1 Lecture #3 of 25 Homework #1 expectations Questions on Assignment #2 Center of Mass Defined Relation to momentum Polar and Spherical Coordinates Worked.

Slides:



Advertisements
Similar presentations
R1-1 Physics I Review 1 Review Notes Exam 1. R1-2 Definitions.
Advertisements

MOMENTUM AND COLLISIONS
Center of Mass and Linear Momentum
PHYS16 – Lecture 21 Ch. 9 Momentum and Collisions.
PHYS16 – Lecture 12 Review and Momentum October 6, 2010.
1 Lecture #9 of 24 Test advice Review problems Moment of Inertia of disk w/ hole Line Integrals Energy conservation problems Others of interest Energy.
1 Lecture #4 of 25 Review HW problem 1.9 Explain 3 in-class problems from Tuesday Angular Momentum And torque And Central force Moment of Inertia – Worked.
1 Lecture #5 of 25 Moment of inertia Retarding forces Stokes Law (viscous drag) Newton’s Law (inertial drag) Reynolds number Plausibility of Stokes law.
1 Class #7 Review previous class Kinetic Energy and moment of inertia Angular Momentum And moment of inertia And torque And Central force Moment of Inertia.
1 Lecture #2 Questions on Assignment #1? Homework Expectations /Office hours Impulse and momentum conservation Rocket propulsion Worked problems Cross-product.
1 Lecture #2 Questions on Assignment #1? Homework Expectations /Office hours Impulse and momentum conservation Rocket propulsion Worked problems Cross-product.
Department of Physics and Applied Physics , F2010, Lecture 21 Physics I LECTURE 21 11/24/10.
1 Class #6 Center of Mass Defined Relation to momentum Worked problems DVD Demonstration on momentum cons. and CM motion Angular Momentum And moment of.
PHY PHYSICS 231 Lecture 14: Collisions II: The momentum strikes back. Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom.
Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Impulse and Momentum l Today’s lecture will be a review of Chapters and l New material:
Department of Physics and Applied Physics , F2010, Lecture 18 Physics I LECTURE 18 11/15/10.
Impulse and momentum conservation Rocket propulsion Worked problems
1 Lecture #4 Angular Momentum And moment of inertia And torque And Central force Moment of Inertia Difference between it and CM Worked examples :10.
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Physics 121. Tuesday, March 4, 2008.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures
1 Class #7 of 30 Integration of vector quantities CM problems revisited Energy and Conservative forces Stokes Theorem and Gauss’s Theorem Line Integrals.
1 Class #6 Center of Mass Defined Relation to momentum Worked problems DVD Demonstration on momentum cons. and CM motion Angular Momentum And moment of.
Physics 218, Lecture XVII1 Physics 218 Lecture 17 Dr. David Toback.
1 Lecture #2 of 25 Questions on Assignment #1? Homework Expectations /Office hours/Reserve (REA Mechanics Problem Solver, ISBN $25) Impulse.
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Physics 121. Thursday, February 28, 2008.
Linear Momentum and Collisions المحاضرة العاشرة. Linear Momentum and Collisions Chapter 9.
1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.
Today: Momentum – chapter 9 11/03 Finish momentum & review for exam 11/8 Exam 2 (5 – 8) 11/10 Rotation 11/15 Gravity 11/17 Waves & Sound 11/22 Temperature.
Kinematics What rules govern an objects motion?. Answer Me!!! List three things that come to mind when you hear the term motion? After creating your list,
Wednesday, Sept. 8, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #5 Wednesday, Sept. 8, 2004 Dr. Jaehoon Yu 1.One Dimensional.
Linear Momentum. 5-1 Linear Momentum Linear Momentum, p – defined as mass x velocity The unit is kg·m/s A quantity used in collisions So a small object.
Momentum and Collisions Unit 5, Presentation 1. Momentum  The linear momentum of an object of mass m moving with a velocity is defined as the product.
Momentum An object of mass m traveling at velocity has a linear momentum (or just momentum),, given by Units have no special name: kg-m/s With no net force.
Impulse and Momentum Collisions and conservation of momentum
Linear Momentum AP Physics 2. Definitions Second law, again.
Chapter 8 Impulse and Momentum THE LINEAR MOMENTUM  Momentum = mass times velocity  “Think of it as inertia in motion” Units - kg m/s or sl ft/s.
Proportionality between the velocity V and radius r
Linear Momentum October 31, Announcements Turn in homework due today:  Chapter 8, problems 28,29,31  Next week, W-F, Rocket Project.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 9 Physics, 4 th Edition James S. Walker.
Ch 8 : Conservation of Linear Momentum 1.Linear momentum and conservation 2.Kinetic Energy 3.Collision 1 dim inelastic and elastic nut for 2 dim only inellastic.
Spring 2002 Lecture #11 Dr. Jaehoon Yu 1.Center of Mass 2.Motion of a System of Particles 3.Angular Displacement, Velocity, and Acceleration 4.Angular.
Solution: Electricity: 1 kw-hr = (1 x10 3 J/s)(3.6 x10 3 s) = 3.6 x10 6 J 1 kw-hr = (1 x10 3 J/s)(3.6 x10 3 s) = 3.6 x10 6 J E/$ = 3.6 x10 6 /$0.1 = 3.6.
Linear Momentum. 5-1 Linear Momentum Linear Momentum, p – defined as mass x velocity The unit is kgm/s A quantity used in collisions So a small object.
Momentum. The p = m = mass v = velocity Unit: Vector Direction of momentum is determined by the direction of the.
Monday, Sept. 20, 2010PHYS , Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #5 Monday, Sept. 20, 2010 Dr. Jaehoon Yu One Dimensional.
Equations: Conservation of Momentum: Vocabulary:. Law of conservation of momentum. Elastic collision. Inelastic collision. Perfectly inelastic collision.
Monday, Nov. 3, 2008PHYS , Fall 2008 Dr. Jaehoon Yu 1 PHYS , Fall 2008 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #15 Monday, Nov.
Warm up A 3.00 kg crate slides down a 7 m ramp. The height of the ramp is 5 m off the ground. The velocity of the crate at the bottom of the ramp is 5.
1 The Center of Mass Finding the Center of Mass by Integration (Omit)
Wednesday, Feb. 4, 2004PHYS , Spring 2004 Dr. Jaehoon Yu 1 PHYS 1441 – Section 004 Lecture #5 Wednesday, Feb. 4, 2004 Dr. Jaehoon Yu Chapter two:
PHY 101: Lecture The Impulse-Momentum Theorem 7.2 The Principle of Conservation of Linear Momentum 7.3 Collision in One Dimension 7.4 Collisions.
Momentum & Impulse Day #1: Introduction HW #7. Momentum & Collisions: Define Momentum: Momentum, p, is defined as the product of mass and velocity. Units:
Momentum.
Today: (Ch. 7) Momentum and Impulse Conservation of Momentum Collision.
6. Center of mass, Collisions
Momentum And Impulse.
Chapter 9 Objectives: 1) Define momentum.
Cylindrical – Polar Coordinates
ATOC 4720 class31 1. Coordinate systems 2. Forces.
Longitude and Latitude
Momentum and Impulse.
Chapter 5 Momentum.
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
Semester Review Jeopardy.
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
Stacked Ball Drop Define momentum: resistance to give up kinetic energy, quantity of motion of a moving body.
Linear Momentum and Collisions.
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
Physics I LECTURE 21 12/2/09.
Momentum and Its Conservation
Presentation transcript:

1 Lecture #3 of 25 Homework #1 expectations Questions on Assignment #2 Center of Mass Defined Relation to momentum Polar and Spherical Coordinates Worked problems DVD Demonstration on momentum cons. and CM motion :10

2 Center of Mass Center of Mass and Center of gravity happen to be equivalent For a multi-particle discrete mass-distribution For a continuous mass-distribution. :15

3 Linear Momentum and CM :20

4 Spherical Coordinates and Earth Radius on surface of earth is fixed, so two coordinates are sufficient to specify any point on Earth Coordinates are: Latitude (North-south)  “Co-latitude” is 90 degrees minus latitude Longitude (East-West) Spherical coordinates “Phi” or “Fee”  – East-west same as longitude “Theta”  – North-south, same as Colatitude   is 0 at north pole, 180 at south pole, 90 at equator For third dimension, add “r” (radius) :25

5 Cylindrical and Spherical Coordinates :30

6 Impulse II -- Problem #L2-3 “Another car crash” James and Joan are partly recovered from their previous injuries, and haven’t learned from their experience. They are drinking Jack Daniels and not wearing seat- belts. James’ vehicle has velocity vector Joan’s vehicle has Both vehicles’ mass=M. Both people’s mass=70 kg. Solve for case of inelastic and elastic collisions of vehicles. Joan has an airbag in her vehicle. It takes her 100 millisec to reduce her velocity relative to her vehicle to zero. James stops 5 millisec after impacting the steering wheel. What impulse does each person experience? What is average force for each? How many “g’s” do they feel. :40

7 Worked Example L3-1 – Discrete masses Given m 1 to m 10 m  = m m  = 3m y x y x O1O1 O2O2 1 unit 2 units Calculate Given origin O1O1 For homework given O 2 :50

8 Worked Example L3-2 – Continuous mass Given quarter circle with uniform mass-density  and radius 2 km: Calculate M total Write r in polar coords Write out double integral, both r and phi components Solve integral  r O1O1 2 km Calculate Given origin O1O1 :60

9 Lecture #3 Wind-up. Office hours Today 2:30-4, tomorrow 4-5:30. Homework problems in Taylor, Handout, Galileo problem – check the web. Second homework due in class Thursday 9/5 :72