/*! 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 21 (a) Calculate the absolute press... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

(a) Calculate the absolute pressure at the bottom of a fresh-water lake at a depth of \(27.5 \mathrm{~m}\). Assume the density of the water is \(1.00 \times 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\) and the air above is at a pressure of \(101.3 \mathrm{kPa}\). (b) What force is exerted by the water on the window of an underwater vehicle at this depth if the window is circular and has a diameter of \(35.0 \mathrm{~cm}\) ?

Short Answer

Expert verified
The absolute pressure at the bottom of the lake is \(370.8 \mathrm{kPa}\) and the force exerted by the water at this depth on the window is \(35.6 \mathrm{kN}\).

Step by step solution

01

Deriving absolute pressure at depth

Lets first calculate the absolute pressure at the bottom of the lake. This can be calculated by adding pressure due to the water column and the atmospheric pressure. The pressure due to a fluid column is given by the equation \(P = \rho g h\), where \(P\) is the fluid pressure, \(\rho\) is the fluid density, \(g\) is acceleration due to gravity and \(h\) is the height of the fluid column. Here, \(\rho = 1.00 \times 10^{3} \mathrm{~kg/m^3}\), \(g = 9.8 \mathrm{~m/s^2}\) (approximated value of gravity on Earth), and \(h = 27.5 \mathrm{~m}\). So, \(P_{Fluid} = \rho g h = 1.00 \times 10^{3} \mathrm{~kg/m^3} \times 9.8 \mathrm{~m/s^2} \times 27.5 \mathrm{~m} = 269.5 \mathrm{kPa}\). The atmospheric pressure \(P_{Atmospheric} = 101.3 \mathrm{kPa}\). Hence the absolute pressure \(P_{Absolute}\) at a depth of 27.5 m can be calculated by adding the atmospheric pressure to the fluid pressure. So, \(P_{Absolute} = P_{Fluid} + P_{Atmospheric} = 269.5 \mathrm{kPa} + 101.3 \mathrm{kPa} = 370.8 \mathrm{kPa}\)
02

Calculate the area of the window

Before determining the force exerted by the water on the window, let's first calculate the area of the window. Given the window is in circular shape, we use the area formula for a circle: \(\mathrm{Area} = \pi(\mathrm{Diameter}/2)^2\). Here, the diameter of the window is \(35.0 \mathrm{cm}\), so the radius is \(Diameter / 2 = 35.0 \mathrm{cm} / 2 = 17.5 \mathrm{cm} = 0.175 \mathrm{m}\), (converted from cm to m). So, \(\mathrm{Area} = \pi * (0.175 \mathrm{m})^2 = 0.096 \mathrm{m^2}\).
03

Calculate the force exerted by the water

We can now calculate the force exerted by the water on the window. The force exerted by fluid pressure is given by the equation \(Force = Pressure \times Area\). Here, Pressure is the absolute pressure we calculated in Step 1 and Area is the area of the window we calculated in Step 2. Hence, \(Force = P_{Absolute} \times \mathrm{Area} = 370.8 \mathrm{kPa} \times 0.096 \mathrm{m^2} = 35.6 \mathrm{kN}\). As the pressure is high, Force is given in kilo Newtons (kN).

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!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Pressure Calculation
Understanding how to calculate pressure in fluid mechanics is crucial. Pressure is the force exerted by a fluid per unit area on an object's surface. In our exercise, we looked for the absolute pressure at the bottom of a lake. To find this, we add the pressure from the water column to the atmospheric pressure above the surface.

The pressure due to the water column can be calculated using the formula \(P = \rho gh\). Here, \(\rho\) stands for the density of the fluid, \(g\) is the acceleration due to gravity, and \(h\) is the height of the fluid column.

  • Density of water \(\rho = 1.00 \times 10^3 \ \text{kg/m}^3\)
  • Gravity \(g = 9.8 \ \text{m/s}^2\)
  • Depth \(h = 27.5 \ m\)
This gives us the water pressure as 269.5 kPa. Adding the atmospheric pressure of 101.3 kPa, the absolute pressure at the lake's bottom becomes 370.8 kPa.
Fluid Statics
Fluid statics, also known as hydrostatics, deals with fluids at rest. The fundamental principle here is that any part of a fluid at rest is in a state of equilibrium. This means that any pressure applied to the fluid is transmitted uniformly in all directions within the fluid.

In this case, there is fluid (water) exerting pressure due to its weight at a certain depth. This pressure increases with depth because of the weight of the overlaying fluid.

  • At greater depths, more water exerts force.
  • This is why submarines are built to withstand high pressures.
Fluid statics is essential in designing anything that is intended to be submerged, as it emphasizes how pressures increase with depth.
Force on Submerged Surfaces
When designing structures like the window of an underwater vehicle, calculating the force exerted by the fluid on the submerged surface is crucial. To find this force, you multiply the pressure by the area of the surface.

In our exercise, we calculated:
  • The area of a circular window: Using \(\text{Area} = \pi (\text{radius})^2\), we found the area to be 0.096 \(\mathrm{m^2}\) for a window with a 35 cm diameter.
  • The force: Calculated using \(\text{Force} = \text{Pressure} \times \text{Area}\), resulting in 35.6 kN.
This exemplifies why precise calculations are needed in engineering. It ensures that structures can tolerate the immense pressures exerted by fluids at depth.

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

The aorta in humans has a diameter of about \(2.0 \mathrm{~cm}\), and at certain times the blood speed through it is about \(55 \mathrm{~cm} / \mathrm{s}\). Is the blood flow turbulent? The density of whole blood is \(1050 \mathrm{~kg} / \mathrm{m}^{3}\), and its coefficient of viscosity is \(2.7 \times 10^{-3} \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^{2}\).

The total cross-sectional area of the load-bearing calcified portion of the two forearm bones (radius and ulna) is approximately \(2.4 \mathrm{~cm}^{2}\). During a car crash, the forearm is slammed against the dashboard. The arm comes to rest from an initial speed of \(80 \mathrm{~km} / \mathrm{h}\) in \(5.0 \mathrm{~ms}\). If the arm has an effective mass of \(3.0 \mathrm{~kg}\) and bone material can withstand a maximum compressional stress of \(16 \times 10^{7} \mathrm{~Pa}\), is the arm likely to withstand the crash?

Four acrobats of mass \(75.0 \mathrm{~kg}, 68.0 \mathrm{~kg}, 62.0 \mathrm{~kg}\), and \(55.0 \mathrm{~kg}\) form a human tower, with each acrobat standing on the shoulders of another acrobat. The \(75.0-\mathrm{kg}\) acrobat is at the bottom of the tower. (a) What is the normal force acting on the \(75-\mathrm{kg}\) acrobat? (b) If the area of each of the 75.0-kg acrobat's shoes is \(425 \mathrm{~cm}^{2}\), what average pressure (not including atmospheric pressure) does the column of acrobats exert on the floor? (c) Will the pressure be the same if a different acrobat is on the bottom?

Suppose two worlds, each having mass \(M\) and radius \(R\), coalesce into a single world. Due to gravitational contraction, the combined world has a radius of only \(\frac{3}{4} R\). What is the average density of the combined world as a multiple of \(\rho_{0}\), the average density of the original two worlds?

(a) Calculate the mass flow rate (in grams per second) of blood \(\left(\rho=1.0 \mathrm{~g} / \mathrm{cm}^{3}\right)\) in an aorta with a crosssectional area of \(2.0 \mathrm{~cm}^{2}\) if the flow speed is \(40 \mathrm{~cm} / \mathrm{s}\). (b) Assume that the aorta branches to form a large number of capillaries with a combined cross-sectional area of \(3.0 \times 10^{3} \mathrm{~cm}^{2}\). What is the flow speed in the capillaries?

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.