Kinematics in 2-D (II)

Similar documents
Physics 111 Lecture 5 Circular Motion

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Relative motion (Translating axes)

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1

Physics 101 Lecture 6 Circular Motion

3.2 Centripetal Acceleration

PS113 Chapter 5 Dynamics of Uniform Circular Motion

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Physics 201, Lecture 6

Uniform Circular Motion

Phys 201A. Homework 5 Solutions

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

Describing Circular motion

6.4 Period and Frequency for Uniform Circular Motion

ω = θ θ o = θ θ = s r v = rω

Sections and Chapter 10

Chapter 5. Uniform Circular Motion. a c =v 2 /r

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving

Centripetal Force. Lecture 11. Chapter 8. Course website:

r cos, and y r sin with the origin of coordinate system located at

Chapter 5: Uniform Circular Motion

Name. Date. Period. Engage Examine the pictures on the left. 1. What is going on in these pictures?

Ch04: Motion in two and three dimensions (2D and 3D)

Circular Motion. Mr. Velazquez AP/Honors Physics

Objective Notes Summary

Uniform Circular Motion

Motion in Two Dimensions

Chapter 12: Kinematics of a Particle 12.8 CURVILINEAR MOTION: CYLINDRICAL COMPONENTS. u of the polar coordinate system are also shown in

Uniform Circular Motion

Chapter 8. Accelerated Circular Motion

Chapter 7-8 Rotational Motion

Physics 107 TUTORIAL ASSIGNMENT #8

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?

PHYSICS 220. Lecture 08. Textbook Sections Lecture 8 Purdue University, Physics 220 1

DYNAMICS OF UNIFORM CIRCULAR MOTION

4. Two and Three Dimensional Motion

Motion in a Plane Uniform Circular Motion

Motions and Coordinates

Chapter 12. Kinetics of Particles: Newton s Second Law

INTRODUCTION. 2. Vectors in Physics 1

Rotational Motion. Every quantity that we have studied with translational motion has a rotational counterpart

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed?

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.

Physics 207 Lecture 5. Lecture 5

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.

Chapters 5-8. Dynamics: Applying Newton s Laws

Chap 5. Circular Motion: Gravitation

PHYS 1114, Lecture 21, March 6 Contents:

Physics 201 Homework 4

PHYS Summer Professor Caillault Homework Solutions. Chapter 9

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Physics 231 Lecture 17

Translation and Rotation Kinematics

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion

MCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.

constant t [rad.s -1 ] v / r r [m.s -2 ] (direction: towards centre of circle / perpendicular to circle)

Chapter 13 Gravitation

Momentum is conserved if no external force

Circular motion. Objectives. Physics terms. Assessment. Equations 5/22/14. Describe the accelerated motion of objects moving in circles.

Kinematics of rigid bodies

Written as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.

Physics 2112 Unit 14

MAGNETIC FIELD INTRODUCTION

Flux. Area Vector. Flux of Electric Field. Gauss s Law

ISSUED BY K V - DOWNLOADED FROM CIRCULAR MOTION

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Quiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible)

PHYS Summer Professor Caillault Homework Solutions. Chapter 5

Physics 2001 Problem Set 5 Solutions

rt () is constant. We know how to find the length of the radius vector by r( t) r( t) r( t)

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

Physics 181. Assignment 4

When a mass moves because of a force, we can define several types of problem.

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature)

Circular-Rotational Motion Mock Exam. Instructions: (92 points) Answer the following questions. SHOW ALL OF YOUR WORK.

7.2. Coulomb s Law. The Electric Force

b) (5) What average force magnitude was applied by the students working together?

Spring 2001 Physics 2048 Test 3 solutions

Chapter 4. Newton s Laws of Motion

Newton s Laws, Kepler s Laws, and Planetary Orbits

21 MAGNETIC FORCES AND MAGNETIC FIELDS

Δt The textbook chooses to say that the average velocity is

Chapter 5. Applying Newton s Laws. Newton s Laws. r r. 1 st Law: An object at rest or traveling in uniform. 2 nd Law:

Fri Angular Momentum Quiz 10 RE 11.a; HW10: 13*, 21, 30, 39 Mon , (.12) Rotational + Translational RE 11.b Tues.

Look over Chapter 22 sections 1-8 Examples 2, 4, 5, Look over Chapter 16 sections 7-9 examples 6, 7, 8, 9. Things To Know 1/22/2008 PHYS 2212

PHYSICS NOTES GRAVITATION


3.3 Centripetal Force

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY

The study of the motion of a body along a general curve. the unit vector normal to the curve. Clearly, these unit vectors change with time, u ˆ

Chapter 5 Force and Motion

Relative motion. measurements by taking account of the motion of the. To apply Newton's laws we need measurements made

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

Chapter 5 Force and Motion

Chapter. s r. check whether your calculator is in all other parts of the body. When a rigid body rotates through a given angle, all

AP Physics 1 - Circular Motion and Gravitation Practice Test (Multiple Choice Section) Answer Section

FREE Download Study Package from website: &

Related Rates - the Basics

Transcription:

Kinematics in 2-D (II) Unifom cicula motion Tangential and adial components of Relative velocity and acceleation a Seway and Jewett 4.4 to 4.6 Pactice Poblems: Chapte 4, Objective Questions 5, 11 Chapte 4, Poblems 39, 41, 43, 47, 53, 79 Physics 1D03 - Lectue 6

Unifom Cicula Motion unifom means constant speed v velocity v changes (diection changes) acceleation : find v by subtacting vectos, a v lim t 0 t = 1) Is v t as t 0? 2) What is the value of v/ t, as t 0? v 1 1 2 v 2 cente Physics 1D03 - Lectue 6

Subtact velocities: v 1 θ v 2 v v 1 1 2 θ v 2 Compae with displacements: Simila tiangles, 1 2 θ v v Note v is pependicula to = Physics 1D03 - Lectue 6

Fom pevious slide: as t 0, v a t v = v, v t v and so a = v 2 Diection: Since v is pependicula to, a is pependicula to v So, a is towads the cente of the cicle ( centipetal ). Physics 1D03 - Lectue 6

In geneal, diection and speed both change: v 1 v 2 v 1 v v = v 2 v1 2 v has components paallel and pependicula to dv v the motion ; and a = dt t Physics 1D03 - Lectue 6

The adial (centipetal) component is due to the change in diection. a a t a a = v 2, pependicula to path The tangential component (tangent to the path) is equal to the ate of change of speed: d v a t = dt Physics 1D03 - Lectue 6

Concept Quiz You ae diving at constant speed aound a cuve. Seeing a ada tap, you apply the bakes. Compae the magnitude of you acceleation just befoe and just afte you apply the bakes : a) a is zeo befoe, and non-zeo afte b) a is not zeo befoe, and inceases immediately as you apply the bakes c) a is not zeo befoe, and deceases immediately as you apply the bakes Physics 1D03 - Lectue 6

Relative Motion Example: A wasp is flying fom noth to south at 30 km/h. You ae iding you bicycle notheast at 20 km/h. What is the velocity of the wasp elative to you? If it acceleates, what is its acceleation elative to you? Thee ae two efeence fames (coodinate axes) fo measuing fom: the gound, and the bicycle. At left ae the velocities elative to the gound. How do these look elative to the bicycle? bicycle v b, g waspv w, g Physics 1D03 - Lectue 6

Ty an easie poblem in one dimension : Wind blows southwads, bicycle tavels noth. A cyclist iding at 20 km/h diectly into a 30 km/h wind should feel a 50 km/h headwind. In tems of vectos : v w, b = v w, g vb, g v w, g v b, g v w, b Use the same equation in two o thee dimensions. Re-daw the diagam and solve the oiginal poblem. Physics 1D03 - Lectue 6

Quiz: A wasp is flying fom noth to south at 30 km/h. You ae iding you bicycle notheast at 20 km/h. What is the velocity of the wasp elative to you? Which vecto diagam shows the thee velocities coectly? (The ed vecto is the velocity of the wasp elative to you). A B C D Physics 1D03 - Lectue 6

Suppose we have a stationay efeence fame (axes x,y), and anothe efeence fame x', y' moving at velocity v 0. The elative displacement of the two sets of axes is 0 (which changes with time). The positions ae elated by = + 0 Diffeentiate to get velocities: v = v + v 0 Diffeentiate again. If v 0 is constant, y y' v 0 paticle a = a o x x' The acceleation of a paticle appeas the same in both efeence fames! Physics 1D03 - Lectue 6

Inetial Fames A efeence fame in which Newton s Laws ae tue is called an Inetial Fame. Since Newton s mechanics is based on acceleation (and on elative positions), any fame moving at constant velocity is an inetial fame Physics looks the same in all inetial fames. ( Galileo s Pinciple of Relativity? ) Physics 1D03 - Lectue 6

Dopping a suga cube into a coffee cup in an aiplane taveling 600 km/h. But: Example Dopping a suga cube in a tain going aound a cuve. cube falls vetically cube moves away?? View fom inetial fame (top view) cup follows cuve (away fom cube) cube goes staight Physics 1D03 - Lectue 6

Concept Quiz Bicycle wheel, adius = 35 cm, speed = 10 m/s 2 and acceleation ( 10 m/s ) 2 = 286 m/s = 29 g 0.35m What about a paint spot on the im at its lowest point (almost in contact with the gound, momentaily stationay)? What is a fom the point of view of the ide, and of an ant about to be un ove? a) Both see an upwad acceleation of 29 g b) The ide sees a = 29 g [up], ant sees zeo c) Both see zeo acceleation momentaily Physics 1D03 - Lectue 6

Discussion : what does the motion (position and velocity) of the paint spot look like to the ant? Conside only the shot inteval of time stating and ending when the tie is a few millimetes above the ant. (you may assume the ant is in a small hole in the oad and isn t squashed --- no insects wee hamed in this example) Physics 1D03 - Lectue 6

Summay Acceleation has a tangential component (paallel to motion) and a adial component (pependicula to the motion) a t = ate of incease of speed v = towads the cente of the cicle o ac Inetial efeence fames move at constant velocity elative to a 2 each othe Acceleation is the same in all inetial fames, velocities obey : v a, b + vb, c = va, c Physics 1D03 - Lectue 6