/*! 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 11 An incompressible liquid with a ... [FREE SOLUTION] | 91影视

91影视

An incompressible liquid with a density of \(1250 \mathrm{kg} / \mathrm{m}^{3}\) and negligible viscosity flows steadily through a horizontal pipe of constant diameter. In a porous section of length \(L=\) \(5 \mathrm{m},\) liquid is removed at a constant rate per unit length so that the uniform axial velocity in the pipe is \(u(x)=U(1-x / L)\) where \(U=15 \mathrm{m} / \mathrm{s}\). Develop expressions for and plot the pressure gradient along the centerline. Evaluate the outlet pressure if the pressure at the inlet to the porous section is \(100 \mathrm{kPa}(\text { gage })\)

Short Answer

Expert verified
The pressure gradient along the centerline is described by the equation \(p = -\rho U^2 \frac{x^2}{2L} + 100kPa\), and the pressure at the outlet is \(56.875 kPa\)

Step by step solution

01

Identify Fluid Dynamics Concepts

This problem involves the concept of fluid dynamics in a system in which an incompressible fluid is flowing through a porous pipe. It's crucial to remember that fluid continuity, which is given by the equation \(A_1v_1 = A_2v_2\), must be preserved if the system is to remain steady. The Bernoulli equation, \(p1 + .5蟻v1^2 + 蟻gA_1 = p2 + .5蟻v2^2 + 蟻gA_2\), is also valuable 鈥 a fundamental principle stating that the total mechanical energy of the flowing fluid, system density, and gravitational acceleration remains constant.
02

Derive the Equation for the Pressure Gradient

We can begin by calculating the pressure gradient from the Bernoulli principle with respect to \(x\), which leads to: \[-\frac{dp}{dx} = \rho\frac{du}{dx}U(1-\frac{x}{L})\]Solving for the pressure yields:\[p = -\rho U^2 \frac{x^2}{2L} + C\]where \(C\) is the integration constant. Given that at \(x=0\), \(p=p_i=100kPa=100000Pa\) we can find the value of \(C\). Hence \(C=100000Pa\). Thus our equation for pressure becomes \(p = -\rho U^2 \frac{x^2}{2L} + 100000Pa\).
03

Evaluate the Outlet Pressure

Lastly, the outlet pressure is evaluated when \(x = L = 5m\). Substituting these values into the pressure equation:\[p = -1250 kg/m^3 * (15 m/s)^2 * 5^2/(2*2*5 m) + 100000Pa = 56875 Pa = 56.875 kPa\]
04

Visualize the Pressure Gradient

A graph with x-values ranging from \(0-5m\) could be plotted using the pressure equation. It gives an idea of how the pressure changes across the length of the porous part of the pipe. It should be a downward parabola beginning at \(100kPa\) and terminating at around \(56.875kPa\) at \(x = 5m\).

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 91影视!

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

Water flows steadily up the vertical 1-in.-diameter pipe and out the nozzle, which is 0.5 in. in diameter, discharging to atmospheric pressure. The stream velocity at the nozzle exit must be \(30 \mathrm{ft} / \mathrm{s}\). Calculate the minimum gage pressure required at section (1). If the device were inverted, what would be the required minimum pressure at section (1) to maintain the nozzle exit velocity at \(30 \mathrm{ft} / \mathrm{s} ?\)

In a laboratory experiment, water flows radially outward at moderate speed through the space between circular plane parallel disks. The perimeter of the disks is open to the atmosphere. The disks have diameter \(D=150 \mathrm{mm}\) and the spacing between the disks is \(h=0.8 \mathrm{mm} .\) The measured mass flow rate of water is \(\dot{m}=305 \mathrm{g} / \mathrm{s}\). Assuming frictionless flow in the space between the disks, estimate the theoretical static pressure between the disks at radius \(r=50 \mathrm{mm} .\) In the laboratory situation, where some friction is present, would the pressure measured at the same location be above or below the theoretical value? Why?

\(\mathrm{A}\) crude model of a tornado is formed by combining a \(\operatorname{sink},\) of strength \(q=2800 \mathrm{m}^{2} / \mathrm{s},\) and a free vortex, of strength \(K=5600 \mathrm{m}^{2} / \mathrm{s} .\) Obtain the stream function and velocity potential for this flow field. Estimate the radius beyond which the flow may be treated as incompressible. Find the gage pressure at that radius.

Heavy weights can be moved with relative ease on air cushions by using a load pallet as shown. Air is supplied from the plenum through porous surface \(A B .\) It enters the gap vertically at uniform speed, \(q\). Once in the gap, all air flows in the positive \(x\) direction (there is no flow across the plane at \(x=0\) ). Assume air flow in the gap is incompressible and uniform at each cross section, with speed \(u(x),\) as shown in the enlarged view. Although the gap is narrow \((h \ll L)\) neglect frictional effects as a first approximation. Use a suitably chosen control volume to show that \(u(x)=q x / h\) in the gap. Calculate the acceleration of a fluid particle in the gap. Evaluate the pressure gradient, \(\partial p / \partial x,\) and sketch the pressure distribution within the gap. Be sure to indicate the pressure at \(x=L\)

Consider the flow field represented by the potential function $\phi=A x^{2}+B x y-A y^{2} .$ Verify that this is an incompressible flow and determine the corresponding stream function.

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.