Aim: How do we explain rotational kinematics?

Slides:



Advertisements
Similar presentations
PHYS 1441 – Section 002 Lecture #20 Wednesday, April 10, 2013 Dr. Jaehoon Yu Equations of Rotational Kinematics Relationship Between Angular and Linear.
Advertisements

Rotational Energy. Rigid Body  Real objects have mass at points other than the center of mass.  Each point in an object can be measured from an origin.
Rotation of a Rigid Body (Chapter 10)
Measuring Rotational Motion
Wednesday, Oct. 27, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Fundamentals on Rotational Motion 2.Rotational Kinematics 3.Relationship between angular.
Measuring Rotational Motion
Cutnell/Johnson Physics 7th edition
Section 8-2: Kinematic Equations Recall: 1 dimensional kinematic equations for uniform (constant) acceleration (Ch. 2). We’ve just seen analogies between.
Circular Motion Tangential & Angular Acceleration
Angular Mechanics - Kinematics Contents:
From Ch. 5 (circular motion): A mass moving in a circle has a linear velocity v & a linear acceleration a. We’ve just seen that it also has an angular.
Formative Assessment. 1. A bicycle going 13.5 m/s has cm diameter wheels. What is the angular velocity of the wheels in rad/s? in RPM? (39.7 rad/sec,
Chapter 7 Rotational Motion.
Angular Motion, General Notes
Finish Momentum Start Spinning Around
Rotational Kinematics
Chapter 8 Rotational Kinematics. 8.1 Rotational Motion and Angular Displacement In the simplest kind of rotation, points on a rigid object move on circular.
Ch 8. Rotational Kinematics
Chapter 8 Rotational Kinematics. The axis of rotation is the line around which an object rotates.
Physics 111 Practice Problem Statements 09 Rotation, Moment of Inertia SJ 8th Ed.: Chap 10.1 – 10.5 Contents 11-4, 11-7, 11-8, 11-10, 11-17*, 11-22, 11-24,
STARTER Consider two points, A and B, on a spinning disc. 1. Which point goes through the greatest distance in 1 revolution? 2. Which point goes through.
Rotational Motion 2 Coming around again to a theater near you.
Wednesday, Nov. 7, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #18 Wednesday, Nov. 7, 2007 Dr. Jae Yu Rolling Motion.
Chapter 8: Rotational Kinematics Essential Concepts and Summary.
Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.
Wednesday, Apr. 15, 2009PHYS , Spring 2009 Dr. Jaehoon Yu PHYS 1441 – Section 002 Lecture #19 Wednesday, Apr. 15, 2009 Dr. Jaehoon Yu Relationship.
Angular Motion Objectives: Define and apply concepts of angular displacement, velocity, and acceleration.Define and apply concepts of angular displacement,
ConcepTest 7.1aBonnie and Klyde I Bonnie Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim.
Wednesday, July 2, 2014PHYS , Summer 2014 Dr. Jaehoon Yu 1 PHYS 1441 – Section 001 Lecture #16 Wednesday, July 2, 2014 Dr. Jaehoon Yu Rotational.
Rotational Kinematics
Circular Motion. Rotational Quantities A O r  dAdA A point on an object, located a distance r from a fixed axis of rotation, rotates in such a way that.
In mathematics and physics, a specific form of measurement is used to describe revolution and fractions of revolutions. In one revolution, a point on.
Ying Yi PhD Chapter 8 Rotational Kinematics 1 PHYS HCC.
1 Rotational Kinematics Rotational Motion and Angular Displacement Chapter 8 Lesson 3.
Cutnell/Johnson Physics 8th edition
Chapter 7 – Angular Motion Things that turn have both a linear velocity and an angular velocity.
Angular Mechanics - Radians r  s Full circle: 360 o = 2  Radians  = s/r Radians = m/m = ? TOC.
Spring 2002 Lecture #12 Dr. Jaehoon Yu 1.Motion of a System of Particles 2.Angular Displacement, Velocity, and Acceleration 3.Angular Kinematics.
Angular Motion AP Physics 1. Revolving Motion vs Rotating Motion The Earth ____________ around the Sun while _____________ around an axis. Revolving Rotating.
Rotational Motion Phys 114 Eyres. Circles: Remember T is time to go around once.
Chapter 11A – Angular Motion
Angular Mechanics - Kinematics Contents:
Rotational Motion: x v a(tangent) What is a radian?
Chapter 8 Rotational Motion.
Angular Mechanics - Centripetal and radial accel Contents:
Angular Mechanics - Kinematics Contents:
PHYS 1443 – Section 002 Lecture #17
Rotational Kinematics
Chapter 11A – Angular Motion
Rotational Kinematics
PHYS 1443 – Section 003 Lecture #12
Chapter 8 Rotational Kinematics.
Chapter 8: Rotational Motion
Rotation As you come in, please set clicker to channel 44 and then answer the following question (before the lecture starts). Quiz – You are building.
PHYS 1443 – Section 003 Lecture #16
Kinematic Equations.
Rotational Kinematics
PHYS 1441 – Section 002 Lecture #19
Chapter 11A – Angular Motion
1. Rotational Kinematics
Rotational motion AH Physics.
ANGULAR MOTION © 2007.
Chapter 7 Rotational Motion and the Law of Gravity
Rotation Kinematics.
Aim: How do we explain rotational kinematics?
Aim: How do we explain rotational kinematics?
Rotational Motion Let’s begin with Rotational Kinematics!!
Aim: How do we explain rotational kinematics?
Aim: How do we explain rotational kinematics?
Rotational Kinematics
Presentation transcript:

Aim: How do we explain rotational kinematics?

Rotational Kinematics Equations ωf=ωi + αt θf=θi +ωit +1/2αt2 ωf2=ωi2 +2α(θf-θi)

Thought Question 1 Consider again the pairs of angular positions for the rigid body listed in the previous thought questions. If the object starts from rest at the initial angular position, moves counterclockwise with constant angular acceleration, and arrives at the final angular position with the same angular speed, for which choice is the angular acceleration the highest? [a. 3 rad, 6 rad][b. -1 rad, 1 rad][c.1 rad, 5 rad] The answer is b. Looking at the equation: ωf2=ωi2 +2α(θf-θi). Since each rotation has the same final angular velocity and initial angular velocity, we see that the rotation which has the smallest change in angle, must have the greatest angular acceleration. b

Rotating wheel problem A wheel rotates with a constant angular acceleration of 3.50 rad/s2. If the angular speed is 2.00 rad/s at t = 0. Through what angles does the wheel rotate between t= 0s and t = 2s? Θ=ωit+1/2αt2=2(2)+1/2(3.5)(2)2=11 rad b)What is the angular speed of the wheel at t= 2s? ωf=ωi+αt ωf=2+3.5(2)=9.5 rad/s c)Find the angle through which the wheel rotates between t=2s and t=3s. Θ=ωit+1/2αt2 =2(3)+1/2(3.5)(3)2=21.75 rad So between 2 and 3 seconds, θ=21.75 rad-11 rad=10.75 rad 11 rad 9 rad/s 10.8 rad

Relations between rotational and translational quantities v=rω at=rα ac= v2/r = rω2

Thought Question 2 When a wheel of radius R rotates about a fixed axis, Do all the points on the wheel have the same angular speed? YES Do they all have the same tangential speed? NO If the angular speed is constant and equal to ω, describe the tangential speeds and total translational accelerations of the points located at r = 0, r=R/2, and r = R, where the points are measured from the center of wheel. At r=0, v=rω=0(0)=0 ac=rω2=r(0)2=0 At r=R/2, v=rω=(R/2)ω ac=(R/2)ω2 At r=R, v=rω=Rω ac=Rω2 Yes, no, v=rw/2 a=rw^2/2 v=rw a=rw^2

Thought Question 3 A phonograph record is rotated so that the surface sweeps past the laser at a constant tangential speed. Consider two circular grooves of information on an LP-one near the outer edge and one near the inner edge. Suppose the outer groove “contains” 1.8s of music. Does the inner groove also contain the same time interval of music? The same amount of music must be contained in each groove.

Thought Question 4 The launch area for the European Space Agency is not in Europe-it is in South America. Why? Near the equator in South America, the Earth is spinning faster than anywhere in Europe. Therefore, a space craft does not need to be accelerated to as great a speed from the equator as from Europe.

Problem 2 A disk 8.00 cm in radius rotates about its central axis at a constant rate of 1200 rev/min. Determine Its angular speed Its tangential speed at a point 3.00 cm from its center The radial acceleration of a point on the rim The total distance a point on the rim moves in 2.00s ω=1200(2π/60)= 40π rad/s or 125.6 m/s v=rω=0.03(125.6)=3.768 m/s ac=rω2=0.08(125.6)2=1,262 m/s2 ω=θ/t 125.6=θ/2 so θ= 151.2 rad d=rθ d=0.08(151.2)=12.096 m a)126 rad/s b) 3.77 m/s c)1.26 km/s2 d)20.1m

Problem 3 A car accelerates uniformly from rest and reaches a speed of 22 m/s in 9s. If the diameter of the tire is 58.0 cm, find The number of revolutions the tires makes during this motion, assuming that no slipping occurs. What is the final rotational speed of a tire in revolutions per second? a) r=29 cm=0.29 m a=Δv/Δt=22/9=2.4 m/s2 a=rα 2.4=0.29α α=8.3 rad/s2 Θ=ωit+1/2αt2 Θ=0(9)+1/2(8.3)92=336.15 rad We can divide this by 2π which is the number of radians in one revolution to find the number of revolutions. 336.15/(2π)=53.52 revolutions b) v=rω 22=0.29ω ω=75.86 rad/s …To convert into revolutions per second, divide by 2π, and ω=12 rev/s a) 54.3 rev b) 12.1 rev/s