Physics 101: Lecture 10, Pg 1 Physics 101: Lecture 10 Potential Energy & Energy Conservation l Today’s lecture will cover Textbook Sections 6.5 - 6.8 Hour.

Slides:



Advertisements
Similar presentations
Potential Energy, Conservation of Energy
Advertisements

Energy Conservation 1.
Energy and its Conservation
Chapter 6: Conservation of Energy
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.
Conservation of Energy
Work and Energy Chapter 7.
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
Work & Energy. Energy is Conserved Energy is “Conserved” meaning it can not be created nor destroyed –Can change form –Can be transferred Total Energy.
Physics 101: Lecture 13, Pg 1 Physics 101: Lecture 13 l Quick Review of Last Time, Example Problems l Power, Work done by a variable force l Reminders:
1a. Positive and negative work
Example: The simple pendulum l Suppose we release a mass m from rest a distance h 1 above its lowest possible point. ç What is the maximum speed of the.
Chapter 5 Work and Energy
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,
Introduction to Work Monday, September 14, 2015 Work Work tells us how much a force or combination of forces changes the energy of a system. Work is.
Chapter 5 Work, Energy, Power Work The work done by force is defined as the product of that force times the parallel distance over which it acts. The.
2/19/03Physics 103, Spring 2004, U. Wisconsin1 Physics 103: Lecture 9 Energy Conservation, Power Today’s lecture will cover Potential Energy Conservation.
Chapter 5 Work and Energy. Review  x = v i  t + ½ a  t 2  x = ½ (v i + v f )  t v f = v i + a  t v f 2 = v i 2 + 2a  x.
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Physics 201: Lecture 13, Pg 1 Lecture 13 l Goals  Introduce concepts of Kinetic and Potential energy  Develop Energy diagrams  Relate Potential energy.
Potential Energy and Conservative Forces
Thursday, June 26, 2014PHYS , Summer 2014 Dr. Jaehoon Yu 1 PHYS 1441 – Section 001 Lecture #13 Thursday, June 26, 2014 Dr. Jaehoon Yu Potential.
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)
Sect. 7-4: Kinetic Energy; Work-Energy Principle.
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.
Energy Conservation And Non-Conservative Forces. Conservation of Mechanical Energy Definition of mechanical energy: (8-6) Using this definition and considering.
2008 Physics 2111 Fundamentals of Physics Chapter 8 1 Fundamentals of Physics Chapter 8 Potential Energy & Conservation of Energy 1.Potential Energy 2.Path.
Monday, Mar. 24, 2008 PHYS , Spring 2008 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #16 Monday, Mar. 24, 2008 Dr. Jaehoon Yu Potential Energy.
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More gravitational potential energy Potential energy of a spring Work-kinetic.
Physics 1501: Lecture 14, Pg 1 Physics 1501: Lecture 14 Today’s Agenda l Midterm graded by next Monday (maybe …) l Homework #5: Due Friday Oct. 11:00.
Lecture 11: Potential Energy & Energy Conservation.
Physics 101: Lecture 13, Pg 1 Physics 101: Lecture 13 l Quick Review of Last Time, Example Problems l Power, Work done by a variable force l Reminders:
Work - Work is calculated by multiplying the force applied by the distance the object moves while the force is being applied. W = Fs.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Work has a specific definition in physics
Potential Energy & Energy Conservation. Work Done by Gravity 1 l Example 1: Drop ball Y i = h Y f = 0 mg S y x Y i = h Y f = 0 mg S y x 10.
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.
Physics 101: Lecture 3, Pg 1 Kinematics Physics 101: Lecture 03 l Today’s lecture will cover Textbook Sections
Potential Energy and Conservation of Energy
Wednesday June 15, PHYS , Summer I 2005 Dr. Andrew Brandt PHYS 1443 – Section 001 Lecture #9 Wednesday June 15, 2005 Dr. Andrew Brandt Lightning.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections  Hour Exam 1, Monday.
Wednesday, June 30, 2004PHYS , Summer 2004 Dr. Jaehoon Yu 1 PHYS 1441 – Section 501 Lecture #9 Wednesday, June 30, 2004 Dr. Jaehoon Yu Conservative.
ENERGY Objectives: After completing this module, you should be able to: Define kinetic energy and potential energy, along with the appropriate units.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Physics 101: Lecture 10, Pg 1 Physics 101: Lecture 10 Potential Energy & Energy Conservation l Today’s lecture will cover Textbook Sections
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.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy  Hour Exam 1, Tomorrow! – Exam 2.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections Exam II.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections
UB, Phy101: Chapter 6, Pg 1 Physics 101: Chapter 6 Work and Kinetic Energy l New stuff: Chapter 6, sections
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections Exam II.
PHY 101: Lecture Work Done by a Constant Force
Monday, Mar. 30, 2009PHYS , Spring 2009 Dr. Jaehoon Yu PHYS 1441 – Section 002 Lecture #14 Monay, Mar. 30, 2009 Dr. Jaehoon Yu Work-Kinetic Energy.
Physics 101: Lecture 10, Pg 1 Physics 101: Lecture 10 Potential Energy & Energy Conservation l Today’s lecture will cover Textbook Sections Hour.
Do Now: 1. You push a crate up a ramp with a force of 10 N, but despite your pushing the crate slides 4 m down the ramp. How much work did you do? 2. A.
Physics 101: Lecture 10 Potential Energy & Energy Conservation
PHYS 1443 – Section 001 Lecture #9
Physics 101: Lecture 10 Potential Energy & Energy Conservation
Physics 101: Lecture 9 Work and Kinetic Energy
Physics 101: Lecture 10 Potential Energy & Energy Conservation
Physics 101: Lecture 9 Work and Kinetic Energy
Work and Kinetic Energy
Potential Energy and Energy Conservation
Work Who does the most work? Definition of work in physics:
PHYS 1443 – Section 001 Lecture #13
Potential Energy and Energy Conservation
Mechanical Energy.
Purdue University, Physics 220
Presentation transcript:

Physics 101: Lecture 10, Pg 1 Physics 101: Lecture 10 Potential Energy & Energy Conservation l Today’s lecture will cover Textbook Sections Hour Exam 1: One week away! -exam time / conflicts -exam locations -how to study / exam review Sun. 8pm -sign up for conflict exam before Thurs. -if you have a double conflict, contact Prof. Bob Clegg,

Physics 101: Lecture 10, Pg 2Review  Work: Transfer of Energy by Force W F = |F| |S| cos  Kinetic Energy (Energy of Motion) K = 1/2 mv 2 Work-Kinetic Energy Theorem:  W =  K Preview Potential (Stored) Energy U

Physics 101: Lecture 10, Pg 3 Preflight 4 What concepts were most difficult to understand in preparing for this lecture? “everything” “nothing” “Work Energy- Theorem; What is it!?” “The equations were kind of confusing…” “Understanding what the symbols mean” “…confused as to the significance of the lower case ‘k’” Lecture / Lab / HW / Discussion order USA vs. Canada Olympic hockey was too awesomely distracting to think very hard about the pre-lecture, sorry. “the last problem the one with baseball on the moon. ” “signs for work... ” What is a conservative force anyway?

Physics 101: Lecture 10, Pg 4 Work Done by Gravity 1 l Example 1: Drop ball Y i = h Y f = 0 W g = (mg)(S)cos  S = h W g = mghcos(0 0 ) = mgh  y = y f -y i = -h W g = -mg  y mg S y x Y i = h Y f = 0 mg S y x

Physics 101: Lecture 10, Pg 5 Work Done by Gravity 2 Example 2: Toss ball up W g = (mg)(S)cos  S = h W g = mghcos(180 0 ) = -mgh  y = y f -y i = +h W g = -mg  y Y f = h Y i = 0 mg S y x

Physics 101: Lecture 10, Pg 6 Work Done by Gravity 3 Example 3: Slide block down incline W g = (mg)(S)cos  S = h/cos  W g = mg(h/cos  )cos  W g = mgh  y = y f -y i = -h W g = -mg  y h  mg S

Physics 101: Lecture 10, Pg 7 Work and Potential Energy l Work done by gravity independent of path  W g = -mg (y f - y i ) l Define U g =mgy l Works for any CONSERVATIVE force l Modify Work-Energy theorem

Physics 101: Lecture 10, Pg 8 Conservation ACT Which of the following statements correctly define a Conservative Force: A. A force is conservative when the work it does on a moving object is independent of the path of the motion between the object's initial and final positions. B. A force is conservative when it does no net work on an object moving around a closed path, starting and finishing at the same point. C. Both of the above statements are correct. D. Neither of the above statements is correct. correct

Physics 101: Lecture 10, Pg 9 Skiing Example (no friction) A skier goes down a 78 meter high hill with a variety of slopes. What is the maximum speed she can obtain if she starts from rest at the top? Conservation of energy:  W nc =  K +  U K i + U i = K f + U f ½ m v i 2 + m g y i = ½ m v f 2 + m g y f 0 + g y i = ½ v f 2 + g y f v f 2 = 2 g (y i -y f ) v f = sqrt( 2 g (y i -y f )) v f = sqrt( 2 x 9.8 x 78) = 39 m/s 26 0 = K f -K i + U f - U i

Physics 101: Lecture 10, Pg 10 Pendulum ACT l As the pendulum falls, the work done by the string is 1) Positive2) Zero3) Negative How fast is the ball moving at the bottom of the path? W = F d cos . But  = 90 degrees so Work is zero. h Conservation of Energy (W nc =0)  W nc =  K +  U 0 = K final - K initial + U final - U initial K initial + U initial = K final +U final 0 + mgh = ½ m v 2 final + 0 v final = sqrt(2 g h)

Physics 101: Lecture 10, Pg 11 Pendulum Demo With no regard for his own personal safety your physics professor will risk being smashed by a bowling ball pendulum! If released from a height h, how far will the bowling ball reach when it returns? h Conservation of Energy (W nc =0)  W nc =  K +  U 0 = K final - K initial + U final - U initial K initial + U initial = K final +U final 0 + mgh initial = 0 + mgh final h initial = h final

Physics 101: Lecture 10, Pg 12 Lecture 10, Preflight 1 Imagine that you are comparing three different ways of having a ball move down through the same height. In which case does the ball get to the bottom first? A. Dropping B. Slide on ramp (no friction) C. Swinging down D. All the same “they will all have the same speed at the bottom.” correct “The ball being dropped will reach the ground fastest since it doesn't have to travel as far.”

Physics 101: Lecture 10, Pg 13 Lecture 10, Preflight 2 Imagine that you are comparing three different ways of having a ball move down through the same height. In which case does the ball reach the bottom with the highest speed? 1. Dropping 2. Slide on ramp (no friction) 3. Swinging down 4. All the same correct Conservation of Energy (W nc =0)  W nc =  K +  U K initial + U initial = K final +U final 0 + mgh = ½ m v 2 final + 0 v final = sqrt(2 g h)

Physics 101: Lecture 10, Pg 14 Skiing w/ Friction A 50 kg skier goes down a 78 meter high hill with a variety of slopes. She finally stops at the bottom of the hill. If friction is the force responsible for her stopping, how much work does it do? Work Energy Theorem: W nc = K f -K i + U f -U i = ½ m v f 2 - ½ m v i 2 + m g y f – m g y i = g y i m = – 764 x 50 Joules = Joules Similar to bob sled homework

Physics 101: Lecture 10, Pg 15 Galileo’s Pendulum ACT How high will the pendulum swing on the other side now? A) h 1 > h 2 B) h 1 = h 2 C) h 1 < h 2 h1h1 h2h2 m Conservation of Energy (W nc =0)  W nc =  K +  U K initial + U initial = K final +U final 0 + mgh 1 = 0 + mgh 2 h 1 = h 2

Physics 101: Lecture 10, Pg 16 Power (Rate of Work) P = W /  t  Units: Joules/Second = Watt l How much power does it take for a (70 kg) student to run up the stairs in 151 Loomis (5 meters) in 7 sec? P = W / t = m g h / t = (70 kg) (9.8 m/s 2 ) (5 m) / 7 s = 490 J/s or 490 Watts

Physics 101: Lecture 10, Pg 17Summary  Conservative Forces »Work is independent of path »Define Potential Energy U n U gravity = m g y n U spring = ½ k x 2  Work – Energy Theorem  Chapter 6, problems 27, 31, 35