Motion in a 2 and 3 dimensions Ch 4 HRW

Similar documents
Motion in Two and Three Dimensions

CHAPTER 3 MOTION IN TWO AND THREE DIMENSIONS

Motion in Two and Three Dimensions

Lesson 2. Physics 168. Luis Anchordoqui

Chapter 4. Motion in two and three dimensions

Chapter 4. Motion in Two Dimensions

(483 km) ( 966 km) km. tan km

Chapter 4. Motion in Two Dimensions

Lecture4- Projectile Motion Chapter 4

Chapter 4. Motion in two and three dimensions

In this activity, we explore the application of differential equations to the real world as applied to projectile motion.

Motion in 2- and 3-dimensions. Examples: non-linear motion (circles, planetary orbits, etc.) flight of projectiles (shells, golf balls, etc.

MOTION IN TWO OR THREE DIMENSIONS

Chapter 4. Motion in Two Dimensions

Department of Physics, Korea University Page 1 of 8

Halliday/Resnick/Walker 7e Chapter 4

Motion in Two or Three Dimensions

Chapter 3. Kinematics in Two Dimensions

b) (6) How far down the road did the car travel during the acceleration?

Chapter 4. Motion in Two Dimensions. Professor Wa el Salah

Physics 1: Mechanics

Components of a Vector

Chapter 4. Motion in Two Dimensions. With modifications by Pinkney

Vectors and 2D Kinematics. AIT AP Physics C

KINEMATICS OF A PARTICLE. Prepared by Engr. John Paul Timola

Chapter 4 Kinematics II: Motion in Two and Three Dimensions

(b) A sketch is shown. The coordinate values are in meters.

CH 4 Motion in two and three Dimensions

Chapter 3: Kinematics in Two Dimensions

Chapter 4 - Motion in 2D and 3D

Kinematics in Two Dimensions; Vectors

Chapter 3 Kinematics in Two Dimensions; Vectors

INTRODUCTION & RECTILINEAR KINEMATICS: CONTINUOUS MOTION

2-D Vector Equations have the same form as 1-D Kinematics. f i i

PHYSICS - CLUTCH CH 02: 1D MOTION (KINEMATICS)

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009

Vectors. However, cartesian coordinates are really nothing more than a way to pinpoint an object s position in space

Chapter 2. Kinematics in One Dimension. continued

Kinematics in Two-Dimensions

Principles and Problems. Chapter 6: Motion in Two Dimensions

Phys 201, Lecture 5 Feb.2. Chapter 3: Mo;on in Two and Three Dimensions

Chapter 3 Motion in two or three dimensions

Topic 3 Motion in two dimensions Position of points in two dimensions is represented in vector form

1. A baseball player throws a ball horizontally. Which statement best describes the ball's motion after it is thrown? [Neglect the effect of

PHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010

Phys101 First Major-111 Zero Version Monday, October 17, 2011 Page: 1

B C = B 2 + C 2 2BC cosθ = (5.6)(4.8)cos79 = ) The components of vectors B and C are given as follows: B x. = 6.

Q3.1. A. 100 m B. 200 m C. 600 m D m E. zero. 500 m. 400 m. 300 m Pearson Education, Inc.

Text PHYSJC and your answer to 22333

Physics 4A Solutions to Chapter 4 Homework

Random sample problems

Kinematics. Vector solutions. Vectors

KINEMATICS REVIEW VECTOR ALGEBRA - SUMMARY

Two Dimensional Motion

Chapter 3: 2D Kinematics Tuesday January 20th

1. (P2.1A) The picture below shows a ball rolling along a table at 1 second time intervals. What is the object s average velocity after 6 seconds?

A. Basic Concepts and Graphs

Problem: Projectile (CM-1998) Justify your answer: Problem: Projectile (CM-1998) 5 10 m/s 3. Show your work: 3 m/s 2

Trigonometry Basics. Which side is opposite? It depends on the angle. θ 2. Y is opposite to θ 1 ; Y is adjacent to θ 2.

vector of point will be and if the point P is in a space and its coordinates are (x, y, z) then position vector can be expressed as

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics

Exam. Name. 1) For general projectile motion with no air resistance, the horizontal component of a projectile's velocity A) B) C) D)

Chapter 3. Motion in Two or Three dimensions. 3.1 Position and Velocity Vectors

CHAPTER # 2 VECTORS THEORETICAL QUESTIONS PAST PAPERS

Such a life, with all vision limited to a Point and all motion to a Straight Line, seemed to me inexplicably dreary -Edwin Abbott Abbott (

Chapter 2: Motion along a straight line

Motion in Two or Three Dimensions

Describing motion: Kinematics in two dimension

Uniform Circular Motion AP

( ) ( ) A i ˆj. What is the unit vector  that points in the direction of A? 1) The vector A is given by = ( 6.0m ) ˆ ( 8.0m ) Solution A D) 6 E) 6

Chapter 6 Motion in Two Dimensions

Welcome back to Physics 211

170 Test example problems CH1,2,3

PH Fall - Section 05 - Version C DRAFT

Kinematics (2) - Motion in Three Dimensions

Answer: Scalars: Volume, mass, speed, density, number of moles, angular frequency. Vectors: Acceleration, velocity, displacement, angular velocity.

Phys101 First Major-061 Zero Version Coordinator: Abdelmonem Monday, October 30, 2006 Page: 1

Full file at


Physics 114A Introduction to Mechanics (without calculus)

Phys 2425: University Physics I Summer 2016 Practice Exam 1

CHAPTER 3 KINEMATICS IN TWO DIMENSIONS; VECTORS

Downloaded from 3. Motion in a straight line. Study of motion of objects along a straight line is known as rectilinear motion.

LAHS Physics Semester 1 Final Practice Multiple Choice

PHY 1114: Physics I. Quick Question 1. Quick Question 2. Quick Question 3. Quick Question 4. Lecture 5: Motion in 2D

POP QUIZ: 1. List the SI Units for the following: (a) Acceleration: (b) Displacement: (c) Velocity. (d) Time. (e) Speed.

Motion in one dimension

Introduction to 2-Dimensional Motion

5 Projectile Motion. Projectile motion can be described by the horizontal and vertical components of motion.

AP Calculus AB Chapter 2 Test Review #1

Linear Motion. By Jack, Cole, Kate and Linus

Problem: Projectile (CM-1998)

ISSUED BY K V - DOWNLOADED FROM KINEMATICS

Chapter 2. Motion along a Straight Line

MOTION IN A PLANE. Chapter Four MCQ I. (a) 45 (b) 90 (c) 45 (d) 180

State, for each of the following physical quantities, if it is a scalar or a vector:

Physics 201, Midterm Exam 1, Fall Answer Key

Vectors and Scalars. Scalar: A quantity specified by its magnitude only Vector: A quantity specified both by its magnitude and direction.

Two-Dimensional Motion Worksheet

Definitions In physics we have two types of measurable quantities: vectors and scalars.

Transcription:

Motion in a and 3 dimensions Ch 4 HRW Motion in a plane D Motion in space 3D Projectile motion Position and Displacement Vectors A position vector r extends from a reference point (usually the origin O) to particle. r xi yj zk r 3ij5 k m If there is a change in the position vector from r to r 1 then the particle s displacement is r r r r r i r r j r r k 1 x 1x y 1y z 1z rir j rk x y z P Go through Sample Problem p59. 1

Average and Instantaneous Velocity Following the same approach as in Ch we define average velocity: displacement average velocity = time r ri x ry jrk z vavg t t r r x y rz i j k t t t t t + Δt When speaking of velocity we usually mean the instantaneous velocity given by: dr v dt Direction of is always tangent (gradient)to the particles path. v 3 Average and Instantaneous Velocity When speaking of velocity we usually mean the instantaneous velocity given by: dr d xi yjzk v dt dt dx dy dz i j k dt dt dt viv j vk x y z Direction of v is always tangent to the particles path. Scalar components: vx dx v dy dz y vz dt dt dt Go through Sample problem p6 4

Checkpoint 1 The figure shows a circular path taken by a particle. If the instantaneous velocity of the particle is m/s m/s through which quadrant is the particle moving at that instant if it is travelling (a) clockwise and (b) counterclockwise around the circle? For both cases, draw on the figure. v i j 5 Average and Instantaneous Acceleration When a particle s velocity changes in a time interval Dt the average acceleration is: As previously discussed the instantaneous acceleration is then: dv d a v xi vy jvzk dt dt dv dv x y dvz i j k dt dt dt aia j ak Scalar components: change in velocity average acceleration = time interval v v1 v aavg t t x y z dv dv x y dvz ax ay az dt dt dt 6 3

Checkpoint Here are four descriptions of the position (in meters) of a puck as it moves in an xy plane: 1.. 3. 4. x 3t 4t and y 6t 4t x t t y t r t i 4t3 j 3 r 4t t i3j 3 3 4 and 5 6 Are the x and y acceleration components constant? Is the acceleration constant? 7 Problem A particle with velocity v.0i 4.0 j(in meters per second) at t = 0 undergoes a constant acceleration a magnitude a = 3.0 m/s at an angle q =130 from the positive direction of the x axis. What is the particle s velocity v at t = 5 s? What do we know? a = 3.0 m/s at an angle q=130 to x axis of 8 4

Projectile Motion Special case: -D motion Projectile motion: particle moves in a vertical plane with an initial velocity v 0 but acceleration is always the freefall of gravity a g 9.8 m/s Assume no air resistance Path is shown Initial launch velocity 9 0y 0 Projectile motion v 0 v0xi v0y j g v0x v0cos v v sin Position vector and velocity vector change continuously. Acceleration is ALWAYS constant directed downwards NO horizontal acceleration. The horizontal motion is independent of the vertical motion. Solve the two dimensions separately. 10 5

Projectile Motion Analysed Launch point: x0 and y0 Can be at the origin (but not necessarily) Horizontal motion: No acceleration Displacement x x v t v t cos 0 0x 0 Vertical motion: Acceleration is constant Can use equations from ch -9 Displacement y y0 v0yt½at 0 sin ½ Other equations vy v0 sin gt sin y v t g t v v g y 0 11 Projectile Motion Analysed Horizontal range: When object reaches the ground y y o = 0 There are solutions for x if y = y o = 0 y tan 0 x v0cos0 Horizontal displacement (Range): x x o = R R v0cos0t and y 0v0sin0tgt Eliminate t then v0 R sin 0 g Only valid if landing height = launch height Max R when q = 45 (How do we figure this out?) gx R 1 6

Projectile Motion Analysed Time of Flight: (Not in HRW) At max height the time taken is half the total journey. t = ½T v = 0 m/s ½T Time of flight T vy v0 sin gt T 0v0 sin g v0 sin T g R 13 Projectile Motion Analysed Max. height: (Not in HRW) At max height is reached halfway through the journey. t = ½T ½T v = 0 m/s Max height y y v sin t½gt h 0 0 T T hv0 sin ½g v0sin v0sin v0 sin ½g g g v0 sin h g R Go through Sample problems p69, p70 14 7

Problem A rifle with a muzzle velocity v 0 = 450 m/s shoots a bullet at a target 50 m away. How high above the target must the barrel be pointed? Assume the muzzle and the target are at the same height. Given: v 0 = 450 m/s R = 50 m g = 9.8 m/s 15 Problem At time t = 0 a golf ball is shot from ground level into the air, as shown in the fig. The angle q between the balls direction of travel and the positive x axis is given as a function of time t. The ball lands at t = 6.00 s. What is the magnitude v 0 of the ball s launch velocity? At what height (y-y 0 ) above the launch level does the ball land? What is the balls direction of travel just before it lands? 16 8

Uniform Circular Motion A particle is in uniform circular motion if: It travels in a circular arc At a constant speed. Although speed is constant, there is acceleration Velocity is changing direction Velocity is directed tangent to the circle Acceleration is directed to centre of the circle centripetal acceleration. Acceleration v a. r Period of revolution r T. v 17 Uniform Circular Motion-derivation of v a r Recall - v is tangent to path (position) of particle. At P : coordinates: x, y position: r is at angle to x-axis v position v is at angle to perpendicular at P (Fig(b)) v v sin cos xi vy j v i v j Using Fig (a) yp x p v v i v j r r p p 18 9

Uniform Circular Motion yp x p v v i v j r r dv v dy p dx v p v v a i j cos i sin j dt r dt r dt r r v v a ax ay cos sin r r Direction of acceleration: along radius of circle towards centre a v sin y tan r tan ax v cos r 19 Checkpoint 5 An object moves at constant speed along a circular path in a horizontal xy plane, with the centre at the origin. When the object is at x = -m, its velocity is (4m/s) ĵ. Give the object s (a) velocity and (b) acceleration at y = m. 0 10

Problem A satellite is at an altitude h = 00 km above the earth (g = 9. m.s ). Determine the satellite s velocity and its period. The earth s radius is 6.37 10 6 m. 1 Relative Motion 1-D Suppose you watch a passenger on a bus travelling east at 40 km/h. To a passenger on another bus, travelling next to the first at the same velocity, the first passenger seems to be stationary. Velocity of particle depends on reference frame of the observer. Reference frame is a physical object to which we attach coordinate system. 11

Relative Motion 1-D Suppose Alex is parked at side of road watching car P. Bob also watches car P from his car as he moves along the road at constant speed. If both Alex and Bob measure the position of car P at the same time: xpa xpb xba Determining the velocities (derivative): dxpa dxpb dxba dt dt dt v v v PA PB BA Velocity components: The velocity of P as measured by A =the velocity of P as measured by B plus the velocity of B as measured by A. 3 Relative Motion 1-D Determine acceleration: dvpa dvpb dvba dt dt dt a a a a 0 PA PB BA PB Observers on different frames of reference that move at constant velocity relative to each other will measure the same acceleration for a moving particle. 4 1

Sample Problem p74 Suppose that Bob s velocity relative to Alex is a constant v BA = 5 km/h and car P is moving in the negative direction of the x axis. (a) If Alex measures a constant v PA = -78 km/h for car P, what velocity v PB will Bob measure? (b) If car P brakes to stop relative to Alex in time t = 10 s at constant acceleration, what is its acceleration a PA relative to Alex? (c) What is the acceleration a PB of car P relative to Bob during braking? 5 Relative Motion -D Two observers watch a particle P from the origins of their reference frames A and B B moves at a constant velocity v BA relative to A. At a particular instant: rpa rpb rba vpa vpb vba a a a a 0 PA PB BA PB 6 13

Sample Problem p75 A plane moves due E while the pilot points the plane somewhat S of E, toward a steady wind that blows to the NE. The plane has velocity v PW relative to the wind, with an airspeed, relative to the wind of 15 km/h directed at angle S of E. The wind has a velocity v WG relative to the ground with a speed 65 km/h, directed 0.0 E of N. What is the magnitude of the velocity v PG of the plane relative to the ground, and what is. 7 Problems 4. The minute hand on a clock is 10 cm long from tip to support point around which it rotates. Determine the magnitude and angle of the displacement vector of the tip for the following time intervals: (a) quarter past the hour to half past the hour. (b) the next half hour. (c) the next hour after that. 8. A plane flies 483 km E from city A to city B in 45.0 min and then 966 km south from city B to city C in 1.50 h. For the whole trip, what are (a) magnitude and direction of the plane s displacement (b) magnitude and direction of average velocity and (e) the plane s average speed? 33. A plane, diving with constant speed at at angle of 53 with the vertical, releases a projectile at an altitude of 730 m. The projectile hits the ground 5.00 s after release. (a) What is the speed of the plane? (b) How far does the projectile travel horizontally during its flight? What are the (c) horizontal and (d) vertical components of its velocity just before striking the ground? 64. A particle moves horizontally in uniform circular motion, over a horizontal xy plane. At one instant, it moves through the point at coordinates (4.00m, 4.00m) with a velocity of -5.00 î m/s and an acceleration of + 1.5 ĵ m/s. What are the x and y coordinates of the centre of the circular path? 8 14

Solutions 4(a) (10 cm)i r and r ( 10 cm) j. 1 1 r ( 10 cm) ( 10 cm) 14 cm. 10 cm 1 tan 45 or 135. 10 cm 4(b) Dr = 0 cm, IDrI = 0 cm q = 90 4(c) Dr = 0 cm, IDrI = 0 cm q = 0 8(a) r AC r AB r BC (483 km)i (966 km)j 3 rac (483 km) ( 966 km) 1.0810 km. 1 966 km tan 63.4. 483 km (483 km)i (966 km)j (15 km/h)i (49 km/h)j. 8(b) vavg.5 h v (15 km/h) ( 49 km/h) 480 km/h. avg 6.6 east of south 8(c) distance 483 km 966 km speed = 644 km/h. time.5 h r r r ( 10 cm)i ( 10 cm)j. 9 15