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Magnetic Effect of Electric Current: Oersted's Experiment, Right Hand Thumb Rule, Solenoid, Electromagnet, Fleming's Left Hand Rule, Electric Motor, and Complete CBSE Class 10 Guide

A comprehensive guide to the magnetic effect of electric current for CBSE Class 10 Physics Chapter 13 — Oersted's discovery, magnetic field patterns due to straight wire, circular loop, and solenoid, right hand thumb rule, Maxwell's right hand screw rule, electromagnets, force on current-carrying conductor in magnetic field, Fleming's left hand rule, working of an electric motor, and five CBSE exam-ready solved problems.
6 August 2026 by
Magnetic Effect of Electric Current: Oersted's Experiment, Right Hand Thumb Rule, Solenoid, Electromagnet, Fleming's Left Hand Rule, Electric Motor, and Complete CBSE Class 10 Guide
AJKANT OVERSEAS, AJKANT OVERSEAS
● CBSE Class 10 Physics — Chapter 13: Magnetic Effect of Electric Current

In 1820, Danish physicist Hans Christian Oersted made a chance discovery that would transform science and engineering: a wire carrying electric current deflects a nearby compass needle. This simple observation revealed for the first time that electricity and magnetism are not separate phenomena but are deeply connected — a discovery that directly led to the invention of the electric motor, the generator, the transformer, and eventually, the electrification of the entire world.

The magnetic effect of electric current is the principle that a current-carrying conductor creates a magnetic field around itself. The shape and strength of this magnetic field depend on the configuration of the conductor — whether it is a straight wire, a circular loop, or a solenoid. When a current-carrying conductor is placed inside an external magnetic field, it experiences a force (which is the working principle of every electric motor ever built). Conversely, when a conductor moves inside a magnetic field, a current is induced (Faraday’s law — the working principle of every electric generator).

For CBSE Class 10 Physics Chapter 13 (Magnetic Effects of Electric Current), this is one of the highest-weightage chapters in the board examination. It covers: Oersted’s experiment, magnetic field patterns (straight wire, circular loop, solenoid), right hand thumb rule, Maxwell’s right hand screw rule, the electromagnet, force on a current-carrying conductor, Fleming’s left hand rule, the electric motor, and a brief introduction to the generator. This guide covers all these topics with clear explanations, rules, diagrams, applications, and five exam-ready solved problems.

Magnetic Effect of Electric Current — Key Facts at a Glance
1820
Year Oersted discovered that current creates magnetic field
🤖
F = BIL
Force on a current-carrying conductor in a magnetic field
🌞
3 Rules
Right Hand Thumb, Maxwell Screw, Fleming Left Hand Rule
🔌
4 Parts
Armature, Magnets, Split-ring Commutator, Brushes in DC Motor

1. Oersted’s Experiment — Discovery of Magnetic Effect

● Oersted’s Experiment (1820)
Setup: A long straight wire AB is connected to a battery through a switch K. A magnetic compass (pivoted needle) is placed horizontally below the wire.

Observations:
(1) When no current flows (switch open): The compass needle points in its usual North–South direction (along Earth’s magnetic field). No deflection.
(2) When current flows from A to B (switch closed): The compass needle deflects. If current is from A to B (West to East), needle deflects in a specific direction.
(3) When current direction is reversed (B to A): The compass needle deflects in the opposite direction.
(4) When the compass is placed above the wire: Deflection is opposite to when it is placed below.

Conclusion (Oersted’s Discovery):
• A current-carrying conductor produces a magnetic field in the region around it.
• The magnetic field exists only when current flows — stops when switch is opened.
• The direction of the magnetic field reverses when the direction of current reverses.
• The magnetic field is in a plane perpendicular to the direction of current flow.

Significance: This was the first experimental proof that electricity and magnetism are related — the foundation of electromagnetism. It led directly to Ampere’s law, the solenoid, the electromagnet, the galvanometer, the electric motor, and the generator.

2. Magnetic Field Patterns

Straight Current-Carrying Wire
Right Hand Thumb Rule
Magnetic field lines are concentric circles centred on the wire, in planes perpendicular to the wire. The circles get larger (field weakens) as distance increases. Field strength: B = μ₀I / (2πr), where r = distance from wire. No magnetic poles — field lines are closed loops.
Circular Current Loop
Right Hand Rule (loop)
The magnetic field at the centre of a circular loop is perpendicular to the plane of the loop: B = μ₀I / (2R). The field lines emerge from one face (North pole of the loop) and enter the other face (South pole). The two faces act like the poles of a bar magnet.
📈
Solenoid
Right Hand Grip Rule
A solenoid is a long cylindrical coil of many turns of wire. Its magnetic field is similar to a bar magnet: uniform and strong inside the solenoid, weak and diverging outside. One end acts as a North pole, the other as a South pole. B = μ₀nI, where n = turns per metre. Used to make electromagnets.

📈 Solenoid Magnetic Field Diagram

N pole S pole | | ===|===============================================|=== | | Field lines inside solenoid (uniform, -->) | | | |--> --> --> --> --> --> --> --> --> --> --> -->| | | | | | ===|===============================================|=== | | Coil turns (current flowing in circles around axis) Outside: field lines curve from N to S (like bar magnet) Inside: B = mu_0 * n * I [very strong, uniform]

The solenoid is the most important application of the magnetic effect of electric current. Increasing the number of turns per metre (n) or the current (I) increases the magnetic field strength (B = μ₀nI). Adding a soft iron core inside the solenoid dramatically increases B — this is the electromagnet.

3. Right Hand Thumb Rule and Maxwell’s Right Hand Screw Rule

For Straight Wire
Right Hand Thumb Rule
Statement: If a current-carrying straight conductor is held in the right hand such that the thumb points in the direction of current, then the fingers curling around the conductor give the direction of the magnetic field lines (the direction in which they circle the wire).

Practical use: Point your right thumb in the direction of conventional current (+ to −) in the wire. Your fingers naturally curl in the direction of the magnetic field circles around the wire.
👌 Thumb = Current direction | Curled fingers = Magnetic field direction
For Solenoid / Circular Loop
Right Hand Grip Rule (Clock Rule)
For solenoid: If the solenoid is gripped in the right hand such that the fingers point in the direction of current in the coil turns, then the thumb points toward the North pole of the solenoid (the direction of the magnetic field inside the solenoid).

Clock rule for circular loop: Looking at a face of the coil, if current flows anticlockwise → that face is a North pole. If current flows clockwise → that face is a South pole.
👌 Fingers = Current in coil | Thumb = North pole direction
For Any Current-Carrying Conductor
Maxwell’s Right Hand Screw Rule (Corkscrew Rule)
Statement: If a right-handed screw (or corkscrew) is rotated such that its tip moves in the direction of the conventional current, then the direction of rotation of the screw gives the direction of the magnetic field around the conductor.

This rule is equivalent to the Right Hand Thumb Rule and can be applied to both straight conductors and coils. It is particularly intuitive for visualising the rotational nature of the magnetic field around a current-carrying wire.
🔧 Screw tip moves = Current direction | Screw rotation = Magnetic field direction

4. Electromagnet — Construction, Factors, Applications

🤖 Electromagnet
Definition: An electromagnet is a temporary magnet made by winding a coil of insulated copper wire around a soft iron core and passing electric current through the coil. The strong magnetic field of the solenoid magnetises the soft iron core, creating a very powerful magnet.

Why soft iron core? Soft iron is a magnetically soft material — it magnetises strongly when placed inside a solenoid (high permeability μ) and demagnetises completely when current is switched off (low retentivity). This allows the electromagnet to be switched on and off, unlike permanent magnets made of steel (which retains magnetism).

Factors that increase electromagnet strength:
Increase current (I): More current = more powerful magnetic field (B ∝ I).
Increase number of turns (n): More turns = stronger solenoid field (B ∝ n).
Use a soft iron core: Iron core amplifies field by factor of several hundred (high relative permeability μᵅ ≈ 200–5000).
Use a horseshoe (U) shape: Concentrates both poles, maximising lifting force.

Advantages over permanent magnets:
• Magnetic strength can be adjusted by changing current.
• Can be switched on and off electrically (essential for cranes, MRI machines, maglev trains).
• Can be made extremely powerful (MRI machine fields: 1.5–7 Tesla; permanent magnets max: 0.5 T).
🏗
Scrap Yard Cranes
Giant electromagnets (10,000+ kg lifting capacity) pick up and drop scrap iron and steel in scrap yards and steel factories. The electromagnet is switched off to release the load — impossible with a permanent magnet.
🏥
MRI Scanners (Medicine)
Magnetic Resonance Imaging uses superconducting electromagnets (cooled to −269°C) generating fields of 1.5–7 Tesla to image soft tissue inside the human body. No radiation used — MRI is completely safe.
🚨
Electric Bell
When current flows, the electromagnet attracts the iron armature, which hits the gong. The movement breaks the circuit, demagnetising the electromagnet. The spring pulls the armature back, reconnecting the circuit. This cycle repeats rapidly — creating the ringing sound.
Maglev Trains
Magnetic levitation trains use powerful electromagnets to levitate the train 1–10 cm above the track, eliminating friction. The same electromagnetic system propels the train forward at speeds up to 600 km/h. Japan’s SCMaglev holds the world rail speed record: 603 km/h.

5. Force on a Current-Carrying Conductor in a Magnetic Field

Force on Current-Carrying Conductor (Lorentz Force)
F = BIL sinθ   |   Maximum when θ = 90°: F = BIL
F = force on conductor (Newton, N)  |  B = magnetic field strength (Tesla, T)  |  I = current in conductor (Ampere, A)
L = length of conductor in the field (metres)  |  θ = angle between current direction and magnetic field B
When θ = 0° (current parallel to B): F = 0 (no force)
When θ = 90° (current perpendicular to B): F = BIL (maximum force)
▶ How Force Depends on B, I, and L
Experiments show:
F ∝ B: Stronger magnetic field = greater force (e.g., using a more powerful magnet).
F ∝ I: Greater current = greater force (e.g., connecting more batteries).
F ∝ L: Longer conductor in the field = greater force.
• Force is maximum when current is perpendicular to B (θ = 90°).
• Force is zero when current is parallel to B (θ = 0°).

Direction of force: The direction of the force is perpendicular to both the current direction AND the magnetic field direction. This is determined by Fleming’s Left Hand Rule. The force cannot be along the current or along the field — it is always perpendicular to both. This is a consequence of the cross-product nature of the magnetic force (F = IL × B in vector form).

6. Fleming’s Left Hand Rule

☚ Fleming’s Left Hand Rule (FLHR) — Direction of Force on Conductor
Statement: Stretch the thumb, forefinger, and middle finger of the left hand mutually perpendicular to each other (at 90° to each other). If the forefinger points in the direction of the magnetic field (B), and the middle finger points in the direction of the current (I), then the thumb points in the direction of the force (F) (or motion) experienced by the conductor.

Memory aids:
Forefinger = Field (B) — F for both Field and Forefinger
Middle finger = Motion of current (conventional current direction)
THumb = Thrust / Force on conductor
• FBI mnemonic: Force (thumb), B field (forefinger), I current (middle finger)

Application: This rule is used for motors (converting electrical energy to mechanical energy). The opposite rule, Fleming’s Right Hand Rule, is used for generators (converting mechanical energy to electrical energy — the induced current direction).

Why left hand for motors? For positive charges (conventional current), the force on a current-carrying conductor in a magnetic field follows the left-hand rule. For negative charges (electron current), it follows the right-hand rule. Since conventional current is the standard, motors use the left hand.

7. Electric Motor (DC Motor) — Working Principle

🔌 DC Motor — Parts Diagram

N (North pole of magnet) | ======|=========================================================== | | | | [Armature Coil ABCD] | | A----->-----B | | | | (Coil rotates between N and S poles) | | D-----<-----C | | | | ======|=========================================================== | S (South pole of magnet) [Split-ring commutator] connected to coil ends A,D [Carbon brushes] press on commutator, connect to battery Battery (+) --> Brush 1 --> Commutator --> Coil ABCD --> Commutator --> Brush 2 --> Battery (-)

Working: Current flows through ABCD. By Fleming’s Left Hand Rule: force on AB is upward, force on CD is downward. This pair of forces creates a torque, rotating the coil. When coil reaches vertical position, the split-ring commutator reverses the current direction in the coil, keeping the rotation in the same direction. The coil continues rotating as long as current flows.

📈
Armature Coil (ABCD)
Rectangular coil of insulated copper wire wound around a soft iron core. Placed between the poles of a magnet. The current through the coil interacts with the magnetic field to produce force (torque), causing rotation.
🪪
Permanent Magnets (N and S poles)
Provide the external magnetic field (B) between which the armature coil rotates. In large motors, these may be electromagnets (field windings) for more powerful and adjustable fields. The poles face each other with the coil in between.
🔗
Split-Ring Commutator
A copper ring split into two halves, each connected to one end of the armature coil. As the coil rotates, the commutator reverses the direction of current in the coil every half-rotation, ensuring the coil always rotates in the same direction (unidirectional rotation).
Carbon Brushes
Two stationary carbon blocks that press against the rotating split-ring commutator. They maintain electrical contact between the stationary external circuit (battery) and the rotating coil, allowing current to flow continuously into and out of the rotating armature.

8. Electric Motor vs Electric Generator — Comparison

PropertyElectric Motor (DC)Electric Generator (AC)
Principle usedMagnetic effect of current (motor effect): force on current-carrying conductor in B fieldElectromagnetic induction (Faraday’s law): changing flux induces EMF
Energy conversionElectrical energy → Mechanical energyMechanical energy → Electrical energy
InputElectric current from battery or power supplyMechanical rotation (turbine, steam engine, windmill, water)
OutputRotational mechanical motion (shaft rotation)Alternating current (AC) or direct current (DC)
Current direction deviceSplit-ring commutator (reverses current every half-rotation)Slip rings (AC) or commutator (DC generator)
Rule usedFleming’s Left Hand Rule (direction of force)Fleming’s Right Hand Rule (direction of induced current)
ApplicationsElectric fans, pumps, compressors, electric vehicles, trainsPower stations, portable generators, wind turbines, bicycle dynamos

9. Solved Numerical Problems

Q1. A straight wire of length 0.5 m carries a current of 2 A and is placed perpendicular to a magnetic field of 0.4 T. Calculate the force acting on the wire.
Given: L = 0.5 m  |  I = 2 A  |  B = 0.4 T  |  θ = 90° (perpendicular)
F = BIL sinθ = 0.4 × 2 × 0.5 × sin 90° = 0.4 × 2 × 0.5 × 1
F = 0.4 N
Q2. A wire of length 30 cm carries a current of 5 A and is placed at an angle of 30° to a magnetic field of 0.8 T. Find the force on the wire.
Given: L = 30 cm = 0.3 m  |  I = 5 A  |  B = 0.8 T  |  θ = 30°
F = BIL sinθ = 0.8 × 5 × 0.3 × sin 30° = 0.8 × 5 × 0.3 × 0.5 = 1.2 × 0.5
F = 0.6 N
Q3. A solenoid has 200 turns per metre and carries a current of 3 A. Calculate the magnetic field inside the solenoid. (μ₀ = 4π × 10²&sup7; T·m/A)
Given: n = 200 turns/m  |  I = 3 A  |  μ₀ = 4π × 10²&sup7; T·m/A = 1.257 × 10²&sup6; T·m/A
B = μ₀nI = 4π × 10²&sup7; × 200 × 3
B = 4 × 3.14159 × 10²&sup7; × 600
B = 1.257 × 10²&sup6; × 600
B = 7.54 × 10²⁴ T ≈ 7.5 × 10²⁴ T
Q4. If the force on a wire of length 0.5 m in a magnetic field of 0.6 T is 0.9 N, find the current in the wire. (Wire is perpendicular to field.)
Given: L = 0.5 m  |  B = 0.6 T  |  F = 0.9 N  |  θ = 90°
F = BIL sinθ ⇒ I = F / (BL sinθ)
I = 0.9 / (0.6 × 0.5 × 1) = 0.9 / 0.3
I = 3 A
Q5. The distance between two parallel wires carrying currents of 4 A and 6 A is 0.2 m. Find the force per unit length on each wire. (μ₀ = 4π × 10²&sup7; T·m/A)
Given: I₁ = 4 A  |  I₂ = 6 A  |  d = 0.2 m  |  μ₀ = 4π × 10²&sup7; T·m/A
Force per unit length: F/L = μ₀I₁I₂ / (2πd)
F/L = (4π × 10²&sup7; × 4 × 6) / (2π × 0.2)
F/L = (4π × 10²&sup7; × 24) / (0.4π)
F/L = (96π × 10²&sup7;) / (0.4π) = 240 × 10²&sup7;
F/L = 2.4 × 10²⁵ N/m (attractive if same direction, repulsive if opposite)

10. Frequently Asked Questions (FAQ)

Q1. What did Oersted discover? What was the significance of his experiment?

Oersted’s Discovery (1820): Hans Christian Oersted discovered that a current-carrying conductor (wire) produces a magnetic field in the region around it. He observed that a compass needle, placed near a wire connected to a battery, deflected when current flowed through the wire, and returned to normal when the current was switched off.

Key findings:
(1) A magnetic field exists around a current-carrying conductor, in a plane perpendicular to the current.
(2) The field exists only when current flows — no current, no field.
(3) Reversing current reverses the direction of the magnetic field.

Significance: This was the first proof that electricity and magnetism are related phenomena — the birth of electromagnetism. It led to Ampere’s circuit law, the galvanometer, the solenoid, the electromagnet, the electric motor, and Faraday’s electromagnetic induction. Without Oersted’s discovery, the electrification of the modern world would not have been possible.

Q2. State Fleming’s Left Hand Rule and explain where it is used.

Fleming’s Left Hand Rule: Stretch the thumb, forefinger, and middle finger of the left hand so that they are mutually perpendicular to each other. If the forefinger points in the direction of the magnetic field (B), and the middle finger points in the direction of the conventional electric current (I), then the thumb points in the direction of the force (F) or motion of the conductor.

FBI Mnemonic:
• F = Force (Thumb)
• B = Magnetic field (Forefinger)
• I = Current (Middle finger)

Where it is used: Fleming’s Left Hand Rule is used to find the direction of force on a current-carrying conductor placed in a magnetic field. It is the operating principle of all electric motors — determining which way the motor armature coil rotates when current flows through it. Every electric fan, pump, compressor, electric vehicle, and train motor operates on this rule. (Note: Fleming’s Right Hand Rule is used for generators — finding the direction of induced current).

Q3. Explain the working principle of an electric motor with a diagram.

Principle: An electric motor works on the principle that a current-carrying conductor placed in a magnetic field experiences a mechanical force (motor effect). This force rotates the armature coil, converting electrical energy to mechanical (rotational) energy.

Parts: (1) Armature coil ABCD — rectangular coil of copper wire wound on soft iron core. (2) Permanent magnets (N and S poles) — provide the magnetic field B. (3) Split-ring commutator — reverses current every half-rotation to maintain unidirectional rotation. (4) Carbon brushes — transfer current from stationary circuit to rotating coil.

Working:
• Current flows through ABCD from the battery via brushes and commutator.
• By Fleming’s Left Hand Rule: force on AB is in one direction (say upward), force on CD is in the opposite direction (downward).
• This creates a couple (torque) that rotates the coil.
• When coil reaches vertical position, the split-ring commutator reverses the current direction, so the forces continue rotating the coil in the same direction.
• The coil spins continuously, converting electrical energy to rotational mechanical energy.

Applications: Electric fans, washing machines, electric cars, trains, elevators, pumps, compressors, and thousands of other devices.

Q4. What is the difference between an electromagnet and a permanent magnet?

Electromagnet: Made by winding a coil of insulated copper wire around a soft iron core and passing electric current through the coil. Creates a temporary magnetic field only when current flows.
Permanent magnet: Made from magnetically hard materials like steel, alnico, or neodymium. Retains magnetism without any external current.

Key differences:
(1) Control: Electromagnet can be switched ON/OFF; permanent magnet cannot.
(2) Strength: Electromagnet strength adjustable by changing current; permanent magnet fixed.
(3) Temperature dependence: Both lose magnetism above Curie temperature, but electromagnet can be re-energised; permanent magnet permanently demagnetises.
(4) Materials: Electromagnet uses soft iron core (low retentivity, high permeability); permanent magnet uses steel/neodymium (high retentivity).
(5) Applications: Electromagnets: cranes, MRI, electric bells, motors. Permanent magnets: compass needles, loudspeakers, fridge magnets, hard drives.
(6) Maximum field: Superconducting electromagnets (MRI): up to 7+ Tesla. Best permanent magnets (neodymium): up to 1.5 Tesla.

Q5. Why does a current-carrying conductor experience no force when placed parallel to a magnetic field?

The force on a current-carrying conductor in a magnetic field is given by: F = BIL sinθ, where θ is the angle between the direction of current and the direction of the magnetic field B.

When the conductor is placed parallel to the magnetic field, θ = 0° (or 180° for opposite direction). sin 0° = 0.
Therefore: F = BIL × 0 = 0 N. No force acts on the conductor.

Physical explanation: The force on a current-carrying conductor is a result of the interaction between the magnetic field created by the current and the external magnetic field. These two fields only produce a net force when they are not parallel. When current is parallel to B, the magnetic field of the wire and the external field add and subtract in the same plane, creating no sideways net force — only a tension along the wire.

Maximum force: When the conductor is perpendicular to B (θ = 90°), sin 90° = 1, and F = BIL (maximum force). This is the condition maintained in efficient electric motors by placing the armature coil perpendicular to the magnetic field initially.

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