Download presentation
Presentation is loading. Please wait.
Published byMerry Griffith Modified over 9 years ago
1
Work and Energy CHAPTER 6
2
A New Perspective on Motion We have been analyzing motion through the perspective of Newton’s Laws dealing with acceleration, velocity, and displacement. In this chapter, we will look at motion from a different perspective – that of work and energy.
3
What is Work? When a force acts upon an object and causes its displacement, it is said that work has been done on the object. The force MUST cause a displacement! No work is done if the object doesn’t move.
4
Is There Work? 1. A woman pushes a shopping cart across the floor. YES – Force causing displacement. 2. A man pushes against a wall. NO – No displacement 3. A book falls off a table to the ground. YES – Gravity provides the force to cause displacement 4. A child holds a book over her head while she stands on a moving walkway. NO – The force is not causing the displacement.
5
Calculating Work
7
Units for Work
8
Example #1
9
Example #2
10
Example #3
11
Example #4
12
Energy Energy (E) – the ability to do work. Types of energy: Mechanical – kinetic energy + potential energy Electrical Nuclear Heat Chemical Sound
13
Kinetic Energy
14
Kinetic Energy Example
15
Work-Energy Theorem
16
Work-Energy Theorem Example 1
17
Work-Energy Theorem Example 2
18
Work Done by the Force of Gravity
19
Work Done by Gravity Example 1
20
Work Done by Gravity Example 2
21
Gravitational Potential Energy
22
Potential Energy Example
23
Next Class: Quiz on Work and Energy (What we’ve learned so far) Concepts and problem-solving applications related to: Work done by forces (including gravity and friction) Kinetic and potential energy Work-Energy Theorem
24
Conservative vs. Nonconservative Forces Conservative force – total Work on a closed path is zero. (ex: gravity) Nonconservative force – total Work on a closed path is NOT zero. (ex: friction) Energy 24 -W+W -W Gravity- down Motion- up Friction – left Motion - right Friction - right Motion- left Gravity- down Motion- down
25
Conservation of Energy
26
Conservation of Mechanical Energy
28
Conceptual Example 1: Pendulum Pendulum - Kinetic and Potential Energy Pendulum - Kinetic and Potential Energy In the absence of air resistance and friction… the pendulum would swing forever example of conservation of mechanical energy Potential → Kinetic → Potential and so on… In reality, air resistance and friction cause mechanical energy loss, so the pendulum will eventually stop.
29
Conceptual Example 2: Roller Coaster Roller Coaster - Kinetic and Potential Energy Roller Coaster - Kinetic and Potential Energy
30
Conceptual Example 3: Downhill Skiing Downhill Skiing - Kinetic and Potential Energy Downhill Skiing - Kinetic and Potential Energy This animation neglects friction and air resistance until the bottom of the hill. Friction is provided by the unpacked snow. Mechanical energy loss (nonconservative force) Negative work
31
Mousetrap Cars
32
Problem Solving Insights Determine if non-conservative forces are included. If yes: ME f = ME 0 + W nc If no: ME f = ME 0 Eliminate pieces that are zero before solving Key words: starts from rest (KE 0 = 0), ends on the ground (PE f = 0), etc.
33
Example 1 The Magnum XL-200 at Cedar Point includes a vertical drop of 59.4m. Assume the roller coaster has a speed of nearly zero at the crest of the hill. Neglecting friction, find the speed of the coaster at the bottom of the hill. ME f = ME 0 KE f + PE f = KE 0 + PE 0 ½ mv f 2 + mgh f = ½ mv 0 2 + mgh 0 ½ mv f 2 = mgh 0 (mass cancels!) v f 2 = 2(9.8)(59.4) → v f = 34.1 m/s
34
Example 2 A 55.0 kg skateboarder starts out with a speed of 1.80 m/s. He does +80.0J of work on himself by pushing with his feet against the ground. In addition, friction does -265 J of work on him. The final speed of the skateboarder is 6.00 m/s. a) Calculate the change in gravitational potential energy. b) How much has the vertical height of the skater changed, and is the skater above or below the starting point?
35
Example 3 A 2.00kg rock is released from rest from a height of 20.0m. Ignore air resistance & determine the kinetic, potential, & mechanical energy at each of the following heights: 20.0m, 12.0m, 0m (Round g to 10 m/s 2 for ease)
36
Example 4 Find the potential energy, kinetic energy, mechanical energy, velocity, and height of the skater at the various locations below. 36 Energy max
37
Power Power : Rate of doing work. The work done per unit time. Equation P = W/t or P =(F d)/t P is power ( Watts, ft lb/s, ft lb/min) Horsepower : another unit for measuring power. 1 horsepower = 746 Watts (or 1 horsepower = 550 ftlb/s) To find horsepower, divide P (in Joules) by 746.
38
Power Example #1 A weight lifter lifts a 75 kg weight from the ground to a height of 2.0 m. He performs this feat in 1.5 seconds. Find the weight lifter’s average power in A) Watts and B)Horsepower.
39
Power Example #2 A runner sprints 100 m up a hill in 25 seconds. Her average power during this run is 800 Watts. Find the force that the runner exerts during the run.
40
Power Example #3 A car accelerates from rest to 20.0 m/s is 5.6 seconds along a level stretch of road. Ignoring friction, determine the average power required to accelerate the car if A. The weight of the car is 9,000 N B. The weight of the car is 14,000 N.
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.