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Electric force and coulomb's law

Twelve Standard >> Electric force and coulomb's law

 
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Electric Force and Coulomb’s Law: Derivation, Direction, and Applications

Electric force governs how static electric charges influence each other at a distance. It plays a key role in electrostatics and determines whether particles attract or repel one another. Coulomb’s Law is a mathematical expression that quantifies the electric force between charges, developed based on the experimental findings of Charles-Augustin de Coulomb.

Definition of Electric Force

The electric force is the interaction that occurs between any two charged objects. The nature and intensity of the electric force are influenced by both the sign and magnitude of the interacting charges:

  • Charges with the same polarity push each other away.
  • Charges with opposite signs attract.

This interaction plays a key role in electrostatics, operating along the direct line between the centers of the two charges. Being a vector quantity, it possesses both size and direction.

Proportionality and Derivation of Coulomb’s Law

Based on experimental data, Coulomb found that the force between two stationary point charges is:

  • Increases with the product of the absolute values of the charges involved: \( F \propto q_1 q_2 \)
  • Inversely proportional to the square of the distance between them: \( F \propto \frac{1}{r^2} \)

By merging these two expressions and incorporating the constant of proportionality, we get:

\( F = k \cdot \frac{q_1 q_2}{r^2} \)

Where \( k \) is the electrostatic constant and in vacuum or free space:

\( k = \frac{1}{4\pi\varepsilon_0} \), with \( varepsilon_0 \approx 8.854 \times 10^{-12} \, {C}^2/{N·m}^2 \)

So the full expression becomes:

\( F = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1 q_2}{r^2} \)

Effect of Medium: Dielectric Constant

When charges are situated within a material medium instead of a vacuum, the electric force between them decreases because of the medium’s dielectric properties. The formula is modified as:

\( F = \frac{1}{4\pi\varepsilon} \cdot \frac{q_1 q_2}{r^2} \)

Here, \( \varepsilon = \varepsilon_r \varepsilon_0 \), where \( \varepsilon_r \) represents the relative permittivity (also known as the dielectric constant) of the surrounding medium.

This gives:

\( F_{medium} = \frac{F_{vacuum}}{\varepsilon_r} \)

Vector Form of Coulomb's Law

To incorporate direction, Coulomb’s law is written in vector form as:

\( \vec{F}_{12} = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1 q_2}{r^2} \hat{r}_{21} \)

Where \( hat{r}_{21} \) is the unit vector pointing from charge 1 to charge 2. This vector form helps calculate directionally dependent forces in multiple-charge systems.

Matrix Representation of Forces

In systems involving multiple charges, forces can also be expressed and added using vector components or even matrices in Cartesian coordinates. The components of the force along the x, y, and z axes from multiple charges can be evaluated individually and then assembled using matrix techniques to determine the total force acting on a charge.

Magnitude of Electric Force

The scalar expression for the magnitude of the electric force between two point charges (without considering direction) is as follows:

\( F = \left| \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1 q_2}{r^2} \right| \)

This magnitude helps in calculating energy, pressure, and motion in electric fields.

Superposition Principle

In the presence of more than two charges, the net electric force on any single charge is found by adding the individual forces vectorially. This is called the superposition principle:

\( \vec{F}_{net} = \vec{F}_1 + \vec{F}_2 + \vec{F}_3 + \cdots \)

Units and Dimensions

  • SI Unit: Newton (N)
  • Dimensional Formula: \( [F] = MLT^{-2} \)

Key Conditions for Validity

  • The law applies strictly to point charges or spherically symmetric charge distributions.
  • Distance between charges must be much larger than the size of the charges.
  • Charges must be stationary (electrostatic conditions).

Conclusion

Coulomb’s law is foundational to understanding electric interactions. It describes how charged particles exert forces on each other and provides tools to compute those forces both in vacuum and within materials. Its vector and scalar forms, and the superposition principle, allow for solving complex problems involving multiple charges in various configurations.

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