Class 11 > Unit # 08: Electric Fields > Coulomb's Law


Coulomb's Law and Electrostatic Force - Talha's Physics Academy

Talha's Physics Academy

Coulomb's Law and Electrostatic Force

Video Lecture

Watch the complete video lecture below to understand Coulomb's law, electrostatic force between point charges, and the effect of dielectric media on electric force.

Coulomb's Law

Statement

"According to this law, the electric force between two point charges is directly proportional to the product of the magnitude of charges and inversely proportional to the square of the distance between them."

Consider two point charges $q_1$ and $q_2$ separated by a distance $r$ from each other. By this law, the magnitude of the force $F$ exerted by either of the charges on the other is given by:

$$F \propto \frac{q_1 q_2}{r^2}$$

$$F = k \frac{q_1 q_2}{r^2} \quad \text{--- (i)}$$

Where $k$ is a constant of proportionality, and its value depends on the medium between the charges. For free space (vacuum), the value of $k$ is:

$$k = \frac{1}{4\pi \varepsilon_0}$$

$$k = 9 \times 10^9 \, \text{N}\cdot\text{m}^2/\text{C}^2$$

Substituting the value of $k$ in equation (i) for free space:

$$F = \frac{1}{4\pi \varepsilon_0} \frac{q_1 q_2}{r^2}$$

Where $\varepsilon_0$ = permittivity of free space.

Effect of Medium

If instead of free space there is some insulating material or dielectric medium between the charges, then the proportionality constant becomes:

$$k = \frac{1}{4\pi \varepsilon}$$

Where $\varepsilon$ is the absolute permittivity of the medium, which can be expressed as:

$$\varepsilon = \varepsilon_0 \varepsilon_r$$

Here, $\varepsilon_r$ represents the relative permittivity (or dielectric constant) of the medium.

Thus, equation (i) for a material medium becomes:

$$F = \frac{1}{4\pi \varepsilon} \frac{q_1 q_2}{r^2}$$

$$F = \frac{1}{4\pi \varepsilon_0 \varepsilon_r} \frac{q_1 q_2}{r^2}$$

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

Nature of Force: The electrostatic force will be attractive if the charges are dissimilar (unlike charges) and repulsive if the charges are similar (like charges).

Fig: Electrostatic forces between two point charges $q_1$ and $q_2$ separated by distance $r$.

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