Monday, Nov. 5, 2007 PHYS 1443-002, Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #17 Monday, Nov. 5, 2007 Dr. Jae Yu Fundamentals of Rotational.

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Monday, Nov. 5, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #17 Monday, Nov. 5, 2007 Dr. Jae Yu Fundamentals of Rotational Motions Rotational Kinematics Rolling Motion of a Rigid Body Relationship between angular and linear quantities Today’s homework is HW #11, due 9pm, Monday, Nov. 12!!

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 2 Announcements There were 36 of you at Dr. Seo’s colloquium  Impressive!! There will be a Ph.D. defense right after this class today!! –You all are welcome!! Will have to have two midterm grade discussions –Today: Last name, A - L –Wednesay: Last name, M - Z 2 nd term exam results –Class average:51.8/100 Term 1: 58/100 –Top Score: 90 Evaluation policy –Exams: 22.5/exam  45%: Will take two best –Homework: 25% –Lab: 20% –Quizzes: 10% –Extra credit: 10% Quiz on Wednesday, Nov. 7

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 3 Therefore the angle, , is. And the unit of the angle is in radian. It is dimensionless!! Fundamentals of Rotational Motions Linear or translational motions can be described as the motion of the center of mass with all the mass of the object concentrated on it. Is this still true for rotational motions? No, because different parts of the object have different linear velocities and accelerations. Consider a motion of a rigid body – an object that does not change its shape – rotating about the axis protruding out of the slide. One radian is the angle swept by an arc length equal to the radius of the arc. Since the circumference of a circle is 2  r, The relationship between radian and degrees is The arc length is

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 4 Rotational Kinematics The first type of motion we have learned in linear kinematics was under a constant acceleration. We will learn about the rotational motion under constant angular acceleration, because these are the simplest motions in both cases. Just like the case in linear motion, one can obtain Angular Speed under constant angular acceleration: Angular displacement under constant angular acceleration: One can also obtain

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 5 Using what we have learned in the previous slide, how would you define the angular displacement? Angular Displacement, Velocity, and Acceleration How about the average angular speed? And the instantaneous angular speed? By the same token, the average angular acceleration is defined as… And the instantaneous angular acceleration? When rotating about a fixed axis, every particle on a rigid object rotates through the same angle and has the same angular speed and angular acceleration. ii ff Unit?rad/s Unit?rad/s Unit?rad/s 2 Unit?rad/s 2

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 6 Example for Rotational Kinematics A wheel rotates with a constant angular acceleration of 3.50 rad/s 2. If the angular speed of the wheel is 2.00 rad/s at t i =0, a) through what angle does the wheel rotate in 2.00s? Using the angular displacement formula in the previous slide, one gets

Monday, Nov. 5, 2007PHYS , Fall 2007 Dr. Jaehoon Yu 7 Example for Rotational Kinematics cnt’d What is the angular speed at t=2.00s? Using the angular speed and acceleration relationship Find the angle through which the wheel rotates between t=2.00s and t=3.00s. Using the angular kinematic formula At t=2.00s At t=3.00s Angular displacement