Electric Charges and Fields Study Notes
Chapter One: Electric Charges and Fields
1.1 Introduction
- Static Electricity: Phenomenon observed when synthetic clothes or sweaters produce sparks or crackling noises, especially in dry weather.
- Lightning: Another common example of electric discharge linked to static electricity.
- Electric Shocks: Sensations felt upon touching objects after sliding from a seat, due to electric charge discharge.
- Cause: Accumulation of electric charges through the rubbing of insulating surfaces. The chapter focuses on static electricity.
1.2 Electric Charge
- Historical Insight: Thales of Miletus (around 600 BC) discovered that amber rubbed with wool attracts light objects.
- Etymology: The term 'electricity' derives from the Greek word "elektron," meaning amber.
- Electrification: Two kinds of charge exist: positive and negative.
- Observation:
- Like charges repel each other.
- Unlike charges attract each other. - Polarity of Charge:
- Glass rods rubbed with silk obtain a positive charge while silk obtains a negative charge.
- When a charged object touches another of the opposite charge, they neutralize each other's effect. - Terminology: Franklin's designation of charges - glass rod’s charge as positive, plastic rod’s charge as negative.
- Electric Charge: A body is said to be charged when it possesses electric charge ( ). If it has none, it is electrically neutral.
1.3 Conductors and Insulators
- Conductors: Substances that allow electricity to pass through easily, e.g., metals, human bodies, and earth. Electrons in conductors move freely.
- Insulators: Substances that do not allow electricity to pass, e.g., glass, porcelain, plastics, nylon, and wood. Charges on insulators remain localized.
- Examples of charging: A plastic comb gets charged when used on dry hair, while metal does not due to its conductivity.
1.4 Basic Properties of Electric Charge
- Types of Charges: Positive and negative. Their effects cancel each other out.
1.4.1 Additivity of Charges
- Total charge of a system with point charges q1, q2,…, qn is given by:
Qexttotal=q1+q2+…+qn - Charges are scalars, thus their signs must be considered during addition.
1.4.2 Charge Conservation
- Law of Conservation: Total charge in an isolated system remains constant; no charge is created or destroyed.
- Implications: Transfer of charge between bodies does not change the overall charge in an isolated system.
1.4.3 Quantization of Charge
- All free charges are integral multiples of a basic charge unit, denoted by e.
- Electric charge, q, can be quantified as:
q=nimese
where n is any integer (positive or negative). - Charge of an electron is .602192 × 10-19 C; charge of a proton is +e. The charge is constant but significant at the macroscopic level.
1.5 Coulomb's Law
- Description: Coulomb's law describes the force (F) between two point charges (q1 and q2) located on a distance r from each other:
F=kr2q1q2
where k is a constant determined by charge and distance. - Demonstration by Coulomb: using a torsion balance to relate forces between charged bodies.
- Experimental significance of charges leads to the consideration of units (Coulombs, C).
1.6 Forces Between Multiple Charges
- Superposition Principle: The total force on any charge due to multiple charges is the vector sum of individual forces acting on that charge.
1.7 Electric Field
- Concept of Electric Field: Created by charges, characterized by how a test charge would experience a force in that field due to another charge. It is defined mathematically as:
E=qF - Directionality: The field is directed radially outward for positive charges and inward for negative charges.
1.7.1 Electric Field due to a System of Charges
- Using superposition, the electric field from multiple charges is derived from summing fields from each charge.
1.8 Electric Field Lines
- Representation: Electric field lines illustrate the direction of electric fields, showing density where fields are stronger.
- Properties include:
- Lines starting from positive and ending at negative charges.
- Lines never cross each other.
- Lines do not loop back on themselves.
1.9 Electric Flux
- Electric Flux Definition: Defined as the product of the electric field (E) and the area (S) through which it flows.
extFlux=EimesSimesextcos(heta) - Electric flux through a closed surface is related directly to the charge within.
1.10 Electric Dipole
- Definition: An electric dipole consists of two opposite charges separated by distance 2a, resulting in a dipole moment defined as:
p=qimes2a - The field of a dipole varies with distance and shows distinct behavior compared to single charges, falling off as 1/r3.
1.11 Continuous Charge Distribution
- Charges can be distributed over an area, line, or volume. Term definition:
- Surface charge density: AQ
- Linear charge density: lQ
- Volume charge density: VQ - Continuous charge distributions can be analyzed using integrals of electric fields contributed by differential charge elements.
1.12 Gauss's Law
- Definition: Electric flux through a closed surface is proportional to the total charge enclosed in that surface:
ext{Electric Flux} = rac{Q}{
o}
Examples of Gauss's Law Applications
- For an infinite straight charged wire:
E = rac{
o}{2
o r} - For a uniformly charged infinite plane sheet:
E = rac{
o}{2
o} - For a thin spherical shell:
- Outside: E = rac{Q}{4
o r^2}
- Inside: E=0
Summary
- Key points: Electric charges exist as two types, follow properties such as conservation, and can generate electric fields and fluxes.
- Applications: Gauss's law plays vital roles in understanding electric fields in symmetrical distributions and has extensive applications in electrostatics.
Exercises
- Calculations regarding Coulomb’s law forces, electric fields, and the application of Gauss’s law based on configurations and setups as per provided exercises.