Ch. 22 Section Summary - College Physics 2e _ OpenStax
22.1 Magnets
Magnetism Overview
Concerns properties of magnets and their effects on moving charges.
Creation of magnetic fields through electric currents.
Types of Magnetic Poles
North and south magnetic poles exist in pairs.
North magnetic poles are attracted toward Earth's geographic north pole.
Like poles repel; unlike poles attract.
22.2 Ferromagnets and Electromagnets
Ferromagnetic Materials
Examples include iron, exhibiting strong magnetic effects.
Atoms in these materials act as small magnets (due to atomic currents).
Can align in domains; larger domains create permanent magnets.
The process of becoming magnetic is called magnetization.
Beyond Curie temperature: thermal agitation disrupts atomic alignment, and ferromagnetism vanishes.
Electromagnets
Created using electric currents to generate magnetic fields.
Often enhanced by using ferromagnetic materials.
22.3 Magnetic Fields and Magnetic Field Lines
Representation
Pictorially represented as magnetic field lines.
Properties of Magnetic Field Lines
Direction is tangent to the field line.
Field strength is proportional to line density.
Field lines cannot intersect.
Always form closed loops.
22.4 Magnetic Field Strength: Force on a Moving Charge
Formula:
Magnitude of force on charge q moving through a magnetic field is given by:F = qvB sin θ.
Where θ is the angle between charge direction and magnetic field.
SI Unit:
Magnetic field strength is measured in tesla (T).
Right Hand Rule 1 (RHR-1):
Thumb points in the direction of velocity, fingers in the direction of the magnetic field, palm perpendicular indicates force direction.
22.5 Force on a Moving Charge in a Magnetic Field: Examples and Applications
Centripetal Force:
Magnetic force can act as centripetal force, causing circular motion.
Radius of the motion derived from component of velocity perpendicular to magnetic field.
22.6 The Hall Effect
Definition:
Hall effect generates a voltage (Hall emf) across a current-carrying conductor in a magnetic field.
Formula:
Hall emf provided by the width of the conductor and speed of charges moving through it.
22.7 Magnetic Force on a Current-Carrying Conductor
Formula:
F = IlB sin θ,
I is the electric current, l is the length of the conductor, and B is the magnetic field strength.
Right Hand Rule 1 (RHR-1) applies here as well.
22.8 Torque on a Current Loop: Motors and Meters
Torque Formula:
Torque on a current-carrying loop in a magnetic field: τ = NIAB sin θ.
N = number of turns, I = current, A = area of the loop, B = magnetic field strength, θ = angle between the field and perpendicular to the loop.
22.9 Magnetic Fields Produced by Currents: Ampere’s Law
Strength of Magnetic Field from a Wire:
Given by: B = (μ0I)/(2πr),where μ0 is the permeability of free space, I is the current, and r is the distance from the wire.
Right Hand Rule 2 (RHR-2):
Thumb in current direction, fingers curl to show magnetic field direction.
Magnetic Field in a Loop and Solenoid:
At center of loop: B = (μ0I)/(2R).
22.10 Magnetic Force between Two Parallel Conductors
Force Formula Per Unit Length:
F/l = (μ0I1I2)/(2πr).
Attraction if currents go in the same direction, repulsion if in opposite directions.
22.11 More Applications of Magnetism
Crossed Electric and Magnetic Fields:
Act as a velocity filter for charges with velocity perpendicular to the fields, governed by: v = E/B.