Moving Charges and Magnetism

0.0(0)
Studied by 0 people
call kaiCall Kai
Locked
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/17

flashcard set

Earn XP

Description and Tags

Practice vocabulary flashcards based on the fundamental concepts of electromagnetism, Lorentz force, Biot-Savart law, and galvanometers from chapter four.

Last updated 12:38 PM on 7/14/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai
Chat

No analytics yet

Send a link to your students to track their progress

18 Terms

1
New cards

Hans Christian Oersted

Danish physicist who discovered in 1820 that an electric current in a straight wire caused a deflection in a nearby magnetic compass needle.

2
New cards

Lorentz Force

The total force acting on a point charge qq moving with velocity v\mathbf{v} in the presence of both electric field E\mathbf{E} and magnetic field B\mathbf{B}, expressed as F=q[E(r)+v×B(r)]\mathbf{F} = q [ \mathbf{E}(\mathbf{r}) + \mathbf{v} \times \mathbf{B}(\mathbf{r}) ].

3
New cards

Tesla (TT)

The SI unit of magnetic field; the magnitude is 11 unit when the force on a charge of 1C1\,C moving perpendicular to the field at 1m/s1\,m/s is 1N1\,N.

4
New cards

Gauss (GG)

A non-SI unit used to measure magnetic field, where 1G=104tesla1\,G = 10^{-4}\,tesla.

5
New cards

Cyclotron Frequency (νc\nu_c)

The frequency of uniform circular motion for a charge in a plane normal to a magnetic field, given by the formula νc=qB2πm\nu_c = \frac{qB}{2\pi m}.

6
New cards

Pitch (pp)

The distance moved by a charged particle along the magnetic field during one rotation in helical motion, given by p=vT=2πmvqBp = v_{\parallel} T = \frac{2\pi m v_{\parallel}}{qB}.

7
New cards

Biot-Savart Law

A vector relationship defining the magnetic field dBd\mathbf{B} produced by an infinitesimal current element IdlI d\mathbf{l} at distance rr, given by dB=μ04πIdl×rr3d\mathbf{B} = \frac{\mu_0}{4\pi} \frac{I d\mathbf{l} \times \mathbf{r}}{r^3}.

8
New cards

Permeability of free space (μ0\mu_0)

The proportionality constant in the Biot-Savart law with an exact value of 4π×107Tm/A4\pi \times 10^{-7}\,T\,m/A.

9
New cards

Ampere's Circuital Law

States that the line integral of the magnetic field B\mathbf{B} over a closed loop is equal to μ0\mu_0 times the total current II passing through the surface: Bdl=μ0I\oint \mathbf{B} \cdot d\mathbf{l} = \mu_0 I.

10
New cards

Amperian Loop

A closed loop chosen such that at each point, the magnetic field is either tangential with constant magnitude, normal to the loop, or vanishes, facilitating the evaluation of magnetic fields.

11
New cards

Solenoid

A device consisting of a long wire wound in the form of a helix with closely spaced turns; the internal magnetic field is uniform and given by B=μ0nIB = \mu_0 n I.

12
New cards

Ampere (AA)

The value of a steady current which, when maintained in each of two very long, straight, parallel conductors placed 1m1\,m apart in vacuum, produces a force of 2×107newtons2 \times 10^{-7}\,newtons per metre of length.

13
New cards

Magnetic Moment (m\mathbf{m})

A vector quantity for a current loop of area A\mathbf{A} with NN turns carrying current II, defined as m=NIA\mathbf{m} = N I \mathbf{A}.

14
New cards

Moving Coil Galvanometer (MCG)

An instrument consisting of a coil free to rotate in a uniform radial magnetic field; the steady angular deflection ϕ\phi is proportional to the current II.

15
New cards

Current Sensitivity

The deflection per unit current in a galvanometer, expressed by the constant NABk\frac{NAB}{k}, where kk is the torsional constant of the spring.

16
New cards

Voltage Sensitivity

The deflection per unit voltage in a galvanometer, given by ϕV=NABkR\frac{\phi}{V} = \frac{NAB}{kR}.

17
New cards

Shunt Resistance (rsr_s)

A small resistance connected in parallel with a galvanometer coil to convert it into an ammeter for measuring higher currents.

18
New cards

Torque (on a current loop)

The rotational force experienced by a loop of magnetic moment m\mathbf{m} in a uniform magnetic field B\mathbf{B}, given by τ=m×B\boldsymbol{\tau} = \mathbf{m} \times \mathbf{B}.