EGR 280 Mechanics 9 – Particle Kinematics II. Curvilinear motion of particles Let the vector from the origin of a fixed coordinate system to the particle.

Slides:



Advertisements
Similar presentations
Chapter 11 KINEMATICS OF PARTICLES
Advertisements

Chapter 9: Vector Differential Calculus Vector Functions of One Variable -- a vector, each component of which is a function of the same variable.
2.4 Rates of Change and Tangent Lines. What you’ll learn about Average Rates of Change Tangent to a Curve Slope of a Curve Normal to a Curve Speed Revisited.
Meanings of the Derivatives. I. The Derivative at the Point as the Slope of the Tangent to the Graph of the Function at the Point.
CHS Physics Motion in Two and Three Dimensions. Position  The position of an object in two or three dimensions is given by a position vector.  The vector.
Uniform circular motion – Another specific example of 2D motion
PHYS 218 sec Review Chap. 3 Motion in 2 or 3 dimensions.
BNG 202 – Biomechanics II Lecture 14 – Rigid Body Kinematics Instructor: Sudhir Khetan, Ph.D. Wednesday, May 1, 2013.
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
Chapter 16 Planar Kinematics of a Rigid Body
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 3.
We’ve already discussed and used accelerations tangential ( a t ) and normal ( a n ) to the path of motion. We’ve calculated a n from a n = v 2 /r (circular.
Particle Kinematics: Intro to Curvilinear Motion Current unit: Particle Kinematics Last two classes: Straight Line Motion Today: (a) Intro to Curvilinear.
Chapter 8: Rotational Kinematics Lecture Notes
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 6.
Dynamics ENGR 215, Section 01 –Goals –Start from the general and work down 1.
Normal-Tangential coordinates
Mechanics of rigid body StaticsDynamics Equilibrium Galilei Newton Lagrange Euler KinematicsKinetics v=ds/dt a=dv/dt Σ F = 0 Σ F = m a mechanics of rigid.
Normal-Tangential coordinates
Chapter 3 Vectors in Physics.
EGR 280 Mechanics 14 – Kinematics of Rigid Bodies.
Kinematics - Plane motion Jacob Y. Kazakia © Types of Motion Translation ( a straight line keeps its direction) 1.rectilinear translation 2.curvilinear.
EGR 280 Mechanics 12 – Work and Energy of Particles.
Chapter 14 Section 14.3 Curves. x y z To get the equation of the line we need to know two things, a direction vector d and a point on the line P. To find.
Vector-Valued Functions Section 10.3a. Standard Unit Vectors Any vector in the plane can be written as a linear combination of the two standard unit vectors:
10.3 Vector Valued Functions Greg Kelly, Hanford High School, Richland, Washington.
Y 1 y 2 x 1 x 2 Using Cartesian Coordinates to Describe 2D Motion motion path described by the particle on 2D X Y P 1 P 2 i = (1,0) j = (0,1) R = x i +
Kinematics in 1-D. Learning Target I can differentiate between position, distance, displacement, speed, and velocity.
Objective Rectangular Components Normal and Tangential Components
Section 17.2 Position, Velocity, and Acceleration.
Kinematics Kinematics is the branch of physics that describes the motion of points, bodies (objects) and systems of bodies (groups of objects) without.
NORMAL AND TANGENTIAL COMPONENTS
Chapter 2 – kinematics of particles
Rotational Motion 2 Coming around again to a theater near you.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 5.
DESCRIBING MOTION: Kinematics in One Dimension CHAPTER 2.
MOTION RELATIVE TO ROTATING AXES
المحاضرة الخامسة. 4.1 The Position, Velocity, and Acceleration Vectors The position of a particle by its position vector r, drawn from the origin of some.
Chapter 12 Vector-Valued Functions. Copyright © Houghton Mifflin Company. All rights reserved.12-2 Definition of Vector-Valued Function.
Any vector can be written as a linear combination of two standard unit vectors. The vector v is a linear combination of the vectors i and j. The scalar.
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today’s Objectives: Students will be able to: 1.Describe the motion of a particle traveling along.
V ECTORS AND C ALCULUS Section 11-B. Vectors and Derivatives If a smooth curve C is given by the equation Then the slope of C at the point (x, y) is given.
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today’s Objectives: Students will be able to: 1.Describe the motion of a particle traveling along.
Theoretical Mechanics KINEMATICS * Navigation: Right (Down) arrow – next slide Left (Up) arrow – previous slide Esc – Exit Notes and Recommendations:
Motion in Two and Three Dimensions. 4-2 Position and Displacement The position vector is typically used to indicate the location of a particle. The position.
Curvilinear Motion  Motion of projectile  Normal and tangential components.
Mechanics for Engineers: Dynamics, 13th SI Edition R. C. Hibbeler and Kai Beng Yap © Pearson Education South Asia Pte Ltd All rights reserved. CURVILINEAR.
KINEMATICS OF PARTICLES RELATIVE MOTION WITH RESPECT TO TRANSLATING AXES.
PHY 151: Lecture 4B 4.4 Particle in Uniform Circular Motion 4.5 Relative Velocity.
Vector Differentiation If u = t, then dr/dt= v.
Figure shows a car moving in a circular path with constant linear speed v. Such motion is called uniform circular motion. Because the car’s.
GENERAL & RECTANGULAR COMPONENTS
NORMAL AND TANGENTIAL COMPONENTS
Two special unit vectors:
Vector-Valued Functions and Motion in Space
– KINEMATIC OF RECTILINEAR MOTION
NORMAL AND TANGENTIAL COMPONENTS
Motion Along a Line: Vectors
GENERAL & RECTANGULAR COMPONENTS
King Fahd University of Petroleum & Minerals
NORMAL AND TANGENTIAL COMPONENTS
Homework Aid: Cycloid Motion
A#40 Vectors Day 6 Paper #1 Review.
Vectors Scalars and Vectors:
Conceptual Dynamics Part II: Kinematics of Particles Chapter 3
Conceptual Dynamics Part II: Particle Kinematics Chapter 3
Motion, Velocity, Acceleration
12.5: Vector PVA.
GENERAL & RECTANGULAR COMPONENTS
Fundamentals of Physics School of Physical Science and Technology
Presentation transcript:

EGR 280 Mechanics 9 – Particle Kinematics II

Curvilinear motion of particles Let the vector from the origin of a fixed coordinate system to the particle be the position vector r The time derivative of position is velocity: P x y z r s

The magnitude of velocity is speed, and is the time rate of change of arc length. Speed is a scalar quantity. The time derivative of velocity is acceleration:

Motion of several particles r B = r A + r AB = r A + r B/A v B = v A + v B/A a B = a A + a B/A A B x y z rArA rBrB r AB =r B/A

Intrinsic coordinate system Define a coordinate system that moves with the particle: e t = unit tangent vector. Always tangent to the path of the particle e n = unit normal vector. Perpendicular to e t,, always points into the curve As the particle moves along the curve, the unit tangent vector moves in the direction of the unit normal vector: de t /dθ = e n etet enen dθdθ

Intrinsic coordinate system The velocity, by definition, is always tangent to the curve: v = v e t The acceleration is the time rate of change of velocity: The intrinsic coordinate system is used often to describe circular motion.