Electrostatics Vocabulary
Electrostatics: Complete Lessons Guide
Lesson 1: Basics of Electric Charge
- What is Electric Charge?
- Fundamental property of matter.
- Two types: Positive (+) and Negative (−).
- Like charges repel; opposite charges attract.
- Charge is Quantized
- q=ne, where n is an integer.
- Law of Conservation of Charge
- Total charge remains constant in an isolated system.
- Charge is transferred, not created or destroyed.
- Conductors vs Insulators
- Conductor:
- Electrons move freely; charge spreads on the surface.
- Examples: Metals, human body.
- Insulator:
- Electrons are bound; charge stays localized.
- Examples: Rubber, plastic, glass.
- Charging Methods
- Friction: Transfer of charge through rubbing.
- Conduction: Transfer of charge through direct contact.
- Induction: Redistribution of charge without direct contact.
Lesson 2: Coulomb's Law
- Formula:
- F=kr2∣q<em>1q</em>2∣, where k is Coulomb's constant, q<em>1 and q</em>2 are the magnitudes of the charges, and r is the distance between the charges.
- k=4πϵ<em>01, where ϵ</em>0 is the permittivity of free space.
- ϵ0=8.854×10−12C2/Nm2
- k≈8.99×109Nm2/C2
- F: magnitude of force.
- Nature of Force
- Attractive if charges are opposite.
- Repulsive if charges are like.
- Vector Nature
- Force acts along the line joining the charges.
- Use vector addition when more than two charges are present.
- Superposition Principle
- The net force on a charge is the vector sum of the forces from all other charges.
Lesson 3: Electric Fields
- Definition:
- E=qF, where E is the electric field, F is the electric force on a test charge q.
- Units: N/C or V/m
- Field from a Point Charge:
- E=kr2∣q∣
- Direction: Away from positive charges, toward negative charges.
- Electric Field Lines
- Away from positive charges, toward negative charges.
- More lines indicate a stronger field.
- Lines never cross.
- The electric field is tangent to the lines at any point.
- Superposition of Fields
- Add vector components to find the net electric field.
- Common Configurations:
- Point charge: Electric field radiates spherically.
- Infinite line: Electric field radiates cylindrically.
- Infinite plane: Electric field is constant and perpendicular to the plane.
- Parallel plates: Uniform electric field between the plates.
Lesson 4: Electric Potential
- What is Electric Potential?
- Scalar quantity.
- Work done per unit charge to move a test charge from a reference point to a specific point in the electric field.
- V=qW
- Relation to Electric Field
- V=−∫E⋅dl
- Equipotential Surfaces
- Surfaces where the electric potential is constant.
- Always perpendicular to electric field lines.
- No work is done moving a charge along an equipotential surface.
Lesson 5: Gauss's Law
- Statement:
- ∮E⋅dA=ϵ</em>0Q<em>enc
- The electric flux through any closed surface is proportional to the enclosed electric charge.
- Applies to symmetric charge distributions for easy calculation of electric fields.
- Applications:
- Spherical symmetry (point charge, sphere).
- Cylindrical symmetry (infinite wire).
- Planar symmetry (infinite sheet).
Lesson 6: Conductors in Electrostatics
- Key Properties:
- E=0 inside a conductor in electrostatic equilibrium.
- Excess charge resides on the surface of a conductor.
- The surface of a conductor is an equipotential.
- The electric field just outside a conductor is perpendicular to the surface with magnitude σ/ϵ0, where σ is the surface charge density.
- Shielding:
- Conductors block external electric fields.
- Used in Faraday cages to protect sensitive equipment from external electric fields.
Lesson 7: Capacitors
- Capacitance:
- C=VQ, where C is capacitance, Q is the charge stored, and V is the potential difference.
- Unit: Farad (F).
- Parallel Plate Capacitor:
- C=ϵ0dA, where A is the plate area and d is the distance between the plates.
- Energy Stored:
- U=21CV2=21QV=21CQ2
- Dielectrics:
- Inserting a dielectric increases capacitance.
- C′=KC, where K is the dielectric constant.
Lesson 8: Electric Dipoles
- Definition:
- Two equal and opposite charges (+q and −q) separated by a distance d.
- Dipole moment:
- p=qd, where p is the dipole moment vector, pointing from the negative charge to the positive charge.
- Torque in Electric Field:
- τ=p×E
- τ=pEsin(θ)
- Potential Energy:
- U=−p⋅E
- U=−pEcos(θ)
- Electric Field of a Dipole (approx., far away):
- Along the axis: E=r32kp
- Perpendicular to the axis: E=r3kp