/*! 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 74 Water flows steadily through a f... [FREE SOLUTION] | 91影视

91影视

Water flows steadily through a fire hose and nozzle. The hose is \(75 \mathrm{mm}\) inside diameter, and the nozzle tip is \(25 \mathrm{mm}\) ID; water gage pressure in the hose is \(510 \mathrm{kPa}\), and the stream leaving the nozzle is uniform. The exit speed and pressure are \(32 \mathrm{m} / \mathrm{s}\) and atmospheric, respectively. Find the force transmitted by the coupling between the nozzle and hose. Indicate whether the coupling is in tension or compression.

Short Answer

Expert verified
Use the short answer field to input the calculated force and the nature of the force i.e., tension or compression.

Step by step solution

01

Determine the mass flow rate

The mass flow rate can be calculated using the formula for flow speed, cross-sectional area of the pipe, and water density. Because the flow is steady, the mass flow rate is the same at every cross-section of the hose and nozzle. The formula for flow rate is \( \dot{m} = 蟻 * A * v \), where 蟻 is the density of the water (1000 kg/m鲁), A is the cross-sectional area of the hose which is \( 蟺*(d^2)/4 \) and v is the velocity of water. Here, the diameter d of the hose is 75mm or 0.075m, and the velocity v is not given for this section of the hose but will be the same as at the exit (32 m/s). By substituting these values, compute for mass flow rate.
02

Compute for exit pressure

The exit pressure is provided as being atmospheric, which is equal to zero gauge pressure.
03

Apply momentum equation

The linear momentum equation is given by \( 危F = \dot{m}*(V_{out} - V_{in}) \), which is the sum of all forces equal to the change in momentum. Since fluid enters the control volume with negligible velocity as compared to the exit velocity, the equation simplifies to \( 危F = \dot{m}*V_{out} \). Here, 危F is the vector sum of external forces acting on the control volume, \(\dot{m}\) is the mass flow rate, \(V_{out}\) is the exit speed, and \(V_{in}\) is the inlet speed. By plugging in the known values, compute for 危F.
04

Determine the nature of the force

If the force computed is positive, the coupling is in tension. If the force is negative, it signifies that the force is acting in the opposite direction, thereby implying that the coupling is in compression.

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

A block of copper of mass 5 kg is heated to \(90^{\circ} \mathrm{C}\) and then plunged into an insulated container containing 4 L of water at \(10^{\circ} \mathrm{C}\). Find the final temperature of the system. For copper, the specific heat is \(385 \mathrm{J} / \mathrm{kg} \cdot \mathrm{K},\) and for water the specific heat is \(4186 \mathrm{J} / \mathrm{kg} \cdot \mathrm{K}\).

A pipe branches symmetrically into two legs of length \(L,\) and the whole system rotates with angular speed \(\omega\) around its axis of symmetry. Each branch is inclined at angle \(\alpha\) to the axis of rotation. Liquid enters the pipe steadily, with zero angular momentum, at volume flow rate \(Q\). The pipe diameter, \(D,\) is much smaller than \(L\) Obtain an expression for the external torque required to turn the pipe. What additional torque would be required to impart angular acceleration \(\dot{\omega} ?\)

\( \mathrm{A}\) small round object is tested in a 0.75 -m diameter wind tunnel. The pressure is uniform across sections (D and (2). The upstream pressure is \(30 \mathrm{mm} \mathrm{H}_{2} \mathrm{O}\) (gage), the downstream pressure is \(15 \mathrm{mm} \mathrm{H}_{2} \mathrm{O}\) (gage), and the mean air speed is \(12.5 \mathrm{m} / \mathrm{s}\). The velocity profile at section (2) is linear; it varies from zero at the tunnel centerline to a maximum at the tunnel wall. Calculate (a) the mass flow rate in the wind tunnel, (b) the maximum velocity at section \((2),\) and \((\mathrm{c})\) the drag of the object and its supporting vane. Neglect viscous resistance at the tunnel wall.

\( \mathrm{A}\) pump draws water from a reservoir through a 150-mm-diameter suction pipe and delivers it to a \(75-\mathrm{mm}\) diameter discharge pipe. The end of the suction pipe is \(2 \mathrm{m}\) below the free surface of the reservoir. The pressure gage on the discharge pipe \((2 \mathrm{m}\) above the reservoir surface) reads 170 kPa. The average speed in the discharge pipe is \(3 \mathrm{m} / \mathrm{s}\). If the pump efficiency is 75 percent, determine the power required to drive it.

Airat standard conditions enters a compressor at \(75 \mathrm{m} / \mathrm{s}\) and leaves at an absolute pressure and temperature of \(200 \mathrm{kPa}\) and \(345 \mathrm{K}\), respectively, and speed \(V=125 \mathrm{m} / \mathrm{s}\). The flow rate is \(1 \mathrm{kg} / \mathrm{s}\). The cooling water circulating around the compressor casing removes 18 kJ/kg of air. Determine the power required by the compressor.

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.