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 15SSC

(a)

To determine

To explain: the consequences in terms of work and energy.

To draw: a bar graph for this situation.

(a)

Expert Solution
Check Mark

Explanation of Solution

Introduction:

Work done on an object is equal to the product of the force applied on the object F and the displacement of the object s in the direction of force.

The expression for the work done is given by

  W=F.s  ......(1)

The person uses an air hose to apply force on the puck and thus the force displaces the puck to a certain distance. So, from the definition of work done, work is said to be done on the puck. If the person applied a force F on the puck, it is displaced to a distance of d m, then the work done on the puck is

  W=F.d  ......(2)

Work done on object is used to change the energy of the object. Initially, work is done on the puck to move it a certain distance and a because of the work done on the puck, it undergoes motion. Therefore, the puck possesses kinetic energy in the final state.

Final kinetic energy is KEf .

Initial kinetic energy is KEi .

Equation for work done on the puck is

  W=KEfKEi

  W=12mvf212mvi2  ......(3)

Since the puck is initially at rest, vi=0m/s .

Equation (3) becomes,

  W=12mvf2  ......(4)

The following is the energy bar graph of the puck on the frictional air table. Initial kinetic energy of the puck is zero. The work done on the puck is equal to final kinetic energy.

  Glencoe Physics: Principles and Problems, Student Edition, Chapter 11.1, Problem 15SSC

(b)

To determine

To describe: The manner kinetic energy and work done should differ from those in the first situation.

(b)

Expert Solution
Check Mark

Explanation of Solution

Introduction:

Work done on an object is equal to the product of the force applied on the object F and the displacement of the object s in the direction of force.

If the mass of the puck is reduced to half m2 and the same amount of force F is applied on the puck, then the puck will undergo same displacement as that of displacement of the puck of mass m because both masses move equal distances on a frictionless surface. Thus, the work done on the puck of mass m2 , W is equal to the work done on the puck of mass m .

The expression the work done W is

  W=12(m2)v2f

Work done on the puck of mass m2 is equal to the change in the kinetic energy of the puck and it is also equal to the work done on the puck of mass m . So, the change in the kinetic energy of the puck of mass m2 also equal to the change in the kinetic energy of the puck of mass m .

Since the work done on the puck of mass m and m2 is equal, one can write,

  W=W12mvf2=12(m2)vf2vf=2vfvf=1.41vf

Conclusion:

Hence, the smaller mass puck moves with a velocity that is 1.41 times that of the velocity of the larger puck.

(c)

To determine

To describe: The situation in part a, and b in terms of impulse and momentum.

(c)

Expert Solution
Check Mark

Explanation of Solution

Introduction:

Work done on an object is equal to the product of the force applied on the object F and the displacement of the object s in the direction of force.

Momentum of an object is the product of its mass m and its velocity v .

  p=mv  ......(1)

Impulse is equal to the change in momentum,

  J=dp  ......(2)

Use equation (1) in equation (2)

  J=mvfmvi  ......(3)

The momentum of the puck of mass m is

  p=mvf  ......(4)

The momentum of the puck of mass m2 is

  p=(m2)vf  ......(5)

Divide equation (4) by equation (5)

  pp=mvf(m2)vfs

  pp=2vfvf  ......(6)

Substitute the value of vf in equation (6)

  p=2×1.41vfvfpp=0.707p

From the above equation, it is clear that the pucks of mass m and mass m2 will not have same momentum and the momentum of the pucks of mass m2 is small that that of the pucks of mass m .

The impulse on the puck of mass m is

  J=mvf  ......(7)

The impulse on the puck of mass m2 is

  J=(m2)vf  ......(8)

Divide equation (7) by (8),

  JJ=mvf(m2)vf

  JJ=2vfvf  ......(9)

Substitute the value of vf=1.41vf in equation (9)

  J=1.41vf2vfJJ=0.707J

From the equation, it is clear that the pucks of mass m and mass m2 will not have the same mass impulse and the impulse of the pucks of mass m2 is small that of the pucks of mass m .

Conclusion:

Hence, it is described the situation of part a and b in terms of impulse and momentum.

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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