Chapter 20: Magnetism Study Notes

Chapter 20: Magnetism
Introduction
  • This chapter discusses fundamental concepts related to magnetism including properties of magnets, magnetic fields, and interactions between electric currents and magnetic fields.

  • It is structured into various sections covering different aspects of magnetism and is essential for understanding the principles of physics related to magnetic phenomena.

Contents Overview
  • Topics discussed include:

    • Magnets and Magnetic Fields

    • Electric Currents Produce Magnetic Fields

    • Force on an Electric Current in a Magnetic Field; Definition of B

    • Force on Electric Charge Moving in a Magnetic Field

    • Magnetic Field Due to a Long Straight Wire

    • Force between Two Parallel Wires

    • Solenoids and Electromagnets

    • Ampère’s Law

    • Torque on a Current Loop; Magnetic Moment

    • Applications: Galvanometers, Motors, Loudspeakers

    • Mass Spectrometer

    • Ferromagnetism: Domains and Hysteresis

20-1: Magnets and Magnetic Fields
  • Magnets possess two poles: North and South.

  • Rule of Poles:

    • Like poles repel each other; unlike poles attract each other.

  • Cutting a magnet in half does not produce a single north or south pole but results in two smaller magnets, each with its own north and south pole.

Magnet Properties and Experiments
  • Experiment 4: Magnets can lift certain objects (e.g., paper clips) while some materials (copper, aluminum, glass, plastic) are unaffected.

  • Experiment 5: A magnet near an electroscope does not affect the leaves unless a charged rod is nearby, which may cause minor polarization effects.

Summary of Experiments
  • Conclusions drawn from experiments indicate:

    • Magnetism is distinct from electricity.

    • Magnetic poles share similar but not identical behaviors compared to electric charges.

20-2: Electric Currents Produce Magnetic Fields
  • Electric current generates a magnetic field around conductors, which can be determined using the Right-Hand Rule.

  • 2nd Right-Hand Rule: Demonstrates the direction of the produced magnetic field based on the direction of current.

20-3: Force on an Electric Current in a Magnetic Field; Definition of B
  • A magnet affects a current-carrying wire. The force exerted on the wire is determined by its current, length, orientation, and the magnetic field present.

  • Definition of magnetic field: B (Tesla)

  • Unit: 1T=1NAm1 T = 1\frac{N}{A \cdot m}

  • Alternative unit: Gauss (G) - 1G=104T1 G = 10^{-4} T

20-4: Force on Electric Charge Moving in a Magnetic Field
  • A magnetic field exerts a force on a charge that is moving.

  • Key observations:

    • No magnetic force exists when the charged particle is stationary.

    • No magnetic force if the particle moves parallel to the magnetic field.

    • Maximum force occurs when the angle (α) between the particle's velocity and the magnetic field is 9090^{\circ}.

  • If the charged particle moves perpendicularly to a magnetic field, it follows a circular path due to the continuous magnetic force acting as a centripetal force.

  • Magnetic force (for perpendicular motion):

    F=qvBF = qvB

  • Equated with circular motion force, F=mv2rF = \frac{mv^2}{r} leading to the gyroradius: r=mvqBr = \frac{mv}{qB}

20-5: Magnetic Field Due to a Long Straight Wire
  • The magnetic field (B) from a straight wire is inversely proportional to the distance from that wire.

  • Relationship: B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}

    • Field strength decreases with distance.

  • Permeability of Free Space: μ0=4π×107Tm/A\mu_0 = 4\pi \times 10^{-7} T\cdot m/A

20-6: Force between Two Parallel Wires
  • Parallel wires carrying current exert forces on each other; this force depends on the direction of the currents.

  • Rule: Parallel currents attract, antiparallel currents repel.

  • Force per unit length relationship for parallel wires formula:

    F<em>12=μ</em>02πrI<em>1I</em>2F<em>{12} = \frac{\mu</em>0}{2\pi r} I<em>1 I</em>2

20-7: Solenoids and Electromagnets
  • A solenoid is a coil of wire that produces a magnetic field when electric current passes through it.

  • A tightly wound solenoid exhibits a nearly uniform interior magnetic field.

  • Inserting iron into the solenoid increases the magnetic field significantly, thus functioning as an electromagnet with numerous applications.

20-8: Ampère’s Law
  • Ampère’s law connects the magnetic field within a closed loop to the total current enclosed by that loop:

  • Formula:

    B=μ<em>02I</em>encB = \frac{\mu<em>0}{2}I</em>{enc}

  • Useful for analyzing systems with high symmetry.

20-9: Torque on a Current Loop; Magnetic Moment
  • The interaction of a current loop in a magnetic field can cause a torque, which causes the loop to rotate.

  • Torque Magnitude Relation:

    • τ=M×B\tau = M \times B where M is the magnetic moment defined as M=NIAM = NIA

20-10: Applications: Galvanometers, Motors, Loudspeakers
  • Galvanometers utilize induced torque to measure electric current.

  • Electric Motors: Transform electrical energy to mechanical energy through the torque on current loops.

  • Loudspeakers: Utilize forces on current wires within magnetic fields to convert electrical signals into sound.

20-11: Mass Spectrometer
  • A mass spectrometer is employed to measure the masses of atoms.

  • Charged particles traversing perpendicular electric and magnetic fields experience select speeds without deflection, a phenomenon termed velocity selection.

20-12: Ferromagnetism: Domains and Hysteresis
  • Ferromagnetic materials (e.g., iron, nickel) can become strongly magnetized due to the alignment of internal domains, which can be either randomly oriented (unmagnetized) or aligned (magnetized).

  • The hysteresis curve illustrates the relation between an external magnetic field and an internal magnetic field within a ferromagnet, showing how magnetization levels change with varying external influences.