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 Incoming links: Holding force on a contracting nozzle

Use the ideal steady incompressible-flow model, neglecting height change across the smooth nozzle. Flow conservation gives inlet and outlet speeds

u_{0} = Q / A_{0}

and

u_{1} = Q / A_{1}

p_{0} = \frac{ρ}{2} (u_{1}^{2} - u_{0}^{2}) = \frac{ρ Q ^{2}}{2} (\frac{1}{A _{1}^{2}} - \frac{1}{A _{0}^{2}}) .

Choose a control volume containing the fluid in the nozzle, with the positive axis pointing toward the outlet. The integral momentum equation gives

p_{0} A_{0} + F_{wall on fluid} = ρQ (u_{1} - u_{0}) .

Thus the fluid's force on the nozzle is

p_{0} A_{0} - ρQ (u_{1} - u_{0})

, in the outlet direction. Substitute the pressure and velocities:

F_{fluid on nozzle} = ρ Q^{2} [\frac{A _{0}}{2 A _{1}^{2}} - \frac{1}{A _{1}} + \frac{1}{2 A _{0}}] = \frac{ρ Q ^{2}}{2 A _{0}} (\frac{A _{0}}{A _{1}} - 1)^{2} .

The fireman's holding force is equal and opposite. Therefore the required force points upstream and has magnitude

F = \frac{ρ Q ^{2}}{2 A _{0}} (\frac{A _{0}}{A _{1}} - 1)^{2} .

This is the holding force on a contracting nozzle; retaining the inlet pressure force is essential to its sign and value.