Foundations of Electrostatics: Charge, Coulomb Interaction, and Realistic Charge Distributions

0.0(0)
Studied by 0 people
0%Unit 1 Mastery
0%Exam Mastery
Build your Mastery score
multiple choiceMultiple Choice
call kaiCall Kai
Supplemental Materials
Card Sorting

1/24

Last updated 3:12 PM on 3/12/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

25 Terms

1
New cards

Electric charge

A fundamental property of matter that causes electric interactions; like charges repel and unlike charges attract (charge is the “source” of electric forces/fields).

2
New cards

Charge conservation

Principle that the total charge of an isolated system remains constant: if no charge enters/leaves, then Qinitial = Qfinal (charge can be transferred between objects, but total stays fixed).

3
New cards

Elementary charge (e)

The fundamental unit of charge magnitude: e = 1.602×10^−19 C (protons have +e, electrons have −e).

4
New cards

Quantization of charge

Charge exists in discrete amounts; any net charge is an integer multiple of e: q = n e, where n is an integer.

5
New cards

Conductor

Material in which charges (typically electrons) move freely; excess charge redistributes and, at electrostatic equilibrium, resides on the surface.

6
New cards

Insulator

Material in which charges are bound to atoms/molecules and do not move freely through the object.

7
New cards

Polarization

Slight separation/shift of positive and negative charge within a neutral object (e.g., molecular distortion in insulators or electron movement in conductors), enabling attraction to a nearby charged object without changing net charge.

8
New cards

Electrostatic equilibrium (conductor)

State where charge on a conductor has finished redistributing; in this state, excess charge is on the surface (not throughout the volume).

9
New cards

Charging by friction (triboelectric effect)

Charging process where rubbing transfers electrons between materials; one object gains electrons (becomes negative) and the other loses electrons (becomes positive).

10
New cards

Charging by conduction (contact)

Charging process where a charged conductor touches another conductor and charge flows until they reach the same electric potential; total charge is conserved.

11
New cards

Charging by induction

Charging without contact: a nearby charge rearranges charges in a conductor; with a grounding step and proper removal sequence, the conductor can end with a net charge.

12
New cards

Grounding

Providing a conducting path to Earth so electrons can flow to/from an object during induction, depending on whether the external charge attracts or repels electrons.

13
New cards

Coulomb’s law

Law giving the electrostatic force between two point charges at rest: magnitude F = k |q1 q2| / r^2, along the line joining the charges.

14
New cards

Coulomb’s constant (k)

Constant in Coulomb’s law: k = 1/(4π ε0) ≈ 8.99×10^9 N·m^2/C^2.

15
New cards

Permittivity of free space (ε0)

Physical constant relating to electric interactions in vacuum: ε0 = 8.854×10^−12 C^2/(N·m^2).

16
New cards

Point charge

Idealized charge whose size is negligible compared with the distances involved, allowing it to be treated as located at a single point.

17
New cards

Inverse-square dependence

Relationship where a force magnitude decreases as 1/r^2; in Coulomb’s law, doubling r makes the force 1/4 as large.

18
New cards

Vector form of Coulomb force

Force on q1 due to q2 written with direction explicitly: F⃗{1←2} = k (q1 q2 / r^2) r̂{1←2}, where the sign of q1 q2 sets attraction vs. repulsion.

19
New cards

Unit vector r̂_{1←2}

A unit vector pointing from charge q2 toward charge q1; used to encode direction in Coulomb’s law vector form.

20
New cards

Superposition principle (electric force)

Net electrostatic force on a charge equals the vector sum of forces from all other charges: F⃗net = Σ F⃗{←i}.

21
New cards

Charge distribution

Model where charge is spread continuously over an object (line/surface/volume); you divide into small pieces dq and integrate their Coulomb-law contributions.

22
New cards

Differential charge element (dq)

An infinitesimal piece of charge used in integrals for distributions; typically dq = λ dl, dq = σ dA, or dq = ρ dV.

23
New cards

Linear charge density (λ)

Charge per unit length along a line/rod: λ = dq/dl (units: C/m). For uniform density, λ = Q/L.

24
New cards

Surface charge density (σ)

Charge per unit area on a surface: σ = dq/dA (units: C/m^2).

25
New cards

Volume charge density (ρ)

Charge per unit volume in a region: ρ = dq/dV (units: C/m^3).

Explore top notes

note
Biology - Evolution
Updated 1477d ago
0.0(0)
note
Essay
Updated 1501d ago
0.0(0)
note
iPhone SE 4_ What To Expect.mp4
Updated 930d ago
0.0(0)
note
Chemistry of Life, Biology
Updated 1771d ago
0.0(0)
note
Chemical bonds
Updated 975d ago
0.0(0)
note
Photons
Updated 901d ago
0.0(0)
note
Biology - Evolution
Updated 1477d ago
0.0(0)
note
Essay
Updated 1501d ago
0.0(0)
note
iPhone SE 4_ What To Expect.mp4
Updated 930d ago
0.0(0)
note
Chemistry of Life, Biology
Updated 1771d ago
0.0(0)
note
Chemical bonds
Updated 975d ago
0.0(0)
note
Photons
Updated 901d ago
0.0(0)

Explore top flashcards

flashcards
faf
40
Updated 958d ago
0.0(0)
flashcards
faf
40
Updated 958d ago
0.0(0)