Water of density \(998.2 \mathrm{~kg} / \mathrm{m}^{3}\) is moving at negligible speed under a pressure of \(101.3 \mathrm{kPa}\) but is then accelerated to high speed by the blades of a spinning propeller. The vapor pressure of the water at the initial temperature of \(20.0^{\circ} \mathrm{C}\) is \(2.3388 \mathrm{kPa}\). At what flow speed will the water begin to boil? This effect, known as cavitation, limits the performance of propellers in water

Short Answer

Expert verified
Answer: The water will begin to boil when its flow speed reaches approximately 3.05 m/s due to cavitation.

Step by step solution

01

Recall Bernoulli's equation

The Bernoulli's equation for an incompressible fluid can be written as: $$ P_1 + \frac{1}{2}\rho v_1^2 + \rho g h_1 = P_2 + \frac{1}{2} \rho v_2^2 + \rho g h_2 $$ where \(P_1\) and \(P_2\) are pressures of fluid at points 1 and 2, \(\rho\) is the fluid density, \(v_1\) and \(v_2\) are the fluid speeds at points 1 and 2, \(h_1\) and \(h_2\) are the height of the fluid at points 1 and 2, respectively. Since the problem states that the initial flow speed is negligible, we can assume \(v_1 = 0\). And since its the same fluid and the heights are not given, the term \(\rho g h\) can be dropped (as it would be equal for both the points). The equation will then reduce to: $$ P_1 = P_2 + \frac{1}{2} \rho v_2^2 $$
02

Calculate the boiling pressure

To find the flow speed at which water begins to boil, we will first calculate the boiling pressure by adding the vapor pressure to the initial pressure (remember that the boiling pressure is the pressure at which the liquid transitions into a vapor). The vapor pressure is given to be \(2.3388 \mathrm{kPa}\), and the initial pressure is \(101.3 \mathrm{kPa}\). Therefore, $$ P_{boil} = P_1 - P_{vapor} = 101.3 - 2.3388 = 98.9612\, \mathrm{kPa} $$
03

Use Bernoulli's equation to find the flow speed

Now that we have the boiling pressure, we can use Bernoulli's equation to calculate the flow speed at the point where cavitation begins. Substitute the boiling pressure for \(P_2\) in the equation from step 1: $$ P_1 = P_{boil} + \frac{1}{2} \rho v_2^2 $$ We are given the initial pressure \(P_1 = 101.3 \mathrm{kPa}\), the density of water \(\rho = 998.2 \mathrm{~kg} / \mathrm{m}^{3}\), so we can solve for the flow speed \(v_2\). Rearrange the equation to solve for \(v_2\): $$ v_2 = \sqrt{\frac{2(P_1 - P_{boil})}{\rho}} $$ Plug in the known values: $$ v_2 = \sqrt{\frac{2(101.3 - 98.9612) \times 10^3}{998.2}} = \sqrt{\frac{4676}{998.2}} $$ Calculate the flow speed: $$ v_2 \approx 3.05 \mathrm{m/s} $$ The water will begin to boil when its flow speed reaches \(3.05 \mathrm{m/s}\) due to cavitation.

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 Vaia!

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

Calculate the ratio of the lifting powers of helium (He) gas and hydrogen (H \(_{2}\) ) gas under identical circumstances. Assume that the molar mass of air is \(29.5 \mathrm{~g} / \mathrm{mol}\).

An airplane is moving through the air at a velocity \(v=200 . \mathrm{m} / \mathrm{s} .\) Streamlines just over the top of the wing are compressed to \(80.0 \%\) of their original area, and those under the wing are not compressed at all. a) Determine the velocity of the air just over the wing. b) Find the difference in the pressure between the air just over the wing, \(P\), and that under the wing, \(P\). c) Find the net upward force on both wings due to the pressure difference, if the area of the wing is \(40.0 \mathrm{~m}^{2}\) and the density of the air is \(1.30 \mathrm{~kg} / \mathrm{m}^{3}\).

Analytic balances are calibrated to give correct mass values for such items as steel objects of density \(\rho_{s}=\) \(8000.00 \mathrm{~kg} / \mathrm{m}^{3}\). The calibration compensates for the buoyant force arising because the measurements are made in air, of density \(\rho_{\mathrm{a}}=1.205 \mathrm{~kg} / \mathrm{m}^{3}\). What compensation must be made to measure the masses of objects of a different material, of density \(\rho\) ? Does the buoyant force of air matter?

Salt water has a greater density than freshwater. A boat floats in both freshwater and salt water. The buoyant force on the boat in salt water is that in freshwater. a) equal to b) smaller than c) larger than

A block of cherry wood that is \(20.0 \mathrm{~cm}\) long, \(10.0 \mathrm{~cm}\) wide, and \(2.00 \mathrm{~cm}\) thick has a density of \(800 . \mathrm{kg} / \mathrm{m}^{3}\). What is the volume of a piece of iron that, if glued to the bottom of the block makes the block float in water with its top just at the surface of the water? The density of iron is \(7860 \mathrm{~kg} / \mathrm{m}^{3},\) and the density of water is \(1000 . \mathrm{kg} / \mathrm{m}^{3}\).

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.

Sign-up for free