There are two nonconducting spheres having uniform volume charge densities `rho` and `- rho` . Both spheres have equal radius `R`. The spheres are now laid down such that they overlap as shown in Fig.2.125. Take `vec(d) = O_(1) vec(O_(2))`.
The potential difference `Delta V` between the centres of the two spheres for `d = R` is
A. `(rho)/( 3 epsilon _(0)) d^(2)`
B. `(rho)/( epsilon_(0)) vec(d^(2))`
C. zero
D. `( 2rho)/( epsilon_(0)) d^(2)`