Suppose the radius at A is R and it decreases uniformaly to r at B where S = πR2 and s = πr2 . Assume also that the semi-vertical angle at 0 is α. Then
where y is the radius at the point P distant x from the vertex O. Suppose the velocity with which the liquid flows out is V at A, v at B and u at P. Then by the equation of continuity
where Pp is the pressure at P and Po is the atmospheric pressure which is the pressure just outside of B. The force on the nozzle tending to pull it out is then
We have subtracted Po which is the force due to atmosphenic pressure the factor sinθ gives horizontal component of the force and ds is the length of the element of nozzle surface, ds = dx sec θ and
If we try to calculate F from the momentum change of the liquid flowing out will be wrong even as regards the sign of the force.
There is of course the effect of pressure at S and s but quantitative derivation of F from Newton's law is difficult.