RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES

Slides:



Advertisements
Similar presentations
Vectors A vector is basically an arrow that represents the magnitude and direction of a measurement. The length of the vector represents its magnitude.
Advertisements

10.6: Vectors in Geometry Expectation:
Fill in missing numbers or operations
Components or resolved forces
Basic Trig Dr. Robert MacKay Clark College Physics.
Law of Sines.
Right Triangle Trigonometry
Physics: Principles with Applications, 6th edition
Hosted By Prissy & Stephy Multiplying exponents Negative exponents Dividing exponent percents
Chapter 1 Force and motion.
August 29 AP physics.
Part 1. Motion of Objects Projected Horizontally
Who Wants To Be A Millionaire?
£1 Million £500,000 £250,000 £125,000 £64,000 £32,000 £16,000 £8,000 £4,000 £2,000 £1,000 £500 £300 £200 £100 Welcome.
Welcome to Who Wants to be a Millionaire
RECTILINEAR KINEMATICS: ERRATIC MOTION
Introduction to Projectile Motion
(Copy only the key facts)(Have your HW out on your desk) A 10kg block being held at rest above the ground is released in freefall. At the instant that.
Kinematics of Projectile Motion
Motion in Two and Three Dimensions; Vectors
Today’s Objectives: Students will be able to :
Slide 6-1 COMPLEX NUMBERS AND POLAR COORDINATES 8.1 Complex Numbers 8.2 Trigonometric Form for Complex Numbers Chapter 8.
Chapter 4 Motion in two dimensions (Chap. 2 in the textbook page 30)
Physics 12 - Kinematics.
Non-Central Coordinate System
S Fi = S miai S (ri x Fi ) = S (ri x miai) SYSTEMS OF PARTICLES
Kinetics of Particles So far, we have only studied the kinematics of particle motion, meaning we have studied the relationships between position, velocity,
Chapter 1: Expressions, Equations, & Inequalities
8 2.
PS-5 Test Review. Questions 1 & 2 Distance – 60m/ magnitude only Displacement 10 m east/ magnitude and direction.
Motion in Two and Three Dimensions
Unit 2 - Right Triangles and Trigonometry
Kinematics Review.
PHYSICS UNIT 1: KINEMATICS (Describing Motion)
Chapter 6 Equations 6.1 Solving Trigonometric Equations 6.2 More on Trigonometric Equations 6.3 Trigonometric Equations Involving Multiples Angles 6.4.
Right Triangle Trigonometry
Trigonometric Functions of Any Angle
UNIT 2 Two Dimensional Motion
Vector Algebra One Mark Questions PREPARED BY:
Kinematics of Rigid Bodies
Kinematics of Particles
ABSOLUTE MOTION ANALYSIS
Systems of Particles.
Mechanics Lecture 2, Slide 1 Vectors and 2d-Kinematics Continued Relevant Equations How to use them Homework Hints.
Right Triangle Trigonometry
Completing the Square Topic
Sep. 12, 2001 Dr. Larry Dennis, FSU Department of Physics1 Physics 2053C – Fall 2001 Chapter 4 Forces and Newton’s Laws of Motion.
CONSERVATION OF LINEAR MOMENTUM FOR A SYSTEM OF PARTICLES (Sections ) Today’s Objectives: Students will be able to: a) Apply the principle of.
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM FOR A SYSTEM OF PARTICLES AND CONSERVATION OF LINEAR MOMENTUM FOR A SYSTEM OF PARTICLES Today’s Objectives: Students.
ENGINEERING MECHANICS CHAPTER 7
THESE TIMES ARE EQUAL The time it takes for an object thrown horizontally to hit the ground The time it takes for that object to hit the ground if I just.
ABSOLUTE MOTION ANALYSIS (Section 16.4)
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
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
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
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.
PHYSICS: Vectors and Projectile Motion. Today’s Goals Students will: 1.Be able to describe the difference between a vector and a scalar. 2.Be able to.
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
In chapter 1, we talked about parametric equations. Parametric equations can be used to describe motion that is not a function. If f and g have derivatives.
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.
Kinematics in Two Dimensions Vectors
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES
RELATIVE-MOTION ANALYSIS OF TWO PARTICLES USING TRANSLATING AXES
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: • Relative Position, Velocity and Acceleration • Vector & Graphical Methods

APPLICATIONS When you try to hit a moving object, the position, velocity, and acceleration of the object must be known. 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 travels at 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. 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 Cartesian vectors and the resulting scalar 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 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 review, their formulations are provided below. a b c C B A 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 = 600 km/hr vB = 700 km/hr 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 = (- 1191.5 i + 344.1 j ) km/hr EXAMPLE (continued) Solution: vA = 600 cos 35 i – 600 sin 35 j = (491.5 i – 344.1 j ) km/hr vB = -700 i km/hr a) Vector Method: vB/A = vB – vA = (- 1191.5 i + 344.1 j ) km/hr hr km v A B 2 . 1240 ) 1 344 ( 5 1191 / = + where ° - 16 tan q

Note that the vector that measures the tip of B relative to A is vB/A. EXAMPLE (continued) b) Graphical Method: ° 145 vB = 700 km/hr vA = 600 km/hr vB/A Note that the vector that measures the tip of B relative to A is vB/A. Law of Cosines: - + = cos ) 600 )( 700 ( 2 / A B v q hr km . 1240 Law of Sines: q sin ) 145° sin( / A B v = or ° 1 . 16

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 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

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 30 Answers 1. A 2. B

GROUP PROBLEM SOLVING Given: vA = 10 m/s vB = 18.5 m/s (at)A = 5 m/s2 aB = 2 m/s2 Find: vA/B aA/B Plan: Write the velocity and acceleration vectors for A and B and determine vA/B and aA/B by using vector equations. Solution: The velocity of A is: vA = 10 cos(45)i – 10 sin(45)j = (7.07i – 7.07j) m/s

GROUP PROBLEM SOLVING (continued) The velocity of B is: vB = 18.5i (m/s) The relative velocity of A with respect to B is (vA/B): vA/B = vA – vB = (7.07i – 7.07j) – (18.5i) = -11.43i – 7.07j or vA/B = (11.43)2 + (7.07)2 = 13.4 m/s q = tan-1( ) = 31.73° q 7.07 11.43

GROUP PROBLEM SOLVING (continued) The acceleration of A is: aA = (at)A + (an)A = [5 cos(45)i – 5 sin(45)j] + [-( ) sin(45)i – ( ) cos(45)j] aA = 2.83i – 4.24j (m/s2) 102 100 The acceleration of B is: aB = 2i (m/s2) The relative acceleration of A with respect to B is: aA/B = aA – aB = (2.83i – 4.24j) – (2i) = 0.83i – 4.24j aA/B = (0.83)2 + (4.24)2 = 4.32 m/s2 b = tan-1( ) = 78.9° b 4.24 0.83

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 B A y x VA VB VB/A Solution: vB/A = vB – vA = 100 i – (60cos30 i + 60sin30 j ) km/hr = (48i - 30j ) km/hr Answers: 1. C 2. D

rB/A = ( vB/A). t = (5)(5)=25 ft ATTENTION QUIZ 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 A B q s ft v 3 = 4 A B q=90 s ft v 3 = 4 B/A 5 rB/A = ( vB/A). t = (5)(5)=25 ft