AgentSkillsCN

15 Magnetism

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SKILL.md
--- frontmatter
id: magnetism
subject: physics
display_name: Magnetism
description: |
  Covers magnetic fields, magnetic forces on moving charges and current-carrying wires, and electromagnetic induction.
  Use when students need to solve problems involving magnetic forces, field calculations, or Faraday's law.

grade_band: 9-12
khan_tags: [physics, magnetism, magnetic-force, electromagnetic-induction, faraday-law]
standards:
  - NGSS.HS-PS2-5
  - NGSS.HS-PS3-5

objectives:
  - Calculate magnetic force on a moving charge using F = qvB sin(theta)
  - Apply the right-hand rule to determine force direction
  - Calculate force on a current-carrying wire using F = BIL
  - Determine magnetic field from a long straight wire using B = mu_0 I / (2 pi r)
  - Understand magnetic field in solenoids
  - Apply Faraday's law to calculate induced EMF
  - Use Lenz's law to determine direction of induced current

prerequisites:
  - circuits
  - circular-motion

estimated_time_minutes: 75

validator:
  type: numeric_solver
  config:
    unit_library: physics
    default_tolerance: 0.02
    require_units: true

sources:
  - name: OpenStax College Physics
    chapter: 22-23
    url: https://openstax.org/books/college-physics/pages/22-introduction-to-magnetism
    license: CC-BY-4.0

Magnetism

Misconceptions

MisconceptionCorrection
"Magnetic force does work on charged particles"Magnetic force is always perpendicular to velocity, so it does zero work
"Magnetic poles can be isolated"Magnetic poles always come in north-south pairs; no magnetic monopoles exist
"Current flows through a magnetic field to create force"Force arises from the interaction of moving charges with the magnetic field
"Induced EMF depends on the magnetic flux"Induced EMF depends on the rate of change of flux, not the flux itself
"Lenz's law creates energy"Lenz's law opposes change and is consistent with energy conservation

Key Concepts

Magnetic Field

A magnetic field B is a vector field that exerts forces on moving charges. Magnetic field lines point from north to south poles outside the magnet and form closed loops.

Units: Tesla (T) = kg/(A·s²) = Wb/m²

Magnetic Force on a Moving Charge

A charge q moving with velocity v in a magnetic field B experiences a force:

F = qvB sin(θ)

Where θ is the angle between v and B.

Key properties:

  • Force is perpendicular to both v and B
  • Force is zero when v is parallel to B
  • Use the right-hand rule: fingers point in v direction, curl toward B, thumb points in F direction (for positive charges)
  • For negative charges, force is opposite to right-hand rule

Magnetic Force on a Current-Carrying Wire

A wire of length L carrying current I in a magnetic field B experiences a force:

F = BIL sin(θ)

Where θ is the angle between the wire and B.

Circular Motion in a Magnetic Field

Since magnetic force is always perpendicular to velocity, a charged particle in a uniform magnetic field moves in a circle (or helix if there's a component parallel to B).

Radius of circular path: r = mv/(qB)

Period: T = 2πm/(qB) (independent of speed!)

Magnetic Field from a Long Straight Wire

A long straight wire carrying current I produces a magnetic field at distance r:

B = μ₀I/(2πr)

Where μ₀ = 4π × 10⁻⁷ T·m/A is the permeability of free space.

Direction: Use right-hand rule - thumb in current direction, fingers curl in direction of B.

Magnetic Field in a Solenoid

A solenoid with n turns per unit length carrying current I produces a uniform field inside:

B = μ₀nI

The field is nearly uniform inside and approximately zero outside.

Faraday's Law of Induction

The induced EMF in a loop equals the negative rate of change of magnetic flux:

EMF = -N × (ΔΦ/Δt)

Where Φ = BA cos(θ) is the magnetic flux, N is the number of turns.

Lenz's Law

The direction of induced current creates a magnetic field that opposes the change in flux that produced it.

Equations

code
[1] F = qvB sin(θ) (magnetic force on moving charge)
[2] F = BIL sin(θ) (force on current-carrying wire)
[3] r = mv/(qB) (radius of circular motion)
[4] T = 2πm/(qB) (period of circular motion)
[5] B = μ₀I/(2πr) (field from long wire)
[6] B = μ₀nI (field in solenoid)
[7] Φ = BA cos(θ) (magnetic flux)
[8] EMF = -N(ΔΦ/Δt) (Faraday's law)
[9] μ₀ = 4π × 10⁻⁷ T·m/A (permeability of free space)

Worked Examples

Example 1: Force on a Moving Proton

Problem: A proton (q = 1.6 × 10⁻¹⁹ C) moves at 3 × 10⁶ m/s perpendicular to a 0.5 T magnetic field. What is the magnetic force?

Solution:

  1. Use F = qvB sin(θ) with θ = 90°
  2. F = (1.6 × 10⁻¹⁹)(3 × 10⁶)(0.5)(1)
  3. F = 2.4 × 10⁻¹³ N

Example 2: Circular Motion of an Electron

Problem: An electron (m = 9.11 × 10⁻³¹ kg, q = 1.6 × 10⁻¹⁹ C) moves at 2 × 10⁷ m/s in a 0.01 T field. Find the radius of its circular path.

Solution:

  1. Use r = mv/(qB)
  2. r = (9.11 × 10⁻³¹)(2 × 10⁷) / [(1.6 × 10⁻¹⁹)(0.01)]
  3. r = 1.82 × 10⁻²³ / 1.6 × 10⁻²¹
  4. r = 0.0114 m = 1.14 cm

Example 3: Induced EMF

Problem: A 50-turn coil with area 0.02 m² is in a magnetic field that decreases from 0.8 T to 0.2 T in 0.1 s. What is the induced EMF?

Solution:

  1. ΔΦ = A × ΔB = 0.02 × (0.2 - 0.8) = -0.012 Wb
  2. EMF = -N × ΔΦ/Δt = -50 × (-0.012)/0.1
  3. EMF = 6 V

Explanation Patterns

  1. Identify the physical situation - Is it force on a charge, force on a wire, or induction?
  2. Draw the geometry - Show B field, velocity/current direction, and use right-hand rule
  3. Identify the angle - Carefully determine θ between the relevant vectors
  4. Apply the appropriate formula - F = qvB, F = BIL, or Faraday's law
  5. Check direction using right-hand rule - Especially important for force problems
  6. Verify units - Tesla = kg/(A·s²), Weber = T·m²

Common Problem Types

  1. Force on moving charges: Calculate force magnitude and direction
  2. Circular motion in B field: Find radius, period, or frequency
  3. Force on current-carrying wires: Calculate force on straight or curved wires
  4. Magnetic field calculations: Find B from wires or solenoids
  5. Faraday's law problems: Calculate induced EMF from changing flux
  6. Lenz's law: Determine direction of induced current