/*! 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 49 A swimming pool is 5.0 \(\mathrm... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A swimming pool is 5.0 \(\mathrm{m}\) long, 4.0 \(\mathrm{m}\) wide, and 3.0 \(\mathrm{m}\) deep. Compute the force exerted by the water against (a) the bottom; and (b) either end. (Hint: Calculate the force on a thin, horizontal strip at a depth \(h\) , and integrate this over the end of the pool.) Do not include the force due to air pressure.

Short Answer

Expert verified
The force on the bottom is 588,000 N; on either end, it's 176,400 N.

Step by step solution

01

Calculate the Volume of the Pool

The pool is a rectangular prism. To find its volume, use the formula: \( V = \text{length} \times \text{width} \times \text{depth} \). Substituting the given values: \( V = 5.0 \times 4.0 \times 3.0 = 60.0 \; \text{m}^3 \).
02

Compute the Force on the Bottom

The force exerted by the water on the bottom of the pool is equal to the weight of the water above. This is given by \( F = \rho \cdot V \cdot g \), where \( \rho = 1000 \; \text{kg/m}^3 \) is the density of water and \( g = 9.8 \; \text{m/s}^2 \) is the acceleration due to gravity. Substituting the values: \( F = 1000 \times 60.0 \times 9.8 = 588,000 \; \text{N} \).
03

Setup The Integral for Force on an End

The force on either end is calculated by considering a differential strip at depth \( h \) with thickness \( dh \) and running the width of the end, which is 4.0 \( \mathrm{m} \). The pressure at a depth \( h \) is \( P = \rho gh \). The differential area \( dA \) of the strip is \( 4.0 \times dh \). The differential force is: \( dF = PdA = 1000 \times 9.8 \times h \times 4.0 \times dh \).
04

Integrate to Find Total Force on an End

Integrate \( dF \) from \( h = 0 \) to \( h = 3.0 \) to find the total force: \( F = \int_0^{3.0} 1000 \times 9.8 \times h \times 4.0 \, dh \). This simplifies to: \( 39200 \int_0^{3.0} h \, dh \) and results in: \( 39200 \left[ \frac{h^2}{2} \right]_0^{3.0} \). Calculating further gives \( 39200 \times \frac{9}{2} = 176,400 \; \text{N} \).

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 in Fluids
Understanding pressure in fluids is crucial when calculating hydrostatic forces. Pressure in a fluid is the force exerted per unit area. It's an important property because it determines how forces are distributed in a fluid system, like a swimming pool.
\
In a resting fluid, such as water in a pool, pressure increases with depth due to the weight of the fluid above. This is why deeper points in the pool experience higher pressures. The pressure at a certain depth is given by the formula: \( P = \rho gh \). Here, \( \rho \) is the density of the fluid, \( g \) is the acceleration due to gravity, and \( h \) is the depth. This formula shows that pressure doesn't depend on the total volume of water but rather on the depth at which you're measuring.
\
In the exercise, you calculated the force on different parts of the swimming pool walls by knowing the pressure at certain depths and using this pressure to find the force. The direct relationship between pressure and depth is key to these calculations, illustrating how pressure affects hydrostatic force in any fluid system.
Integration in Physics
Integration plays a vital role in physics, especially when calculating forces over a continuous area or volume. In hydrostatics, integration allows for the determination of total forces by summing contributions from infinitely small elements.
\
When dealing with a body of fluid, such as water in a pool, different parts of the surface experience different pressures because of varying depths. Calculating force for each thin horizontal strip and adding them all up gives the total force. This process is achieved using the mathematical technique of integration.
\
For instance, in the exercise solution, we considered small strips of water at a depth \( h \) and set up an integral to calculate the total hydrostatic force on either end of the pool. The integral \( \int_0^{3.0} 39200h \, dh \) allowed us to capture the contributions of force from each infinitesimally small strip along the depth of the pool. Integration thus provides a powerful tool to handle variable forces, leading to precise computations over complex shapes and volumes in physics.
Density of Water
The density of water is a staple concept in understanding hydrostatic pressure and forces. Water's density, commonly expressed as \( 1000 \; \text{kg/m}^3 \), serves as a fundamental constant in many physics equations involving fluids.
\
Density is defined as mass per unit volume. It's a measure of how much mass is contained in a given volume. For most practical purposes, water can be considered incompressible, meaning its density remains consistent, making calculations straightforward.
\
In the context of the exercise, knowing the density of water allowed us to calculate pressures and forces accurately using the formula \( F = \rho V g \). This consistency in density simplifies the calculation of hydrostatic force, as seen when determining the force the water exerts on the bottom of the pool. By maintaining this consistency, the density of water aids us in deriving reliable and accurate outcomes in any fluid mechanics problem involving water.

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 hydrometer consists of a spherical bulb and a cylindrical stem with a cross- sectional area of 0.400 \(\mathrm{cm}^{2}\) (see Fig. 14.13a). The total volume of bulb and stem is \(13.2 \mathrm{cm}^{3} .\) When immersed in water, the hydrometer floats with 8.00 \(\mathrm{cm}\) of the stem above the water surface. When the hydrometer is immersed in an organic fluid, 3.20 \(\mathrm{cm}\) of the stem is above the surface. Find the density of the organic fluid. (Nore: This illustrates the precision of such a hydrometer. Relatively small density differences give rise to relatively large differences in hydrometer readings.)

(a) Calculate the difference in blood pressure between the feet and top of the head for a person who is 1.65 \(\mathrm{m}\) tall. (b) Consider a cylindrical segment of a blood vessel 2.00 \(\mathrm{cm}\) long and 1.50 \(\mathrm{mm}\) in diameter. What additional outward force would such a vessel need to withstand in the person's feet compared to a similar vessel in her head?

Assume that crude oil from a supertanker has density 750 \(\mathrm{kg} / \mathrm{m}^{3}\) . The tanker runs aground on a sandbar. To refloat the tanker, its oil cargo is pumped out into steel barrels, each of which has a mass of 15.0 \(\mathrm{kg}\) when empty and holds 0.120 \(\mathrm{m}^{3}\) of oil. You can ignore the volume occupied by the steel from which the barrel is made. (a) If a salvage worker accidentally drops a filled, sealed barrel overboard, will it float or sink in the seawater? (b) If the barrel floats, what fraction of its volume will be above the water surface? If it sinks, what minimum tension would have to be exerted by a rope to haul the barrel up from the ocean floor? (c) Repeat parts (a) and (b) if the density of the oil is 910 \(\mathrm{kg} / \mathrm{m}^{3}\) and the mass of each empty barrel is 32.0 \(\mathrm{kg}\) .

A tall cylinder with a cross-sectional area 12.0 \(\mathrm{cm}^{2}\) is partially filled with mercury; the surface of the mercury is 5.00 \(\mathrm{cm}\) above the bottom of the cylinder. Water is slowly poured in on top of the mercury, and the two fluids don't mix. What volume of water must be added to double the gauge pressure at the bottom of the cylinder?

A firehose must be able to shoot water to the top of a building 35.0 \(\mathrm{m}\) tall when aimed straight up. Water enters this hose at a steady rate of 0.500 \(\mathrm{m}^{3} / \mathrm{s}\) and shoots out of a round nozzle. (a) What is the maximum diameter this nozzle can have? (b) If the only nozzle available has a diameter twice as great, what is the highest point the water can reach?

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.