1.1 Frictional Electricity & Two Types of Charges
When two suitable non-conducting insulating bodies are vigorously rubbed together, they acquire the property of attracting small, lightweight objects (such as tiny scraps of dry paper, dust particles, or pith balls). This phenomenon is known as Frictional Electricity or Static Electricity (স্থির তড়িৎ) because the electric charges generated remain localized at the points of friction and do not flow.
Through systematic historic experiments, American scientist Benjamin Franklin (1706–1790) classified electric charges into two fundamental types:
- Positive Charge (+): The charge acquired by a clean glass rod when rubbed with a pure silk cloth. (Silk acquires an equal negative charge).
- Negative Charge (-): The charge acquired by an ebonite rod (or hard rubber/amber) when rubbed with flannel or animal wool. (Flannel acquires an equal positive charge).
Fundamental Law of Electrostatics: Like charges repel each other, whereas unlike (opposite) charges attract each other.
1.2 Electron Theory of Electrification & Charge Conservation
Modern atomic physics reveals that matter is composed of electrically neutral atoms consisting of a dense, positively charged nucleus surrounded by negatively charged orbiting electrons. In any neutral atom:
$$\text{Total Number of Protons } (+) = \text{Total Number of Electrons } (-)$$Mechanism of Frictional Charging: Protons are tightly bound within the atomic nucleus by powerful strong nuclear forces and cannot move. However, loosely held valence electrons in the outermost atomic shells of materials with lower work functions can be transferred through mechanical rubbing friction:
- Body Losing Electrons: Develops a deficit of negative electrons and consequently acquires a net Positive Charge ($+Q$).
- Body Gaining Electrons: Develops an excess of electrons and consequently acquires an equal net Negative Charge ($-Q$).
Law of Conservation of Electric Charge: Electric charge can neither be created nor destroyed; in any isolated system, the algebraic sum of positive and negative charges remains strictly constant. Charging by rubbing is merely a transfer of electrons from one body to another.
Quantization of Charge: Any observable electric charge $Q$ is always an integral multiple of the elementary electron charge $e$ ($1.602 \times 10^{-19}\text{ C}$):
$$Q = \pm n \cdot e \quad (n = 1, 2, 3, \dots)$$1.3 Electrostatic Induction (Free vs. Bound Charges)
Electrostatic Induction (স্থির তড়িৎ আবেশ): The temporary redistribution of electrical charges in an uncharged conductor caused by the proximity of a nearby charged body without any direct physical contact is called electrostatic induction.
Experimental Demonstration:
- Mount an insulated, uncharged cylindrical brass conductor on a dry glass stand.
- Bring a strongly positively charged glass rod near its left end ($A$) without touching it.
- Free mobile conduction electrons in the brass conductor are electrostatically attracted toward end $A$, creating an accumulation of negative charge at $A$. Concurrently, the remote right end ($B$) experiences an electron deficit, developing an equal positive charge.
Classification of Induced Charges:
- Bound Charge (বদ্ধ আধান): The opposite charge produced at the nearer end ($A$). It is held captive by the electrostatic attraction of the inducing rod and cannot escape to earth if grounded.
- Free Charge (মুক্ত আধান): The similar charge produced at the farther end ($B$). It is repelled by the inducing rod. If end $B$ is touched with a finger (earthed), free electrons surge up from the Earth to neutralize this free positive charge.
Golden Maxim of Electrostatics: Induction precedes attraction. When a charged comb attracts neutral paper scraps, it first induces an opposite bound charge on the nearer side of the paper, creating an attractive force that exceeds the repulsion on the farther side.
1.4 The Gold-Leaf Electroscope: Structure & Working
The Gold-Leaf Electroscope (স্বর্ণপত্র তড়িৎবীক্ষণ যন্ত্র) is an indispensable laboratory instrument designed to detect the presence, magnitude, and polarity (sign) of electric charge on a body.
Structural Anatomy:
- Brass Disc / Cap: Positioned at the top to receive or interact with charged bodies.
- Vertical Brass Rod: Passes through an insulating ebonite/rubber stopper into an enclosed glass jar.
- Gold Leaves: Two extremely thin, lightweight foils of gold or aluminum hinged at the lower tip of the brass rod.
- Glass Case & Tinfoil Strips: A transparent bell jar shielded from air currents, fitted with earthed interior tinfoil strips on the sides to increase sensitivity and safely discharge excessive charges.
Operational Procedures:
- Detecting Charge: Touch or bring a body near the brass disc. If the body is charged, charge transfers or induces down the rod into both gold leaves. Having identical charges, the two leaves diverge (repel each other). If uncharged, the leaves remain completely collapsed.
- Testing Nature of Charge (Positive or Negative): Charge the electroscope with a known charge (e.g., positive, so leaves are diverged). Now bring the unknown body near the disc:
- If the divergence of the leaves increases, the unknown body has the same sign as the electroscope (Positive).
- If the divergence decreases, the body is either oppositely charged or neutral.
Crucial Rule: Repulsion is the only sure test of electrification because attraction can occur between a charged body and an uncharged neutral conductor via induction.
1.5 Coulomb's Law of Electrostatic Force
In 1785, French physicist Charles-Augustin de Coulomb formulated the fundamental quantitative law governing the electrostatic force acting between two stationary point electric charges in a vacuum or air:
Statement of Coulomb's Law: The magnitude of the electrostatic attraction or repulsion force between two point charges is directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance separating them.
$$\mathbf{F = k \cdot \frac{|q_1 \cdot q_2|}{r^2}}$$Where:
- $q_1, q_2$ are the magnitudes of electric charges in Coulombs ($\text{C}$).
- $r$ is the separation distance between charges in meters ($\text{m}$).
- $k$ is the electrostatic constant ($k = \frac{1}{4\pi\varepsilon_0} \approx 9 \times 10^9\text{ N}\cdot\text{m}^2/\text{C}^2$ in air/vacuum).