Escape velocity The condition for escape is to have KE > U Far from earth, g decreases so U = mgh.

Slides:



Advertisements
Similar presentations
Conservation of Energy
Advertisements

Work Done by a Constant Force
ConcepTest Clicker Questions
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Gravitational potential energy. Conservation of energy
AP Physics C I.C Work, Energy and Power. Amazingly, energy was not incorporated into physics until more than 100 years after Newton.
An object is released from rest on a planet that
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 mechanical energy Lecture Conservation of Mechanical Energy Under the influence of conservative forces only (i.e. no friction or.
Adv Physics Chapter 5 Sections 3 & 4.
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 231 INTRODUCTORY PHYSICS I
1a. Positive and negative work
Work and Energy Definition of Work Kinetic Energy Potential Energy
Chapter 6 Work and Energy. 6.1 Work Done by a Constant Force.
Chapter 6 Work and Energy. 6.1 Work Done by a Constant Force.
Physics 6A Work and Energy examples Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Chapter 6 Work and Energy. Main thrust Work done by a constant force –Projection, Scalar product (force that result in positive work). –negative work?,
Chapter 5 Work and Energy. Force, displacement  WORK.
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Work, Energy & Power AP Physics 1. There are many different TYPES of Energy. Energy is expressed in JOULES (J) Energy can be expressed more specifically.
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
AP Physics C I.C Work, Energy and Power. Amazingly, energy was not incorporated into physics until more than 100 years after Newton.
Units: 1Newton . 1 meter = 1 joule = 1J
Conservation of mechanical energy
Copyright © 2010 Pearson Education, Inc. Chapter 8 Potential Energy and Conservation of Energy.
Energy Conservation And Non-Conservative Forces. Conservation of Mechanical Energy Definition of mechanical energy: (8-6) Using this definition and considering.
Sect. 6-5: Conservative Forces. Conservative Force  The work done by that force depends only on initial & final conditions & not on path taken between.
Chapter 6 Notes. Chapter Work  Work is equal to the product of the magnitude of the displacement times the component of the force parallel to the.
Conservative and non-conservative forces Potential energy Total mechanical energy Energy conservation Lecture 11: Potential energy.
Chapter 6 Work and Energy. Force,displacement  WORK.
Work and Energy.
Energy. WORK ENERGY THEOREM For an object that is accelerated by a constant force & moves in the same direction… Lets derive this…
Work - Work is calculated by multiplying the force applied by the distance the object moves while the force is being applied. W = Fs.
REVISION NEWTON’S LAW. NEWTON'S UNIVERSAL GRAVITATION LAW Each body in the universe attracts every other body with a force that is directly proportional.
332 – UNIT 6 WORK & ENERGY.
Chapter-6 Work and Energy Work Done by a Constant Force Work is done when a force F pushes a car through a displacement s. Work = Force X Displacement.
Wednesday, Mar. 12, 2008 PHYS , Spring 2008 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #15 Wednesday, Mar. 12, 2008 Dr. Jaehoon Yu Work done.
Ch 6. Work and Energy Example 1 Suitcase-on-Wheels Find work done if force is 45.0-N, angle is 50.0 degrees, and displacement is 75.0 m.
Chapter-6 Work and Energy
Chapter-6 Work and Energy Work Done by a Constant Force.
Thursday, Oct. 2, 2014PHYS , Fall 2014 Dr. Jaehoon Yu 1 PHYS 1443 – Section 004 Lecture #12 Thursday, Oct. 2, 2014 Dr. Jaehoon Yu Work-Kinetic.
Everyone grab a small whiteboard and a dry erase marker.
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.
Section 6-3 Gravitational Potential Energy. Warm-Up #1 A sailboat is moving at a constant velocity. Is work being done by a net external force acting.
Today: (Ch. 6 & Review)  Work and Energy  Review (Chapter 1 to 5)
Section 6-2 The Work Energy Theorem and Kinetic Energy.
PHY 101: Lecture Work Done by a Constant Force
Work, energy, and power. If the net force is in the direction of motion work is positive If the net force is in the direction opposite that of motion.
Kinetic Energy (E K ) Energy an object has due to its motion Potential Energy (E P ) Energy an object has due to its position/location Mechanical Energy.
Work-Energy Relationship Already understand that lifting an object will increase the object’s gravitational potential energy. W=ΔPE= mgΔh No friction.
ENGINEERING PHYSICS SEMESTER /2012. ENGINEERING PHYSICS SUB-CHAPTERS: ● Work and standard units ● Power concept & Power Calculation ● Kinetic energy.
PHY 102: Lecture 4A 4.1 Work/Energy Review 4.2 Electric Potential Energy.
Miscellaneous Mechanics
Conservation of Mechanical Energy
Potential Energy and Conservation of Energy
List five sources of energy that might be able to produce
1a. Positive and negative work
Chapter 7 Work and Energy
Work -   Work is calculated by multiplying the force applied by the distance the object moves while the force is being applied.   W = Fs.
Work Done by a Constant Force
Work Done by a Constant Force
Acceleration due to Gravity
System: ball Surroundings: Earth Let distance fallen = h.
PHYS 1441 – Section 001 Lecture # 9
Work Who does the most work? Definition of work in physics:
Chapter 6 Work and Energy.
Presentation transcript:

Escape velocity The condition for escape is to have KE > U Far from earth, g decreases so U = mgh

Energy and Gravity To get into orbit and object has to be launched _____ enough. The speed needed to achieve orbit is called __________ velocity. The speed needed to outright break free of a planets gravity (a.k.a. to leave orbit) is called ____________. You should be able to create formulas for these velocities using Physics formulas we have already learned….. fast orbital Escape velocity

Conservative Forces A force is called conservative if ……….. …..work is independent of path, and depends only on position. When it gets back to the same spot, E =0. It does no net work on an object moving around a closed path. Conservative Gravity Spring Force Electric Force Nonconservative Friction Tension Normal Force Air resistance Magnetism

Conservation of Mechanical Energy Energy can not be created or destroyed, it just changes forms.

If this person starts from rest, holding the rope horizontal, swings downward and lets the rope go at the bottom, can we use conservation of energy even though there is tension on him? Yes, because T is perpendicular to the direction of motion and does no work. If he is 4 m from the surface of the water when he jumps and 0.8 m when he lets go, find v f.

Find v f 46.2m/s

A 120 kg crate is on a flatbed truck that is moving with a=+1.5m/s 2. The crate does not slip as the truck covers a distance of d = 65m. What is the total work done by all forces acting on the crate?

A 58 kg skier is coasting down a 25 0 slope. A kinetic frictional force F k = 70N opposes her motion. Near the top of the slope her speed is v o = 3.6 m/s. Determine her speed v f at a point that is displaces 57m down the hill.

1.Since work is force x distance find the ΣF 2.How much of it is in the direction of motion? 3.Multiply that part of the force by the distance it is applied over. 9700J