An object moving with speed v around a point at distance r, has an angular velocity. m/s m

Similar documents
PHYSICS 1210 Exam 1 University of Wyoming 14 February points

Physics Worksheet Lesson 4: Linear Motion Section: Name:

Physics 101 Lecture 4 Motion in 2D and 3D

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information.

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

A 1.3 m 2.5 m 2.8 m. x = m m = 8400 m. y = 4900 m 3200 m = 1700 m

PHY2048 Exam 1 Formula Sheet Vectors. Motion. v ave (3 dim) ( (1 dim) dt. ( (3 dim) Equations of Motion (Constant Acceleration)

Physics 2A HW #3 Solutions

1. Consider a PSA initially at rest in the beginning of the left-hand end of a long ISS corridor. Assume xo = 0 on the left end of the ISS corridor.

Average & instantaneous velocity and acceleration Motion with constant acceleration

A Kalman filtering simulation

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.

Phys 110. Answers to even numbered problems on Midterm Map

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =

Physics 100: Lecture 1

3 Motion with constant acceleration: Linear and projectile motion

Version 001 test-1 swinney (57010) 1. is constant at m/s.

Motion in a Straight Line

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Chapter 12: Velocity, acceleration, and forces

September 20 Homework Solutions

SOME USEFUL MATHEMATICS

ME 141. Engineering Mechanics

CHAPTER 2: Describing Motion: Kinematics in One Dimension

Lecture 3: 1-D Kinematics. This Week s Announcements: Class Webpage: visit regularly

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

FM Applications of Integration 1.Centroid of Area

Chapter 3 Kinematics in Two Dimensions

CHAPTER 2 KINEMATICS IN ONE DIMENSION ANSWERS TO FOCUS ON CONCEPTS QUESTIONS

t s (half of the total time in the air) d?

Physics for Scientists and Engineers I

Unit 1 Test Review Physics Basics, Movement, and Vectors Chapters 1-3

(c) Several sets of data points can be used to calculate the velocity. One example is: distance speed = time 4.0 m = 1.0 s speed = 4.

Chapter 3: Motion in One Dimension

when t = 2 s. Sketch the path for the first 2 seconds of motion and show the velocity and acceleration vectors for t = 2 s.(2/63)

One-Dimensional Kinematics

Chapter 2 PROBLEM SOLUTIONS

= + t ] can be used to calculate the angular

What distance must an airliner travel down a runway before reaching

Chapter Direct Method of Interpolation

Name: Per: L o s A l t o s H i g h S c h o o l. Physics Unit 1 Workbook. 1D Kinematics. Mr. Randall Room 705

Linear Motion I Physics

e t dt e t dt = lim e t dt T (1 e T ) = 1

NEWTON S SECOND LAW OF MOTION

Introduction to LoggerPro

LAB # 2 - Equilibrium (static)

ES2A7 - Fluid Mechanics Example Classes Example Questions (Set IV)

( ) ( ) ( ) ( u) ( u) = are shown in Figure =, it is reasonable to speculate that. = cos u ) and the inside function ( ( t) du

Magnetostatics Bar Magnet. Magnetostatics Oersted s Experiment

2/5/2012 9:01 AM. Chapter 11. Kinematics of Particles. Dr. Mohammad Abuhaiba, P.E.

Mathematical Modeling

Equations of motion for constant acceleration

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas

Physics 101: Lecture 03 Kinematics Today s lecture will cover Textbook Sections (and some Ch. 4)

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Physics Notes - Ch. 2 Motion in One Dimension

Brock University Physics 1P21/1P91 Fall 2013 Dr. D Agostino. Solutions for Tutorial 3: Chapter 2, Motion in One Dimension

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

Sph3u Practice Unit Test: Kinematics (Solutions) LoRusso

Contraction Mapping Principle Approach to Differential Equations

Temperature Rise of the Earth

CHAPTER 11 PARAMETRIC EQUATIONS AND POLAR COORDINATES

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

T-Match: Matching Techniques For Driving Yagi-Uda Antennas: T-Match. 2a s. Z in. (Sections 9.5 & 9.7 of Balanis)

Physics 218 Exam 1. with Solutions Fall 2010, Sections Part 1 (15) Part 2 (20) Part 3 (20) Part 4 (20) Bonus (5)

HW #1 Solutions. Lewis Structures: Using the above rules, determine the molecular structure for Cl2CO. Hint: C is at the center.

Physics 201 Lecture 2

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf

A B C D September 25 Exam I Physics 105. Circle the letter of the single best answer. Each question is worth 1 point

1. The graph below shows the variation with time t of the acceleration a of an object from t = 0 to t = T. a

( ) 2 a b ab. To do this, we are to use the Ricci identity (which we use to evaluate the RHS) and the properties of the Lie derivative.

6.003 Homework #9 Solutions

Suggested Practice Problems (set #2) for the Physics Placement Test

14. The fundamental theorem of the calculus

Some Basic Information about M-S-D Systems

6.003 Homework #9 Solutions

Two Coupled Oscillators / Normal Modes

Applications of the Basic Equations Chapter 3. Paul A. Ullrich

1. (16 points) Answer the following derivative-related questions. dx tan sec x. dx tan u = du d. dx du tan u. du tan u d v.

Structural Dynamics and Earthquake Engineering

Module II, Part C. More Insight into Fiber Dispersion

4.8 Improper Integrals

Solutions to Problems from Chapter 2

Traveling Waves. Chapter Introduction

KINEMATICS IN ONE DIMENSION

NMR Spectroscopy: Principles and Applications. Nagarajan Murali Advanced Tools Lecture 4

INSTANTANEOUS VELOCITY

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

MATH 124 AND 125 FINAL EXAM REVIEW PACKET (Revised spring 2008)

graph of unit step function t

The law of conservation of mass: Mass can be neither created nor destroyed. It can only be transported or stored.

1. Six acceleration vectors are shown for the car whose velocity vector is directed forward. For each acceleration vector describe in words the

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253

Three Dimensional Coordinate Geometry

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction.

I. OBJECTIVE OF THE EXPERIMENT.

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 10: The High Beta Tokamak Con d and the High Flux Conserving Tokamak.

Transcription:

Roion The mosphere roes wih he erh n moions wihin he mosphere clerly follow cure phs (cyclones, nicyclones, hurricnes, ornoes ec.) We nee o epress roion quniiely. For soli objec or ny mss h oes no isor uring roion, we use he erm ngulr elociy (Greek omeg). Ler, we will ssign he erm oriciy o he roion of flui such s he mosphere. Angulr elociy epresses he re of roion of boy n is efine s he ngle in rins hrough which he boy urns in uni ime. The unis of re herefore rins/secon. Remember hough h rin is frcion of complee reoluion ( rins 360 o ) n i is no funmenl imension (like ime or lengh) h mus be crrie hrough in ny clculion inoling. An objec moing wih spee roun poin isnce r, hs n ngulr elociy r r m/s m s Angulr elociy is ecor quniy. We op he conenion h he ecor ssocie wih he roion is ligne wih he is of roion in he sense of righ-hn screw (he righ hn rule: wih your humb ligne wih is of roion n poining in he irecion of he ecor, your fingers, curling roun he plm of your hn, will gie he irecion of roion).

The ngulr elociy of he erh The erh roes owrs he es n, herefore, he ecor ngulr elociy poins ouwrs from he norh pole (n ino he souh pole). The mgniue of is one reoluion ( rins) per y bu we mus clcule i from he urion of he sierel y, relie o he srs n no o he sun. The sierel y is 3 hrs 56 minues N (3 hrs 56 min) 7.9 0-5 r/s Since mos mosphere moion is prllel o he erh s surfce n he mosphere is ery hin shee encircling he globe, we re concerne primrily wih he mgniue of he componen of he erh s ngulr elociy long he locl ericl irecion. This is roion in locl horizonl plne.

N z is liue ngle z is he locl ericl componen of he ngulr elociy. A he norh pole, z (- he S-pole) A he equor, 0 z In generl, z sin. The Coriolis effec The Coriolis effec is he ppren eiion of ny boy or mss of ir in moion h resuls from he roion of he erh. The mosphere is couple o he erh only hrough griy n fricion he surfce. Oherwise, i is free o moe inepenenly. Any nlysis of he moion of he mosphere in erms of Newon s lws of moion mus be me in frme of reference oriene o he srs (in ineril frme of reference). Howeer, he erh roes in his frme of reference n is herefore non-ineril frme. To compense for he influence of he erh s roion, we inrouce n ppren force, he Coriolis force, h llows us o re he mosphere using he bsic lws of moion. Consier n objec (or mss of ir) moing on surfce h is roing bou some locl ericl is wih ngulr elociy. Suppose he objec is no subjec o ny eernl forces n is hus moing consn spee owrs some reference poin ousie he 3

roing surfce. O A' A,B' B * reference poin (fie sr) A he sr, he poin A is ligne wih he reference poin n he objec hes irecly for i. Howeer, in he inerl of ime i kes for he objec o rech his ril isnce, poin A hs roe o A. The objec rries poin B on he surfce which hs roe o B, in line wih he reference poin. Anlyzing he moion s n obserer on he roing surfce, we woul see he objec moing in cure ph s shown on he plo below. A O B * The cure ph O o B is s seen by he surfce boun obserer, while he srigh line O o B is he ph s iewe by n obserer ousie he roion coorine sysem. The cure ph ppers s eiion o he righ of he moion in his cse in which he roion is niclockwise (s is he roion of he norhern hemisphere). In he roing frme of reference, we cn eplin his moion by inroucing he Coriolis force n Coriolis ccelerion. 4

The mgniue of he Coriolis ccelerion Consier n objec in moion in he norhern hemisphere subjec only o he Coriolis force cing o urn i o he righ from is curren irecion of moion. O << Le Coriolis ccelerion be, hen he isnce rele o he righ where is he rel ime, which cn be rele o he spee of he objec n he isnce rele such h n, herefore Now, he siewys moion cn lso be clcule from he ngulr elociy of he rge bou he origin. Le his ngulr elociy be, hen 5

Equing hese wo epressions for, we obin giing (no moion, no force) If is h ue o he erh s roion bou locl ericl is, such h sin hen ( f sin ) where f sin is clle he Coriolis prmeer Clculing f ifferen liues, Liue f(s - ) 0 0 5 3.8 0-5 30 7.3 0-5 45 0.3 0-5 (mi liues 0-4 ) 60.6 0-5 75 4. 0-5 90 4.6 0-5 (wice ) 6

This ocumen ws cree wih WinPDF ilble hp://www.nepririe.com. The unregisere ersion of WinPDF is for eluion or non-commercil use only.