Let `omega` be the angular speed of the rotation of the bowl. Two forces are (a) normal reaction, `N` and (b) weight, `mg`.
The ball is rotating in a circle of radius `r( = R sin theta )` with center at `A` at an angular speed `omega` Than
`N sin theta = mr omega^(2)`
` = mR omega^(2)`
` N = mR omega^(2)`…(i)
`and N cos theta = mg `….(ii)
Dividing Eqs (i) by(ii), we get
` (1)/(cos theta) = (omega ^(2)R)/(g)`
`omega = sqrt((g)/(R cos theta))`