Hey,
This reply might be a bit late but could help others who are looking for information on this kind of problem. I am a chemical engineering student working on a project for which I am designing a laminar nozzle. I needed to find the break up length (arc length to which the jet begins to break up - laminar to turbulent) of the jet of water fired from the nozzle from the angle of the initial jet, the velocity of the jet and the horizontal length of the break up point from the nozzle outlet. I have devised the following equation for finding this arc length from projectile motion physics:
X = jet break up point/point along arc we wish to find the arc length to from origin
BL = horizontal break up length/x axis displacement of point X
θ = jet angle
u = jet velocity
so initially tBL = BL/u gives the time at which the jet breaks up (time to arc point X)
From projectile motion arc length can be shown as:
L = ∫√(ux2 + uy2) dt from t=0 to t=tBL (or any time chosen)
L = ∫√((ucosθ)2 + (usinθ - gt)2) dt
To make things easier:
a = ucosθ
z = usinθ - gt
Giving:
L = 1/g ∫√(a2 + z2) dz
1/g since dt = 1/g*dz
converting the integral boundaries:
when t = 0; z = -usinθ
when t = tBL:
Sx = utcosθ → BL = utBLcosθ (x-axis displacement of point X)
tBL = BL/(ucosθ)
∴ z = gBL/(ucosθ) - usinθ
Simplifying the boundaries:
when t = 0; -usinθ = -gtBL - z = b
when t = tBL; g*BL/(ucosθ) - usinθ = gBL/a - gtBL - z = c
Finally once the arc length equation is integrated:
L = 1/g[0.5*z*√(a2+z2) + 0.5*a2* ln(z + √(a2+z2))]bc
(b & c being the integral boundaries)
Once b & c are substituted into the equation in place of "z", L will be the length of the arc to point X along the parabola.
Hope this helps!