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Physics (Class 12)November 13, 2026
Physics (Class 12)2-4 Questions (8-16 Marks)15 Free Practice MCQs

Moving Charges and Magnetism NEET Syllabus & 15-MCQ Online Test

Complete NTA NEET 2027 chapter syllabus breakdown, 5-year question weightage analysis, and 15 free NCERT line-by-line MCQs with official +4 / -1 marking.

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Moving Charges and Magnetism 15-MCQ Test

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Question 1 of 15Magnetic field due to a circulating charge (electron)

In a hydrogen atom, the electron is making 6.6×10156.6 \times 10^{15} revolutions per second around the nucleus in an orbit of radius 0.53 A˚0.53 \text{ \AA}. The magnetic field produced at the center of the orbit is:

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Reviewed by NEETnova Academic Council. Updated for NEET 2027 Syllabus.

Official NTA Data Verified

Comprehensive Master Guide: Moving Charges and Magnetism for NEET UG


Section 1: Official NTA NEET Syllabus & Sub-Topic Checklist

To secure a top percentile in NEET UG Physics, preparation must align strictly with the National Testing Agency (NTA) blueprint and NCERT Class 12 textbooks (Part 1, Chapter 4).

Detailed Sub-Topic Checklist

  • Concept of Magnetic Field & Oersted's Experiment: Evidence of magnetic field due to current-carrying conductors.
  • Biot-Savart Law: Vector form, magnitude, and direction via Right-Hand Thumb Rule.
  • Application of Biot-Savart Law: Magnetic field due to a circular current-carrying loop at its center and along its axis.
  • Ampere’s Circuital Law: Statement, proof, and its application to infinitely long straight wire, straight solenoid, and toroid (qualitative/quantitative treatment).
  • Lorentz Force: Magnetic force on a moving charge (F⃗=q(v⃗×B⃗)\vec{F} = q(\vec{v} \times \vec{B})), magnetic force on a current-carrying conductor (F⃗=I(L⃗×B⃗)\vec{F} = I(\vec{L} \times \vec{B})).
  • Motion of Charged Particle in Uniform Fields: Uniform magnetic field (circular path, radius, time period, frequency) and combined uniform electric and magnetic fields (Velocity Selector, Cyclotron principle, limitations, and resonance condition).
  • Force between Two Parallel Current-Carrying Conductors: Definition of standard Ampere, attractive vs. repulsive forces based on current directions.
  • Torque on a Current Loop: Magnetic dipole moment (M⃗=NIAn^\vec{M} = NIA\hat{n}), torque in a uniform magnetic field (τ⃗=M⃗×B⃗\vec{\tau} = \vec{M} \times \vec{B}).
  • Moving Coil Galvanometer: Principle, construction, current sensitivity, voltage sensitivity, and conversion into an ammeter and a voltmeter using shunt and series resistances.

NTA NEET UG Syllabus: Retained vs. Deleted Topics

Sub-Topic / ConceptStatus for NEET UGAcademic Directive / Rationale
Biot-Savart Law & Circular Loop ApplicationsRETAINEDHigh numerical and conceptual yield; frequently tested via direct formulas.
Ampere's Circuital Law & Solenoid/ToroidRETAINEDCore foundation; derivations omitted in NCERT rationalization, but final formulas are essential.
Lorentz Force & Motion in Magnetic FieldRETAINEDCritical for conceptual and graphical problems (v⃗⊥B⃗\vec{v} \perp \vec{B} and v⃗∥B⃗\vec{v} \parallel \vec{B}).
Cyclotron (Detailed Construction/Working)DELETEDRemoved from rationalized NCERT; however, the cyclotron frequency formula (f=qB/2πmf = qB / 2\pi m) is retained as an application of uniform circular motion in magnetic fields.
Earth's Magnetism & Magnetic ElementsMOVEDTransferred to Chapter 5 ("Magnetism and Matter") in rationalized NCERT; do not study under Moving Charges.

Section 2: Previous 5-Year NEET Question Distribution (2022-2026) & Marks Weightage

Moving Charges and Magnetism is a high-yielding chapter in NEET Physics, consistently contributing 2 to 4 questions (8 to 16 marks) per paper.

Sub-Topic Question Distribution (NEET 2024–2026)

Sub-TopicNEET 2022NEET 2023NEET 2024NEET 2025NEET 2026Estimated Weightage (%)
Biot-Savart Law & Magnetic Field of Loops11101~25%
Ampere’s Law, Solenoid & Toroid10111~25%
Lorentz Force & Particle Motion in Fields11121~30%
Parallel Conductors & Torque on Loop01010~10%
Moving Coil Galvanometer & Conversions11101~10%

NEETnova Strategic Insight

  1. Trend Analysis: NTA has shifted away from direct, single-formula substitution questions toward multi-concept integration (e.g., combining Newton's laws/kinematics with magnetic Lorentz force, or combining Ampere's law with electromagnetic induction).
  2. Question Styles:
  • Assertion-Reasoning: Frequently tests the vector nature of the Biot-Savart law and the independence of magnetic force on particle speed component parallel to the field (v⃗∥\vec{v}_\parallel).
  • Matching Lists: Commonly used for matching galvanometer conversions, magnetic field formulas for various geometries, and dimensional analysis of physical quantities (μ0\mu_0, B⃗\vec{B}, magnetic moment).
  • Graphical Analysis: Trajectory plots of charged particles entering transverse magnetic fields with varying momenta.

Section 3: High-Yield NCERT Line-by-Line Core Concepts & Exceptions

1. Biot-Savart Law & Magnetic Field Calculations

The magnetic field dB⃗d\vec{B} due to an element dldl carrying current II at a distance rr is given by: dB⃗=μ04πI(dl×r^)r2=μ04πIdlsin⁡θr2d\vec{B} = \frac{\mu_0}{4\pi} \frac{I (dl \times \hat{r})}{r^2} = \frac{\mu_0}{4\pi} \frac{I dl \sin\theta}{r^2}

  • Permeability of Free Space (μ0\mu_0): 4π×10−7 T⋅m⋅A−14\pi \times 10^{-7} \, \text{T}\cdot\text{m}\cdot\text{A}^{-1} (or Wb⋅A−1⋅m−1\text{Wb}\cdot\text{A}^{-1}\cdot\text{m}^{-1}).
  • Circular Loop:
  • At the center: B=μ0I2RB = \frac{\mu_0 I}{2R} (for NN turns: B=μ0NI2RB = \frac{\mu_0 N I}{2R}).
  • Along the axis at distance xx from the center: B=μ0IR22(R2+x2)3/2B = \frac{\mu_0 I R^2}{2(R^2 + x^2)^{3/2}}

2. Ampere’s Circuital Law

Line integral of magnetic field B⃗\vec{B} around any closed loop is equal to μ0\mu_0 times the total current IenclosedI_{\text{enclosed}} threading through the loop: ∮B⃗⋅dl⃗=μ0Ienclosed\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enclosed}}

  • Infinitely Long Straight Wire: B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}
  • Long Solenoid (tightly wound): B=μ0nIB = \mu_0 n I (where n=N/Ln = N/L is the number of turns per unit length). Note: B=0B = 0 outside the ideal solenoid; at the ends of a semi-infinite solenoid, B=12μ0nIB = \frac{1}{2}\mu_0 n I.
  • Toroid: B=μ0nI=μ0NI2πrB = \mu_0 n I = \frac{\mu_0 N I}{2\pi r} (where rr is the mean radius).

3. Lorentz Force & Motion of Charged Particles

Total force on a charge qq moving with velocity v⃗\vec{v} in combined electric (E⃗\vec{E}) and magnetic (B⃗\vec{B}) fields: F⃗=qE⃗+q(v⃗×B⃗)\vec{F} = q\vec{E} + q(\vec{v} \times \vec{B})

Trajectory Analysis based on Angle θ\theta between v⃗\vec{v} and B⃗\vec{B}:

  • θ=0∘\theta = 0^\circ or 180∘180^\circ: Particle moves in an unaccelerated straight line (Fm=0F_m = 0).
  • θ=90∘\theta = 90^\circ: Particle moves in a uniform circular path.
  • Magnetic force provides the centripetal force: mv2R=qvB  ⟹  R=mvqB=pqB=2mKqB\frac{mv^2}{R} = qvB \implies R = \frac{mv}{qB} = \frac{p}{qB} = \frac{\sqrt{2mK}}{qB}
  • Time period (TT): T=2πmqBT = \frac{2\pi m}{qB} (Independent of velocity vv and radius RR).
  • Frequency (ff): f=qB2πmf = \frac{qB}{2\pi m}
  • 0∘<θ<90∘0^\circ < \theta < 90^\circ: Particle traces a helical path.
  • Pitch (pp): p=vcos⁡θ×T=2πmvcos⁡θqBp = v \cos\theta \times T = \frac{2\pi m v \cos\theta}{qB}

4. Force between Two Parallel Conductors

Force per unit length (Fl\frac{F}{l}) between two long parallel conductors separated by distance dd carrying currents I1I_1 and I2I_2: Fl=μ0I1I22πd\frac{F}{l} = \frac{\mu_0 I_1 I_2}{2\pi d}

  • Direction Rule: Currents in the same direction attract each other; currents in opposite directions repel each other. (Exception/Inversion to electrostatic charge rules: like currents attract, unlike currents repel).

5. Torque on a Current Loop & Moving Coil Galvanometer (MCG)

  • Magnetic Dipole Moment: M⃗=IAn^\vec{M} = I A \hat{n} (Direction of n^\hat{n} given by Right-Hand Thumb Rule).
  • Torque: τ⃗=M⃗×B⃗  ⟹  τ=NIABsin⁡θ\vec{\tau} = \vec{M} \times \vec{B} \implies \tau = NIAB \sin\theta (where θ\theta is the angle between area vector A⃗\vec{A} and B⃗\vec{B}).
  • Galvanometer Principle: Deflection θ\theta is directly proportional to current II because a radial magnetic field ensures sin⁡θ=1\sin\theta = 1: I=(kNBA)ϕ  ⟹  I=GϕI = \left(\frac{k}{NBA}\right) \phi \implies I = G \phi where kk is the restoring torque per unit twist, and GG is the galvanometer constant.
  • Conversion Formulas:
  • Ammeter (Measuring range II with galvanometer resistance GG and full-scale current IgI_g): Shunt resistance S=IgGI−Ig\text{Shunt resistance } S = \frac{I_g G}{I - I_g} Effective resistance of ammeter: RA=GSG+S≈SR_A = \frac{GS}{G+S} \approx S (very small).
  • Voltmeter (Measuring range VV with galvanometer resistance GG and full-scale current IgI_g): Series resistance R=VIg−G\text{Series resistance } R = \frac{V}{I_g} - G Effective resistance of voltmeter: RV=G+RR_V = G + R (very large).

Section 4: Negative Marking Pitfalls & Calculation/Conceptual Traps

  1. Direction of Magnetic Force (v⃗×B⃗\vec{v} \times \vec{B}):
  • Trap: Applying the Right-Hand Rule incorrectly for negative charges (electrons).
  • Correction: For a negative charge (q=−∣e∣q = -|e|), the direction of the magnetic force is strictly opposite to the vector cross-product v⃗×B⃗\vec{v} \times \vec{B}. Always use the Left-Hand Rule for negative charges or reverse the final vector direction.
  1. Angle Definitions in Torque and Magnetic Flux:
  • Trap: Using the angle θ\theta between the plane of the coil and the magnetic field B⃗\vec{B}.
  • Correction: The formula τ=NIABsin⁡θ\tau = NIAB \sin\theta uses θ\theta as the angle between the normal to the coil (area vector A⃗\vec{A}) and B⃗\vec{B}. If the problem states "coil makes an angle α\alpha with the magnetic field," then θ=90∘−α\theta = 90^\circ - \alpha.
  1. Units and Conversion Traps:
  • Trap: Mixing CGS and SI units, or failing to convert centimeters to meters and Gauss to Tesla (1 Gauss=10−4 Tesla1 \, \text{Gauss} = 10^{-4} \, \text{Tesla}).
  • Correction: Always convert radius rr to meters and magnetic field BB to Teslas before computing radii (R=mvqBR = \frac{mv}{qB}) or forces.
  1. Solenoid Magnetic Field Boundary Conditions:
  • Trap: Applying B=μ0nIB = \mu_0 n I blindly to finite solenoids.
  • Correction: The formula B=μ0nIB = \mu_0 n I applies strictly to infinite solenoids or points deep inside the interior where length L≫RL \gg R. For points near the ends of a finite solenoid, the field drops to approximately half: Bend=12μ0nIB_{\text{end}} = \frac{1}{2}\mu_0 n I.
  1. Galvanometer Conversion Terminology:
  • Trap: Confusing current sensitivity (ϕI=\fracNBAk\frac{\phi}{I} = \fracNBAk) with voltage sensitivity (ϕV=NBAkRG\frac{\phi}{V} = \frac{NBA}{k R_G}).
  • Correction: Increasing the number of turns NN increases current sensitivity directly, but does not necessarily increase voltage sensitivity proportionally because resistance RGR_G also increases with NN.

Section 5: Step-by-Step 5-Day Mastery Strategy for NEET Aspirants

Day 1: Biot-Savart Law & Magnetic Field Geometry

  • Focus: Master vector integration for circular arcs, straight wires, and coaxial rings.
  • NCERT Reading: Chapter 4, Sections 4.1, 4.2, and 4.3.
  • Problem Practice: Solve 30 MCQs focusing on magnetic fields at the center and axis of circular loops with varying fractions of a circle (34th\frac{3}{4}\text{th} loop, semi-circle).

Day 2: Ampere’s Circuital Law, Solenoid & Toroid

  • Focus: Symmetry exploitation using Ampere's law; deriving and applying formulas for infinite sheets, solenoids, and toroids.
  • NCERT Reading: Chapter 4, Section 4.4.
  • Problem Practice: Solve 25 MCQs involving enclosed currents, hollow cylinders (internal vs. external magnetic fields), and solenoid turn-density alterations.

Day 3: Lorentz Force & Motion in Magnetic/Electric Fields

  • Focus: Trajectory dynamics (circular, helical, rectilinear); radius, time period, and pitch calculations.
  • NCERT Reading: Chapter 4, Section 4.5.
  • Problem Practice: Solve 35 high-yield numericals on proton/alpha-particle trajectory comparisons in uniform magnetic fields (mα=4mp,qα=2qpm_\alpha = 4m_p, q_\alpha = 2q_p).

Day 4: Parallel Conductors, Torque & Moving Coil Galvanometer

  • Focus: Force per unit length between parallel wires, torque on rectangular loops, and galvanometer conversions (shunt and multiplier resistors).
  • NCERT Reading: Chapter 4, Sections 4.6, 4.7, and 4.8.
  • Problem Practice: Solve 30 numericals on converting a galvanometer of resistance GG into an ammeter of range II and voltmeter of range VV.

Day 5: Full-Chapter Mixed Question Bank & Error Analysis

  • Focus: Time-bound test simulation (45 questions in 45 minutes) covering previous years' NEET questions and assertion-reasoning items.
  • Task: Review every incorrect answer, record conceptual slips in a revision notebook, and re-read highlighted NCERT summary points.

Chapter Sub-Topics for Revision

1Biot-Savart Law and Ampere's Circuital Law
2Lorentz Force, Motion of Charge in Combined Electric & Magnetic Fields
3Force between Two Parallel Conductors and Moving Coil Galvanometer
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Common queries and official guidelines verified by NEETnova Academic Council.

Moving Charges and Magnetism is a high-yield chapter in NEET Physics, typically contributing 2-4 questions (8-16 marks) every year. Key topics like Ampere's Circuital Law, Lorentz Force, and the Moving Coil Galvanometer are recurrent favorites in NEET exams.

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