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Chapter 11 Lecture. Chapter 11 Work. Chapter Goal: To develop a more complete understanding of energy and its conservation. Slide 11-2. Chapter 11 Preview. Slide 11-3. Chapter 11 Preview. Slide 11-3. Chapter 11 Preview. Slide 11-5. Chapter 11 Preview. Slide 11-6. Chapter 11 Preview.
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Chapter 11 Work Chapter Goal: To develop a more complete understanding of energy and its conservation. Slide 11-2
Chapter 11 Preview Slide 11-3
Chapter 11 Preview Slide 11-3
Chapter 11 Preview Slide 11-5
Chapter 11 Preview Slide 11-6
Chapter 11 Preview Slide 11-7
Chapter 11 Preview Slide 11-8
Chapter 11 Reading Quiz Slide 11-9
Reading Question 11.1 The statement K = W is called the • Law of conservation of energy. • Work-kinetic energy theorem. • Kinetic energy equation. • Weight-kinetic energy theorem. Slide 11-10
Reading Question 11.1 The statement K = W is called the • Law of conservation of energy. • Work-kinetic energy theorem. • Kinetic energy equation. • Weight-kinetic energy theorem. Slide 11-11
Reading Question 11.2 The transfer of energy to a system by the application of a force is called • Dot product. • Power. • Work. • Watt. • Energy transformations. Slide 11-12
Reading Question 11.2 The transfer of energy to a system by the application of a force is called • Dot product. • Power. • Work. • Watt. • Energy transformations. Slide 11-13
Reading Question 11.3 A vector has magnitude C. Then the dot product of the vector with itself, is • 0. • C/2. • C. • 2C. • C2. Slide 11-14
Reading Question 11.3 A vector has magnitude C. Then the dot product of the vector with itself, is • 0. • C/2. • C. • 2C. • C2. Slide 11-15
Reading Question 11.4 The work done by a dissipative force like friction, Wdiss, is • Always zero. • Always positive. • Always negative. Slide 11-16
Reading Question 11.4 The work done by a dissipative force like friction, Wdiss, is • Always zero. • Always positive. • Always negative. Slide 11-17
Reading Question 11.5 Light bulbs are typically rated in terms of their watts. The watt W is a measure of • The change in the bulb’s potential energy. • The energy consumed. • The force exerted on the bulb holder. • The power dissipated. Slide 11-18
Reading Question 11.5 Light bulbs are typically rated in terms of their watts. The watt W is a measure of • The change in the bulb’s potential energy. • The energy consumed. • The force exerted on the bulb holder. • The power dissipated. Slide 11-19
Chapter 11 Content, Examples, and QuickCheck Questions Slide 11-20
The Basic Energy Model W > 0: The environment does work on the system and the system’s energy increases. W < 0: The system does work on the environment and the system’s energy decreases. Slide 11-21
The Basic Energy Model • The energy of a system is a sum of its kinetic energy K, its potential energy U, and its thermal energy Eth. • The change in system energy is: Energy can be transferred to or from a system by doing work Won the system. This process changes the energy of the system: Esys = W. Energy can be transformed within the system among K,U, and Eth. These processes don’t change the energy of the system: Esys = 0. Slide 11-22
QuickCheck 11.1 A skier is gliding down a slope at a constant speed. What energy transformation is taking place? K Ug Ug K Eth K Ug Eth K Eth Slide 11-23
QuickCheck 11.1 A skier is gliding down a slope at a constant speed. What energy transformation is taking place? K Ug Ug K Eth K Ug Eth K Eth Slide 11-24
Work and Kinetic Energy • The word “work” has a very specific meaning in physics. • Work is energy transferred to or from a body or system by the application of force. • This pitcher is increasing the ball’s kinetic energy by doing work on it. Slide 11-25
Work and Kinetic Energy • Consider a force acting on a particle which moves along the s-axis. • The force component Fs causes the particle to speed up or slow down, transferring energy to or from the particle. • The force does work on the particle: • The units of work are N m, where 1 N m = 1 kg m2/s2 = 1 J. Slide 11-26
The Work-Kinetic Energy Theorem • The net force is the vector sum of all the forces acting on a particle . • The net work is the sum Wnet = Wi, where Wi is the work done by each force . • The net work done on a particle causes the particle’s kinetic energy to change. Slide 11-27
An Analogy with the Impulse-Momentum Theorem • The impulse-momentum theorem is: • The work-kinetic energy theorem is: • Impulse and work are both the area under a force graph, but it’s very important to know what the horizontal axis is! Slide 11-28
QuickCheck 11.2 A tow rope pulls a skier up the slope at constant speed. What energy transfer (or transfers) is taking place? W Ug W K W Eth Both A and B. Both A and C. Slide 11-29
QuickCheck 11.2 A tow rope pulls a skier up the slope at constant speed. What energy transfer (or transfers) is taking place? W Ug W K W Eth Both A and B. Both A and C. Slide 11-30
Work Done by a Constant Force • A force acts with a constant strength and in a constant direction as a particle moves along a straight line through a displacement . • The work done by this force is: • Here is the angle makes relative to . Slide 11-31
Example 11.1 Pulling a Suitcase Slide 11-32
Example 11.1 Pulling a Suitcase Slide 11-33
QuickCheck 11.3 A crane lowers a girder into place at constant speed. Consider the work Wg done by gravity and the work WT done by the tension in the cable. Which is true? Wg > 0 andWT > 0 Wg > 0 andWT < 0 Wg < 0 andWT > 0 Wg < 0 andWT < 0 Wg = 0 andWT = 0 Slide 11-34
QuickCheck 11.3 A crane lowers a girder into place at constant speed. Consider the work Wg done by gravity and the work WT done by the tension in the cable. Which is true? Wg > 0 andWT > 0 Wg > 0 andWT < 0 Wg < 0 andWT > 0 Wg < 0 andWT < 0 Wg = 0 andWT = 0 The downward force of gravity is in the direction of motion positive work. The upward tension is in the direction opposite the motion negative work. Slide 11-35
Tactics: Calculating the Work Done by a Constant Force Slide 11-36
Tactics: Calculating the Work Done by a Constant Force Slide 11-37
Tactics: Calculating the Work Done by a Constant Force Slide 11-38
QuickCheck 11.4 Robert pushes the box to the left at constant speed. In doing so, Robert does ______ work on the box. positive negative zero Slide 11-39
QuickCheck 11.4 Robert pushes the box to the left at constant speed. In doing so, Robert does ______ work on the box. positive negative zero Force is in the direction of displacement positive work Slide 11-40
QuickCheck 11.5 A constant force pushes a particle through a displacement . In which of these three cases does the force do negative work? Both A and B. Both A and C. Slide 11-41
QuickCheck 11.5 A constant force pushes a particle through a displacement . In which of these three cases does the force do negative work? Both A and B. Both A and C. Slide 11-42
Example 11.2 Work During a Rocket Launch Slide 11-43
Example 11.2 Work During a Rocket Launch Slide 11-44
Example 11.2 Work During a Rocket Launch Slide 11-45
Example 11.2 Work During a Rocket Launch Slide 11-46
QuickCheck 11.6 Which force below does the most work? All three displacements are the same. The 10 N force. The 8 N force The 6 N force. They all do the same work. sin60 = 0.87 cos60 = 0.50 Slide 11-47
QuickCheck 11.6 Which force below does the most work? All three displacements are the same. The 10 N force. The 8 N force The 6 N force. They all do the same work. sin60 = 0.87 cos60 = 0.50 Slide 11-48
QuickCheck 11.7 A light plastic cart and a heavy steel cart are both pushed with the same force for a distance of 1.0 m, starting from rest. After the force is removed, the kinetic energy of the light plastic cart is ________ that of the heavy steel cart. greater than equal to less than Can’t say. It depends on how big the force is. Slide 11-49
QuickCheck 11.7 A light plastic cart and a heavy steel cart are both pushed with the same force for a distance of 1.0 m, starting from rest. After the force is removed, the kinetic energy of the light plastic cart is ________ that of the heavy steel cart. greater than equal to less than Can’t say. It depends on how big the force is. Same force, same distance same work done Same work change of kinetic energy Slide 11-50