Difficulty: Easy
Correct Answer: v = sqrt(2 * g * H)
Explanation:
Introduction / Context:Torricelli's theorem gives the ideal (lossless) efflux velocity under a head H as if a particle fell freely through that head. It underpins orifice and nozzle calculations before applying discharge and velocity coefficients for real flows.
Given Data / Assumptions:
Concept / Approach:Bernoulli between the free surface and the jet section with atmospheric pressure on both locations reduces to v^2/(2g) = H, so v = sqrt(2 * g * H). Real jets use v = Cv * sqrt(2 * g * H) with Cv < 1.
Step-by-Step Solution:
Apply Bernoulli: (p/ρg + z + v^2/(2g)) constant.Atmospheric pressure cancels; surface velocity ~ 0.Thus v^2/(2g) = H ⇒ v = sqrt(2gH).Verification / Alternative check:Dimensional check: g has m/s^2, H has m; product gives m^2/s^2; square root gives m/s as required.
Why Other Options Are Wrong:
Common Pitfalls:Forgetting to take the square root; confusing head at vena contracta with upstream head; mixing up Cv and Cd.
Final Answer:v = sqrt(2 * g * H)
Discussion & Comments