General Physics I: Day 17 Conservation of Energy & Energy Diagrams

Slides:



Advertisements
Similar presentations
ConcepTest Clicker Questions
Advertisements

Gravitational potential energy. Conservation of energy
6-7 Problem Solving Using Conservation of Mechanical Energy
Physics 218, Lecture XV1 Physics 218 Lecture 15 Dr. David Toback.
An object is released from rest on a planet that
Sect. 8-3: Mechanical Energy & It’s Conservation.
Conservative Forces & Potential Energy
Chapter 9 Potential Energy & Conservation of Energy
Energy Chapter 5. Mechanical Energy Energy due to movement or position. Energy due to movement or position. Kinetic Energy – energy of motion Kinetic.
Dr. Joseph W. Howard ©Spring 2008 Energy What is it? It is how nature keeps score. Like a “currency” of the universe. To cause a change requires energy.
 A weightlifter lifts a barbell 0.65 m with a constant force of 435 N. If it takes 280 W to move the barbell, how many seconds did it take?
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.
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 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV.
Physics 151 Week 10 Day 2 Topics: Apparent Weight & Conservation of Energy  Apparent Weight  Conservation of Energy.
Conservative Forces Lecturer: Professor Stephen T. Thornton
1a. Positive and negative work
Energy Something that enables an object to work is called energy. What are some different forms of energy? –Potential –Electrical –Mechanical –Kinetic.
Conservation of Energy November The conservation of energy.  In a closed system, energy is neither created nor destroyed. Energy simply changes.
1. A 1250 Kg car going 23 m/s can gain how much elevation on a very tall hill if it loses no energy to friction? (27 m)
Chapter 7 The Conservation of Energy. Consider an object dropped near the surface of the earth. If the distance is small then the gravitational force.
Conservation of Energy Chapter 5 Section 3. What is Conservation? When something is conserved, it is said that it remains constant. The same holds true.
Week.  Student will: laws of conservation of energy  Demonstrate and apply the laws of conservation of energy in terms of  KineticPotential Energy.
Warm up – 1. Sogand 2. Kevin A 3. Nadya 4. Courtney 5. Ilian 6. Kevin C 7. Jack 8. Dylan 9. Alexa 10. Taylor 11. Mark 12. Kylie Find your assigned seat.
The Law of Conservation of Energy states: Conservation of Energy Energy cannot be created or destroyed Energy can be transformed from one form to another.
Chapter 6 Work and Energy.
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Unit 3 Section 3 Notes Conservation of Energy. Energy Transformations Energy is most noticeable as it transforms from one type to another. What are some.
Energy Conservation And Non-Conservative Forces. Conservation of Mechanical Energy Definition of mechanical energy: (8-6) Using this definition and considering.
6-4: Conservative and Nonconservative Forces The gravitational force has an interesting property that when an object is moved from one place to another,
Sect. 6-5: Conservative Forces. Conservative Force  The work done by that force depends only on initial & final conditions & not on path taken between.
Conservation of Mechanical Energy. Introduction “The laws of conservation are the cornerstone of physics.”
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Reading and Review. A mass attached to a vertical spring causes the spring to stretch and the mass to move downwards. What can you say about the spring’s.
Conservation of Energy
Conservation of Energy IT’S THE LAW. Lifting a Ball When you lift a ball to a certain height you do work on it. When you lift a ball to a certain height.
Chapter 6 Work and Energy 6.1 – Work Work Formula & Units Positive & Negative Work 6.2 – Work-Energy Theorem & Kinetic Energy KE Formula & Units 6.3 –
Last Thoughts on Work Work can be done by friction Friction always opposes motion so the work it does is usually negative. (exceptions are like conveyor.
Work - Work is calculated by multiplying the force applied by the distance the object moves while the force is being applied. W = Fs.
6-4: Conservative and Non-conservative Forces A force is a conservative force if the net work it does on a particle moving around any closed path, from.
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.
Potential Energy and Conservation of Energy
Mechanical Energy What is it? What makes it change?
Work&EnergyWork&Energy. 4.1 Work Done by a Constant Force.
Wednesday June 15, PHYS , Summer I 2005 Dr. Andrew Brandt PHYS 1443 – Section 001 Lecture #9 Wednesday June 15, 2005 Dr. Andrew Brandt Lightning.
Chapter 5.2. What do you think? What is meant when scientists say a quantity is conserved? Describe examples of quantities that are conserved. Are they.
Examples: Mechanical Energy Conservation
Work, Power & Energy How do they relate? (Stone, Ebener, Watkins)
Energy Physics 4 th Six Weeks. What is Energy? Energy is defined as the ability to produce a force. Energy is also defined as the ability to cause a change.
Systems and energy pg. 43. Objectives Define a physical system. Calculate the mechanical energy of a physical system. Demonstrate and apply the law of.
Conservation of Energy IT’S THE LAW. Lifting a Ball When you lift a ball to a certain height you do work on it. When you lift a ball to a certain height.
Unit 5 - Work and Energy CHAPTER 8 CONCEPTUAL PHYSICS BOOK CHAPTER 6 PHYSICS BOOK.
Class WORK 4/28/16 Throughout the PowerPoint ( review of Energy there were 7 questions Follow the PowerPoint lecture to answer the questions. The 7 questions.
PHY 101: Lecture Work Done by a Constant Force
Unit 7 – Work, Energy, and Power CHAPTER 8 CONCEPTUAL PHYSICS BOOK.
Conservation of Energy Chapter 13.4 Notes. Energy Transformations Energy readily changes from one form to another For example, think about when you ride.
Dissipative Forces. Reality? In reality, non-conservative forces cannot be ignored: friction really does act Dissipative force is one that reduces the.
Work-Energy Relationship Already understand that lifting an object will increase the object’s gravitational potential energy. W=ΔPE= mgΔh No friction.
Work & Energy Review.
1a. Positive and negative work
Chapter 5.3 Review.
Aim: How is energy Conserved?
Instructor: Dr. Tatiana Erukhimova
6 8 5 Energy Breakout Solutions 750 J 1500 W 225 N 2700 J
6 8 5 Energy Breakout Solutions 750 J 1500 W 225 N 2700 J
Mechanical Energy.
Group 1 Group 2 Group 3 Group 4 61 m 35 m 52 m 35 m 63 m 40 m 54 m
Group 1 Group 2 Group 3 Group 4 61 m 35 m 52 m 35 m 63 m 40 m 54 m
In this section you will:
Presentation transcript:

General Physics I: Day 17 Conservation of Energy & Energy Diagrams

Using Energy Diagrams Tool for visualizing how energy is transformed Example: Object oscillating on a spring

WarmUp: Adding Kinetic A truck initially at rest at the top of a hill is allowed to roll down. At the bottom, its speed is 14 m/s. Next, the truck is again rolled down the hill, but this time it does not start from rest. It has an initial speed of 14 m/s at the top before it starts rolling down the hill. How fast is it going when it gets to the bottom? ~24% → 14 m/s ~9% → 17 m/s ~18% → 20 m/s ~9% → 24 m/s ~40% → 28 m/s True if no energy were added (flat). 2x the energy means… 2x the speed?

An object hangs motionless from a spring An object hangs motionless from a spring. Think about the sum of the elastic potential energy of the spring and the gravitational potential energy of the object and Earth ( 𝑈 Spr +𝑈 g ). When the object is pulled down and held, this sum increases. stays the same. decreases.

Worked-Example: Spring Safety System Suppose the system does fail when the car is at an elevation of 25 meters. If the 600-kg car is carrying six 100-kg passengers, (a) how fast is the car moving when it connects with the spring and (b) how much does the spring compress when it finally stops the car? Mcar = 600 kg Mpassengers = 600 kg k = 36 kN/m h = 25 m vmax=? xspring = ?

Worked-Example: Spring Safety System

Worked-Example: Spring Safety System

Worked-Example: Spring Safety System

Worked-Example: Spring Safety System

Sample Problem (tricky, but cool) A small cap is placed on top of a smooth inverted spherical mixing bowl (as shown on the board). If the cap is nudged slightly, and we ignore friction, at what height will the cap leave the surface of the bowl? mg cos O = mv2/r → v2 = rg cos O mgr = ½ m v2 + mgr cos O → cos O = 2/3 Thus h = 2/3 r

Warm-Up: Coaster A real-world roller coaster is shown. A coaster car is released at point A and coasts without external power. Friction is not negligible in the real world. Does the roller coaster have the same mechanical energy at points B and C? ~33% → Yes ~67% → No Is the total energy conserved during the coaster ride? ~77% → Yes ~23% → No

Warm-Up: Coaster Give a qualitative statement about what forms the energy has when it is halfway down the hill after B. ~17% → Described 𝐾, 𝑈𝑔 and 𝑈 int ~42% → Left out 𝑈𝑔 ~17% → Left out 𝑈 int generated by friction ~17% → Left out 𝐾 ~17% → Described energy “lost” to friction ~8% → Described energies that don’t exist

Warm-Up: Coaster Conceptual miss-steps “C) force energy, potential energy” “c. The energy is still there. It turns into different energies: kinetic and potential.” “c. Some of the energy is lost due to friction and air resistance. The total energy it had at the beginning is not equal to the total after it reached point C.” Watch out for “potential energy” is too vague. Energy is never lost. It has to be there somewhere.

Warm-Up: Coaster “a) No, because Emech = U + K, we know that U is dependent upon the height per the equation U = ugh. So the coaster will have different mechanical energies at points B and C because they are different heights. b) The total energy is conserved but the mechanical energy is not conserved because the sum of KE and PE constantly decreases due to friction.”

Warm-Up: Coaster “a)For mechanical energy solely, yes. At the roller coaster hits points B and C, it has a relationship between potential energy and kinetic energy. 100% PE occurred at Point A, while at the other points the car converts some KE to PE as it climbs each hill. b)Yes, it is continuously converted between potential, kinetic, and internal/non-conservative energies (is friction and air resistance external or internal?) c)U[potential],U[internal], K”

Conservation of Energy! If we only allow conservative forces (quite limited): What if we allow other forces? They can appear in two ways:

Applying Conservation Energy Choose a system! Choose an initial and final situation. Are there non-conservative forces? Do they do work on your system? Alternatively, did the internal energy of the system change? Write down knowns and unknowns for initial and final potential and kinetic energies. Go:

Empire State Penny: If you drop a penny from the top of the Empire State Building (373 m), how fast will it be going at the bottom? First, lets ignore air resistance (a horrible approximation): 60 m/s 86 m/s 7300 m/s

Empire State Penny: A real penny (2 Empire State Penny: A real penny (2.5 g after 1982) has a terminal velocity. One empirical measurement gave 25 mph (11 m/s). How much thermal energy is created as the penny falls from the top of the Empire State Building (373 m) down to the pavement below? 9.0 J 9.1 J -9.1 J 9000 J

Friction & 𝐸 mech. Someone says: “friction causes a loss of mechanical energy”. True? Lots of counter-examples. Often this is about how we define our system. Static friction can do positive or negative work: Sit in the back of a truck, change speed (+ or –). If we choose our system poorly, even kinetic friction can increase Emech.: Pulling a table cloth out from under dishes. Motorcylce tablecloth video http://www.youtube.com/watch?v=KcSwxT_z6io

A child gets on a shallow playground slide A child gets on a shallow playground slide. After pushing himself to get started down the slide he slides at a constant speed all the way to the bottom. Compare the change in gravitational potential energy of the child to the work done on the child by non-conservative forces. 𝑊𝑓 is greater than Δ𝑈𝑔 𝑊𝑓 is less than Δ𝑈𝑔 𝑊𝑓 is equal to Δ𝑈𝑔

Coming up… Tuesday (10/21) → 8.1 – 8.2 WarmUp due Monday by 10:00 PM (w/Image) Ch. 7 Homework due Sunday by 11:59 PM