Potentials at the centre
`V_(1)=(1)/(4piepsilon_(0))(q)/(r), V_(2)=(1)/(4piepsilon_(0))(q)/(r)`
Potential energy in situation `I` is
`U_(1)=3xx(1)/(4piepsilon_(0))((9//3))^(2)/((sqrt(3)R))` `=(1)/(12sqrt(3)piepsilon_(0))(q^(2))/(R)`
When one charge is removed, the field intensity at the centre is due to the removed charge only.
`E_(1)=(1)/(4piepsilon_(0))(q//3)/(r^(2))`
`E_(2)=(1)/(4piepsilon_(0))(q//4)/(r^(2)) therefore(E_(1))/(E_(2))=(4)/(3)`
