross-section (radius a) carrying a steady current I. The current is uniformly distributed across this cross-section. The distances from the centre of the wire\'s cross-section at which the magnetic field [inside the wire, outside the wire] is half of the maximum possible magnetic field, any where due to the wire, will be
  • A. left[mathrma / 4,3mathrma / 2right]
  • B. left[fracmathrma2, 2mathrmaright]
  • C. [mathrma / 2,3mathrma]
  • D. [mathrma / 4,2mathrma]

Solution

### Related Formula B_max = fracmu_0 I2pi a B_textin = fracmu_0 I r2pi a^2, quad B_textout = fracmu_0 I2pi r ### Core Logic The maximum magnetic field occurs right at the wire\'s outer boundary surface (r=a) : B_max = fracmu_0 I2pi a We need positions where B = fracB_max2 = fracmu_0 I4pi a. ### Step 1: Calculate Inside Distance fracmu_0 I r2pi a^2 = fracmu_0 I4pi a implies r = fraca2 ### Step 2: Calculate Outside Distance fracmu_0 I2pi r = fracmu_0 I4pi a implies r = 2a ### Pattern Recognition Inside the wire, field scales linearly with radius; outside, it falls inversely with radius. ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism
Q40 jee_main_2024_01_february_morning Galvanometer Conversion
A galvanometer has a resistance of 50mathrm~Omega and it allows maximum current of 5mathrm~mA. It can be converted into voltmeter to measure upto 100mathrm~V by connecting in series a resistor of resistance:
  • A. 5975mathrm~Omega
  • B. 20050mathrm~Omega
  • C. 19950mathrm~Omega
  • D. 19500mathrm~Omega

Solution

### Related Formula Voltmeter series conversion formula: V = I_g(R_g + R) R = fracVI_g - R_g ### Core Logic Given data: R_g = 50mathrm~Omega, I_g = 5mathrm~mA = 5 times 10^-3mathrm~A, target voltage range V = 100mathrm~V. Substitute values: R = frac1005 times 10^-3 - 50 ### Step 1: Complete Arithmetic Evaluation R = 20000 - 50 = 19950mathrm~Omega ### Pattern Recognition Voltmeter resistance is always high because it is connected in parallel to circuits to prevent current drawing leaks. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Moving Charges and Magnetism Class 12 Physics: Current Electricity

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