RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES

Slides:



Advertisements
Similar presentations
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES
Advertisements

ABSOLUTE MOTION ANALYSIS (Section 16.4)
RELATIVE MOTION ANALYSIS (Section 12.10) Objectives: a)Understand translating frames of reference. b)Use translating frames of reference to analyze relative.
Chapter 3 Kinematics in Two Dimensions
RELATIVE MOTION ANALYSIS: ACCELERATION
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES Today’s Objectives: Students will be able to: 1.Understand translating frames of reference.
Chapter 3 Kinematics in Two Dimensions; Vectors. Units of Chapter 3 Vectors and Scalars Addition of Vectors – Graphical Methods Subtraction of Vectors,
RELATIVE MOTION ANALYSIS: VELOCITY
PLANAR KINEMATICS OF A RIGID BODY
Kinematics in Two Dimensions
Today’s Objectives: Students will be able to: a) Resolve the acceleration of a point on a body into components of translation and rotation. b) Determine.
Advanced Physics Chapter 3 Kinematics in Two Dimensions; Vectors.
Today’s Objectives: Students will be able to: 1.Describe the velocity of a rigid body in terms of translation and rotation components. 2.Perform a relative-motion.
Dynamics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. Today’s Objectives: Students will be able to:
Chapter 3 Kinematics in Two Dimensions; Vectors
Kinematics in Two Dimensions Vectors
INSTANTANEOUS CENTER (IC) OF ZERO VELOCITY (Section 16.6)
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
Part I Relative Velocity Vector Addition and Subtraction (Graphical)
RELATIVE MOTION ANALYSIS: VELOCITY (Section 16.5)
Motion in Two Dimensions
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
12.10 Relative-Motion Analysis of Two Particles Using Translating Axes
Chapter 3 Kinetics in Two or Three Dimensions, Vectors (1 week)
7.2 Projectile Motion and the Velocity Vector
RELATIVE MOTION ANALYSIS: VELOCITY
INSTANTANEOUS CENTER OF ZERO VELOCITY
ABSOLUTE MOTION ANALYSIS
8-6 Vectors Warm Up Lesson Presentation Lesson Quiz Holt Geometry.
Chapter 3 Kinematics in Two Dimensions; Vectors
RECTANGULAR COORDINATES
RECTANGULAR COORDINATES
IMPACT Today’s Objectives: Students will be able to:
ROTATION ABOUT A FIXED AXIS
INSTANTANEOUS CENTER OF ZERO VELOCITY
FORCE VECTORS, VECTOR OPERATIONS & ADDITION COPLANAR FORCES
Graphical Analysis: Positions, Velocity and Acceleration (simple joints) ME 3230 Dr. R. Lindeke ME /20/2018.
GENERAL & RECTANGULAR COMPONENTS
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
RELATIVE MOTION ANALYSIS: VELOCITY
Vectors.
RELATIVE MOTION ANALYSIS: ACCELERATION
RELATIVE MOTION ANALYSIS: ACCELERATION
Physics: Principles with Applications, 6th edition
MOTION OF A PROJECTILE Today’s Objectives: Students will be able to:
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES
Kinematics in Two Dimensions; Vectors
RIGID BODY MOTION (Section 16.1)
Kinematics in Two Dimensions
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
Objectives Find the magnitude and direction of a vector.
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
RELATIVE MOTION ANALYSIS: VELOCITY
Projectiles… Review Session.
RECTILINEAR KINEMATICS: CONTINUOUS MOTION
ABSOLUTE DEPENDENT MOTION ANALYSIS OF TWO PARTICLES
MOTION OF A PROJECTILE Today’s Objectives: Students will be able to:
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
2-D Motion and Vectors Chapter 3.
8-6 Vectors Warm Up Lesson Presentation Lesson Quiz Holt Geometry.
MOMENT OF A FORCE (SCALAR FORMULATION), CROSS PRODUCT, MOMENT OF A FORCE (VECTOR FORMULATION), & PRINCIPLE OF MOMENTS Today’s Objectives : Students will.
Physics: Principles with Applications, 6th edition
CHAPTER 2 FORCE VECTOR.
GENERAL & RECTANGULAR COMPONENTS
10.7 Parametric Equations parametric equations: a pair of equations, one for x and one for y, relating both to a third variable t.
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM
Presentation transcript:

RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES Today’s Objectives: Students will be able to: Understand translating frames of reference. Use translating frames of reference to analyze relative motion. In-Class Activities: • Check Homework, • Reading Quiz • Applications • Relative Position, Velocity and Acceleration • Vector & Graphical Methods • Concept Quiz • Group Problem Solving • Attention Quiz

1. The velocity of B relative to A is defined as READING QUIZ 1. The velocity of B relative to A is defined as A) vB – vA . B) vA – vB . C) vB + vA . D) vA + vB . 2. Since two dimensional vector addition forms a triangle, there can be at most _________ unknowns (either magnitudes and/or directions of the vectors). A) one B) two C) three D) four Answers: 1. A 2. B

APPLICATIONS When you try to hit a moving object, the position, velocity, and acceleration of the object all have to be accounted for by your mind. You are smarter than you thought! Here, the boy on the ground is at d = 10 ft when the girl in the window throws the ball to him. If the boy on the ground is running at a constant speed of 4 ft/s, how fast should the ball be thrown?

APPLICATIONS (continued) When fighter jets take off or land on an aircraft carrier, the velocity of the carrier becomes an issue. If the aircraft carrier is underway with a forward velocity of 50 km/hr and plane A takes off at a horizontal air speed of 200 km/hr (measured by someone on the water), how do we find the velocity of the plane relative to the carrier? How would you find the same thing for airplane B? How does the wind impact this sort of situation?

RELATIVE POSITION (Section 12.10) The absolute position of two particles A and B with respect to the fixed x, y, z reference frame are given by rA and rB. The position of B relative to A is represented by rB/A = rB – rA Therefore, if rB = (10 i + 2 j ) m and rA = (4 i + 5 j ) m, then rB/A = (6 i – 3 j ) m.

RELATIVE VELOCITY To determine the relative velocity of B with respect to A, the time derivative of the relative position equation is taken. vB/A = vB – vA or vB = vA + vB/A In these equations, vB and vA are called absolute velocities and vB/A is the relative velocity of B with respect to A. Note that vB/A = - vA/B .

RELATIVE ACCELERATION The time derivative of the relative velocity equation yields a similar vector relationship between the absolute and relative accelerations of particles A and B. These derivatives yield: aB/A = aB – aA or aB = aA + aB/A

SOLVING PROBLEMS Since the relative motion equations are vector equations, problems involving them may be solved in one of two ways. For instance, the velocity vectors in vB = vA + vB/A could be written as two dimensional (2-D) Cartesian vectors and the resulting 2-D scalar component equations solved for up to two unknowns. Alternatively, vector problems can be solved “graphically” by use of trigonometry. This approach usually makes use of the law of sines or the law of cosines. Could a CAD system be used to solve these types of problems?

LAWS OF SINES AND COSINES b c C B A Since vector addition or subtraction forms a triangle, sine and cosine laws can be applied to solve for relative or absolute velocities and accelerations. As a review, their formulations are provided below. Law of Sines: C c B b A a sin = Law of Cosines: A bc c b a cos 2 - + = B ac C ab

EXAMPLE Given: vA = 650 km/h vB = 800 km/h Find: vB/A Plan: a) Vector Method: Write vectors vA and vB in Cartesian form, then determine vB – vA b) Graphical Method: Draw vectors vA and vB from a common point. Apply the laws of sines and cosines to determine vB/A.

vB/A = vB – vA = (–1050 i – 692.8 j) km/h EXAMPLE (continued) Solution: vA = (650 i ) km/h vB = –800 cos 60 i – 800 sin 60 j = ( –400 i – 692.8 j) km/h a) Vector Method: vB/A = vB – vA = (–1050 i – 692.8 j) km/h v A B / = (-1050)2 +(-692.8)2 = 1258 km/h  = tan-1( ) = 33.4 q 1050 692.8

(vB/A)2 = (800) 2 + (650) 2 − (800) (650) cos 120 vB/A = 1258 km/h EXAMPLE (continued) b) Graphical Method: Note that the vector that measures the tip of B relative to A is vB/A. vB vA 120 vB/A Law of Cosines: (vB/A)2 = (800) 2 + (650) 2 − (800) (650) cos 120 vB/A = 1258 km/h vB/A vA sin(120 ) sin q = or  = 33.4 Law of Sines:

2. Determine the velocity of plane A with respect to plane B. CONCEPT QUIZ 1. Two particles, A and B, are moving in the directions shown. What should be the angle q so that vB/A is minimum? A) 0° B) 180° C) 90° D) 270° A B q s ft v 3 = 4 2. Determine the velocity of plane A with respect to plane B. A) (400 i + 520 j ) km/hr B) (1220 i - 300 j ) km/hr C) (-181 i - 300 j ) km/hr D) (-1220 i + 300 j ) km/hr Answers 1. A 2. B 30

GROUP PROBLEM SOLVING Given: vA = 30 mi/h vB = 20 mi/h aB = 1200 mi/h2 aA = 0 mi/h2 Find: vB/A aB/A Plan:

GROUP PROBLEM SOLVING Given: vA = 30 mi/h vB = 20 mi/h aB = 1200 mi/h2 aA = 0 mi/h2 Find: vB/A aB/A Plan: Write the velocity and acceleration vectors for A and B and determine vB/A and aB/A by using vector equations. Solution: The velocity of B is: vB = –20 sin(30) i + 20 cos(30) j = (–10 i + 17.32 j) mi/h

GROUP PROBLEM SOLVING (solution continued) The velocity of A is: vA = –30 i (mi/h) The relative velocity of B with respect to A is (vB/A): vB/A = vB – vA = (–10i + 17.32j) – (–30i) = (20 i + 17.32 j) mi/h or vB/A = (20)2 + (17.32)2 = 26.5 mi/h q = tan-1( ) = 40.9° q 17.32 20

GROUP PROBLEM SOLVING (solution continued) The acceleration of B is: aB = (at)B + (an)B = [– 1200 sin(30) i +1200 cos(30) j] + [ ( ) cos(30) i +( ) sin(30) j] aB = 554.7 i +1706 j (mi/h2) 202 0.3 The acceleration of A is zero : aA = 0 The relative acceleration of B with respect to A is: aB/A = aB – aA = 554.7 i +1706 j (mi/h2) aA/B = (554.7)2 + (1706)2 = 1790 mi/h2 b = tan-1(1706 / 554.7) = 72° b

ATTENTION QUIZ 1. Determine the relative velocity of particle B with respect to particle A. A) (48i + 30j) km/h B) (- 48i + 30j ) km/h C) (48i - 30j ) km/h D) (- 48i - 30j ) km/h B A vB=100 km/h vA=60 km/h 30 y x 2. If theta equals 90° and A and B start moving from the same point, what is the magnitude of rB/A at t = 5 s? A) 20 ft B) 15 ft C) 18 ft D) 25 ft Answers: 1. C 2. D A B q s ft v 3 = 4

End of the Lecture Let Learning Continue