Coulomb's Law
Key Questions
-
\vec{F}_{12} = 1/(4\pi\epsilon_o)(q_1q_2)/|\vec{r}_1-\vec{r}_2|^2=-\vec{F}_21 -
Answer:
I shall outline a better method. Not just by assuming the surface is spherical with area
4pir^2 .So, to start with I shall prove it for the field due to a single point charge. (At O)
Since superposition principle applies to electric fields, this can be generalised to any number of charges quite easily.There it is, given below.
Explanation:
Consider a charged particle
q placed at O and is being surrounded and enclosed by a closed surfaceS . (Of arbitrary size and shape).Take an arbitrary surface element
dS on the surface at a distancer from O.Let the normal on
dS make an angletheta with the electric field ofq passing throughdS .Thus,
vec E*dvecS = EdS Cos theta which is equal to the flux through the small area.Now, by Coulomb's law,
E = q/(4piepsilon_0r^2) Which gives,
dphi = q/(4piepsilon_0)*dScos theta/(r^2) Now,
dS Cos theta/(r^2) is the solid angle which can be denoted as,domega Thus, the flux through
dS is,dphi = q/(4piepsilon_0)*domega Integrating over the entire surface,
int int_S vecE*dvecS = q/(4piepsilon_0) int domega But, the net solid angle subtended by a closed surface at an internal point is always
4pi .int int_S vecE*dvecS = q/(4piepsilon_0)*4pi Thus,
int int_S vecE*dvecS = q/epsilon_0 Which is Gauss law in integral form.
One may derive the differential form from Coulomb's law as well by taking the Divergence of the electric field and then proceeding with vector calculus methods.
The differential form looks something like this,
nabla*vec E = rho/epsilon_0 whererho is the charge density. -
Answer:
F=k(Q_1,Q_2)/r^2 Explanation:
assume there are two charges
Q_1, Q_2 the force between them can be found through this relation
F=k(Q_1*Q_2)/r^2 Where k is Coulomb's constant
andr is the distance between the two chargesand the force is attraction if the two charges have different sign
(+ve and -ve )
and repulsion if the two charges have the same sign