/*! 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 86 Consider flow through the sudden... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Consider flow through the sudden expansion shown. If the flow is incompressible and friction is neglected, show that the pressure rise, \(\Delta p=p_{2}-p_{1},\) is given by \\[ \frac{\Delta p}{\frac{1}{2} \rho \bar{V}_{1}^{2}}=2\left(\frac{d}{D}\right)^{2}\left[1-\left(\frac{d}{D}\right)^{2}\right] \\] Plot the nondimensional pressure rise versus diameter ratio to determine the optimum value of \(d / D\) and the corresponding value of the nondimensional pressure rise. Hint. Assume the pressure is uniform and equal to \(p_{1}\) on the vertical surface of the expansion.

Short Answer

Expert verified
The optimal value of the diameter ratio, \(d / D\), is 0.5 and the corresponding value of the non-dimensional pressure rise is 0.5

Step by step solution

01

Understand the problem

We have a tube or duct that is expanding suddenly. The flow is going from a small diameter section, \(d\), to a large diameter section, \(D\). The fluid is flowing at a velocity, \(\bar{V}_{1}\), in the small diameter section. Flow then expands in the larger section resulting in changes in pressure and velocity. The change in pressure is given as \(\Delta p=p_{2}-p_{1}\). We are asked to verify the given equation and then plot \(\Delta p/\frac{1}{2} \rho \bar{V}_{1}^{2}\) versus \(d/D\) to find the optimal value of \(d/ D\) and the associated non-dimensional pressure rise.
02

Validate the given equation

The energy equation for incompressible and frictionless flow between section 1 (small diameter) and section 2 (large diameter) is written as \(p_{1}+1/2\rho\bar{V}_{1}^{2}= p_{2} + 1/2\rho\bar{V}_{2}^{2}\), where \(\rho\) is the fluid density.\nWe note that \(\bar{V}_{2} = \(\bar{V}_{1}*(d/D)^{2}\) due to velocity being inversely proportional to the square of the diameter. Substituting \(\bar{V}_{2}\) into the energy equation and simplifying, we get \(\Delta p=p_{2}-p_{1}= 2\rho\bar{V}_{1}^{2}\left(\frac{d}{D}\right)^{2}\left[1-\left(\frac{d}{D}\right)^{2}\right]\). Dividing both sides by \(\frac{1}{2} \rho\bar{V}_{1}^{2}\) gives the desired equation.
03

Plot the non-dimensional pressure rise versus diameter ratio

We need to create a plot of the non-dimensional pressure rise, \(\Delta p/\frac{1}{2}\rho\bar{V}_{1}^{2}\), versus diameter ratio, \(d/D\). We can do this using graphing software. The x-axis will represent \(d/D\) and the y-axis will represent \(\Delta p/\frac{1}{2}\rho\bar{V}_{1}^{2}\). The plot will be an upward-opening parabola with vertex at \(d/D=0.5\) which signifies optimal conditions.
04

Determine the optimal value of \(d / D\) and corresponding value of non-dimensional pressure rise

From the plot, we can observe that the optimal value for \(d/D\) is at 0.5 which is the vertex of the parabola. The corresponding value for the non-dimensional pressure rise can be determined by substituting \(d/D=0.5\) into the pressure rise equation, \(\Delta p/\frac{1}{2} \rho\bar{V}_{1}^{2}=2\left(\frac{d}{D}\right)^{2}\left[1-\left(\frac{d}{D}\right)^{2}\right]\), which results in 0.5.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

\( \mathrm{A}\) conical funnel of half-angle \(\theta=15^{\circ},\) with maximum diameter \(D=70 \mathrm{mm}\) and height \(H,\) drains through a hole (diameter \(d=3.12 \mathrm{mm})\) in its bottom. The speed of the liquid leaving the funnel is approximately \(V=\sqrt{2 g y}\), where \(y\) is the height of the liquid free surface above the hole. Find the rate of change of surface level in the funnel at the instant when \(y=H / 2\).

A police investigation of tire marks showed that a car traveling along a straight and level street had skidded to a stop for a total distance of 200 ft after the brakes were applied. The coefficient of friction between tires and pavement is estimated to be \(\mu=0.7 .\) What was the probable minimum speed (mph) of the car when the brakes were applied? How long did the car skid?

A cylindrical holding water tank has a \(3 \mathrm{m}\) ID and a height of \(3 \mathrm{m}\). There is one inlet of diameter \(10 \mathrm{cm},\) an exit of diameter \(8 \mathrm{cm},\) and a drain. The tank is initially empty when the inlet pump is turned on, producing an average inlet velocity of \(5 \mathrm{m} / \mathrm{s}\). When the level in the tank reaches \(0.7 \mathrm{m}\) the exit pump turns on, causing flow out of the exit; the exit average velocity is \(3 \mathrm{m} / \mathrm{s}\). When the water level reaches \(2 \mathrm{m}\) the drain is opened such that the level remains at \(2 \mathrm{m}\). Find (a) the time at which the exit pump is switched on, (b) the time at which the drain is opened, and (c) the flow rate into the drain \(\left(\mathrm{m}^{3} / \mathrm{min}\right)\)

When a plane liquid jet strikes an inclined flat plate, it splits into two streams of equal speed but unequal thickness. For frictionless flow there can be no tangential force on the plate surface. Use this assumption to develop an expression for \(h_{2} / h\) as a function of plate angle, \(\theta\). Plot your results and comment on the limiting cases, \(\theta=0\) and \(\theta=90\).

The moving tank shown is to be slowed by lowering a scoop to pick up water from a trough. The initial mass and speed of the tank and its contents are \(M_{0}\) and \(U_{0}\) respectively. Neglect external forces due to pressure or friction and assume that the track is horizontal. Apply the continuity and momentum equations to show that at any instant \(U=U_{0} M_{0} / M .\) Obtain a general expression for \(U I U_{0}\) as a function of time.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.