Physics 1A, Section 2 November 11, 2010. Translation / Rotation translational motionrotational motion position x angular position  velocity v = dx/dt.

Slides:



Advertisements
Similar presentations
Angular Quantities Correspondence between linear and rotational quantities:
Advertisements

R2-1 Physics I Review 2 Review Notes Exam 2. R2-2 Work.
Angular Momentum The vector angular momentum of the point mass m about the point P is given by: The position vector of the mass m relative to the point.
Comparing rotational and linear motion
1. 2 Rotational Kinematics Linear Motion Rotational Motion positionxangular position velocityv = dx/dtangular velocity acceleration a = dv/dt angular.
READING QUIZ angular acceleration. angular velocity. angular mass.
Angular Momentum (of a particle) O The angular momentum of a particle, about the reference point O, is defined as the vector product of the position, relative.
Physics 1901 (Advanced) A/Prof Geraint F. Lewis Rm 557, A29
ENGR 215 ~ Dynamics Section 17.1
Chapter 12: Rolling, Torque and Angular Momentum.
Chapter 10: Rotation. Rotational Variables Radian Measure Angular Displacement Angular Velocity Angular Acceleration.
Summer School 2007B. Rossetto1 8. Dynamics of a rigid body  Theorems r CM : location of the center of mass referred to an inertial frame /Oxyz v CM :
Physics 2211: Lecture 38 Rolling Motion
Department of Physics and Applied Physics , F2010, Lecture 20 Physics I LECTURE 20 11/21/10.
Physics 218 Lecture 18 Dr. David Toback Physics 218, Lecture XVIII.
Physics 111: Elementary Mechanics – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
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.
Rolling. Rotation and Translation  A rolling wheel is moving forward with kinetic energy.  The velocity is measured at the center of mass. K CM = ½.
Rigid Bodies Rigid Body = Extended body that moves as a unit Internal forces maintain body shape Mass Shape (Internal forces keep constant) Volume Center.
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.
PHY PHYSICS 231 Lecture 19: More about rotations Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom Demo: fighting sticks.
I G is the “mass moment of inertia” for a body about an axis passing through the body’s mass center, G. I G is defined as: I G =  r 2 dm Units: kg-m 2.
Physics 1A, Section 2 November 15, Translation / Rotation translational motionrotational motion position x angular position  velocity v = dx/dt.
Angular Momentum. Inertia and Velocity  In the law of action we began with mass and acceleration F = maF = ma  This was generalized to use momentum:
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.
1/17/ L IAP 2006  Last Lecture  Everything you need to know about dynamics of rotation  Today  Pendulums and Kinetic Energy of rotation  Important.
PH 201 Dr. Cecilia Vogel Lecture 20. REVIEW  Constant angular acceleration equations  Rotational Motion  torque OUTLINE  moment of inertia  angular.
Rotational Dynamics. Moment of Inertia The angular acceleration of a rotating rigid body is proportional to the net applied torque:  is inversely proportional.
Advanced Rotational Dynamics for AP Physics
PHYS 218 sec Review Chap. 9 Rotation of Rigid Bodies.
Work Let us examine the work done by a torque applied to a system. This is a small amount of the total work done by a torque to move an object a small.
Copyright © 2012 Pearson Education Inc. Angular momentum Physics 7C lecture 14 Thursday November 14, 8:00 AM – 9:20 AM Engineering Hall 1200.
Physics 1210/1310 Mechanics& Thermodynamics Thermodynamics Lecture R1-7 Rotational Motion.
1 7/26/04 Midterm 2 – Next Friday (7/30/04)  Material from Chapters 7-12 I will post a practice exam on Monday Announcements.
10/22/2015A.PH 105 PH /4 ----Monday, Oct. 8, 2007 Homework: PS8 due Wednesday: conservation of energy Chapter 9: momentum Review Wednesday & Friday:
Find the moments of inertia about the x & y axes:
2008 Physics 2111 Fundamentals of Physics Chapter 10 1 Fundamentals of Physics Chapter 10 Rotation 1.Translation & Rotation 2.Rotational Variables Angular.
Rotational Motion. Angular Quantities Angular Displacement Angular Speed Angular Acceleration.
Rotational Dynamics Chapter 8 Section 3.
Rotational kinematics and energetics
Rotational Kinetic Energy An object rotating about some axis with an angular speed, , has rotational kinetic energy even though it may not have.
Classical. Special Cases of the 2 nd Law: “Recipes” 1d discussion for now. Easily generalized to 3d. Newton’s 2 nd Law equation for a particle has some.
We’re on a roll! The Physics of Rotation. Rotational Momentum and Energy Chapter 12.
Moments of Inertia Fun with math § 9.5–9.6.
Rotation of a body about an axisRIGID n FIXED Every point of body moves in a circle Not fluids,. Every point is constrained and fixed relative to all.
1 Rotation of a Rigid Body Readings: Chapter How can we characterize the acceleration during rotation? - translational acceleration and - angular.
1 Work in Rotational Motion Find the work done by a force on the object as it rotates through an infinitesimal distance ds = r d  The radial component.
Ch 9 Rotation Rotational Variables Rigid Body: definition and motion Kinetic energy of rotation and moment of inertia Parallel Axis Theorem Newton’s 2.
Tuesday 6/9 PHYS 2010 Nathalie Hoffmann University of Utah.
Chapter 11 Rotation.
Chapter 9 Rotational Dynamics
Physics 111 Lecture Summaries (Serway 8 th Edition): Lecture 1Chapter 1&3Measurement & Vectors Lecture 2 Chapter 2Motion in 1 Dimension (Kinematics) Lecture.
Physics 1A, Section 6 November 20, Section Business Homework #8 (fluid mechanics) is due Monday. –Web site has been updated. Extra T.A. office hour.
Chapter 10 Lecture 18: Rotation of a Rigid Object about a Fixed Axis: II.
Rotational Motion AP Physics C. Introduction The motion of a rigid body (an object with a definite shape that does not change) can be analyzed as the.
UNIT 6 Rotational Motion & Angular Momentum Rotational Dynamics, Inertia and Newton’s 2 nd Law for Rotation.
Physics 1A, Section 2 November 8, Quiz #3  was due 3 hours ago.
Rotational Motion.
ROTATIONAL MOTION Rotation axis: rotation occurs about an axis that does not move: fixed axis.
Rotational Equilibrium and Dynamics
Chapter 10: Rotational Motional About a Fixed Axis
Honors Physics 1 Class 12 Fall 2013
Newton’s 2nd Law for Rotation
Rotational Dynamics Torque and Angular Acceleration
Translational-Rotational Analogues
Student Evaluations.
Chapter 11 Rolling, Torque, and Angular Momentum
Rotational Motion Bookwork Assignments
Rotational Motion.
Translation-Rotation Analogues & Connections
Presentation transcript:

Physics 1A, Section 2 November 11, 2010

Translation / Rotation translational motionrotational motion position x angular position  velocity v = dx/dt angular velocity  = d  /dt acceleration a = dv/dt = d 2 x/dt 2 angular acceleration  = d  /dt = d 2  /dt 2 mass mmoment of inertia I momentum p = mv angular momentum L = I  force F = ma torque  = I  kinetic energy ½ mv 2 kinetic energy ½ I  2

Quiz Problem 25

Answer: a) T = a(mR 2 + I )/[R(R-r)] f = a( I + mrR)/[R(R-r)] b)  min = a(kR + r)/[g(R-r)] c) rolls to the right

Moment of Inertia Moments:  0 th moment: ∫dm = mass  useful 1 st moment: ∫ r dm 1/M ∫ r dm is the center of mass  useful 2 nd moment: ∫R 2 dm = moment of inertia  R is the distance from the axis of rotation  Other ways to write the integral: ∫dm = ∫  dV = ∫∫∫  dx dy dz Moment of inertia examples: Frautschi et al. Table 14.1, page 379 Parallel axis theorem: I = I CM + Md 2

Quiz Problem 41

Answer: a)  1 = 8  da 4  2 = ½  da 4  1 /  2 = 16 b)  f = 16  /17 c) No, some lost to friction. K final /K initial = 16/17

Quiz Problem 32 (collision with rotation) Optional, but helpful, to try these in advance. Monday, November 15: