Equations for Projectile Motion

Slides:



Advertisements
Similar presentations
Rotational Equilibrium and Rotational Dynamics
Advertisements

ENGR 214 Chapter 16 Plane Motion of Rigid Bodies:
Conservative vs. Non-conservative Forces
Chapter 11 Angular Momentum
Two-Dimensional Rotational Dynamics W09D2. Young and Freedman: 1
Physics 106: Mechanics Lecture 04
Chapter 9 Rotational Dynamics.
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 =
Rotational Equilibrium and Rotational Dynamics
Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Rolling Objects l Today’s lecture will cover Textbook Chapter Exam III.
Physics 111: Mechanics Lecture 10 Dale Gary NJIT Physics Department.
Dynamics of Rotational Motion
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Rotational Dynamics and Static Equlibrium Teacher: Luiz Izola
Rotational Equilibrium and Rotational Dynamics
Dynamics of a Rigid Body
Department of Physics and Applied Physics , F2010, Lecture 20 Physics I LECTURE 20 11/21/10.
Department of Physics and Applied Physics , F2010, Lecture 21 Physics I LECTURE 21 11/24/10.
Chapter 11 Rolling, Torque, and Angular Momentum In this chapter we will cover the following topics: -Rolling of circular objects and its relationship.
Department of Physics and Applied Physics , F2010, Lecture 19 Physics I LECTURE 19 11/17/10.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 27, 2006.
Physics 106: Mechanics Lecture 02
Useful Equations in Planar Rigid-Body Dynamics
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 20, 2006.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Rotational Dynamics Example
Rotational Dynamics. Moment of Inertia The angular acceleration of a rotating rigid body is proportional to the net applied torque:  is inversely proportional.
Mechanical Energy and Simple Harmonic Oscillator 8.01 Week 09D
Rotational Work and Kinetic Energy Dual Credit Physics Montwood High School R. Casao.
Chapter 11 Angular Momentum.
Two-Dimensional Rotational Dynamics 8.01 W09D2 Young and Freedman: 1.10 (Vector Product), , 10.4, ;
Rotational Kinematics and Energy
PHYS 1441 – Section 002 Lecture #22 Monday, April 22, 2013 Dr. Jaehoon Yu Work, Power and Energy in Rotation Angular Momentum Angular Momentum Conservation.
Q10. Rotational Motion.
Rotational Dynamics and Static Equilibrium (Cont.)
Chapter 7 Rotational Motion.
Rotational Equilibrium and Rotational Dynamics
Chapter 9: Rotational Dynamics
ROTATIONAL MOTION AND EQUILIBRIUM
Chapter 10 - Rotation Definitions: –Angular Displacement –Angular Speed and Velocity –Angular Acceleration –Relation to linear quantities Rolling Motion.
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,
AP Physics C: Mechanics Chapter 11
Conservation of Angular Momentum Dynamics of a rigid object
Chapter 8 Rotational Motion.
Chapter 8 Rotational Motion.
Physics 111 Practice Problem Statements 10 Torque, Energy, Rolling SJ 8th Ed.: Chap 10.6 – 10.9 Contents 11-47, 11-49*, 11-55*, 11-56, 11-60*, 11-63,
Chapter 10 Chapter 10 Rotational motion Rotational motion Part 2 Part 2.
Torque Calculations with Pulleys
Exam 2 Review 8.02 W08D1. Announcements Test Two Next Week Thursday Oct 27 7:30-9:30 Section Room Assignments on Announcements Page Test Two Topics: Circular.
Rotational Kinetic Energy An object rotating about some axis with an angular speed, , has rotational kinetic energy even though it may not have.
Wednesday 6/10 PHYS 2010 Nathalie Hoffmann University of Utah.
Physics CHAPTER 8 ROTATIONAL MOTION. The Radian  The radian is a unit of angular measure  The radian can be defined as the arc length s along a circle.
Lecture 14: Rolling Objects l Rotational Dynamics l Rolling Objects and Conservation of Energy l Examples & Problem Solving.
Unit: NM 8 Topic(s): Rotational Inertia and Torque
Chapter 11 Angular Momentum. The Vector Product and Torque The torque vector lies in a direction perpendicular to the plane formed by the position vector.
T072 : Q13. Assume that a disk starts from rest and rotates with an angular acceleration of 2.00 rad/s 2. The time it takes to rotate through the first.
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.
Two-Dimensional Rotational Dynamics W09D2. Young and Freedman: 1
Chapt. 10: Angular Momentum
 The metric system – units, prefixes  Unit conversions  Algebra and trigonometry  Orders of magnitude.
Today: (Ch. 8)  Rotational Motion.
Rotational Dynamics.
UNIT 6 Rotational Motion & Angular Momentum Rotational Dynamics, Inertia and Newton’s 2 nd Law for Rotation.
ROTATIONAL DYNAMICS. ROTATIONAL DYNAMICS AND MOMENT OF INERTIA  A Force applied to an object can cause it to rotate.  Lets assume the F is applied at.
Physics 1D03 - Lecture 351 Review. Physics 1D03 - Lecture 352 Topics to study basic kinematics forces & free-body diagrams circular motion center of mass.
Two-Dimensional Rotational Dynamics 8.01 W09D2
Dynamics of a System of Particles Prof. Claude A Pruneau Notes compiled by L. Tarini Physics and Astronomy Department Wayne State University PHY 6200 Theoretical.
Dr.Mohammed Abdulrazzaq Mechanical Department College of Enginerring
A pulley of radius R1 and rotational inertia I1 is
Physics I LECTURE 21 12/2/09.
Presentation transcript:

Equations for Projectile Motion Horizontal Vertical ax=0 ay = - g vx= constant

Steps in Solving Problems Draw free-body diagram for every object that is ”free” Select coordinate system such that one of the axis is along the direction of acceleration Write out the equations of motion for the x and y coordinate: Step 2 should guarantee that the sum of the forces in at all but one direction equals zero. Solve the equations simultaneously

Non-Conservative Forces If work is done by non-conservative forces: The sign of WNC is very important A motor adds energy so WNC is positive and E2 > E1 Friction dissipates energy so WNC is negative and E2 < E1

Example 6-5 (43) The roller-coaster car shown is dragged up to point 1 where it is released from rest. Assuming no friction, calculate the speed at points 2, 3, and 4. Let point be the height where P.E. = 0 Ch 6 5

Continued Example 6-5 (43) The roller-coaster car shown is dragged up to point 1 where it is released from rest. Assuming no friction, calculate the speed at points 2, 3, and 4. Let point be the height where P.E. = 0 Ch 6 6

Conservation of Momentum In the collision of two isolated objects, the only forces are between the two objects—these are called internal forces. In this case: initial momentum = final momentum The total momentum of an isolated system of bodies remains constant.

Radial and Tangential Acceleration A point on a rotating wheel always has centripetal acceleration and it will have tangential acceleration if the wheel has angular acceleration.

Kinematic Equations for Uniformly Accelerated Motion The angular equations for constant angular acceleration are derived the same as for constant linear acceleration.

Rotational Dynamics Torque is necessary for angular acceleration This is expressed as where I is called the moment of inertia Compare this with Newton’s Second Law: τ is the equivalent of force for rotational motion I is the equivalent of mass for rotational motion

A 1.5 kg mass is attached to a cord wrapped around a heavy pulley of mass 4.00 kg and radius 33.0 cm. The pulley is a solid cylinder. Calculate the acceleration of the mass. Example 8-5 m