Electric Charge and Electric Field – Chapter 1 Review

0.0(0)
studied byStudied by 0 people
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
Card Sorting

1/43

flashcard set

Earn XP

Description and Tags

These question-and-answer cards cover fundamental definitions, laws, formulas, and conceptual insights from Chapter 1 on Electric Charge and Electric Field, including Coulomb’s law, Gauss’s law, dipoles, field lines, and charge distributions.

Study Analytics
Name
Mastery
Learn
Test
Matching
Spaced

No study sessions yet.

44 Terms

1
New cards

What is the magnitude of the fundamental (minimum) charge on an electron or proton?

e = 1.6 × 10⁻¹⁹ C

2
New cards

State the quantization of charge equation.

Total charge Q on a body is Q = n e, where n = 0, ±1, ±2 …

3
New cards

In everyday (macroscopic) situations, why is charge quantization often ignored?

Because the charges involved are so large that the discrete steps of ±e are negligible.

4
New cards

Name two common methods of charging a body.

Friction (triboelectric effect) and induction.

5
New cards

When a glass rod is rubbed with silk, which object becomes positively charged and why?

The glass rod becomes +ve because it loses electrons to the silk.

6
New cards

State Coulomb’s law in scalar form for vacuum.

F = k |q₁q₂| / r², where k = 9 × 10⁹ N m² C⁻².

7
New cards

What is the expression for Coulomb’s constant k in terms of ε₀?

k = 1 / (4π ε₀).

8
New cards

Give the SI unit and symbol for permittivity of free space.

ε₀ = 8.85 × 10⁻¹² C² N⁻¹ m⁻²

9
New cards

How does force between two charges change inside a dielectric medium?

Fmedium = Fvacuum / K, where K (or ε_r) is the dielectric constant (>1).

10
New cards

Write Coulomb’s law in vector form for force on q₂ due to q₁.

𝐅₂₁ = (1/4π ε₀) (q₁q₂ / r³) 𝐫̂₁₂, directed along the line joining q₁ to q₂.

11
New cards

What principle explains that multiple forces add vectorially on a charge?

Superposition Principle.

12
New cards

Define electric field intensity at a point.

𝐄 = 𝐅 / q₀, the force per unit positive test charge placed at that point.

13
New cards

Write the field due to a point charge Q at distance r.

E = k Q / r², directed radially outward if Q > 0 and inward if Q < 0.

14
New cards

List two characteristics of electric field lines.

They originate on +ve charges and terminate on –ve charges; two lines never intersect.

15
New cards

What is electric flux through a surface?

Φ = ∬ 𝐄 · d𝐀, scalar measure of field lines crossing the surface.

16
New cards

State Gauss’s law in words.

The net electric flux through any closed surface equals the enclosed charge divided by ε₀.

17
New cards

Write Gauss’s law in integral form.

∯ 𝐄 · d𝐀 = Q_enclosed / ε₀.

18
New cards

Define linear charge density and give its symbol.

λ = Q / L, charge per unit length (C m⁻¹).

19
New cards

Give the electric field magnitude at distance r from an infinitely long uniformly charged wire.

E = λ / (2π ε₀ r).

20
New cards

For an infinite plane sheet of charge with surface density σ, what is the electric field near the sheet?

E = σ / (2 ε₀), directed normal to the sheet.

21
New cards

Inside a uniformly charged hollow conducting sphere, what is the electric field?

E = 0 (field inside a conductor is zero).

22
New cards

Outside a uniformly charged spherical shell (radius R, total charge Q), what is the field at distance r (r>R)?

E = k Q / r², as if all charge were concentrated at the centre.

23
New cards

Define an electric dipole.

Two equal and opposite charges separated by a finite distance 2a.

24
New cards

What is the vector definition of electric dipole moment?

𝐩 = q (2a) 𝐧̂ from –q to +q.

25
New cards

Write the torque on an electric dipole in a uniform field.

τ = 𝐩 × 𝐄 = pE sinθ, tending to align 𝐩 with 𝐄.

26
New cards

For a dipole on its axial line (r ≫ a), give the electric field magnitude.

E_axial ≈ 2k p / r³.

27
New cards

For a dipole on its equatorial line (r ≫ a), give the electric field magnitude.

E_equatorial ≈ k p / r³, directed opposite to the dipole moment.

28
New cards

What is the relation between Eaxial and Eequatorial for a point dipole?

Eaxial = 2 Eequatorial.

29
New cards

State the law of conservation of charge.

Charge can neither be created nor destroyed; it can only be transferred within an isolated system.

30
New cards

When two identical charged conductors are connected, what quantity becomes equal?

Their charges redistribute to give equal charge (average); potentials were already equal because they are identical.

31
New cards

When two non-identical conductors are connected, what becomes equal after connection?

Their potentials become equal.

32
New cards

If a conductor is grounded, what potential does it acquire?

Zero potential (earth potential).

33
New cards

How many electrons must be removed to give a body a charge of +1 μC?

n = Q/e = (1 × 10⁻⁶ C) / (1.6 × 10⁻¹⁹ C) ≈ 6.25 × 10¹² electrons.

34
New cards

What is the expression for electric field inside a uniformly charged solid sphere (radius R) at distance r<R?

E = (k Q r) / R³ (directly proportional to r).

35
New cards

Give the standard SI unit for electric field.

Newton per Coulomb (N C⁻¹) or equivalently Volt per metre (V m⁻¹).

36
New cards

What is meant by relative permittivity (dielectric constant) ε_r?

ε_r = ε / ε₀; ratio of permittivity of a medium to that of free space.

37
New cards

Write the condition for stable equilibrium of a dipole in a uniform field.

θ = 0°, dipole moment parallel to field; torque is zero and stable.

38
New cards

Why do two electric field lines never cross?

Because a unique tangent (direction of E) must exist at every point; crossing would imply two directions at one point.

39
New cards

What happens to the electric flux through a closed surface if the enclosed charge is doubled?

Flux doubles; Φ ∝ Q_enclosed.

40
New cards

Give the expressions for surface and volume charge densities.

σ = Q/A (C m⁻²); ρ = Q/V (C m⁻³).

41
New cards

State the superposition formula for net force on charge q₁ due to n other charges.

𝐅₁ = Σ (1/4π ε₀) (q₁ q_j / r₁j²) 𝐫̂₁j for j = 2 to n.

42
New cards

Does Gauss’s law determine the electric field uniquely everywhere?

Only when high symmetry (spherical, cylindrical, planar) allows field to be taken constant on Gaussian surfaces.

43
New cards

What is the direction of electric field just outside a positively charged conductor?

Normal outward to the surface.

44
New cards

Explain why electric field inside a conductor is zero in electrostatic equilibrium.

Free charges rearrange until internal field cancels; otherwise charges would continue to move.