Glencoe Physics: Principles and Problems, Student Edition
Glencoe Physics: Principles and Problems, Student Edition
1st Edition
ISBN: 9780078807213
Author: Paul W. Zitzewitz
Publisher: Glencoe/McGraw-Hill
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Chapter 11.1, Problem 9PP
To determine

The changes in the energy of box-Earth system and change in total energy of the system.

Expert Solution & Answer
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Answer to Problem 9PP

The change in the box-Earth system’s energy to lift the box to the table is W1=1.1×102 J .

The change in the box-Earth system’s energy to slide the box across the table is W2=0 J .

The change in the box-Earth system’s energy to lower the box to the floor is W3=1.1×102 J .

The system’s total energy change is W=0 J .

Explanation of Solution

Given:

The mass of the box is m=10.1 kg .

The height of the box from the floor is 1.1 m .

Formula used:

The expression for the gravitational potential energy is,

PE=mgh

Here, m is the mass, g is the acceleration due to gravity, and h is the distance from the reference level.

Calculation:

Consider the value of acceleration due to gravity as g=9.8m/s2 .

The change in the box-Earth system’s energy to lift the box to the table is,

W1=ΔPEW1=mg(hfhi)W1=(10.1 kg)×(9.8m/s2)×(1.1 m0.0)W1=1.1×102 J

The height of the reference level does not change across the table and ignore the friction. The change in the box-Earth system’s energy to slide the box across the table is,

W2=ΔPEW2=mg(hfhi)W2=(10.1 kg)×(9.8m/s2)×(1.1 m1.1 m)W2=0 J

The change in the box-Earth system’s energy to lower the box to the floor is,

W3=ΔPEW3=mg(hfhi)W3=(10.1 kg)×(9.8m/s2)×(0.0 m1.1 m)W3=1.1×102 J

The system’s total energy change is,

W=W1+W2+W3W=(1.1×102 J)+(0 J)+(1.1×102 J)W=0 J

The system’s total energy change is W=0 J .

Conclusion:

Thus, the change in the box-Earth system’s energy to lift the box to the table is W1=1.1×102 J .

Thus, the change in the box-Earth system’s energy to slide the box across the table is W2=0 J .

Thus, the change in the box-Earth system’s energy to lower the box to the floor is W3=1.1×102 J .

Thus, the system’s total energy change is W=0 J .

Chapter 11 Solutions

Glencoe Physics: Principles and Problems, Student Edition

Ch. 11.1 - Prob. 11SSCCh. 11.1 - Prob. 12SSCCh. 11.1 - Prob. 13SSCCh. 11.1 - Prob. 14SSCCh. 11.1 - Prob. 15SSCCh. 11.2 - Prob. 16PPCh. 11.2 - Prob. 17PPCh. 11.2 - Prob. 18PPCh. 11.2 - Prob. 19PPCh. 11.2 - Prob. 20PPCh. 11.2 - Prob. 21PPCh. 11.2 - Prob. 22PPCh. 11.2 - Prob. 23PPCh. 11.2 - Prob. 24SSCCh. 11.2 - Prob. 25SSCCh. 11.2 - Prob. 26SSCCh. 11.2 - Prob. 27SSCCh. 11.2 - Prob. 28SSCCh. 11.2 - Prob. 29SSCCh. 11.2 - Prob. 30SSCCh. 11 - Prob. 31ACh. 11 - Prob. 32ACh. 11 - Prob. 33ACh. 11 - Prob. 34ACh. 11 - Prob. 35ACh. 11 - Prob. 36ACh. 11 - Prob. 37ACh. 11 - Prob. 38ACh. 11 - Prob. 39ACh. 11 - Prob. 40ACh. 11 - Prob. 41ACh. 11 - Prob. 42ACh. 11 - Prob. 43ACh. 11 - Prob. 44ACh. 11 - Prob. 45ACh. 11 - Prob. 46ACh. 11 - Prob. 47ACh. 11 - Prob. 48ACh. 11 - Prob. 49ACh. 11 - Prob. 50ACh. 11 - Prob. 51ACh. 11 - Prob. 52ACh. 11 - Prob. 53ACh. 11 - Prob. 54ACh. 11 - Prob. 55ACh. 11 - Prob. 56ACh. 11 - Prob. 57ACh. 11 - Prob. 58ACh. 11 - Prob. 59ACh. 11 - Prob. 60ACh. 11 - Prob. 61ACh. 11 - Prob. 62ACh. 11 - Prob. 63ACh. 11 - Prob. 64ACh. 11 - Prob. 65ACh. 11 - Prob. 66ACh. 11 - Prob. 67ACh. 11 - Prob. 68ACh. 11 - Prob. 69ACh. 11 - Prob. 70ACh. 11 - Prob. 71ACh. 11 - Prob. 72ACh. 11 - Prob. 73ACh. 11 - Prob. 74ACh. 11 - Prob. 75ACh. 11 - Prob. 76ACh. 11 - Prob. 77ACh. 11 - Prob. 78ACh. 11 - Prob. 79ACh. 11 - Prob. 80ACh. 11 - Prob. 81ACh. 11 - Prob. 82ACh. 11 - Prob. 83ACh. 11 - Prob. 84ACh. 11 - Prob. 85ACh. 11 - Prob. 86ACh. 11 - Prob. 87ACh. 11 - Prob. 88ACh. 11 - Prob. 89ACh. 11 - Prob. 90ACh. 11 - Prob. 91ACh. 11 - Prob. 92ACh. 11 - Prob. 93ACh. 11 - Prob. 94ACh. 11 - Prob. 95ACh. 11 - Prob. 96ACh. 11 - Prob. 97ACh. 11 - Prob. 98ACh. 11 - Prob. 99ACh. 11 - Prob. 100ACh. 11 - Prob. 101ACh. 11 - Prob. 1STPCh. 11 - Prob. 2STPCh. 11 - Prob. 3STPCh. 11 - Prob. 4STPCh. 11 - Prob. 5STPCh. 11 - Prob. 6STPCh. 11 - Prob. 7STPCh. 11 - Prob. 8STPCh. 11 - Prob. 9STP

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