Difficulty: Medium
Correct Answer: a/A = 1 / √(8 f L / D)
Explanation:
Introduction / Context:When a nozzle is attached to a long pipeline, increasing the nozzle diameter raises discharge but also increases pipe velocity and friction loss, reducing available head at the nozzle. There is a specific area ratio that maximizes the transmitted power P = ρ Q V_jet^2 / 2.
Given Data / Assumptions:
Concept / Approach:Balancing available head with friction loss in the pipe yields a relation between pipe velocity and nozzle area. Maximizing jet power with respect to nozzle area leads to a classical optimum: (8 f L / D) * (a/A)^2 = 1, hence a/A = 1 / √(8 f L / D).
Step-by-Step Solution:
Let A = pipe area, a = nozzle area; continuity gives Q = A V_p = a V_j.Head loss in pipe: h_f = f (L/D) * V_p^2 / (2 g).Available head at nozzle converts to jet velocity: V_j = √(2 g (H − h_f)).Express power P = ρ Q V_j^2 / 2 and optimize with respect to a/A to obtain (8 f L / D) (a/A)^2 = 1.Verification / Alternative check:This optimum is equivalent to the condition that the pipe friction head equals one-third of the supply head at maximum power for the end-nozzle configuration.
Why Other Options Are Wrong:Other forms invert or misplace parameters, leading to non-optimal or dimensionally inconsistent relationships. The presence of the 8 f L / D group is critical and must be in the denominator under the square root.
Common Pitfalls:Confusing Darcy and Fanning friction factors (factor of 4 difference); ignoring minor losses when they are significant, which would shift the exact optimum.
Final Answer:a/A = 1 / √(8 f L / D)
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