Review for Test #3  Responsible for: - Chapters 9 (except 9.8), 10, and 11 (except 11.9) - The spring (6.2, 7.3, 8.2-8.3) - Problems worked in class,

Slides:



Advertisements
Similar presentations
AP Physics C Mechanics Review.
Advertisements

Rotational Equilibrium and Rotational Dynamics
PLANAR KINETICS OF A RIGID BODY: CONSERVATION OF ENERGY
L24-s1,8 Physics 114 – Lecture 24 §8.5 Rotational Dynamics Now the physics of rotation Using Newton’s 2 nd Law, with a = r α gives F = m a = m r α τ =
Rigid body rotations inertia. Constant angular acceleration.
Rotational Dynamics Chapter 9.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 5 Rotation of a Rigid Body. §5-5 Angular Momentum of a rigid Body Conservation of Angular Momentum §5-1 Motion of a Rigid body §5-2 Torque The.
Monday, November 3 Review for Exam III Chapters 6, 7, 8(springs only) 9.
Physics 121 Newtonian Mechanics Lecture notes are posted on Instructor Karine Chesnel April 2, 2009.
Department of Physics and Applied Physics , S2010, Lecture 23 Physics I LECTURE 23 5/10/10.
Rotational Kinetic Energy Conservation of Angular Momentum Vector Nature of Angular Quantities.
Physics 101: Lecture 18, Pg 1 Physics 101: Lecture 18 Rotational Dynamics l Today’s lecture will cover Textbook Sections : è Quick review of last.
Department of Physics and Applied Physics , F2010, Lecture 21 Physics I LECTURE 21 11/24/10.
December 2, 2004 Physics 211 Today’s Topics Pick up copy of sample final exam Solutions will be posted in glass cabinet early next week Information about.
Department of Physics and Applied Physics , F2010, Lecture 19 Physics I LECTURE 19 11/17/10.
Useful Equations in Planar Rigid-Body Dynamics
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 20, 2006.
Rotational Dynamics. Moment of Inertia The angular acceleration of a rotating rigid body is proportional to the net applied torque:  is inversely proportional.
FE Exam: Dynamics review
Classical Mechanics Review 4: Units 1-19
Chapter 8 Rotational Motion
Spring Topic Outline for Physics 1 Spring 2011.
Chap. 11B - Rigid Body Rotation
Tuesday, Oct. 28, 2014PHYS , Fall 2014 Dr. Jaehoon Yu 1 PHYS 1443 – Section 004 Lecture #18 Tuesday, Oct. 28, 2014 Dr. Jaehoon Yu Torque and Angular.
Give the expression for the velocity of an object rolling down an incline without slipping in terms of h (height), M(mass), g, I (Moment of inertia) and.
FE Exam: Dynamics review D. A. Lyn School of Civil Engineering 21 February 2012.
Chapter 10 Rotational Kinematics and Energy. Units of Chapter 10 Angular Position, Velocity, and Acceleration Rotational Kinematics Connections Between.
Chapter 9: Rotational Dynamics
ROTATIONAL MOTION AND EQUILIBRIUM
1 Physics 1100 – Spring 2009 Review for Exam I Friday, February 27 th Chapters
ENGR 214 Chapter 17 Plane Motion of Rigid Bodies:
Example Problem The parallel axis theorem provides a useful way to calculate I about an arbitrary axis. The theorem states that I = Icm + Mh2, where Icm.
Equations for Projectile Motion
Chapter 8 Rotational Motion.
Chapter 11: Rotational Dynamics  As we did for linear (or translational) motion, we studied kinematics (motion without regard to the cause) and then dynamics.
DYNAMICS VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Tenth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P.
Moment Of Inertia.
Review for Final Exam  Exam format: - 9 problems, 3 from the last 3 chapters, 10 pts - Set of short-answer conceptual questions, 10 pts - Time: Wed. Dec.
Review for Final Exam  Exam format: - 25 problems; 5 from the last 3 chapters; 3 advanced, 3 intermediate, 19 simple - Time: Wed. Dec. 11, noon-3pm -
Rotational Dynamics and Static Equilibrium
Thursday, Oct. 30, 2014PHYS , Fall 2014 Dr. Jaehoon Yu 1 PHYS 1443 – Section 004 Lecture #19 Thursday, Oct. 30, 2014 Dr. Jaehoon Yu Rolling Kinetic.
Review for Test #1  Responsible for: - Chapters 1, 2, 3, and 4 - Notes from class - Problems worked in class - Homework assignments  Test format: - 15.
1 Rotation of a Rigid Body Readings: Chapter How can we characterize the acceleration during rotation? - translational acceleration and - angular.
NM Unit 8 Topic(s): Angular Momentum Learning Goals: Adapt linear collision analysis for rotational collision analysis Develop a solution strategy to solve.
Review for Test #2  Responsible for: - Chapters 5, 6 (except springs in 6.2), 7 (except 7.3), 8 (except springs), and 12 ( only), as well as 1-4.
Chapter 9 Rotational Dynamics
1 Semester Review EP I. 2 1 Vector Addition Graphical Algebraic.
Wednesday, Nov. 10, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Moment of Inertia 2.Parallel Axis Theorem 3.Torque and Angular Acceleration 4.Rotational.
Physics 111 Lecture Summaries (Serway 8 th Edition): Lecture 1Chapter 1&3Measurement & Vectors Lecture 2 Chapter 2Motion in 1 Dimension (Kinematics) Lecture.
Particle Kinematics Direction of velocity vector is parallel to path Magnitude of velocity vector is distance traveled / time Inertial frame – non accelerating,
Energy and Work. Work done by a Force Distance x Force x Distance x Force x Distance x Force x Textbook defines work due to a force as the product of.
Units of N/m m 2 = N m = J  Total potential energy is Example: Problem A block (m = 1.7 kg) and a spring (k = 310 N/m) are on a frictionless incline.
Today: (Ch. 8)  Rotational Motion.
Physics 1D03 - Lecture 351 Review. Physics 1D03 - Lecture 352 Topics to study basic kinematics forces & free-body diagrams circular motion center of mass.
Rotational Energy Kinetic Energy ( E k ) - The ability to produce change due to an object’s motion. Linear Kinetic EnergyRotational Kinetic Energy.
ROTATIONAL MOTION Rotation axis: rotation occurs about an axis that does not move: fixed axis.
Rotational Kinetic Energy
Classical Mechanics Review 4: Units 1-22
Class Introduction The Works of the Lord are great, sought out of all them that have pleasure therein. Ps.111:2.
9/16/2018 Physics 253.
Honors Physics 1 Class 12 Fall 2013
Rotational Kinematics and Energy
AP MC Problems A how to guide..
Physics 207, Lecture 17, Nov. 1 Work/Energy Theorem, Energy Transfer
Chapter 8 Rotational Motion.
Spring 2002 Lecture #15 Dr. Jaehoon Yu Mid-term Results
Rotational kinetic energy
Finding the Moment of Inertia using calculus
Physics I LECTURE 21 12/2/09.
Presentation transcript:

Review for Test #3  Responsible for: - Chapters 9 (except 9.8), 10, and 11 (except 11.9) - The spring (6.2, 7.3, ) - Problems worked in class, class notes - Homework assignments  Test format: - 13 problems, 11 simple, 1 intermediate, 1 advanced, 7.7 pts each - Time: 50 minutes only  Test materials: - Pencil, paper, eraser, and calculator - No formulae sheet - Closed textbook and notes

Material Covered  Chapter 9: Impulse and Momentum - Impulse-momentum theorem - Conservation of Linear momentum - 1 and 2D collisions - Center of mass  Chapter 10: Rotational Kinematics and Energy - , , , a r, and a t - Rotational kinematic equations - Rolling motion (tire) - Moment of inertia - Rotational work and kinetic energy - Conservation of Energy with rotation

Example Problem, Grades returned by next Monday? A m bar with a mass of kg is released from rest in the vertical position. A spring is  Chapter 11: Rotational Dynamics and Static Equilibrium - ,  =I  - Applications of  =0,  F=0 - Center of gravity - Angular momentum, conservation of...  The Spring - Force due to a spring (Hooke’s Law) - Work and potential energy of a spring

attached, initially unstrained, and has a spring constant of 25.0 N/m. Find the tangential speed with which the free end strikes the horizontal surface. (drawing to be provided) Solution: Bar rotating with axis at one end  rotational KE, no translational KE Bar falls from some height  gravitional PE (U g ) A spring is attached to bar  spring PE (U s ) Bar  rigid body  need moment of inertia  Use Conservation of Energy

y i  h since this would mean all mass of rod is at y i =h, but mass is distributed. So, take mass to be located at center of gravity

From geometry of problem Return to Conservation of Energy and solve for v t