Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.

Slides:



Advertisements
Similar presentations
Review Chap. 7 Potential Energy and Energy Conservation
Advertisements

Energy Conservation 1. Mechanical energy conservation For closed isolated system 2. Open system 3. Conservative and nonconservative forces Forces such.
Physics 218, Lecture XV1 Physics 218 Lecture 15 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 24.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 18.
Chapter 8: Potential Energy and Conservation of Energy.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 21.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 14.
Basic Physics Velocity versus Speed Newton’s 2 nd Law Gravity Energy Friction as Non-conservative Force.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 24.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 16.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 21.
Physics 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV.
Instructor: Dr. Tatiana Erukhimova
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 42.
Chapter 7 All forces are CONSERVATIVE or NON-CONSERVATIVE.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 10.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 6,7.
Instructor: Dr. Tatiana Erukhimova
Nobel Prize in Physics 2008 Yoichiro Nambu Makoto Kobayashi Toshihide Maskawa "for the discovery of the mechanism of spontaneous broken symmetry in subatomic.
Physics 218, Lecture XII1 Physics 218 Lecture 12 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 27, 28.
LCROSS crashes into the Moon. Image credit: NASA.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 13.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Sections 801, 802, 803 Lecture 7.
Physics 218, Lecture XI1 Physics 218 Lecture 11 Dr. David Toback.
Physics 218 Lecture 11 Dr. David Toback Physics 218, Lecture XI.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
2D case: If or then 2 or 3D cases: Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
Chapter 7: Kinetic Energy and Work. Energy and Work Kinetic energy Work done by a constant force Work–kinetic energy theorem.
Physics 218 Lecture 15 Dr. David Toback Physics 218, Lecture XV.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 20.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 27.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
Physics 111: Elementary Mechanics – Lecture 7 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 9.
2D case: If or then 2 or 3D cases: Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is.
Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)
Chapter 8 Potential Energy. Potential energy is the energy associated with the configuration of a system of objects that exert forces on each other This.
2008 Physics 2111 Fundamentals of Physics Chapter 8 1 Fundamentals of Physics Chapter 8 Potential Energy & Conservation of Energy 1.Potential Energy 2.Path.
Potential Energy ~March 1, 2006.
Chapter 8 Conservation of Energy Introduction: Our approach Conservative and non-conservative forces Potential Energy Mechanical Energy and its conservation.
Ideas about Work and Energy What exactly is energy?
Work and Energy. Scalar (Dot) Product When two vectors are multiplied together a scalar is the result:
Work Readings: Chapter 11.
Work, Energy and Power Ms Houts AP Physics C Chapters 7 & 8.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 16, 17, 18.
Problem 3 p. 45 Electric potential on ring’s axis From Chapter 2:
Instructor: Dr. Tatiana Erukhimova
Mechanics Review – SEMESTER 1
قطار التعرج مجلس أبوظبي للتعليم منطقة العين التعليمية
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
ماذا نعني بأن الطاقة كمية محفوظة؟!
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Electricity and Magnetism
Electricity and Magnetism
Fundamentals of Physics School of Physical Science and Technology
Presentation transcript:

Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22

Examples Strategy: write down the total mechanical energy, E, E = K + U at the initial and final positions of a particle:

Then use or

A gun shoots a bullet at angle θ with the x axis with a velocity of magnitude V m. What is magnitude of the velocity when the bullet returns to the ground? How high it will go?

L H Spring constant is k; L, H, m are given How close the block will get to the floor? y=0

Conservative Forces If there are only conservative forces in the problem, then there is conservation of mechanical energy Conservative: Can go back and forth along any path and the potential energy and kinetic energy keep turning into one another –Good examples: Gravity and Springs Non-Conservative: As you move along a path, the potential energy or kinetic energy is turned into heat, light, sound etc… Mechanical energy is lost. –Good example: Friction (like on Roller Coasters)

Law of Conservation of Energy Mechanical Energy NOT always conserved If you’ve ever watched a roller coaster, you see that the friction turns the energy into heating the rails, sparks, noise, wind etc. Energy = Kinetic Energy + Potential Energy + Heat + Others… –Total Energy is what is conserved! K 1 +U 1 = K 2 +U 2 +E Heat…

Total Energy is what is conserved! K 1 +U 1 = K 2 +U 2 +E Heat …

Initial E 1 =KE 1 +U 1 …

Final E 2 =KE 2 +U 2 Mechanical energy is lost! What about the total energy? IT IS CONSERVED!

or

If or then 2 or 3D cases:

Several dimensions: U(x,y,z) Compact notation using vector del, or nabla: Another notation: Partial derivative is taken assuming all other arguments fixed

Geometric meaning of the gradient Direction of the steepest ascent; Magnitude : the slope in that direction Direction of the steepest descent Magnitude : the slope in that direction

Potential Energy Diagrams For Conservative forces can draw energy diagrams Equilibrium points –Motion will move “around” the equilibrium –If placed there with no energy, will just stay (no force)

Stable vs. Unstable Equilibrium Points The force is zero at both maxima and minima but… –If I put a ball with no velocity there would it stay? –What if it had a little bit of velocity?

Have a great day! Reading: Chapter 9 Hw: All Chapter 9 problems and exercises