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Key vocabulary terms and definitions from the lecture notes on moving charges and magnetism, covering magnetic fields, forces, devices, and conversion formulas.
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Magnetic Field
A vector field around magnets and current-carrying conductors where magnetic effects can be observed; direction aligns with the force on moving charges.
Tesla (T)
SI unit of magnetic flux density; 1 T = 1 Weber per square meter (Wb/m^2); equals 10^4 Gauss.
Gauss (G)
CGS unit of magnetic flux density; 1 T = 10^4 G.
Biot–Savart Law
Describes the magnetic field from a current element dl: dB = (μ0/4π) I dl × r̂ / r^2; integrated over the current gives B.
Ampere's Circuital Law
The line integral of the magnetic field around a closed loop equals μ0 times the current through the loop: ∮ B · dl = μ0 I_enclosed.
Lorentz Force
Force on a charged particle q moving with velocity v in a magnetic field B: F = q v × B.
Magnetic Dipole Moment
For a current loop, M = N I A (N = number of turns, I = current, A = loop area); vector along the loop’s normal.
Solenoid
A hollow tube wound with many turns of insulated wire; inside, it produces a nearly uniform magnetic field: B = μ0 n I (n = turns per unit length).
Magnetic Field Inside a Solenoid
Inside a long solenoid, the magnetic field is uniform and given by B = μ0 n I.
Magnetic Field Due to a Straight Wire
Field at distance r from a long straight current-carrying wire: B = μ0 I /(2π r); direction is tangential (use right-hand rule).
Right-Hand Rule
Rule to determine B direction around a current: point thumb along current; fingers curl in the direction of B.
Permeability of Free Space (μ0)
Constant μ0 = 4π × 10^-7 T·m/A; relates B and H in vacuum (B = μ0 H).
Moving Charged Particle in Magnetic Field
A moving charge experiences F = q v × B; if v ⟂ B, the path is circular with radius r = m v /(q B).
Current-Carrying Conductor in Magnetic Field
Force on a straight wire of length l carrying current I in a magnetic field B: F = I l × B; magnitude F = I l B sin θ.
Ammeter
Instrument to measure current; ideal ammeter has zero resistance and is connected in series.
Voltmeter
Instrument to measure potential difference; ideal voltmeter has infinite resistance and is connected in parallel.
Galvanometer
A coil-based instrument that deflects in proportion to current; the basis for galvanometers used in ammeters and voltmeters.
Conversion: Galvanometer to Ammeter
Add a shunt resistor in parallel with the galvanometer so most current bypasses it; Rs = Rg · Igfs /(Itotal − Igfs) = Rg · Ifs /(Itotal − Ifs).
Conversion: Galvanometer to Voltmeter
Connect a resistor in series with the galvanometer to extend voltage range; Vfs = Igs (Rg + Rseries); thus Rseries = Vfs / Igs − Rg.