The correct option is B √5g/3
Suppose the particle of mass m slides down a smooth sphere of radius R, starting from rest at the top. Suppose the particle leaves the sphere at angle θ with vertical.
The particle slides off when the normal force is zero.
Using Newton's second law,
mv2r=mg(cosθ)
from WE theorem
mv22=mgr(1−cosθ)
from simplification,
mgcosθ=2mg(1−cosθ)
3cosθ=2
cosθ=23
Now tangential acceleration is gsinθ=g√1−(23)2=√5g3