Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

What is buoyancy force? Compare the relative magnitudes of the buoyancy force acting on a body immersed in these media: \((a)\) air, \((b)\) water, \((c)\) mercury, and \((d)\) an evacuated chamber.

Short Answer

Expert verified
Question: Arrange the given media in increasing order of the buoyancy force experienced by an object when submerged: air, water, mercury, and an evacuated chamber. Answer: Evacuated Chamber < Air < Water < Mercury

Step by step solution

01

Understanding Buoyancy and Archimedes' Principle

Buoyancy is the upward force experienced by an object submerged in a fluid (gas or liquid). This force occurs because the pressure in the fluid increases with depth, and there is a pressure difference acting on the bottom and top surfaces of the object. Archimedes' principle states that the buoyant force acting on an object is equal to the weight of the fluid displaced by the object. Mathematically, this can be represented as \(Buoyancy\ Force = Weight\ of\ Displaced\ Fluid\), or in terms of density, volume, and gravitational acceleration: \(F_b = \rho V g\), where \(F_b\) is the buoyancy force, \(\rho\) is the density of the fluid, \(V\) is the volume of the displaced fluid, and \(g\) is the gravitational acceleration.
02

Computing Buoyancy Force for Each Medium

In this step, we will determine the buoyancy force acting on the object when immersed in air, water, mercury, and an evacuated chamber. To make a valid comparison, we need to use a fixed volume (\(V\)) for the object and gravitational acceleration (\(g\)), keeping these values constant for all cases. The densities of air, water, and mercury are approximately: - Air density: \(\rho_{air} \approx 1.2\ kg/m^3\) - Water density: \(\rho_{water} \approx 1000\ kg/m^3\) - Mercury density: \(\rho_{mercury} \approx 13,600\ kg/m^3\) For an evacuated chamber, the density of the fluid medium is considered to be \(0\ kg/m^3\) since there is no fluid present. Using the density values, we can find the buoyancy force for each medium using Archimedes' principle, \(F_b = \rho V g\): \((a) F_{b,air} = \rho_{air} V g\) \((b) F_{b,water} = \rho_{water} V g\) \((c) F_{b,mercury} = \rho_{mercury} V g\) \((d) F_{b,evacuated} = 0 \cdot Vg = 0\)
03

Comparing the Relative Magnitudes of Buoyancy Force

Based on the buoyancy force calculations, we can compare the magnitudes for each medium as follows: - Air has the lowest fluid density, leading to a relatively small buoyancy force. - Water's buoyancy force is significantly greater than air's due to its higher density. - Mercury provides the largest buoyancy force among the given media due to its extremely high density. - In the evacuated chamber, there is no fluid present, meaning there is no buoyancy force acting on the object. In conclusion, the relative magnitudes of buoyancy force for the given media are: Evacuated Chamber < Air < Water < Mercury

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

Is the heat transfer rate through the glazing of a double-pane window higher at the center or at the edge section of the glass area? Explain.

A solar collector consists of a horizontal copper tube of outer diameter $5 \mathrm{~cm}\( enclosed in a concentric thin glass tube of \)9 \mathrm{~cm}$ diameter. Water is heated as it flows through the tube, and the annular space between the copper and glass tube is filled with air at \(1 \mathrm{~atm}\) pressure. During a clear day, the temperatures of the tube surface and the glass cover are measured to be \(60^{\circ} \mathrm{C}\) and $32^{\circ} \mathrm{C}$, respectively. Determine the rate of heat loss from the collector by natural convection per meter length of the tube. A?swer: \(17.4 \mathrm{~W}\)

Consider a double-pane window whose airspace width is \(20 \mathrm{~mm}\). Now a thin polyester film is used to divide the airspace into two 10 -mm-wide layers. How will the film affect \((a)\) convection and \((b)\) radiation heat transfer through the window?

Why are the windows considered in three regions when analyzing heat transfer through them? Name those regions, and explain how the overall \(U\)-value of the window is determined when the heat transfer coefficients for all three regions are known.

An electric resistance space heater is designed such that it resembles a rectangular box \(50 \mathrm{~cm}\) high, \(80 \mathrm{~cm}\) long, and $15 \mathrm{~cm}\( wide filled with \)45 \mathrm{~kg}$ of oil. The heater is to be placed against a wall, and thus heat transfer from its back surface is negligible. The surface temperature of the heater is not to exceed $75^{\circ} \mathrm{C}\( in a room at \)25^{\circ} \mathrm{C}$ for safety considerations. Disregarding heat transfer from the bottom and top surfaces of the heater in anticipation that the top surface will be used as a shelf, determine the power rating of the heater in W. Take the emissivity of the outer surface of the heater to be \(0.8\) and the average temperature of the ceiling and wall surfaces to be the same as the room air temperature. Also, determine how long it will take for the heater to reach steady operation when it is first turned on (i.e., for the oil temperature to rise from \(25^{\circ} \mathrm{C}\) to \(75^{\circ} \mathrm{C}\) ). State your assumptions in the calculations.

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