The large tank of incompressible liquid in Fig. P3.143 is at rest when, at t = 0, the valve is opened to the atmos- phere. Assuming h constant (negligible velocities and accelerations in the tank), use the unsteady frictionless Bernoulli equation to derive and solve a differential equa- tion for V(t) in the pipe. h = constant Valve V (1) -L-

Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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The large tank of incompressible liquid in Fig. P3.143 is
at rest when, at t = 0, the valve is opened to the atmos-
phere. Assuming h= constant (negligible velocities and
accelerations in the tank), use the unsteady frictionless
Bernoulli equation to derive and solve a differential equa-
tion for V(t) in the pipe.
h= constant
D
Valve
V (1)
Transcribed Image Text:The large tank of incompressible liquid in Fig. P3.143 is at rest when, at t = 0, the valve is opened to the atmos- phere. Assuming h= constant (negligible velocities and accelerations in the tank), use the unsteady frictionless Bernoulli equation to derive and solve a differential equa- tion for V(t) in the pipe. h= constant D Valve V (1)
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