So far as we have considered coulomb's law, we assumed charged particles, discrete entity with some amount of charge. Now we are going to consider more realistic case, continuous distribution of charges.
Distribution of charges means, some amount of charge spread over a region of space. If the region of space is
Distribution of charges means, some amount of charge spread over a region of space. If the region of space is
- 0 dimensional, then it is a point charge (charged particle).
- 1 dimensional, then it is linear distribution.
- 2 dimensional, surface distribution.
- 3 dimensional, volume distribution.
the form of field equation would be,
$$E = \dfrac{1}{4\pi{\epsilon_0}} \int_p \dfrac{\lambda (s)}{{r_{st}}^2} dl$$
2 dimensional case: This is the case of surface distribution of charge. If the charge is distributed over a surface with surface charge density, $$\sigma (s)$$
the form of field equation would be,
$$E = \dfrac{1}{4\pi{\epsilon_0}} \int_a \dfrac{\sigma (s)}{{r_{st}}^2} da$$
3 dimensional case: This is the case of volume distribution of charge. If the charge is distributed over a volume with surface charge density, $$\rho (s)$$
the form of field equation would be,
$$E = \dfrac{1}{4\pi{\epsilon_0}} \int_v \dfrac{\rho (s)}{{r_{st}}^2} dv$$