/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 121 A stream of incompressible liqui... [FREE SOLUTION] | 91Ó°ÊÓ

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A stream of incompressible liquid moving at low speed leaves a nozzle pointed directly downward. Assume the speed at any cross section is uniform and neglect viscous effects. The speed and area of the jet at the nozzle exit are \(V_{0}\) and \(A_{0},\) respectively. Apply conservation of mass and the momentum equation to a differential control volume of length \(d z\) in the flow direction. Derive expressions for the variations of jet speed and area as functions of z. Evaluate the distance at which the jet area is half its original value. (Take the origin of coordinates at the nozzle exit.)

Short Answer

Expert verified
The distance at which the jet area is half its original value is \(\frac{3V_0^2}{8g}\)

Step by step solution

01

Applying the principle of conservation of mass

On a small control volume of length \(dz\), the principle of conservation of mass says that the mass flow rate in the stream must remain constant. So, it follows then that \(A_0 V_0 = A V\) where \(A\) and \(V\) are the area and speed at a distance \(z\) from the nozzle exit.
02

Derive expression for speed as a function of z

To derive an expression for speed as a function of z, first express \(A\) as a function of z from the mass conservation derived in Step 1: \(A = V_0 A_0/ V\). Now apply the momentum equation \(p + 1/2 \rho V^2 + \rho g z = constant\), where \(p\) is pressure, \(\rho\) is the fluid density, \(V\) is flow velocity and \(g\) is the acceleration due to gravity. Given the nozzle exit is the reference point and the pressure there is atmospheric pressure, you can define the constant value as \(p_0 + 1/2 \rho V_0^2\), where \(p_0\) is atmospheric pressure. Rewrite this momentum equation, solve it for velocity \(V\) and simplify to get \(V = \sqrt{V_0^2 + 2g z}\).
03

Derive expression for area as a function of z

Substitute the expression for \(V\) derived in Step 2 into the equation \(A = A_0 V_0/ V\) to get the area as a function of z, which is \( A = \frac{A_0 V_0}{\sqrt{V_0^2 + 2g z}}\).
04

Find z when area is halved

To find the value of \(z\) when the area is halved we will set \(A = A_0/2\) and solve for \(z\). Substituting \(A_0/2\) into \(A = \frac{A_0 V_0}{\sqrt{V_0^2 + 2g z}}\) and solving for \(z\) gives \(z = \frac{3V_0^2}{8g}\).

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