Here is a master cheatsheet for the Magnetic Fields (Chapter 20) section of your 9702 Physics syllabus, optimized for Obsidian.
🧲 Chapter 20: Magnetic Fields - Master Cheatsheet
Overview
This chapter covers the interaction between magnetic fields, electric currents, and moving charges, as well as the phenomenon of electromagnetic induction.
1. Concept of a Magnetic Field
- Definition: A region of space where a magnetic material (magnetic pole) or a moving charge experiences a force.
- Representing Fields:
- Magnetic field lines are continuous loops.
- Direction: North to South (outside the magnet).
- Density of lines = Magnitude of Flux Density ().
- 3D Representation:
●(Dot): Out of the page.×(Cross): Into the page.
2. Force on a Current-Carrying Conductor
- Equation:
- = Magnetic force (N)
- = Magnetic flux density (T)
- = Current (A)
- = Length of conductor within the field (m)
- = Angle between the current direction and the magnetic field lines.
- Direction (Fleming’s Left-Hand Rule):
- Thumb: Motion/Force ()
- First Finger: Field ()
- Second Finger: Current () (Conventional: + to -)
Common Pitfalls
- and must be mutually perpendicular for to hold at maximum.
- If the current is parallel to field lines, or , so , .
- Remember: Direction of current for negative charges (electrons) is opposite to their motion.
3. Magnetic Flux Density ()
- Definition: The force per unit length per unit current on a straight wire placed at right angles to the magnetic field.
- Unit: Tesla (T).
- 1 Tesla = 1 Newton per Ampere-metre.
4. Forces on a Moving Charge
- Equation:
- = Charge (C)
- = Velocity (m/s)
- Circular Motion: When is perpendicular to , the magnetic force acts as a centripetal force:
- Radius of path
- Velocity Selector: Used to filter particles with a specific velocity.
- Electric force () equals Magnetic force ().
5. Hall Effect
- Concept: When a conductor carries current in a magnetic field, charges are pushed to one side, creating a potential difference (Hall Voltage, ).
- Equation:
- = number density of charge carriers ()
- = thickness of the slice
- = charge of carrier
- Application: Used to measure magnetic flux density using a Hall probe.
Hall Probe Tip
Smaller (semiconductors) gives a larger , making them better for sensitive measurements than metals like copper.
6. Electromagnetic Induction
Magnetic Flux ()
- Definition: Product of magnetic flux density and the cross-sectional area perpendicular to the field.
- Formula:
- is the angle between the field lines and the normal to the plane of the area.
Magnetic Flux Linkage
- Formula: (for turns)
Faraday’s & Lenz’s Laws
- Faraday’s Law: The magnitude of induced e.m.f. is proportional to the rate of change of magnetic flux linkage.
- Lenz’s Law: The direction of induced e.m.f. is such that it opposes the change in magnetic flux that caused it.
- (The negative sign represents Lenz’s Law).
7. Examiner Guidance & Common Mistakes
Exam Strategy
- Defining Flux Density: Don’t be ambiguous about what is perpendicular. Explicitly state: “The force per unit current, per unit length on a wire placed at right angles to the magnetic field.”
- Lenz’s Law: If asked to explain the direction, do not just define the law. Apply it: “The induced current creates a field that opposes the change (e.g., magnet approaching).”
- Units: Always check units! (), (), ().
- Graphs: If sketching induced e.m.f. from a changing flux graph, remember is proportional to the gradient of the flux graph. If the flux graph has a constant positive gradient, the e.m.f. is a constant negative value.
- Formula confusion: is for wires. is for isolated charges. Don’t mix them up.
- Hall Effect: When describing it, mention that the electric field set up by charge separation balances the magnetic force on the charge carriers.