Electromagnetic effects
What is electromagnetic induction?
Electromagnetic induction is the process where an electromotive force (e.m.f.) (voltage) is generated in a conductor. This happens under two conditions:
- A conductor moves across magnetic field lines.
- A magnetic field linking with a stationary conductor changes.
Why does this happen?
When a conductor cuts through magnetic field lines, the free electrons inside the conductor experience a force. This force pushes the electrons to one end of the wire, creating a potential difference (voltage) across its ends. If the circuit is closed, this induced e.m.f. drives an induced current.
Factors affecting the magnitude of induced e.m.f. (LO 3)
The size of the induced voltage depends on:
- Speed: Faster movement or faster change in magnetic field strength increases the rate at which field lines are cut, increasing the e.m.f.
- Strength of the magnetic field: Stronger magnets produce more field lines to be cut.
- Number of turns: If using a coil, more turns mean more wire cutting the field lines simultaneously.
Experiment to demonstrate induction (LO 2)
To show this practically:
- Connect a sensitive galvanometer (or ammeter) to a coil of wire.
- Move a bar magnet into and out of the coil.
- Observe the galvanometer needle deflecting in opposite directions for each motion.
- If the magnet is held stationary inside the coil, there is no deflection because the magnetic field is not changing.
Correction: A static magnetic field does not induce an e.m.f. There must be relative motion between the conductor and the magnet, or the magnetic field strength must be changing (e.g., using alternating current).
Why examiners accept this: They look for the specific action that causes change. Avoid vague phrases like 'put magnet near wire.'
Correct phrasing: Use terms like 'moving the magnet relative to the coil', 'cutting magnetic field lines', or 'changing the magnetic flux linkage'.
Example: 'The galvanometer deflects because the moving magnet causes a change in the magnetic field linking with the coil, inducing an e.m.f.'
- The speed of movement of the magnet (or coil). 2. The strength of the magnetic field.
The direction of the induced e.m.f. is such that it opposes the change that caused it. This is a consequence of the conservation of energy. If the induced current aided the motion, it would create more current, which would create more force, leading to infinite energy—impossible.
Fleming's Right-Hand Rule (LO 5)
To find the direction of induced current (used in generators/induction):
- Hold your right hand with thumb, first finger, and second finger mutually at right angles (90° to each other).
- First Finger: Points in the direction of the Field (North to South).
- Thumb: Points in the direction of Motion of the conductor.
- Second Finger: Points in the direction of the induced Current (conventional current, + to -).
Note: Use your RIGHT hand for generators/induction. Use your LEFT hand for motors/force.
Correction: Left hand is for Motors (Force on a current-carrying wire). Right hand is for Generators (Induced current from motion). A helpful mnemonic: 'FBI' (Force, B-field, I-current) for Left Hand; 'Motion, Field, Current' for Right Hand.
Why examiners accept this: They require you to explicitly state the rule used and the alignment of fingers.
Correct phrasing: 'Using Fleming's Right-Hand Rule, with the first finger pointing North to South and the thumb in the direction of motion, the second finger points upwards.'
Example: If a wire moves right across a field into the page, the induced current flows upwards.
A simple a.c. generator consists of:
- A rotating coil (armature) placed in a magnetic field.
- Slip rings: Two continuous metal rings attached to the ends of the coil.
- Brushes: Carbon blocks that press against the slip rings to transfer current to the external circuit.
Note: Slip rings allow the current to flow out continuously as the coil rotates, resulting in Alternating Current (a.c.).
How it works
As the coil rotates, the sides of the coil cut through magnetic field lines. The rate at which they cut the lines changes continuously:
- When the coil is vertical (perpendicular to the field), the sides move parallel to the field lines. No lines are cut. Induced e.m.f. = 0.
- When the coil is horizontal (parallel to the field), the sides move perpendicular to the field lines, cutting them at the maximum rate. Induced e.m.f. is at its peak.
Because the direction of motion relative to the field reverses every half-turn, the current alternates direction. This produces a sinusoidal (sine wave) graph of e.m.f. vs. time.
Split-Ring Commutator: A ring split into two halves, used in d.c. motors/generators to reverse the connection every half-turn, ensuring unidirectional current (pulsating d.c.).
Graph Shape: A sine wave starting from zero.
Key Points to Label:
- Zero e.m.f.: Coil is vertical (plane of coil perpendicular to field).
- Peak e.m.f.: Coil is horizontal (plane of coil parallel to field).
- Frequency: The number of complete cycles per second. If the coil rotates faster, the frequency increases (waves get closer together).
Correction: When e.m.f. is zero, the coil is cutting no field lines because it is moving parallel to them. The field is still present, but the rate of change of flux linkage is zero.
Why examiners accept this: They want you to link the physical position of the coil to the electrical output.
Correct phrasing: 'The e.m.f. is zero when the coil is vertical because the sides of the coil are moving parallel to the magnetic field lines, so no lines are cut.'
Example: 'Increasing the speed of rotation increases the frequency (more peaks per second) and the amplitude (higher peak voltage) because the rate of cutting field lines increases.'
Straight Wire (LO 8)
- Pattern: Concentric circles centered on the wire.
- Direction: Use the Right-Hand Grip Rule. Thumb points in direction of current; fingers curl in direction of magnetic field lines.
- Strength (LO 11): Strongest near the wire, decreasing with distance.
Solenoid (LO 8)
A solenoid is a coil of wire. When current flows:
- Pattern: Inside the solenoid, the field is uniform (parallel lines). Outside, it looks like a bar magnet (North at one end, South at the other).
- Direction: Use Right-Hand Grip Rule for coils. Curl fingers in direction of current; thumb points to North pole.
Factors affecting strength (LO 11-12)
The strength of the magnetic field around a wire or solenoid depends on:
- Magnitude of current: Increasing current increases field strength.
- Number of turns (for solenoids): More turns increase field strength.
- Core material: Inserting a soft-iron core greatly increases the field strength because iron is easily magnetized and concentrates the field lines.
For solenoids: Fingers curling = Current direction around coils. Thumb = North pole of the magnetic field.
Method:
- Pass a vertical wire through a horizontal card.
- Sprinkle iron filings on the card and tap it gently.
- The filings align with the magnetic field, showing concentric circles.
- Use a plotting compass to determine direction: place the compass near the wire; the needle points tangent to the circle. Move the compass around to trace the full circle.
Correction: Field lines are only parallel and uniform inside the solenoid. Outside, they curve from North to South pole, similar to a bar magnet.
Why examiners accept this: They look for qualitative relationships (increase/decrease) and direction reversal.
Correct phrasing: 'Increasing the current increases the strength of the magnetic field. Reversing the current reverses the direction of the magnetic field poles.'
Example: 'If the current in the solenoid is doubled, the magnetic field strength doubles.'
The Motor Effect
When a current-carrying conductor is placed in an external magnetic field, it experiences a force. This is because the magnetic field produced by the current interacts with the external magnetic field.
Fleming's Left-Hand Rule (LO 14)
To find the direction of the force:
- Hold your left hand with thumb, first finger, and second finger mutually at right angles.
- First Finger: Points in the direction of the Field (N to S).
- Second Finger: Points in the direction of the Current (+ to -).
- Thumb: Points in the direction of the Force (Motion).
Experiment to show force (LO 13)
- Place a wire between the poles of a strong magnet.
- Connect the wire to a power supply.
- When current flows, the wire jumps out of the gap.
- Reversing Current: The wire jumps in the opposite direction.
- Reversing Field: The wire jumps in the opposite direction.
Turning effect is the rotational force experienced by a coil in a magnetic field. It depends on:
- Number of turns (N)
- Current (I)
- Magnetic field strength (B)
- Area of the coil (A)
Increasing any of these increases the turning effect.
Correction: Left hand is for Motors (Force). Right hand is for Generators (Induced Current). Remember: 'FBI' (Force, B-field, I-current) works with the Left Hand.
Why examiners accept this: They want you to reference Fleming's Left-Hand Rule explicitly.
Correct phrasing: 'Reversing the current reverses the direction of the force because, according to Fleming's Left-Hand Rule, changing the direction of the second finger (current) while keeping the first finger (field) constant reverses the thumb (force).'
Example: 'If both current and field are reversed, the force direction remains the same.'
Operation of a Simple D.C. Motor
A motor converts electrical energy into mechanical energy.
- A coil is placed in a magnetic field.
- Current flows through the coil.
- The sides of the coil experience forces in opposite directions (due to Fleming's Left-Hand Rule), creating a turning effect (torque).
- The coil rotates.
The Split-Ring Commutator (LO 17)
Without a commutator, the coil would rotate half a turn and then stop or reverse because the forces would flip direction as it passes the vertical position.
- The split-ring commutator is a ring split into two halves.
- It reverses the connection to the power supply every half-turn.
- This reverses the current direction in the coil at the right moment, ensuring the force always acts in the same rotational direction, allowing continuous rotation.
Relays
- Construction: A coil wrapped around a soft-iron core, with a pivoted armature and contacts.
- Operation: Small current in the coil creates a magnetic field. The iron core becomes magnetized and attracts the armature. This closes (or opens) a separate, high-current circuit.
- Use: Allows a low-power switch to control a high-power device (e.g., car starter motor).
Loudspeakers
- Construction: A coil attached to a cone, placed in a permanent magnetic field.
- Operation: Alternating current from the amplifier flows through the coil. The coil experiences a varying force (push/pull) due to the interaction with the permanent magnet. This vibrates the cone, producing sound waves.
Correction: The commutator reverses the current in the coil, not the external magnetic field. This ensures the force on the coil sides always pushes in the same rotational direction.
Why examiners accept this: They need the sequence: Current → Force → Rotation → Commutator action.
Correct phrasing: 'The split-ring commutator reverses the current in the coil every half-turn, ensuring that the torque remains in the same direction.'
Example: 'Without the commutator, the coil would oscillate about the vertical position rather than rotating continuously.'
Construction (LO 18)
A transformer consists of:
- Primary coil: Input side.
- Secondary coil: Output side.
- Soft-iron core: Connects the coils magnetically.
Principle of Operation (LO 23)
Transformers only work with Alternating Current (a.c.).
- A.c. in the primary coil creates a changing magnetic field.
- The soft-iron core concentrates and transfers this changing magnetic field to the secondary coil.
- The changing magnetic field induces an e.m.f. in the secondary coil (electromagnetic induction).
Voltage Ratio Equation (LO 20)
\frac{V_p}{V_s} = \frac{N_p}{N_s}
Where:
- V_p = Primary voltage (Volts)
- V_s = Secondary voltage (Volts)
- N_p = Number of turns on primary coil
- N_s = Number of turns on secondary coil
Step-up vs. Step-down (LO 19)
- Step-up transformer: N_s > N_p, so V_s > V_p. Increases voltage.
- Step-down transformer: N_s < N_p, so V_s < V_p. Decreases voltage.
Efficiency and Power (LO 24-25)
For an ideal (100% efficient) transformer:
P_{in} = P_{out}
I_p V_p = I_s V_s
Where I is current.
High-Voltage Transmission (LO 21-22)
- Why high voltage? Power loss in cables is given by P_{loss} = I^2 R, where R is the resistance of the transmission cables.
- Since P = IV, for a fixed power P, increasing voltage V decreases current I.
- Lower current means significantly lower I^2 R losses (heat) in the cables.
Solution:
\frac{V_p}{V_s} = \frac{N_p}{N_s}
\frac{12}{V_s} = \frac{100}{500}
V_s = 12 \times \frac{500}{100} = 60 \text{ V}
This is a step-up transformer.
Correction: Transformers require a changing magnetic field. D.c. provides a constant field, so no induction occurs in the secondary coil.
Mistake 2: Thinking the iron core conducts electricity from primary to secondary.
Correction: The core conducts magnetic flux, not electric current. The coils are electrically isolated.
Why examiners accept this: They want the link between Voltage, Current, and Power Loss.
Correct phrasing: 'Power loss in cables is proportional to I^2 R. By stepping up the voltage, the current is reduced for the same power transmitted. This significantly reduces the energy lost as heat in the cables.'
Example: 'If voltage is doubled, current is halved, and power loss is reduced to one-quarter.'
- Energy lost as heat in the coils (resistance). 2. Energy lost due to hysteresis and eddy currents in the iron core.