The energy of the (n−1)th excited state is given by
E=−13.6n2Z2
Therefore, the released radiations have energy
ΔE1=−13.6Z2(152−142)=2.75 eV
ΔE2=−13.6Z2(142−132)=5.95 eV
Recalling photoelectric effect,
eVo=hf−ϕ
where Vo is the stopping potential and ϕ is the workfunction.
It is given that Vo2=3.95 V
eVo2=ΔE2−ϕ
⟹ϕ=5.95−3.95=2 eV
∴eVo1=ΔE1−ϕ
⟹ eVo1=2.75−2=0.75 eV⟹Vo1=0.75 V