ESCI 342 Atmospheric Dynamics I Lesson 1 Vectors and Vector Calculus

Similar documents
Review of linear algebra. Nuno Vasconcelos UCSD

Rank One Update And the Google Matrix by Al Bernstein Signal Science, LLC

Physics for Scientists and Engineers I

VECTORS VECTORS VECTORS VECTORS. 2. Vector Representation. 1. Definition. 3. Types of Vectors. 5. Vector Operations I. 4. Equal and Opposite Vectors

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

CENTROID (AĞIRLIK MERKEZİ )

Engineering Tensors. Friday November 16, h30 -Muddy Charles. A BEH430 review session by Thomas Gervais.

ragsdale (zdr82) HW6 ditmire (58335) 1 the direction of the current in the figure. Using the lower circuit in the figure, we get

Abhilasha Classes Class- XII Date: SOLUTION (Chap - 9,10,12) MM 50 Mob no

Effects of polarization on the reflected wave

UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II

Learning Enhancement Team

Quiz: Experimental Physics Lab-I

The Number of Rows which Equal Certain Row

4. Eccentric axial loading, cross-section core

6 Roots of Equations: Open Methods

Remember: Project Proposals are due April 11.

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:

GAUSS ELIMINATION. Consider the following system of algebraic linear equations

CISE 301: Numerical Methods Lecture 5, Topic 4 Least Squares, Curve Fitting

Least squares. Václav Hlaváč. Czech Technical University in Prague

Jens Siebel (University of Applied Sciences Kaiserslautern) An Interactive Introduction to Complex Numbers

Chemical Reaction Engineering

Strong Gravity and the BKL Conjecture

INTRODUCTION TO COMPLEX NUMBERS

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Section 8.3 Polar Form of Complex Numbers

LINEAR ALGEBRA APPLIED

Principle Component Analysis

Definition of Tracking

Chemical Reaction Engineering

Vectors and Tensors. R. Shankar Subramanian. R. Aris, Vectors, Tensors, and the Equations of Fluid Mechanics, Prentice Hall (1962).

Announcements. Image Formation: Outline. The course. Image Formation and Cameras (cont.)

The Fundamental Theorem of Algebra. Objective To use the Fundamental Theorem of Algebra to solve polynomial equations with complex solutions

Chapter I Vector Analysis

Chapter 2. Vectors. 2.1 Vectors Scalars and Vectors

The Schur-Cohn Algorithm

DCDM BUSINESS SCHOOL NUMERICAL METHODS (COS 233-8) Solutions to Assignment 3. x f(x)

Things to Memorize: A Partial List. January 27, 2017

along the vector 5 a) Find the plane s coordinate after 1 hour. b) Find the plane s coordinate after 2 hours. c) Find the plane s coordinate

Work and Energy (Work Done by a Varying Force)

Applied Statistics Qualifier Examination

Lecture 2e Orthogonal Complement (pages )

From Biot-Savart Law to Divergence of B (1)

Physics 201, Lecture 4. Vectors and Scalars. Chapters Covered q Chapter 1: Physics and Measurement.

1 Matrix representations of canonical matrices

INTERPOLATION(1) ELM1222 Numerical Analysis. ELM1222 Numerical Analysis Dr Muharrem Mercimek

Kinematics Quantities. Linear Motion. Coordinate System. Kinematics Quantities. Velocity. Position. Don t Forget Units!

Lecture 4: Piecewise Cubic Interpolation

So far: simple (planar) geometries

COMPLEX NUMBERS INDEX

A general N-dimensional vector consists of N values. They can be arranged as a column or a row and can be real or complex.

12. The Hamilton-Jacobi Equation Michael Fowler

Uniform Circular Motion

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. with respect to λ. 1. χ λ χ λ ( ) λ, and thus:

x=0 x=0 Positive Negative Positions Positions x=0 Positive Negative Positions Positions

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 9

Math1110 (Spring 2009) Prelim 3 - Solutions

CAMBRIDGE UNIVERSITY ENGINEERING DEPARTMENT. PART IA (First Year) Paper 4 : Mathematical Methods

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1

a = Acceleration Linear Motion Acceleration Changing Velocity All these Velocities? Acceleration and Freefall Physics 114

2.12 Pull Back, Push Forward and Lie Time Derivatives

Calculus 2: Integration. Differentiation. Integration

Chapter Runge-Kutta 2nd Order Method for Ordinary Differential Equations

ψ ij has the eigenvalue

13.4 Work done by Constant Forces

( ) ( )()4 x 10-6 C) ( ) = 3.6 N ( ) = "0.9 N. ( )ˆ i ' ( ) 2 ( ) 2. q 1 = 4 µc q 2 = -4 µc q 3 = 4 µc. q 1 q 2 q 3

Demand. Demand and Comparative Statics. Graphically. Marshallian Demand. ECON 370: Microeconomic Theory Summer 2004 Rice University Stanley Gilbert

Partially Observable Systems. 1 Partially Observable Markov Decision Process (POMDP) Formalism

ESCI 241 Meteorology Lesson 0 Math and Physics Review

? plate in A G in

Introduction to Numerical Integration Part II

7.2 Volume. A cross section is the shape we get when cutting straight through an object.

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that

Chapter 2 Introduction to Algebra. Dr. Chih-Peng Li ( 李 )

du = C dy = 1 dy = dy W is invertible with inverse U, so that y = W(t) is exactly the same thing as t = U(y),

AQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

A Family of Multivariate Abel Series Distributions. of Order k

FINITE NEUTROSOPHIC COMPLEX NUMBERS. W. B. Vasantha Kandasamy Florentin Smarandache

CHAPTER 4. Vector Spaces

THE COMBINED SHEPARD ABEL GONCHAROV UNIVARIATE OPERATOR

6.6 The Marquardt Algorithm

Dennis Bricker, 2001 Dept of Industrial Engineering The University of Iowa. MDP: Taxi page 1

8. INVERSE Z-TRANSFORM

Logarithms. Logarithm is another word for an index or power. POWER. 2 is the power to which the base 10 must be raised to give 100.

Physics 2A Chapter 3 HW Solutions

Haddow s Experiment:

Reference. Vector Analysis Chapter 2

1 GSW Iterative Techniques for y = Ax

Many-Body Calculations of the Isotope Shift

Partial Derivatives. Limits. For a single variable function f (x), the limit lim

and that at t = 0 the object is at position 5. Find the position of the object at t = 2.

Quadratic Forms. Quadratic Forms

FUNDAMENTALS ON ALGEBRA MATRICES AND DETERMINANTS

Two Coefficients of the Dyson Product

SCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.

Four Bar Linkages in Two Dimensions. A link has fixed length and is joined to other links and also possibly to a fixed point.

= 1.23 m/s 2 [W] Required: t. Solution:!t = = 17 m/s [W]! m/s [W] (two extra digits carried) = 2.1 m/s [W]

Transcription:

ESI 34 tmospherc Dnmcs I Lesson 1 Vectors nd Vector lculus Reference: Schum s Outlne Seres: Mthemtcl Hndbook of Formuls nd Tbles Suggested Redng: Mrtn Secton 1 OORDINTE SYSTEMS n orthonorml coordnte sstem s one n whch the bss vectors re mutull perpendculr nd re of unt length rtesn coordntes re n orthonorml coordnte sstem where the coordnte lnes re not curved We wll be usng orthonorml coordntes n ths clss (ether rtesn or sphercl coordntes The unt bss vectors for our coordnte sstem re î ĵ nd k whch pont towrd the Est North nd up respectvel VETORS Vectors hve both mgntude (length nd drecton Vectors re denoted b ether wrtng them n boldfce ( or b plcng n rrow over the top ( The mgntude of vector s denoted ether b or Vectors re dded b plcng them hed to tl Vector ddton s ο commuttve: ο ssoctve: ( ( Vectors cn be multpled b sclrs Sclr multplcton s ο ssoctve: m( n n( m mn ο dstrbutve: ( m n m n ; m( m m OMPONENTS vector cn be wrtten n terms of components long the coordnte sstem es

k nd k re the unt vectors (mgntude 1 long the nd es respectvel ο The components of vector m hve negtve vlues For emple veloct 1 1 vector gven b m s V 3m s hs component vectors 1 V m s 1 V 3ms ο We would thnk of V s hvng mgntude of m s 1 nd drecton opposte to î whle V hs mgntude of 3 m s 1 nd n the drecton of ĵ ο nother emple s grvt g whch n component form s g gk We s tht the mgntude of grvt s g nd ts drecton s opposte to k In component form vector ddton s ccomplshed b ddng the components b b b ( ( ( k In component form multplcton b sclr s m m m m k The mgntude of vector s found from ts rtesn components (es re norml to one nother usng the Pthgoren formul DOT PRODUT The dot (or sclr product of two vectors s defned s cosθ where θ s the ngle between the two vectors The result of the dot product s sclr not vector! In component form the dot product s b b b If two vectors re norml ther dot product s ero The dot product s ο commuttve: ο dstrbutve: ( ROSS PRODUT The cross product s defned s snθ u where θ s the ngle between the two vectors nd û s the unt vector perpendculr to both nd n the drecton consstent wth the rght-hnd rule ο Note: In Europen tets the cross product s often denoted usng ^ rther thn

The result of the cross product s vector! If two vectors re prllel ther cross product s ero In orthonorml coordntes the component form the cross product s found b fndng the determnnt of mtr whose frst row s the unt vectors long the es nd the second nd thrd rows re the components of the vectors k b b b b b b ( ( ( k b b b The cross product s not commuttve: The cross product s dstrbutve: ( DERIVTIVES OF VETORS vector functon s vector whose mgntude nd drecton depends upon other sclrs (for emple tme The dervtve of vector functon s wrtten n component form s d d d d d d d k k ds ds ds ds ds ds ds The rules for dfferenttng dot nd cross products re nlogous to the product rule for sclr dfferentton d d d ( ds ds ds d d d ( ds ds ds THE GRDIENT The del opertor n rtesn coordntes s defned s k The del opertor ppled to sclr elds vector tht ponts n the drecton of steepest scent (e vector tht s norml to the contours nd pontng towrd hgher vlues k ο When pplng the del opertor to sclr feld the order of the unt vectors nd the prtl dervtves doesn t mtter Ths s wh ou wll often see k s clled the grdent of Worth repetng: The grdent s vector tht s norml to the contours nd ponts towrd hgher vlues! If the sclr s unform n spce (e hs the sme vlue everwhere then the grdent s ero 3

The del opertor cn lso be ppled to vector (contrr to wht some tetbooks stte the result of whch s second-order tensor When pplng the del opertor to vector t s mportnt to wrte the unt coordnte vectors before ech term rther thn fter t k Ths s becuse the order n whch vectors re drectl multpled s not commuttve (e DIVERGENE The dvergence of vector feld s defned s ο In rtesn coordntes The dvergence s sclr! When meteorologsts spek of dvergence the re referrng to the dvergence of the veloct vector ( V u v w k nd so we usull see dvergence wrtten s u v w V Negtve dvergence s clled convergence ο If ο If V > 0 there s dvergence V < 0 there s convergence The phscl menng of dvergence cn be llustrted s follows If the vector feld s pontng w from pont the dvergence t tht pont s postve If the vector feld s pontng nto pont the dvergence t tht pont s negtve Drecton lone cnnot lws be used to determne dvergence or convergence The vectors m be pontng n the sme drecton nd et hve dvergence or convergence (see llustrtons below 4

5 In mn cses ou cnnot tell ust b lookng whether there s dvergence or convergence For emple the llustrton below shows cse where ou would hve to perform the clcultons to determne the dvergence snce t s not obvous b emnng the feld URL The curl of vector feld s defned s The curl s vector whose components re found b fndng the cross product of the del opertor wth the vector In rtesn coordntes the component form the curl s k k The curl of the veloct vector V s clled vortct THE LPLIN The Lplcn opertor s defned s ο In rtesn coordntes For sclr n rtesn coordntes the Lplcn s For vector n rtesn coordntes the Lplcn s

THE DEL OPERTOR IS LINER ( m n m n ( ( SPHERIL OORDINTES On the Erth t mkes sense to use sphercl coordntes rther thn rtesn coordntes In sphercl coordntes for the Erth the poston of pont s gven b ts dstnce from the center of the Erth r; the lttude φ ; nd the longtude λ ο The unt vectors n sphercl coordntes re the sme s n rtesn coordntes wth î ĵ nd k pontng towrd the Est North nd up respectvel The reltonshps between the coordntes ( nd (r φ λ re d r cosφdλ d rdφ d dr The del opertor n rtesn coordntes s k The del opertor epressed n sphercl coordntes s derved from tht for rtesn coordntes s follows: d λ k d φ k d r λ d φ d r d whch usng the reltonshps n (1 gves 1 1 r cosφ λ r φ k (3 r The choce of whch coordnte sstem to use (rtesn or sphercl s strctl up to us The both hve dvntges nd dsdvntges Sphercl coordntes re ttrctve becuse the Erth s sphercl However the del opertor s more cumbersome n sphercl coordntes nd lso gvng poston n (r φ λ s more cumbersome nd less ntutve thn usng ( Let s fce t rtesn coordntes re smpler nd eser to use nd thnk bout! Plus locll the Erth ppers flt to us Fortuntel we cn stll use sphercl coordntes but epress poston n terms of nd rther thn r φ λ Ths s gong to mke our equtons look ver smlr to rtesn coordntes lthough t wll ntroduce some ddtonl terms clled (1 ( 6

curvture terms nto some of our equtons We wll dscuss these terms s the rse n our studes ο When we use sphercl coordntes but use nd n plce of λ φ nd r we wll cll ths prmetered sphercl coordntes 7

8 EXERIISES Three vectors re gven b k c c c k b b b k 1 Show tht ech of the followng s true: ( ( b ( ( ( c ( ( ( Show tht dt d dt d (remember tht s the mgntude of 3 vector s functon of tme gven b k t t t t 5ln 3 ( 3 Fnd dt d 4 For the followng sclr felds fnd the mgntude of the grdent t the pont ndcted ln ( 3 ; ( (4 b sn cos ( ; ( (0 π 1 c 16 ( ; ( ( - 5 For the followng vector felds fnd the dvergence t the pont ndcted k ln 4 3 ( ; ( (4 b sn cos ( ; ( (0 π 1 c ( ( ( ; ( ( 1

6 The geostrophc wnd s vector feld gven b V u g g v 1 p g where u g fρ 1 p nd v g f ρ Show tht f f nd ρ re constnt then the dvergence of the geostrophc wnd ( V g s ero b In relt f s not constnt but nsted ncreses s ou go north Show tht n ths ( ln f cse the dvergence of the geostrophc wnd s gven b Vg vg c For the followng sobr pttern wll the geostrophc wnd be convergent or dvergent? 7 For the followng vector felds fnd the curl t the pont ndcted ( 3 4 ln k ; ( (4 b ( cos sn ; ( (0 π 1 c ( ( ( ; ( ( 1 8 For the followng sclr felds fnd the Lplcn t the pont ndcted 3 ( ln ; ( (4 b ( cos sn ; ( (0 π 1 c ( 16 ; ( ( - 9

9 Show tht the followng denttes nvolvng the del opertor re true Do ths b wrtng the opertors nd vectors n rtesn coordntes nd showng tht the reltonshps hold ecuse these denttes re wrtten n coordnte-free notton f ou prove them to be true n rtesn coordntes the re true n ll coordntes ( s s s( ( s ( ( ( ( ( ( ( ( ( ( ( ( ( s 0 ( 0 ( ( 10