Consider the meter stick. It is an extended object. In other words we can’t simply treat it as a particle. For example if we twirl it, each piece moves.

Slides:



Advertisements
Similar presentations
AP Physics C Mechanics Review.
Advertisements

Uniform Circular Motion
R1-1 Physics I Review 1 Review Notes Exam 1. R1-2 Definitions.
Conservation of Angular Momentum 8.01 W10D2 Young and Freedman:
Linear Momentum and Collisions
Center of Mass and Momentum Lecture 08 Monday: 9 February 2004.
Kinematics, Momentum and Energy BU Photon Outreach December 14, 2010.
Law of Conservation of Momentum. If the resultant external force on a system is zero, then the vector sum of the momentums of the objects will remain.
Collisions & Center of Mass Lecturer: Professor Stephen T. Thornton
Center of Mass and Linear Momentum
Chapter 11 Angular Momentum.
Chapter 11: Forces 11.1: Forces change motion
Linear momentum and Collisions
Chapter 3 Forces.
Linear Momentum and Collisions
Conservation of Angular Momentum 8.01 W10D2
Lecture Outlines Chapter 9 Physics: Principles and Problems.
Chapter 7 Systems of particles
Newton’s Third Law of Motion
Center of Mass. Newtons 2 nd Law and Momentum 1.Forces cause changes in an object’s momentum. That is, forces cause the object’s velocity to change over.
Notes: Chapter 11.3 Newton’s Third Law of Motion and Momentum.
Fundamentals of Rocket Stability It’s (not) rocket science!
Force Newton’s Laws 1 First Law - Inertia Second Law – Force and Acceleration Third Law – Action and Reaction Introduction.
The coordinates of the centre of mass are M is the total mass of the system Use the active figure to observe effect of different masses and positions Use.
Circular Motion. Uniform Circular Motion Motion of an object at constant speed along a circular path.
CIRCULAR MOTION. WHAT IS UNIFORM CIRCULAR MOTION The motion of an object in a circle at constant speed. However, direction and therefore velocity are.
Conservation of Angular Momentum 8.01 W11D2 Fall 2006.
Chapter 8 Momentum and Collisions. Linear Momentum The linear momentum of a particle or an object that can be modeled as a particle of mass m moving with.
Circular Motion. PhET Lady Bug Motion Think about this Click “Show Both” at the top, and “Circular” at the bottom Watch the following and comment: Which.
Center of Mass. Up to now, we’ve been mainly concerned with the motion of single (point) particles. To treat extended objects, we’ve implicitly approximated.
Objectives Define force as part of an interaction. (6.1)
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.
Chapter 11 Rotational Mechanics. Recall: If you want an object to move, you apply a FORCE.
Dr. Michael Cooke Dr. David Schmitz Fermilab
Newton’s Laws AP Physics C. Basic Definitions  Inertia  property of matter that resists changes in its motion.  Mass  measurement of inertia  Force.
Dynamics of Uniform Circular Motion Uniform Circular Motion Centripetal Acceleration Centripetal Force Satellites in Circular Orbits Vertical Circular.
Chapter 7 Linear Momentum.
Linear Momentum. Linear momentum describes motion in which the center of mass of an object or system changes position. We call motion where the c.o.m.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 9 Physics, 4 th Edition James S. Walker.
Where is the center or mass of a wrench?  Center-of-Mass A mechanical system moves as if all of its mass were concentrated at this point A very special.
Unbalanced Forces. Topic Overview A force is a push or a pull applied to an object. A net Force (F net ) is the sum of all the forces on an object (direction.
/ A force is a push or a pull that changes motion. / Forces transfer energy to an object. / The force of gravity causes objects to have weight. / The.
Momentum and Impulse 8.01 W06D2 Associated Reading Assignment: Young and Freedman:
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: Extended objects Center of mass Torque.
1 Two-Dimensional Collision, Before collision Particle 1 is moving at velocity v 1i and particle 2 is at rest In the x-direction, the initial momentum.
Newton’s Laws of Motion Chapter 6. Newton’s Laws of Motion “Law of inertia” First Law of Motion INERTIA - tendency of an object to resist a change in.
Ch. 3 & 4 Motion & Forces VI. Action and Reaction  Newton’s Third Law  Momentum  Conservation of Momentum.
Notes: Chapter 11.3 Newton’s Third Law of Motion and Momentum.
1 6. Center of mass, Collisions 6.1. The center of mass To describe the motion of a system of particles (also for their continuous distribution – a solid.
PHY 151: Lecture 6A 6.1 Newton’s Law of Universal Gravity 6.2 Gravitational Formula 6.3 Extending Particle in Uniform Circular Motion Model.
Physical Science Chapter Four Acceleration Momentum Newton Gravity Free Fall Air Resistance.
If an asymmetrical object, such as an axe, is tossed, its motion seems rather complicated, but one special point moves in a simple __________ path… This.
6. Center of mass, Collisions
Center of Mass.
Newton's Third Law of Motion and Momentum
Chapter-9 Center of Mass and Linear Momentum
Forces.
Newton’s Third Law Chapter 10 Section 4.
Newton’s Second Law of Motion
The Conservation of Momentum Section 9.2
PHYSICS 103: Lecture 13 Review of HW Momentum Agenda for Today:
Acceleration- the rate at which velocity changes over time
Momentum.
6.3 Newton's Third Law pp
Chapter 2-4 Newton’s Third Law.
Newton’s Third Law of Motion
Section 3 Newton’s Third Law p. 360
(a) (9.1) (a) (9.2) (b) Figure 9-2 (a) Two particles of masses m1 and m2 are separated by distance d. The dot labeled com shows the position of the.
Presentation transcript:

Consider the meter stick. It is an extended object. In other words we can’t simply treat it as a particle. For example if we twirl it, each piece moves in a different radius circle with different speeds!

Imagine that this meter stick is moving as well as spinning. Now the motion of each piece of the meter stick is even more complicated!

However, there is one point on the meter stick that moves just like a simple particle!

This point is also special because it is the point on which the meter stick would balance.

In fact, if we threw the meter stick through the air, this point would act just like a projectile, it would follow a parabolic path. Hence, this point acts as if all of the mass of the object is concentrated at that point.

Center of Mass – the point in an object or system of particles which acts as a simple particle – the point at which all of the mass of an object or system of particles can be thought to be concentrated – the balancing point – the point that moves as if all of the external forces were applied at that point Rotating Projectile

The center of mass need not lie within an object. Line of Symmetry

Let’s see how this applies to explosions and collisions between two carts. Momentum of the Center of Mass

As you saw in the demos, if there are no external forces, then the momentum of the center of mass point does not change! For this system of two carts there could be two types of forces. 1. Forces between the carts. 2. External forces on the carts from outside the system. However, by Newton’s Third Law, any force between the two carts would always have an equal and opposite pair and would therefore sum to 0!