Surface potential of a spherical conductor of radius R, carrying charge Q, \(V_{S}=\frac{Q}{4\pi \varepsilon _{0}R}\)
Let Q1 and Q2 are the charges of two spherical conductors having radii R1 and R2 respectively.
When these two charged spherical conductors are connected with the wire, the potential at their surfaces become equal
Therefore, Vs1 = Vs2
\(V_{S}=\frac{Q_{1}}{4\pi \varepsilon _{0}R_{1}}\) = \(V_{S}=\frac{Q_{1}}{4\pi \varepsilon _{0}R_{1}}\)⇒ \(\frac{Q_{1}}{Q_{2}}\)=\(\frac{R_{1}}{R_{2}}\)……(i)
Surface charge density, σ = \(\frac{Charge}{Area}\)
\(\frac{\sigma _{1}}{\sigma _{2}}\) =\(\frac{(\frac{Q_{1}}{4\pi \varepsilon _{0}R_{1}^{2}})}{(\frac{Q_{1}}{4\pi \varepsilon _{0}R_{2}^{2}})}\)= \(\frac{Q_{1}}{Q_{2}}\) × \(\frac{R_{2}^{2}}{R_{1}^{2}}\)
= \(\frac{R_{1}}{R_{2}}\) ×\(\frac{R_{2}^{2}}{R_{1}^{2}}\) = \(\frac{R_{2}}{R_{1}}\)[Using(i)]
Two point charges +q and −q are held at (a, 0) and (−a, 0) in x-y plane. Obtain an expression for the net electric field due to the charges at a point (0, y). Hence, find electric field at a far off point (y ≫ a).
It is the property of subatomic particles that experiences a force when put in an electric and magnetic field.
It is a property associated with each point in space when charge is present in any form. The magnitude and direction of the electric field are expressed by E, called electric field strength or electric field intensity.
Electric charges are of two types: Positive and Negative. It is commonly carried by charge carriers protons and electrons.
Various properties of charge include the following :-
Two kinds of electric charges are there :-
When there is an identical number of positive and negative charges, the negative and positive charges would cancel out each other and the object would become neutral.