To solve this problem, we need to understand the concept of electric fields around spherical conductors when they are in equilibrium and connected by a conducting wire.
When two conductors are connected by a conducting wire, they come to the same potential in equilibrium. The potential \( V \) on the surface of a spherical conductor is given by the formula:
V = \frac{kQ}{r}
where \( k \) is Coulomb's constant, \( Q \) is the charge on the sphere, and \( r \) is the radius of the sphere.
For equilibrium conditions, we have:
V_A = V_B
Substituting the formula for potential, we get:
\frac{kQ_A}{r_A} = \frac{kQ_B}{r_B}
Since the spheres are in equilibrium, their potentials are equal and the constant \( k \) cancels out. This results in:
\frac{Q_A}{r_A} = \frac{Q_B}{r_B}
The electric field \( E \) at the surface of any spherical conductor is given by:
E = \frac{Q}{4\pi \varepsilon_0 r^2}
At equilibrium, when calculating the ratio of the electric fields at the surface of spheres A and B, we have:
\frac{E_A}{E_B} = \frac{\frac{Q_A}{4\pi \varepsilon_0 r_A^2}}{\frac{Q_B}{4\pi \varepsilon_0 r_B^2}} = \frac{Q_A \cdot r_B^2}{Q_B \cdot r_A^2}
Substitute the relation from potential equality:
\frac{E_A}{E_B} = \frac{r_B \cdot r_B^2}{r_A \cdot r_A^2} = \frac{r_B}{r_A}
Given r_A = 5\, \text{mm} and r_B = 10\, \text{mm}, we substitute these values:
\frac{E_A}{E_B} = \frac{10}{5} = 2
Thus, the ratio of the magnitude of the electric fields at the surfaces of spheres A and B is 2:1.
A metallic ring is uniformly charged as shown in the figure. AC and BD are two mutually perpendicular diameters. Electric field due to arc AB to O is ‘E’ magnitude. What would be the magnitude of electric field at ‘O’ due to arc ABC? 