Comprehensive Study Guide: Unit 4 Magnetism and Induction

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39 Terms

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Magnetic Field

Denoted as (\vec{B}), it is the field created by moving electric charges (currents) and intrinsic spin of electrons.

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Source of Magnetic Field

Moving electric charges (currents) or intrinsic spin of electrons.

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Direction of Magnetic Field

Defined as the direction the North pole of a compass would point, with field lines exiting the North pole and entering the South pole.

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Magnetic Field Lines

Always form closed loops and do not have isolated North or South poles.

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SI Unit of Magnetic Field

Tesla (T), where (1 \, T = 1 \, \frac{N}{A \, m}).

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Magnetic Dipole

The fundamental unit of magnetism that can represent even a single atom due to electron spin.

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Ferromagnetism

When material has domains of aligned atomic dipoles, making it a permanent magnet.

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Magnetic Force on a Moving Charge

Given by the equation (F_M = |q|vB\sin(\theta)).

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Variables in Magnetic Force Equation

(q = ) charge (Coulombs), (v = ) speed (m/s), (B = ) magnetic field strength (T), and (\theta = ) angle between velocity and magnetic field.

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Maximum Magnetic Force

Occurs when velocity is perpendicular to the field ((\theta = 90^\circ)).

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Zero Magnetic Force

Occurs when velocity is parallel or anti-parallel to the field ((\theta = 0^\circ) or (180^\circ)).

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Work Done by Magnetic Forces

Magnetic forces do no work on particles; they can change direction but not speed.

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Uniform Circular Motion

Motion of a charged particle in a magnetic field due to the perpendicular magnetic force.

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Radius of Circular Motion

Given by (r = \frac{mv}{qB}).

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Right-Hand Rule #1 (Flat Hand Rule)

To find the magnetic force: thumb in velocity direction, fingers in magnetic field direction; positive charge force out of palm.

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Force on a Current-Carrying Wire

Given by the equation (F_M = I \ell B \sin(\theta)).

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Variables in Wire Force Equation

(I = ) current (A), (\ell = ) length of wire in magnetic field (m), (\theta = ) angle between current and magnetic field.

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Right-Hand Rule for Current

Thumb points in the current direction for a wire; using the same principle as for moving charges.

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Magnetic Field of a Long Straight Wire

Given by (B = \frac{\mu_0 I}{2\pi r}).

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Vacuum Permeability Constant ((\mu_0))

Approximately (4\pi \times 10^{-7} \, T \cdot m/A).

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Right-Hand Rule #2 (Curl Rule)

To find the direction of magnetic field lines around a wire: thumb in current direction, curl fingers.

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Forces Between Parallel Wires

Wires carrying current: same direction attract, opposite direction repel.

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Electromagnetic Induction

Describes how a changing magnetic environment can induce a current.

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Magnetic Flux ((\Phi_B))

Measure of the magnetic field passing through an area, given by (\Phi_B = B \cdot A \cdot \cos(\theta)).

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Defined Units of Magnetic Flux

Measured in Webers (Wb).

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Faraday's Law of Induction

States induced EMF occurs with a change in magnetic flux over time: (\mathcal{E} = -N \frac{\Delta \Phi_B}{\Delta t}).

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Induced EMF ((\mathcal{E}))

Voltage induced in a coil due to change in magnetic flux.

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Lenz's Law

Induced current creates a magnetic field that opposes the change in original magnetic flux.

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Ways to Induce EMF

Changing magnitude of (B), changing area (A), and changing orientation (\theta).

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Motional EMF

Voltage induced when a conducting bar moves through a magnetic field: (\mathcal{E} = B \ell v).

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Comparison of Electric and Magnetic Fields

Electric fields act on charges, can do work; magnetic fields act only on moving charges and cannot do work.

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Electric Fields Start and End

Start on positive charges and end on negative charges.

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Magnetic Fields Form

Form closed loops connecting North to South poles.

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Common Mistakes in Magnets

Confusing normal vector angles in flux calculations and misunderstanding induced EMF.

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Charge Signs

For negative charges, the force direction is opposite to the palm in the Right-Hand Rule.

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Velocity and Force Relation

Only the component of velocity perpendicular to the field creates force; if (v) is parallel to (B), force is zero.

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Induced Field Direction with Lenz's Law

Induced field opposes change in flux, not always opposing external field directly.

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Debugging Right-Hand Rule Confusion

Use right hand consistently for forces and fields, regardless of being left-handed.

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Perpendicular Strength Loss

If the magnetic field runs parallel to the surface, flux is zero.

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