Tutorials in Introductory Physics
Tutorials in Introductory Physics
1st Edition
ISBN: 9780130970695
Author: Peter S. Shaffer, Lillian C. McDermott
Publisher: Addison Wesley
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Textbook Question
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Chapter 26.2, Problem 1aTH

1. Three objects are at rest in three beakers of water as shown.

  1. Compare the mass, volume, and density of the objects to the mass, volume, and density of the displaced water. Explain your reasoning in each case.

Chapter 26.2, Problem 1aTH, 1. Three objects are at rest in three beakers of water as shown. Compare the mass, volume, and , example  1

Chapter 26.2, Problem 1aTH, 1. Three objects are at rest in three beakers of water as shown. Compare the mass, volume, and , example  2

Expert Solution & Answer
Check Mark
To determine

The comparison of mass, volume and density of the object with the displaced water.

Explanation of Solution

Given:

Three objects are at rest in three beakers of water as shown:

FormulaUsed:

Use Archimedes principle which is expressed as follows:

  Fb=ρwatergVd   ......... (1)

Here, the buoyant force is Fb , the density of water is ρwater , acceleration due to gravity is g and the volume of fluid displaced is Vd .

Calculation:

For Object 1

Free body diagram of the 1st object is shown below:

As the object floats on the top of the surface, the displaced volume must be less than the volume of the object. Thus, Vd<V1 .

  Tutorials in Introductory Physics, Chapter 26.2, Problem 1aTH , additional homework tip  1

As the body is floating on the top surface, then the weight of the body is equal to the buoyant force. Thus, for equilibrium,

  mobjectg=Fbmobjectg=ρwatergVd(md=ρ waterVd)mobjectg=gmdmobject=md

Thus, the mass of the object is equal to the mass of the displaced water.

For density, apply summation of force in the vertical direction as follows:

  mobjectg=FbρobjectgVobject=ρwatergVd(m object=ρ objectV object)ρobject=ρwaterVdV object

As the Vd is less than the Vobject , then VdVobject is less than 1. Thus, the density of object must be less than the density of water.

For Object 2, Free body diagram of the 2nd object is shown below:

  Tutorials in Introductory Physics, Chapter 26.2, Problem 1aTH , additional homework tip  2

As the object floats inside the water, the displaced volume must be equal to the volume of the object. Thus, Vd=V2 .

As the body is floating inside the water then the weight of the body is equal to the buoyant force. Thus, for equilibrium,

  mobjectg=Fbmobjectg=ρwatergVd(md=ρ waterVd)mobjectg=gmdmobject=md

Thus, the mass of the object is equal to the mass of the displaced water.

For density apply summation of force in the vertical direction as follows:

  mobjectg=FbρobjectgVobject=ρwatergVd(m object=ρ objectV object)ρobject=ρwaterVdV object(Vd=V object)ρobject=ρwater

Thus, the density of the object must be equal to the density of water.

For Object 3,

Free body diagram of the 3rd object is shown below:

  Tutorials in Introductory Physics, Chapter 26.2, Problem 1aTH , additional homework tip  3

The displaced volume must be equal to the volume of the object as it is kept inside the tank completely. Thus, Vd=V2 .

As the body is not floating inside the water, then the weight of the body is more than the buoyant force. Thus, for equilibrium,

  mobjectg>Fbmobjectg>ρwatergVd(md=ρ waterVd)mobjectg>gmdmobject>md

Thus, the mass of the object is more than the mass of the displaced water.

For density, apply summation of force in the vertical direction as follows:

  mobjectg>FbρobjectgVobject>ρwatergVd(m object=ρ objectV object)ρobject>ρwaterVdV object(Vd=V object)ρobject>ρwater

Thus, the density of object must be more thanthe density of water.

Conclusion:

For object 1,

  Vd<V1 , mobject=md and ρobject<ρwater .

For object 2,

  Vd=V2 , mobject=md and ρobject=ρwater .

For object 3,

  Vd=V2 , mobject>md and ρobject>ρwater .

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