Electrostatics
Misconceptions
| Misconception | Correction |
|---|---|
| "Positive charges are heavier than negative charges" | Protons and electrons have nearly the same magnitude of charge; mass is unrelated to charge sign |
| "Electric field is the same as electric force" | Electric field (E) is force per unit charge; E = F/q. Field exists even without a test charge |
| "Doubling the distance halves the force" | Coulomb's law has inverse-square dependence: F ~ 1/r². Doubling distance reduces force to 1/4 |
| "Electric potential is the same as potential energy" | Potential (V) is energy per unit charge; PE = qV. Potential is a property of position, PE depends on the charge placed there |
| "Insulators cannot have any charge" | Insulators can hold charge; they just don't allow charge to flow freely through them |
Key Concepts
Electric Charge
The fundamental property of matter that causes electromagnetic interactions.
Properties:
- •Two types: positive (+) and negative (-)
- •Like charges repel, opposite charges attract
- •Charge is quantized: q = ne, where e = 1.602 × 10⁻¹⁹ C
- •Charge is conserved in all processes
- •Unit: Coulomb (C)
Coulomb's Law
The electric force between two point charges:
$$F = k\frac{q_1 q_2}{r^2}$$
Where:
- •k = 8.99 × 10⁹ N·m²/C² (Coulomb's constant)
- •q₁, q₂ = charges (in Coulombs)
- •r = distance between charges (in meters)
- •F = force (in Newtons)
Direction:
- •Positive F: repulsive (like charges)
- •Negative F: attractive (opposite charges)
- •Force acts along the line connecting the charges
Electric Field
A vector field that describes the electric force per unit positive test charge:
$$E = \frac{F}{q} = k\frac{Q}{r^2}$$
Where:
- •E = electric field strength (N/C or V/m)
- •Q = source charge creating the field
- •r = distance from the source charge
Direction:
- •Points away from positive charges
- •Points toward negative charges
- •At any point, E indicates the direction a positive test charge would accelerate
Electric Potential
The electric potential energy per unit charge (scalar quantity):
$$V = k\frac{Q}{r}$$
Where:
- •V = electric potential (Volts, V = J/C)
- •Q = source charge
- •r = distance from the source charge
Key points:
- •Positive charges create positive potential
- •Negative charges create negative potential
- •Potential is a scalar (no direction)
- •Potential difference (voltage) drives current
Electric Potential Energy
The energy stored in a system of charges:
$$PE = k\frac{q_1 q_2}{r} = qV$$
Where:
- •PE = potential energy (Joules)
- •q₁, q₂ = the two charges
- •r = separation distance
- •V = potential at the location of charge q
Sign convention:
- •Positive PE: like charges (repulsive, energy required to bring together)
- •Negative PE: opposite charges (attractive, energy released when brought together)
Work Done by Electric Field
Work done by the electric field when moving a charge:
$$W = q(V_i - V_f) = -\Delta PE$$
Where:
- •W = work done by the field (Joules)
- •q = charge being moved
- •Vᵢ, Vf = initial and final potentials
Key points:
- •Field does positive work when moving + charge to lower potential
- •Field does positive work when moving - charge to higher potential
- •Work by field = negative of change in PE
Conductors vs Insulators
Conductors:
- •Allow charges to move freely
- •Excess charge resides on the surface
- •Electric field inside is zero (electrostatic equilibrium)
- •Examples: metals, ionic solutions
Insulators:
- •Charges cannot move freely
- •Charge remains where placed
- •Can be polarized (induced dipoles)
- •Examples: rubber, glass, plastic
Equations
[1] F = kq₁q₂/r² (Coulomb's law) [2] E = F/q = kQ/r² (electric field from point charge) [3] V = kQ/r (electric potential from point charge) [4] PE = kq₁q₂/r = qV (electric potential energy) [5] W = q(Vᵢ - Vf) = -ΔPE (work by electric field) [6] k = 8.99 × 10⁹ N·m²/C² (Coulomb's constant) [7] e = 1.602 × 10⁻¹⁹ C (elementary charge)
Worked Examples
Example 1: Coulomb's Law
Problem: Two charges, q₁ = +3 μC and q₂ = -5 μC, are separated by 0.2 m. What is the magnitude of the electric force between them?
Solution:
- •Convert units: q₁ = 3 × 10⁻⁶ C, q₂ = 5 × 10⁻⁶ C
- •Apply Coulomb's law: F = k|q₁q₂|/r²
- •F = (8.99 × 10⁹)(3 × 10⁻⁶)(5 × 10⁻⁶)/(0.2)²
- •F = (8.99 × 10⁹)(15 × 10⁻¹²)/(0.04)
- •F = 3.37 N (attractive)
Example 2: Electric Field
Problem: What is the electric field 0.5 m from a +8 μC point charge?
Solution:
- •E = kQ/r²
- •E = (8.99 × 10⁹)(8 × 10⁻⁶)/(0.5)²
- •E = (8.99 × 10⁹)(8 × 10⁻⁶)/0.25
- •E = 2.88 × 10⁵ N/C (pointing away from the charge)
Example 3: Electric Potential Energy
Problem: How much work is required to bring a +2 μC charge from infinity to a point 0.3 m from a +6 μC charge?
Solution:
- •Work required = ΔPE = PEf - PEi
- •PEi = 0 (at infinity)
- •PEf = kq₁q₂/r = (8.99 × 10⁹)(2 × 10⁻⁶)(6 × 10⁻⁶)/0.3
- •PEf = (8.99 × 10⁹)(12 × 10⁻¹²)/0.3
- •Work = 0.36 J
Explanation Patterns
- •Identify the charges - What are their signs and magnitudes?
- •Determine what's asked - Force, field, potential, or energy?
- •Draw a diagram - Show charges, distances, and direction of fields/forces
- •Choose the appropriate equation:
- •Force between charges: Coulomb's law
- •Field from a charge: E = kQ/r²
- •Potential from a charge: V = kQ/r
- •Energy of configuration: PE = kq₁q₂/r
- •Watch units - Convert μC to C, cm to m
- •Check signs - Like charges repel, opposite attract
Common Problem Types
- •Coulomb force calculations: Find force magnitude and direction between point charges
- •Electric field from point charges: Calculate field strength and direction
- •Superposition of fields: Add vector fields from multiple charges
- •Electric potential calculations: Find potential at a point from one or more charges
- •Potential energy of charge systems: Calculate energy stored in charge configurations
- •Work-energy problems: Find work to move charges between points
- •Conductor/insulator concepts: Qualitative questions about charge distribution