Motion In Electromagnetic Fields

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Notes de leçon

Magnetic Force on a Current-Carrying Conductor

  • A current-carrying conductor produces its own magnetic field and experiences a force when placed in an external magnetic field.
  • The force is given by F = BIL sin θ, where B is magnetic flux density, I is current, L is the length of conductor in the field, and θ is the angle between the conductor and the B field.
  • The force is maximum when the conductor is perpendicular to the field (θ = 90°, sin θ = 1), giving F = BIL.
  • The force is zero when the conductor is parallel to the field (θ = 0°, sin θ = 0).
  • The force can be increased by increasing the magnetic field strength, the current, or the length of the conductor in the field.
  • The direction of the force is given by Fleming's left-hand rule: thumb = force (motion), first finger = magnetic field, second finger = conventional current.

Setup for demonstrating the force on a current-carrying conductor in a magnetic field.

Setup for demonstrating the force on a current-carrying conductor in a magnetic field.

Representing Magnetic Fields in 3D

  • Dots (or circles with dots) represent a magnetic field directed out of the page.
  • Crosses represent a magnetic field directed into the page.
  • Remember: an arrow approaching head-on shows only its tip (dot); an arrow receding shows the cross of its feathers (cross).
  • Conventional current flows from positive to negative, opposite to the direction of electron flow.

Magnetic field lines

Magnetic field lines

Magnetic Force between Two Parallel Conductors

  • Each current-carrying conductor produces a magnetic field around it, determined by the right-hand thumb rule.
  • Parallel conductors with currents in the same direction attract each other.
  • Parallel conductors with currents in opposite directions repel each other.
  • The force per unit length between two parallel conductors is F/L = μ₀I₁I₂ / (2πr), where r is the separation and μ₀ = 4π × 10⁻⁷ N A⁻².
  • The forces on the two wires are equal and opposite (Newton's third law).

Magnetic Force on a Moving Charge

  • A moving charge produces its own magnetic field and experiences a force when in an external magnetic field.
  • The force is given by F = Bqv sin θ, where q is the charge, v is the speed, and θ is the angle between velocity and the B field.
  • The force is maximum when the charge moves perpendicular to the field (θ = 90°), giving F = Bqv.
  • A charge moving parallel to the magnetic field experiences no force.
  • The force is always perpendicular to both the velocity and the magnetic field.
  • For a negative charge, the direction of conventional current is opposite to its motion; use Fleming's left-hand rule with the current direction.

Charged Particles in Magnetic Fields

  • A charged particle moving perpendicular to a uniform magnetic field travels in a circular path because the magnetic force is always perpendicular to its velocity.
  • The magnetic force provides the centripetal force: mv²/r = BQv.
  • Rearranging gives the radius of the path: r = mv / (BQ).
  • The radius increases with greater mass or speed, and decreases with greater charge or magnetic field strength.
  • The centripetal acceleration is in the same direction as the magnetic force (Newton's second law, F = ma).

Charged Particles in Electric Fields

  • A charged particle in a uniform electric field experiences a constant force and travels in a parabolic trajectory.
  • A positive charge is deflected towards the negative plate; a negative charge towards the positive plate.
  • An uncharged particle (e.g. a neutron) experiences no force and travels straight through.
  • The amount of deflection depends on mass (greater mass → smaller deflection), charge (greater charge → greater deflection), and speed (greater speed → smaller deflection).

Attraction and repulsion of charge

Attraction and repulsion of charge

Charged Particles in Electric & Magnetic Fields

  • When electric and magnetic fields are perpendicular, a charged particle experiences an electric force parallel to E and a magnetic force perpendicular to B.
  • For a positively charged particle, the electric and magnetic forces act in opposite directions; the same is true for a negatively charged particle, but with directions reversed.
  • When the electric and magnetic forces are equal in magnitude, the particle moves in a straight line with constant speed.
  • Equating the forces: qE = Bqv, which gives the speed v = E/B.
  • This principle is used in velocity selectors and in J.J. Thomson's experiment to determine the charge-to-mass ratio of an electron.

Charge-to-Mass Ratio

  • The charge-to-mass ratio is defined as Q/m.
  • For an electron, e/mₑ = 1.76 × 10¹¹ C kg⁻¹; for a proton, e/mₚ = 9.58 × 10⁷ C kg⁻¹.
  • J.J. Thomson used Helmholtz coils (uniform B field) and oppositely charged parallel plates (uniform E field) to determine e/mₑ.
  • The speed of particles is found using perpendicular electric and magnetic fields: v = V / (Bd).
  • The charge-to-mass ratio is then q/m = V / (rB²d), where r is the radius of the circular path when the electric field is switched off.

Diapos

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Questions d'entraînement

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  1. 1.What does the magnetic flux density B represent?

    Easy
    • AThe force per unit current per unit length on a conductor perpendicular to the field
    • BThe total magnetic force on a stationary charge
    • CThe magnetic field strength measured in volts per metre
    • DThe force per unit charge on a stationary charge
  2. 2.A straight wire of length 0.90 m carries a current of 1.5 A and is placed at 45° to a uniform magnetic field of flux density 0.20 T. What is the magnitude of the force on the wire?

    Medium
    • A0.19 N
    • B0.27 N
    • C0.38 N
    • D0.14 N
  3. 3.Which of the following changes would increase the magnitude of the force on a current-carrying wire in a magnetic field? (select all that apply)

    Medium
    • AIncreasing the current in the wire
    • BIncreasing the magnetic flux density
    • CIncreasing the length of wire within the field
    • DRotating the wire so it is parallel to the field
    • EReversing the direction of the current
  4. 4.A current-carrying conductor experiences no magnetic force when it is placed:

    Easy
    • Aat 90° to the magnetic field
    • Bparallel to the magnetic field
    • Cat 45° to the magnetic field
    • Dperpendicular to the magnetic field
  5. 5.Which of the following is the fundamental SI unit of magnetic flux density?

    Easy
    • ATesla (T)
    • BWeber (Wb)
    • CNewton per ampere (N A⁻¹)
    • DVolt (V)
  6. 6.Two parallel wires carrying currents in the same direction attract each other.

    Easy

    True or false?

  7. 7.A charged particle moving parallel to a uniform magnetic field experiences a magnetic force.

    Easy

    True or false?

  8. 8.An electron enters a uniform magnetic field directed into the page, moving from left to right. In which direction does the magnetic force on the electron act?

    Medium
    • AUpwards
    • BDownwards
    • CInto the page
    • DOut of the page

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