Excellent web site with information on various methods and numerical codes for scattering by nonspherical particles:

Size: px
Start display at page:

Download "Excellent web site with information on various methods and numerical codes for scattering by nonspherical particles:"

Transcription

1 Lectue 5. Lght catteng and abopton by atmophec patcuate. at 3: Scatteng and abopton by nonpheca patce: Ray-tacng, T- Matx, and FDTD method. Objectve:. Type of nonpheca patce n the atmophee.. Ray-tacng method. 3. Outne of the T-Matx method. 4. Outne of the FDTD method. Requed Readng: L: 5.3, 5.4, 5.5 Advanced/Addtona Readng: Mhchenko, Hovene, and Tav (Ed.) Lght catteng by nonpheca patce. Academc e.. Exceent web te wth nfomaton on vaou method and numeca code fo catteng by nonpheca patce: Type of nonpheca patce n the atmophee. Reca Lectue 4 about popete of atmophec aeoo and ce cyta. Nonpheca aeoo: Dy at (e.g., dy ufate, ntate, ea-at) Dut Cabonaceou In contat to the pheca patce, the catteng popete of nonpheca patce ao depend on hape of the patce and t oentaton wth epect to the ncdent ght beam.

2 Fo nonpheca patce: Reca Lectue 4: In the fa-fed zone (.e., at the age dtance fom a patce), the outon of the vecto wave equaton can be obtaned a (eq.[4.] + = E E S S S S k kz k E E 4 3 ) exp( and fo the Stoke paamete (ee Eq.[4.5] = o o o V U Q I V U Q I 4 σ whee the phae matx = [5.] Oentaton of the patce: Aeoo patce have andom oentaton n pace, wheea the ce cyta ae often oented. Oentaton aveaged catteng phae functon and catteng co ecton ae σ σ = Θ d d )n, ( ), ( ) ( / [5.] σ σ = d d n ), ( / [5.3] whee ` and ` ae the oentaton ange of a nonpheca patce wth epect to ncdent ght beam.

3 . Ray-tacng method. Ray-tacng method (o geometca optc appoxmaton, o ay optc appoxmaton) an appoxmate method fo computng ght catteng by patce much age than a waveength (.e., the maet ze paamete about 8-). Bac pncpe: Ray-tacng method baed on the aumpton that the ncdent EM wave can be epeented a a coecton of ndependent paae ay. Ray tacng commony pefomed ung a Monte Cao appoach. Ray tacng cont of two pat: ) dffacton theoy fo the fowad catteng peak; ) ay tacng ung Fene efecton and tanmon fomua. Advantage: Ray-tacng method can be apped to any hape (pheca o non pheca) Lmtaton: Ray-tacng method an appoxmate by defnton; Lmted ange of ze paamete; Abobng patce eque peca teatment. Dffacton In geometc optc, ght may be teated a ay, except fo Faunhofe dffacton aound a patce. Babnet pncpe- dffacton patten the ame fom an apetue a fo opaque patce of ame ze. 3

4 Integate the fa fed contbuton of ncdent wave ove the apetue E E = exp( kr ) da Rλ Huygen pncpe each pont a ouce of ccua wave font. Fo phee (ccua apetue), the dffacton patten I A 4 I o x J ( x n Θ) ( Θ) = whee k = /λ, and J Bee functon. R k 4 x n Θ [5.4] [5.5] Exampe: catteng dagam fo dffacton by a ccua dk Dffacton peak n phae functon: wdth Θ ~/x, heght () ~x Ft zeo at x nθ = 3.83 and max at x nθ = 5.4 4

5 Fene efecton and tanmon Sne aw gve efacton ange θ t : n θ = m n θ t [5.6] Fene fomua fo poazed efecton amptude coeffcent: co θ m n θ = [5.7] co θ + m n θ m n θ m co θ = [5.8] m n θ + m co θ Refectvty and tanmon coeffcent fo ntenty: R =, R =, T R =, T = R [5.9] NOTE: Fo θ=, efecton m R = => efectvty nceae wth efactve m + ndex 5

6 Dffacton + efecton and efacton Fgue 5. A chematc epeentaton of the component of the phae functon fo andomy oented hexagona ce cyta (fom Lou, 99) 6

7 3. Outne of the T-Matx method. T-Matx method, TMM, enabe cacuaton of optca popete of patce wth otatonay ymmetc hape (uch a epod, ccua cynde, Chebyhev hape, etc.) NOTE: FORTRAN code of TMM openy avaabe at Bac pncpe: TMM baed on expandng the ncdent EM and catteed fed n vecto pheca wave functon. The T matx tanfom the expanon coeffcent of the ncdent fed nto thoe of catteed fed and, f known, can be ued to compute any catteng chaactetc of a nonpheca patce. The eement of the T matx ae ndependent of the ncdent and catteng fed and depend ony on the hape, ze paamete, and efactve ndex of the catteng patce and on t oentaton wth epect to the efeence fame. Advantage: TTM hghy accuate and computatonay fat Lmtaton: Lmted type of patce hape; Lmted ange of ze paamete (x< 3). 4. Outne of the FDTD method. Fnte Dffeence Tme Doman, FDTD, method enabe cacuaton of optca popete of patce of compcated geomete and compoton. Bac pncpe: FDTD ove the Maxwe cu equaton (ft two equaton n eq.[4.] ) n the tme-doman by ntoducng a fnte dffeence anaog. The pace contanng a catteng patce dcetzed by ung a gd meh. The extence of the patce epeented by agnng utabe eectomagnetc contant n tem of pemttvty, pemeabty and conductvty (dependng on patce popete) ove the gd pont. 7

8 Advantage: FDTD can be apped to patce havng any hape and compoton. Lmtaton: Known mpementaton pobem (fo ntance, tacang effect - due to eecton of Catean meh gd) Lmted ange of ze paamete (up to x =5-) Appcaton Ice cyta: Yang and Lou: FDTD fo ze paamete ~5 and ay-tacng (fo x >5) Dut patce: Mhchenko et a.: T-matx apped to a mxtue of epod Kaahnkova and Sokok (): DDA apped to SEM data of dut patce (ee Lectue 6) Soot aeoo: Mackowk et a.: modfed T-matx apped to facta-ke phee cute. 8

9 How to defne an equvaent phee: ze paamete kl 9

Lecture 5. Molecular (Rayleigh) scattering. Scattering and absorption by aerosol and cloud particles: Mie theory.

Lecture 5. Molecular (Rayleigh) scattering. Scattering and absorption by aerosol and cloud particles: Mie theory. Lectue 5. Molecula (Raylegh) catteng. Scatteng and abopton by aeool and cloud patcle: Me theoy.. Bee-Bougue-Lambet law (Extncton law).. Bac of catteng. 3. Molecula (Raylegh) catteng. 4. Popete of aeool

More information

Lecture 4. Beer-Bouger- Lambert law. Molecular (Rayleigh) scattering. Scattering and absorption by aerosol and cloud particles: Mie theory.

Lecture 4. Beer-Bouger- Lambert law. Molecular (Rayleigh) scattering. Scattering and absorption by aerosol and cloud particles: Mie theory. Lectue 4. Bee-Bouge- Lambet law. Molecula (Raylegh) catteng. Scatteng and abopton by aeool and cloud patcle: Me theoy.. Bee-Bougue-Lambet law (Extncton law).. Bac of catteng. 3. Molecula (Raylegh) catteng.

More information

EE 5337 Computational Electromagnetics (CEM)

EE 5337 Computational Electromagnetics (CEM) 7//28 Instucto D. Raymond Rumpf (95) 747 6958 cumpf@utep.edu EE 5337 Computatonal Electomagnetcs (CEM) Lectue #6 TMM Extas Lectue 6These notes may contan copyghted mateal obtaned unde fa use ules. Dstbuton

More information

Section 3. Radiative Transfer

Section 3. Radiative Transfer Secton 3. Radatve Tanfe Refeence Kdde and Vonde Haa: chapte 3 Stephen: chapte, pp. 65-76; chapte 3, pp. 8-87, 99- Lou: chapte ; chapte, pp. 38-4; chapte 3, pp. 53-56, 6-63; chapte 4, pp. 87-93 Lenoble:

More information

MULTIPOLE FIELDS. Multipoles, 2 l poles. Monopoles, dipoles, quadrupoles, octupoles... Electric Dipole R 1 R 2. P(r,θ,φ) e r

MULTIPOLE FIELDS. Multipoles, 2 l poles. Monopoles, dipoles, quadrupoles, octupoles... Electric Dipole R 1 R 2. P(r,θ,φ) e r MULTIPOLE FIELDS Mutpoes poes. Monopoes dpoes quadupoes octupoes... 4 8 6 Eectc Dpoe +q O θ e R R P(θφ) -q e The potenta at the fed pont P(θφ) s ( θϕ )= q R R Bo E. Seneus : Now R = ( e) = + cosθ R = (

More information

1.050 Engineering Mechanics I. Summary of variables/concepts. Lecture 27-37

1.050 Engineering Mechanics I. Summary of variables/concepts. Lecture 27-37 .5 Engneeng Mechancs I Summa of vaabes/concepts Lectue 7-37 Vaabe Defnton Notes & ments f secant f tangent f a b a f b f a Convet of a functon a b W v W F v R Etena wok N N δ δ N Fee eneg an pementa fee

More information

Chapter Fifiteen. Surfaces Revisited

Chapter Fifiteen. Surfaces Revisited Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)

More information

The Backpropagation Algorithm

The Backpropagation Algorithm The Backpopagaton Algothm Achtectue of Feedfowad Netwok Sgmodal Thehold Functon Contuctng an Obectve Functon Tanng a one-laye netwok by teepet decent Tanng a two-laye netwok by teepet decent Copyght Robet

More information

Scattering cross section (scattering width)

Scattering cross section (scattering width) Scatterng cro ecton (catterng wdth) We aw n the begnnng how a catterng cro ecton defned for a fnte catterer n ter of the cattered power An nfnte cylnder, however, not a fnte object The feld radated by

More information

Detection and Estimation Theory

Detection and Estimation Theory ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu

More information

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the

TRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

Lecture Principles of scattering and main concepts.

Lecture Principles of scattering and main concepts. Lectue 15. Light catteing and aboption by atmopheic paticuate. Pat 1: Pincipe of catteing. Main concept: eementay wave, poaization, Stoke matix, and catteing phae function. Rayeigh catteing. Objective:

More information

CHAPTER 4 TWO-COMMODITY CONTINUOUS REVIEW INVENTORY SYSTEM WITH BULK DEMAND FOR ONE COMMODITY

CHAPTER 4 TWO-COMMODITY CONTINUOUS REVIEW INVENTORY SYSTEM WITH BULK DEMAND FOR ONE COMMODITY Unvety of Petoa etd Van choo C de Wet 6 CHAPTER 4 TWO-COMMODITY CONTINUOU REVIEW INVENTORY YTEM WITH BULK DEMAND FOR ONE COMMODITY A modfed veon of th chapte ha been accepted n Aa-Pacfc Jounal of Opeatonal

More information

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage Median Ranked Set Sampling for Estimating the Population Median Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm

More information

Impact of Polarimetric Dimensionality of Forest Parameter Estimation by Means of Polarimetric SAR interferometry

Impact of Polarimetric Dimensionality of Forest Parameter Estimation by Means of Polarimetric SAR interferometry Impact of Polametc Dmensonalty of Foest Paamete Estmaton by Means of Polametc SAR ntefeomety Jun Su Km, Seung-Kuk Lee, Konstantnos Papathanassou, and Iena Hajnsek Geman Aeospace Cente Mcowaves and Rada

More information

19 The Born-Oppenheimer Approximation

19 The Born-Oppenheimer Approximation 9 The Bon-Oppenheme Appoxmaton The full nonelatvstc Hamltonan fo a molecule s gven by (n a.u.) Ĥ = A M A A A, Z A + A + >j j (883) Lets ewte the Hamltonan to emphasze the goal as Ĥ = + A A A, >j j M A

More information

Solving the Dirac Equation: Using Fourier Transform

Solving the Dirac Equation: Using Fourier Transform McNa Schola Reeach Jounal Volume Atcle Solvng the ac quaton: Ung oue Tanfom Vncent P. Bell mby-rddle Aeonautcal Unvety, Vncent.Bell@my.eau.edu ollow th and addtonal wok at: http://common.eau.edu/na Recommended

More information

(8) Gain Stage and Simple Output Stage

(8) Gain Stage and Simple Output Stage EEEB23 Electoncs Analyss & Desgn (8) Gan Stage and Smple Output Stage Leanng Outcome Able to: Analyze an example of a gan stage and output stage of a multstage amplfe. efeence: Neamen, Chapte 11 8.0) ntoducton

More information

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork

Summer Workshop on the Reaction Theory Exercise sheet 8. Classwork Joned Physcs Analyss Cente Summe Wokshop on the Reacton Theoy Execse sheet 8 Vncent Matheu Contact: http://www.ndana.edu/~sst/ndex.html June June To be dscussed on Tuesday of Week-II. Classwok. Deve all

More information

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1 Machne Leanng -7/5 7/5-78, 78, Spng 8 Spectal Clusteng Ec Xng Lectue 3, pl 4, 8 Readng: Ec Xng Data Clusteng wo dffeent ctea Compactness, e.g., k-means, mxtue models Connectvty, e.g., spectal clusteng

More information

Chapter 3 Vector Integral Calculus

Chapter 3 Vector Integral Calculus hapte Vecto Integal alculus I. Lne ntegals. Defnton A lne ntegal of a vecto functon F ove a cuve s F In tems of components F F F F If,, an ae functon of t, we have F F F F t t t t E.. Fn the value of the

More information

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41. Chapte I Matces, Vectos, & Vecto Calculus -, -9, -0, -, -7, -8, -5, -7, -36, -37, -4. . Concept of a Scala Consde the aa of patcles shown n the fgue. he mass of the patcle at (,) can be epessed as. M (,

More information

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation By Rudy A. Gdeon The Unvesty of Montana The Geatest Devaton Coelaton Coeffcent and ts Geometcal Intepetaton The Geatest Devaton Coelaton Coeffcent (GDCC) was ntoduced by Gdeon and Hollste (987). The GDCC

More information

Physics Exam 3

Physics Exam 3 Physcs 114 1 Exam 3 The numbe of ponts fo each secton s noted n backets, []. Choose a total of 35 ponts that wll be gaded that s you may dop (not answe) a total of 5 ponts. Clealy mak on the cove of you

More information

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges wth Modfed Suface-nomal Vectos fo RCS calculaton of Scattees wth Edges and Wedges N. Omak N. Omak, T.Shjo, and M. Ando Dep. of Electcal and Electonc Engneeng, Tokyo Insttute of Technology, Japan 1 Outlne.

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part V: Velocity and Acceleration Analysis of Mechanisms Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.

More information

Variable Structure Control ~ Basics

Variable Structure Control ~ Basics Varable Structure Control ~ Bac Harry G. Kwatny Department of Mechancal Engneerng & Mechanc Drexel Unverty Outlne A prelmnary example VS ytem, ldng mode, reachng Bac of dcontnuou ytem Example: underea

More information

Density Functional Theory I

Density Functional Theory I Densty Functonal Theoy I cholas M. Hason Depatment of Chemsty Impeal College Lonon & Computatonal Mateals Scence Daesbuy Laboatoy ncholas.hason@c.ac.uk Densty Functonal Theoy I The Many Electon Schönge

More information

4 Recursive Linear Predictor

4 Recursive Linear Predictor 4 Recusve Lnea Pedcto The man objectve of ths chapte s to desgn a lnea pedcto wthout havng a po knowledge about the coelaton popetes of the nput sgnal. In the conventonal lnea pedcto the known coelaton

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant

More information

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15, Event Shape Update A. Eveett A. Savn T. Doyle S. Hanlon I. Skllcon Event Shapes, A. Eveett, U. Wsconsn ZEUS Meetng, Octobe 15, 2003-1 Outlne Pogess of Event Shapes n DIS Smla to publshed pape: Powe Coecton

More information

ˆ x ESTIMATOR. state vector estimate

ˆ x ESTIMATOR. state vector estimate hapte 9 ontolle Degn wo Independent Step: Feedback Degn ontol Law =- ame all tate ae acceble a lot of eno ae necea Degn of Etmato alo called an Obeve whch etmate the ente tate vecto gven the otpt and npt

More information

Bayesian Assessment of Availabilities and Unavailabilities of Multistate Monotone Systems

Bayesian Assessment of Availabilities and Unavailabilities of Multistate Monotone Systems Dept. of Math. Unvesty of Oslo Statstcal Reseach Repot No 3 ISSN 0806 3842 June 2010 Bayesan Assessment of Avalabltes and Unavalabltes of Multstate Monotone Systems Bent Natvg Jøund Gåsemy Tond Retan June

More information

3. A Review of Some Existing AW (BT, CT) Algorithms

3. A Review of Some Existing AW (BT, CT) Algorithms 3. A Revew of Some Exstng AW (BT, CT) Algothms In ths secton, some typcal ant-wndp algothms wll be descbed. As the soltons fo bmpless and condtoned tansfe ae smla to those fo ant-wndp, the pesented algothms

More information

Representation of Saturation in Stability Studies

Representation of Saturation in Stability Studies Inteestng summay: https://www.nap.eu/ea/8477/chapte/3 Repesentaton of atuaton n tabty tues Kunu wtes (pg ) that A goous teatment of synchonous machne pefomance ncung satuaton effects s a fute execse. Any

More information

Outline. Basics of interference Types of interferometers. Finite impulse response Infinite impulse response Conservation of energy in beam splitters

Outline. Basics of interference Types of interferometers. Finite impulse response Infinite impulse response Conservation of energy in beam splitters ntefeometes lectue C 566 Adv. Optics Lab Outline Basics of intefeence Tpes of intefeometes Amplitude division Finite impulse esponse nfinite impulse esponse Consevation of eneg in beam splittes Wavefont

More information

Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo

Inference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development

More information

Classical Electrodynamics

Classical Electrodynamics A Fst Look at Quantum Physcs Cassca Eectodynamcs Chapte 4 Mutpoes, Eectostatcs of Macoscopc Meda, Deectcs Cassca Eectodynamcs Pof. Y. F. Chen Contents A Fst Look at Quantum Physcs 4. Mutpoe Expanson 4.

More information

Chapter 23: Electric Potential

Chapter 23: Electric Potential Chapte 23: Electc Potental Electc Potental Enegy It tuns out (won t show ths) that the tostatc foce, qq 1 2 F ˆ = k, s consevatve. 2 Recall, fo any consevatve foce, t s always possble to wte the wok done

More information

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Themodynamcs of solds 4. Statstcal themodynamcs and the 3 d law Kwangheon Pak Kyung Hee Unvesty Depatment of Nuclea Engneeng 4.1. Intoducton to statstcal themodynamcs Classcal themodynamcs Statstcal themodynamcs

More information

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER Edton CAPTER 8 VECTOR MECANCS FOR ENGNEERS: DYNAMCS Fednand P. Bee E. Russell Johnston, J. Lectue Notes: J. Walt Ole Teas Tech Unvest Knematcs of Rgd Bodes n Thee Dmensons 003 The McGaw-ll Companes, nc.

More information

Learning the structure of Bayesian belief networks

Learning the structure of Bayesian belief networks Lectue 17 Leanng the stuctue of Bayesan belef netwoks Mlos Hauskecht mlos@cs.ptt.edu 5329 Sennott Squae Leanng of BBN Leanng. Leanng of paametes of condtonal pobabltes Leanng of the netwok stuctue Vaables:

More information

Exam 1. Sept. 22, 8:00-9:30 PM EE 129. Material: Chapters 1-8 Labs 1-3

Exam 1. Sept. 22, 8:00-9:30 PM EE 129. Material: Chapters 1-8 Labs 1-3 Eam ept., 8:00-9:30 PM EE 9 Mateal: Chapte -8 Lab -3 tandadzaton and Calbaton: Ttaton: ue of tandadzed oluton to detemne the concentaton of an unknown. Rele on a eacton of known tochomet, a oluton wth

More information

Energy in Closed Systems

Energy in Closed Systems Enegy n Closed Systems Anamta Palt palt.anamta@gmal.com Abstact The wtng ndcates a beakdown of the classcal laws. We consde consevaton of enegy wth a many body system n elaton to the nvese squae law and

More information

PHY126 Summer Session I, 2008

PHY126 Summer Session I, 2008 PHY6 Summe Sesson I, 8 Most of nfomaton s avalable at: http://nngoup.phscs.sunsb.edu/~chak/phy6-8 ncludng the sllabus and lectue sldes. Read sllabus and watch fo mpotant announcements. Homewok assgnment

More information

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements

Simulation of Spatially Correlated Large-Scale Parameters and Obtaining Model Parameters from Measurements Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model Paamete fom PER ZETTERBERG Stockholm Septembe 8 TRITA EE 8:49 Simulation of Spatially Coelated Lage-Scale Paamete and Obtaining Model

More information

Histogram Processing

Histogram Processing Hitogam Poceing Lectue 4 (Chapte 3) Hitogam Poceing The hitogam of a digital image with gay level fom to L- i a dicete function h( )=n, whee: i the th gay level n i the numbe of pixel in the image with

More information

Matrix Elements of Many-Electron Wavefunctions. noninteger principal quantum number. solutions to Schröd. Eq. outside sphere of radius r

Matrix Elements of Many-Electron Wavefunctions. noninteger principal quantum number. solutions to Schröd. Eq. outside sphere of radius r 30 - Matx Eements of Many-Eecton Wavefunctons Last tme: ν = R En, f ( ν, ) g ( ν, ) need both f and g to satsfy bounday condton fo E < 0 as ν = n µ πµ s phase shft of f ( ν, ) nonntege pncpa quantum numbe

More information

CS348B Lecture 10 Pat Hanrahan, Spring 2004

CS348B Lecture 10 Pat Hanrahan, Spring 2004 Page 1 Reflecton Models I Today Types of eflecton models The BRDF and eflectance The eflecton equaton Ideal eflecton and efacton Fesnel effect Ideal dffuse Next lectue Glossy and specula eflecton models

More information

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Input to Terminals

Queuing Network Approximation Technique for Evaluating Performance of Computer Systems with Input to Terminals 6th Intenatonal Confeence on Chemcal Agcultual Envonmental and Bologcal cence CAEB-7 Dec. 7-8 07 Pa Fance ueung Netwo Appoxmaton Technque fo Evaluatng Pefomance of Compute ytem wth Input to Temnal Ha Yoh

More information

Question 1: The dipole

Question 1: The dipole Septembe, 08 Conell Univesity, Depatment of Physics PHYS 337, Advance E&M, HW #, due: 9/5/08, :5 AM Question : The dipole Conside a system as discussed in class and shown in Fig.. in Heald & Maion.. Wite

More information

CFAR BI DETECTOR IN BINOMIAL DISTRIBUTION PULSE JAMMING 1. I. Garvanov. (Submitted by Academician Ivan Popchev on June 23, 2003)

CFAR BI DETECTOR IN BINOMIAL DISTRIBUTION PULSE JAMMING 1. I. Garvanov. (Submitted by Academician Ivan Popchev on June 23, 2003) FA BI EEO I BIOMIAL ISIBUIO PULSE JAMMIG I. Gavanov (Submtted by Academcan Ivan Popchev on June 3, 3) Abtact: In many pactcal tuaton, howeve, the envonment peence of tong pule ammng (PJ) wth hgh ntenty;

More information

Effects of Rotor Air-gap Eccentricity on the Power Factor of Squirrel Cage Induction Machines

Effects of Rotor Air-gap Eccentricity on the Power Factor of Squirrel Cage Induction Machines Effect of Roto A-gap Eccentcty on the Powe Facto of Squel Cage Inducton Machne H. Mehgn-Kelk, J. Mlmonfaed Electc Machne and Dve Laboatoy Depament of Electcal Engneeng Amkab Unvety of echnology ehan 594,

More information

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin Some Appoxmate Analytcal Steady-State Solutons fo Cylndcal Fn ANITA BRUVERE ANDRIS BUIIS Insttute of Mathematcs and Compute Scence Unvesty of Latva Rana ulv 9 Rga LV459 LATVIA Astact: - In ths pape we

More information

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =

Fall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) = 8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt

More information

Capítulo. Three Dimensions

Capítulo. Three Dimensions Capítulo Knematcs of Rgd Bodes n Thee Dmensons Mecánca Contents ntoducton Rgd Bod Angula Momentum n Thee Dmensons Pncple of mpulse and Momentum Knetc Eneg Sample Poblem 8. Sample Poblem 8. Moton of a Rgd

More information

Correspondence Analysis & Related Methods

Correspondence Analysis & Related Methods Coespondence Analyss & Related Methods Ineta contbutons n weghted PCA PCA s a method of data vsualzaton whch epesents the tue postons of ponts n a map whch comes closest to all the ponts, closest n sense

More information

Chemical Reaction Engineering

Chemical Reaction Engineering Lectue hemical Reaction Engineeing (RE) is the field that studies the ates and mechanisms of chemical eactions and the design of the eactos in which they take place. Web Lectue lass Lectue 8-husday Multiple

More information

Suppose the medium is not homogeneous (gravity waves impinging on a beach,

Suppose the medium is not homogeneous (gravity waves impinging on a beach, Slowly vaying media: Ray theoy Suppose the medium is not homogeneous (gavity waves impinging on a beach, i.e. a vaying depth). Then a pue plane wave whose popeties ae constant in space and time is not

More information

Review of Vector Algebra and Vector Calculus Operations

Review of Vector Algebra and Vector Calculus Operations Revew of Vecto Algeba and Vecto Calculus Opeatons Tpes of vaables n Flud Mechancs Repesentaton of vectos Dffeent coodnate sstems Base vecto elatons Scala and vecto poducts Stess Newton s law of vscost

More information

CS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks

CS649 Sensor Networks IP Track Lecture 3: Target/Source Localization in Sensor Networks C649 enso etwoks IP Tack Lectue 3: Taget/ouce Localaton n enso etwoks I-Jeng Wang http://hng.cs.jhu.edu/wsn06/ png 006 C 649 Taget/ouce Localaton n Weless enso etwoks Basc Poblem tatement: Collaboatve

More information

Coordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to

Coordinate Geometry. = k2 e 2. 1 e + x. 1 e. ke ) 2. We now write = a, and shift the origin to the point (a, 0). Referred to Coodinate Geomet Conic sections These ae pane cuves which can be descibed as the intesection of a cone with panes oiented in vaious diections. It can be demonstated that the ocus of a point which moves

More information

( ) F α. a. Sketch! r as a function of r for fixed θ. For the sketch, assume that θ is roughly the same ( )

( ) F α. a. Sketch! r as a function of r for fixed θ. For the sketch, assume that θ is roughly the same ( ) . An acoustic a eflecting off a wav bounda (such as the sea suface) will see onl that pat of the bounda inclined towad the a. Conside a a with inclination to the hoizontal θ (whee θ is necessail positive,

More information

Harmonic Curvatures in Lorentzian Space

Harmonic Curvatures in Lorentzian Space BULLETIN of the Bull Malaya Math Sc Soc Secod See 7-79 MALAYSIAN MATEMATICAL SCIENCES SOCIETY amoc Cuvatue Loetza Space NEJAT EKMEKÇI ILMI ACISALIOĞLU AND KĀZIM İLARSLAN Aaa Uvety Faculty of Scece Depatmet

More information

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. Flux: = da i. Force: = -Â g a ik k = X i. Â J i X i (7. Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum

More information

Dynamical Theory of Electron Diffraction. Dr. Hongzhou Zhang SNIAM

Dynamical Theory of Electron Diffraction. Dr. Hongzhou Zhang SNIAM Dynacal Teoy of lecton Dffacton D. Honou Zan oan@tcd.e SNIAM.6 896 4655 Lectue 4 Indexn Dffacton Patten To etod l, caea contant, ato of te dtance ZOLZ opute Poae ttp://ce.epfl.c/people/tadelann/es/ esv3_68.t

More information

A. Thicknesses and Densities

A. Thicknesses and Densities 10 Lab0 The Eath s Shells A. Thcknesses and Denstes Any theoy of the nteo of the Eath must be consstent wth the fact that ts aggegate densty s 5.5 g/cm (ecall we calculated ths densty last tme). In othe

More information

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 7 Maximal score: 25 Points. 1. Jackson, Problem Points.

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 7 Maximal score: 25 Points. 1. Jackson, Problem Points. Physics 505 Eecticity and Magnetism Fa 00 Pof. G. Raithe Pobem et 7 Maxima scoe: 5 Points. Jackson, Pobem 5. 6 Points Conside the i-th catesian component of the B-Fied, µ 0 I B(x) ˆx i ˆx i d (x x ) x

More information

= y and Normed Linear Spaces

= y and Normed Linear Spaces 304-50 LINER SYSTEMS Lectue 8: Solutos to = ad Nomed Lea Spaces 73 Fdg N To fd N, we eed to chaacteze all solutos to = 0 Recall that ow opeatos peseve N, so that = 0 = 0 We ca solve = 0 ecusvel backwads

More information

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.

Objectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms. Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae

More information

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas C:\Dallas\0_Couses\0_OpSci_330\0 Lectue Notes\04 HfkPopagation.doc: Page of 9 Lectue 04: HFK Popagation Physical Optics II (Optical Sciences 330) (Updated: Fiday, Apil 9, 005, 8:05 PM) W.J. Dallas The

More information

Analytical Design of Takagi-Sugeno Fuzzy Control Systems

Analytical Design of Takagi-Sugeno Fuzzy Control Systems 005 Amecan Conto Confeence June 8-0, 005 Potand, OR, USA WeC75 Anaytca Desgn of aag-sugeno uzzy Conto Systems Guang Ren, Zh-Hong Xu Abstact Based on the popetes anayss of aag- Sugeno (-S) fuzzy systems

More information

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3. 3 Eath s Rotaton 3.1 Rotatng Famewok Othe eadng: Valls 2.1, 2.2; Mashall and Plumb Ch. 6; Holton Ch. 2; Schubet Ch. 3 Consde the poston vecto (the same as C n the fgue above) otatng at angula velocty.

More information

4 SingularValue Decomposition (SVD)

4 SingularValue Decomposition (SVD) /6/00 Z:\ jeh\self\boo Kannan\Jan-5-00\4 SVD 4 SngulaValue Decomposton (SVD) Chapte 4 Pat SVD he sngula value decomposton of a matx s the factozaton of nto the poduct of thee matces = UDV whee the columns

More information

Rigid Bodies: Equivalent Systems of Forces

Rigid Bodies: Equivalent Systems of Forces Engneeng Statcs, ENGR 2301 Chapte 3 Rgd Bodes: Equvalent Sstems of oces Intoducton Teatment of a bod as a sngle patcle s not alwas possble. In geneal, the se of the bod and the specfc ponts of applcaton

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS DOING PHYIC WITH MTLB COMPUTTIONL OPTIC FOUNDTION OF CLR DIFFRCTION THEORY Ian Coope chool of Physics, Univesity of ydney ian.coope@sydney.edu.au DOWNLOD DIRECTORY FOR MTLB CRIPT View document: Numeical

More information

1.2 Differential cross section

1.2 Differential cross section .2. DIFFERENTIAL CROSS SECTION Febuay 9, 205 Lectue VIII.2 Diffeential coss section We found that the solution to the Schodinge equation has the fom e ik x ψ 2π 3/2 fk, k + e ik x and that fk, k = 2 m

More information

Aerodynamics. Finite Wings Lifting line theory Glauert s method

Aerodynamics. Finite Wings Lifting line theory Glauert s method α ( y) l Γ( y) r ( y) V c( y) β b 4 V Glauert s method b ( y) + r dy dγ y y dy Soluton procedure that transforms the lftng lne ntegro-dfferental equaton nto a system of algebrac equatons - Restrcted to

More information

3D Sound Source Localization System Based on Learning of Binaural Hearing

3D Sound Source Localization System Based on Learning of Binaural Hearing 3D ound ouce Localzaton ystem Based on Leanng of Bnaual Heang Homch Nakashma BMC Reseach Cente, RIKEN Anagahoa, hmoshdam, Moyama-ku Nagoya 463-0003, Japan nakas@bmc.ken.p Toshhau Muka BMC Reseach Cente,

More information

Revision of Lecture Eight

Revision of Lecture Eight Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Chemical Reaction Engineering

Chemical Reaction Engineering Lectue 3 hemical Reaction Engineeing (RE) is the field that studies the ates and mechanisms of chemical eactions and the design of the eactos in which they take place. Web Lectue 3 lass Lectue 9-Thusday

More information

and decompose in cycles of length two

and decompose in cycles of length two Permutaton of Proceedng of the Natona Conference On Undergraduate Reearch (NCUR) 006 Domncan Unverty of Caforna San Rafae, Caforna Apr - 4, 007 that are gven by bnoma and decompoe n cyce of ength two Yeena

More information

Chapter 16. Fraunhofer Diffraction

Chapter 16. Fraunhofer Diffraction Chapte 6. Faunhofe Diffaction Faunhofe Appoimation Faunhofe Appoimation ( ) ( ) ( ) ( ) ( ) λ d d jk U j U ep,, Hugens-Fesnel Pinciple Faunhofe Appoimation : ( ) ( ) ( ) λ π λ d d j U j e e U k j jk ep,,

More information

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model 6. ntoucton to anssto mples: oncepts an Small-Sgnal Moel Lectue notes: Sec. 5 Sea & Smth 6 th E: Sec. 5.4, 5.6 & 6.3-6.4 Sea & Smth 5 th E: Sec. 4.4, 4.6 & 5.3-5.4 EE 65, Wnte203, F. Najmaba Founaton o

More information

Vector Spherical Harmonics and Spherical Waves

Vector Spherical Harmonics and Spherical Waves DEPARTMENT OF PHYSICS INDIAN INSTITUTE OF TECHNOLOGY, MADRAS PH5020 Eectomagnetic Theoy Mach 2017 by Suesh Govinaajan, Depatment of Physics, IIT Maas Vecto Spheica Hamonics an Spheica Waves Let us sove

More information

Electromagnetic Waves

Electromagnetic Waves Chapte 32 Electomagnetic Waves PowePoint Lectues fo Univesity Physics, Twelfth Edition Hugh D. Young and Roge A. Feedman Lectues by James Pazun Modified P. Lam 8_11_2008 Topics fo Chapte 32 Maxwell s equations

More information

Integral Expression of EM Fields Summary

Integral Expression of EM Fields Summary Integal Expeion of EM Field ummay 5 Integal Expeion of EM Field.doc 08/07/0 5- In tem of tangential and nomal component of E and on a ρ E= jωφ φ φ d + + { jωφ ( nˆ ( nˆ E φ φ ( nˆ E } d ρ = jω φ φ φ d

More information

q-bernstein polynomials and Bézier curves

q-bernstein polynomials and Bézier curves Jounal of Computatonal and Appled Mathematcs 151 (2003) 1-12 q-bensten polynomals and Béze cuves Hall Ouç a, and Geoge M. Phllps b a Depatment of Mathematcs, Dokuz Eylül Unvesty Fen Edebyat Fakültes, Tınaztepe

More information

Note: Please use the actual date you accessed this material in your citation.

Note: Please use the actual date you accessed this material in your citation. MIT OpenCourseWare http://ocw.mt.edu 6.13/ESD.13J Electromagnetcs and Applcatons, Fall 5 Please use the followng ctaton format: Markus Zahn, Erch Ippen, and Davd Staeln, 6.13/ESD.13J Electromagnetcs and

More information

Principles of multiple scattering in the atmosphere. Radiative transfer equation with scattering for solar radiation in a plane-parallel atmosphere.

Principles of multiple scattering in the atmosphere. Radiative transfer equation with scattering for solar radiation in a plane-parallel atmosphere. Lectue 7 incipes of utipe scatteing in the atosphee. Raiative tansfe equation with scatteing fo soa aiation in a pane-paae atosphee. Objectives:. Concepts of the iect an iffuse scattee soa aiation.. Souce

More information

Closed-loop adaptive optics using a CMOS image quality metric sensor

Closed-loop adaptive optics using a CMOS image quality metric sensor Closed-loop adaptve optcs usng a CMOS mage qualty metc senso Chueh Tng, Mchael Gles, Adtya Rayankula, and Pual Futh Klpsch School of Electcal and Compute Engneeng ew Mexco State Unvesty Las Cuces, ew Mexco

More information

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 29,

Chapter IV Vector and Tensor Analysis IV.2 Vector and Tensor Analysis September 29, hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe 9, 08 47 hapte I ecto and Tenso Analyss I. ecto and Tenso Analyss eptembe 9, 08 48 I. ETOR AND TENOR ANALYI I... Tenso functon th Let A

More information

Phong Model. Reflection Models

Phong Model. Reflection Models Page 1 Reflecton Models Last lectue Reflecton models The eflecton equaton and the BRDF Ideal eflecton, efacton and dffuse Today Phong and mcofacet models Gaussan heght suface Self-shadowng Toance-Spaow

More information

11/13/ LASER Physics. Light Amplification and Inversion. Outline: Biomedical Optics LASER. Atomic Energy States: 2 Level System

11/13/ LASER Physics. Light Amplification and Inversion. Outline: Biomedical Optics LASER. Atomic Energy States: 2 Level System /3/8 Outlne: omedcal Optcs. SE Physcs ompute sssted lncal Medcne Medcal Faculty Mannhem Hedelbeg Unvesty TheodoKutzeUe 3 6867 Mannhem, Gemany Smon Hubetus, M.Sc. smon.hubetus@medma.unhedelbeg.de www.ma.unhedelbeg.de/nst/cbtm/ckm.

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

ME 425: Aerodynamics

ME 425: Aerodynamics ME 5: Aeodynamics D ABM Toufique Hasan Pofesso Depatment of Mechanical Engineeing, BUET Lectue- 8 Apil 7 teachebuetacbd/toufiquehasan/ toufiquehasan@mebuetacbd ME5: Aeodynamics (Jan 7) Flow ove a stationay

More information

Problem 1: To prove that under the assumptions at hand, the group velocity of an EM wave is less than c, I am going to show that

Problem 1: To prove that under the assumptions at hand, the group velocity of an EM wave is less than c, I am going to show that PHY 387 K. Solutons for problem set #7. Problem 1: To prove that under the assumptons at hand, the group velocty of an EM wave s less than c, I am gong to show that (a) v group < v phase, and (b) v group

More information