Chapter 7 Energy and Work. Goals for Chapter 7 Overview energy. Study work as defined in physics. Relate work to kinetic energy. Consider work done by.

Slides:



Advertisements
Similar presentations
Physics 111: Mechanics Lecture 7
Advertisements

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 6: Conservation of Energy Work.
6-7 Problem Solving Using Conservation of Mechanical Energy
Chapter 6: Conservation of Energy
AP Physics B Summer Course 年AP物理B暑假班
Chapter 5 Energy 1. Dot product of vectors 2. Kinetic Energy 3. Potential Energy 4. Work-Energy Theorem 5. Conservative and non-conservative forces 6.
Work, Energy, and Power Samar Hathout KDTH 101. Work is the transfer of energy through motion. In order for work to take place, a force must be exerted.
ENERGY LCHS Dr.E.
Regents Physics Work and Energy.
Work and Energy Chapter 7.
Conservation of Energy Energy is Conserved!. The total energy (in all forms) in a “closed” system remains constant The total energy (in all forms) in.
Chapter 9:Linear Momentum 8-4 Problem Solving Using Conservation of Mechanical Energy 8-5 The Law of Conservation of Energy 8-6 Energy conservation with.
Physics 151: Lecture 15, Pg 1 Today’s Topics l Potential Energy, Ch. 8-1 l Conservative Forces, Ch. 8-2 l Conservation of mechanical energy Ch.8-4.
PHYSICS 231 INTRODUCTORY PHYSICS I
Energy.
General Physics 1, Additional questions By/ T.A. Eleyan
T101Q7. A spring is compressed a distance of h = 9.80 cm from its relaxed position and a 2.00 kg block is put on top of it (Figure 3). What is the maximum.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Notes - Energy A. Work and Energy. What is Energy?  Energy is the ability to produce change in an object or its environment.  Examples of forms of energy:
Work, Energy and Power AP style
Chapter 4 Work & Energy Dr. Ali.
Bellringer 10/25 A 95 kg clock initially at rest on a horizontal floor requires a 650 N horizontal force to set it in motion. After the clock is in motion,
Chapter 6 Conservation of Energy. MFMcGrawCh06 - Energy - Revised: 2/20/102 Conservation of Energy Work by a Constant Force Kinetic Energy Potential Energy.
College Physics, 7th Edition
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Units: 1Newton . 1 meter = 1 joule = 1J
Potential Energy and Conservative Forces
Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component.
Mechanics Work and Energy Chapter 6 Work  What is “work”?  Work is done when a force moves an object some distance  The force (or a component of the.
S-29 This cat is not happy. He is in need of a hair dryer. List five sources of energy that might be able to produce electricity for him.
Chapter 8 - Potential Energy and Conservation of Energy Conservative vs. Non-conservative Forces Definition of Potential Energy Conservation Of Mechanical.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
Work and Energy. Work a force that causes a displacement of an object does work on the object W = Fdnewtons times meters (N·m) or joules (J)
Work and Energy. Work, Power, & Energy Energy offers an alternative analysis of motion and its causes. Energy is transformed from 1 type to another in.
Work and Energy Chapter 7 Conservation of Energy Energy is a quantity that can be converted from one form to another but cannot be created or destroyed.
1 Work When a force moves something, work is done. Whenever work is done, energy is changed into a different form. Chemical energy → Kinetic energy.
Physics 1D03 - Lecture 22 Potential Energy Work and potential energy Conservative and non-conservative forces Gravitational and elastic potential energy.
Conservative Forces: The forces is conservative if the work done by it on a particle that moves between two points depends only on these points and not.
Reading Quiz - Work & Energy
Energy. Analyzing the motion of an object can often get to be very complicated and tedious – requiring detailed knowledge of the path, frictional forces,
Lectures by James L. Pazun 7 Work and Energy. Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley Goals for Chapter 7 Overview energy.
Chapter 7 Lecture Chapter 7: Work and Energy © 2016 Pearson Education, Inc.
Energy and Energy Conservation. Energy Two types of Energy: 1. Kinetic Energy (KE) - energy of an object due to its motion 2. Potential Energy (PE) -
Chapter 7 Energy and Work.
Phys211C7 p1 Kinetic Energy: Energy associated with motion K = ½ mv 2 Work done by a force on an object is that forces contribution to  K may only depend.
Lecture 11: Potential Energy & Energy Conservation.
WORK, ENERGY AND POWER WHY ARE WE WORKING SO HARD?
Conservation of Energy
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Chapter 6 Conservation of Energy. MFMcGraw-PHY 1401Ch06b - Energy - Revised: 6/25/102 Conservation of Energy Work by a Constant Force Kinetic Energy Potential.
Lecture 10: Work & Energy.
Work and Energy x Work and Energy 06.
Ch. 6, Work & Energy, Continued. Summary So Far Work-Energy Theorem: W net = (½)m(v 2 ) 2 - (½)m(v 1 ) 2   KE Total work done by ALL forces! Kinetic.
WORK A force that causes a displacement of an object does work on the object. W = F d Work is done –if the object the work is done on moves due to the.
Examples: Mechanical Energy Conservation
Work, Power, Energy. Work Concepts Work (W) ~ product of the force exerted on an object and the distance the object moves in the direction of the force.
Chapter 7 Conservation of Energy Conservative force Non-conservative force potential energy & potential function March 2, 2010.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Chapter 5 Work and Energy. Mechanical Energy  Mechanical Energy is the energy that an object has due to its motion or its position.  Two kinds of mechanical.
CHAPTER 5 Work and Energy Work: Work:Work done by an agent exerting a constant force is defined as the product of the component of the force in the direction.
Work Work Work –Work is done on an object when a force is applied and it moves in a direction that is parallel to the force acting on it.
Energy Notes Energy is one of the most important concepts in science. An object has energy if it can produce a change in itself or in its surroundings.
Chapter 6 Work and Energy © 2014 Pearson Education, Inc. No need to write information in red.
Warm up – Do old way A boy pulls a large box with a mass of 50 kg up a frictionless incline (
List five sources of energy that might be able to produce
1a. Positive and negative work
Chapter 7 Work and Energy
Unit 7: Work, Power, and Mechanical Energy.
Potential Potential Energy
Presentation transcript:

Chapter 7 Energy and Work

Goals for Chapter 7 Overview energy. Study work as defined in physics. Relate work to kinetic energy. Consider work done by a variable force. Study potential energy. Understand energy conservation. Include time and the relationship of work to power.

Energy Energy is conserved. Kinetic Energy describes motion and relates to the mass of the object and it’s velocity squared. Energy on earth originates from the sun. Energy on earth is stored thermally and chemically. Chemical energy is released by metabolism. Energy is stored as potential energy in object height and mass and also through elastic deformation. Energy can be dissipated as heat and noise.

Energy Transfer and Transformation Energy is transformed from one form to another, but it is not created or destroyed.

Mechanical energy—the energy associated with motion, position, and deformation of objects. Kinetic Energy. Elastic Potential Energy. Gravitational Potential Energy.

Energy can be dissipated by heat (motion transferred at the molecular level. This is referred to as dissipation.

WORK

What is “work” as defined in Physics? Formally, work is the product of a constant force F through a parallel displacement s. W = F.s W is N.m 1 Joule (J) = (1N.m)

Forces applied at angles must be resolved into components. Parallel component = along the displacement

W > 0 W < 0 W = 0

Sliding on a ramp

Work done be several forces

Work Done by a Varying Force

Energy may be stored in compressed springs.

Work and Kinetic Energy work-energy theorem W = K f - K i

Work done be several forces V i = 2.0 m/s

Gravitational Potential Energy (Near Earth’s surface) U = mgy

Gravitational Potential Energy U = mgh Independently of the path

Sliding on a ramp Vf ? M= 100kg, angle = 30 degrees, h =3m

U el = (1/2) kx 2

Work-Energy Theorem W total = K f – K i Conservatives force K f + U f = K i + U i Non-conservative forces K f + U f = K i + U i + W other Power P av = ΔW/Δt The unit is Watt (J/s)

A 1.50 kg book is sliding along a rough horizontal surface. At point A it is moving at 3.21m/s, and at point B it has slowed to 1.25 m/s. How much work was done on the book between A and B ? If J of work is done on the book from B to C, how fast is it moving at point C? How fast would it be moving at C if of work were done on it from B to C?

For its size, the common flea is one of the most accomplished jumpers in the animal world. A 2.0 mm long, 0.50 mg critter can reach a height of 20.0 cm in a single leap. Neglecting air drag, what is the takeoff speed of such a flea? Calculate the kinetic energy of this flea at takeoff and its kinetic energy per kilogram of mass. If a 65.0 Kg, 2.00 m -tall human could jump to the same height compared with his length as the flea jumps compared with its length, how high could he jump, and what takeoff speed would he need?

A 1.50 kg box moves back and forth on a horizontal frictionless surface between two different springs, as shown in the accompanying figure. The box is initially pressed against the stronger spring, compressing it 4.00 cm, and then is released from rest. a) By how much will the box compress the weaker spring? b) What is the maximum speed the box will reach?

Problems with non-conservative forces

You slam on the brakes of your car in a panic and skid a distance d on a straight and level road. If you had been traveling twice as fast, what distance would the car have skidded under the same conditions? Use work energy theorem A) 4d B)2d C) d D) (1/2) d

Consider two frictionless inclined planes with the same vertical height. Plane 1 makes an angle of 25.0 o with the horizontal, and plane 2 makes an angle of 55.0 o with the horizontal. Mass m 1 is placed at the top of plane 1, and mass m 2 is placed at the top of plane 2. Both masses are released at the same time. At the bottom, which mass is going faster? A) m 1 B) m 2 C) neither (both same speed)

The stone in the accompanying figure can be carried from the bottom to the top of a cliff by various paths. Which path requires more work? A) AC B) ABC C) same work for both paths