BackElectrostatics: Calculus-Based Physics Study Notes
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Electrostatics
1. Electric Charge
Electric charge is a fundamental property of matter responsible for electric forces and interactions. It is quantized, conserved, and invariant under changes in reference frame.
Definition: Electric charge (q or Q) is measured in coulombs (C).
Quantization: All observable charges are integer multiples of the elementary charge e:
Carriers: Protons carry +e, electrons carry -e.
Conservation: The total charge in an isolated system remains constant:
Invariance: Charge does not depend on the observer's frame of reference.
Properties of Charge
Like charges repel, unlike charges attract.
Field lines: Originate from positive charges and terminate on negative charges.
SI unit: Coulomb (C).
2. Methods of Charging
Materials can be charged by transferring electrons through various mechanisms.
2.1 Charging Conductors
Friction (Triboelectric Effect): Rubbing two materials transfers electrons.
Conduction (Contact): Touching a charged object to a conductor redistributes charge.
Induction: Bringing a charged object near a conductor causes charge separation; grounding removes one type of charge.
2.2 Charging Insulators (Dielectrics)
Insulators have bound electrons; charge remains localized.
Polarization: External fields displace electron clouds, creating electric dipoles aligned with the field (dielectric polarization).
Feature | Conductor | Insulator / Dielectric |
|---|---|---|
Free carriers | ~1028 e-/m3 | Essentially none |
Charging mechanism | Friction, conduction, induction | Friction (localized), polarization |
Charge distribution | Migrates to surface | Stays where placed |
Field inside (static) | (reduced by ) | |
Examples | Cu, Al, Au | Glass, rubber, plastic |
3. Electrostatic Force — Coulomb’s Law
Coulomb’s Law describes the force between two point charges.
Vector Form:
(permittivity of free space)
points from to
Key Concepts
Inverse-square law:
Superposition Principle: The net force on a charge is the vector sum of forces from all other charges:
Central force: Acts along the line joining the charges.
Conservative force: Work done is path-independent; potential energy can be defined:
Long-range force: Acts over infinite distances.
4. The Electric Field
The electric field describes the influence a charge exerts on the space around it, defined as force per unit positive test charge.
Definition:
Units:
For a point charge at the origin:
Electric Field Lines
Originate on positive charges, terminate on negative charges or at infinity.
The tangent at any point gives the direction of .
Density of lines ∝ .
Field lines never cross.
Perpendicular to conducting surfaces in electrostatic equilibrium.
Superposition of Electric Fields
For N point charges:
5. Effects of the Electric Field on Point Charges
5.1 Force and Acceleration
A charge in field experiences:
5.2 Motion in a Uniform Electric Field
Between parallel plates separated by :
Equations of motion for a particle entering with velocity perpendicular to :
Eliminating :
Trajectory is a parabola (analogous to projectile motion).
5.3 Motion in a Non-Uniform Electric Field
Equation of motion:
Requires numerical integration in general.
Scenario | Uniform Field | Non-Uniform Field |
|---|---|---|
Field pattern | Parallel, equally spaced lines | Varying spacing/direction |
Net force on point charge | Constant | Varies with position |
Trajectory | Parabola (if ) | Complex; integrate numerically |
Net force on dipole | Zero (torque only) | Non-zero (gradient force) |
Example | Parallel plates | Near a point charge or dipole |
Dipole in a Uniform Field:
Dipole in a Non-Uniform Field:
6. Electric Field of Continuous Charge Distributions
For extended objects, replace the sum over point charges with an integral over the charge distribution.
where and is the infinitesimal charge element.
Distribution | Density | Element | Result / Formula |
|---|---|---|---|
Line (1-D) | [C/m] | (infinite line, perpendicular) | |
Surface (2-D) | [C/m2] | (infinite plane, perpendicular) | |
Volume (3-D) | [C/m3] | (inside uniform sphere) | |
Ring (1-D) | (on axis) | ||
Disk (2-D) |
6.1 Example: Ring of Charge
Symmetry: Only the axial component survives at a point on the axis.
Result:
For : (point charge behavior).
For : (center of ring).
Maximum at .
6.2 Infinite Line Charge
Using Gauss’s Law:
6.3 Infinite Plane of Charge
Using a Gaussian pillbox:
6.4 Uniformly Charged Non-conducting Sphere
For a sphere of radius and total charge :
7. Summary Table
Quantity | Formula | Notes |
|---|---|---|
Electric charge | , C | Quantized, conserved, invariant |
Coulomb force | Vector; superposition applies | |
Electric field | ||
Point charge | Radially outward for | |
Line charge | Perpendicular to wire | |
Plane charge | Uniform, perpendicular to plane | |
Ring (on axis) | Max at | |
Solid sphere | Inside: ; Outside: | Gauss’s Law |
Force on dipole | ; | Torque in uniform; net force in gradient |
Example Application: Calculating the electric field at a point on the axis of a charged ring uses symmetry to simplify the integral, resulting in a field that points along the axis and depends on the distance from the center.
Additional info: These notes are designed for calculus-based physics students and assume familiarity with vector calculus, integrals, and basic mechanics. Worked examples and derivations should be added for practice and deeper understanding.