Image Reconstruction in Photoacoustic Tomography taking acoustic attenuation into account

Size: px
Start display at page:

Download "Image Reconstruction in Photoacoustic Tomography taking acoustic attenuation into account"

Transcription

1 Imag Rcostructio i Photoacoustic Tomography takig acoustic attuatio ito accout Ptr Burghozr Rsarch Ctr for No Dstructiv Tstig GmbH, Liz, Austria Ti Fbruary 9: Uppr Austria Rsarch GmbH, Liz, Austria Sit RECENDT 9 Ptr Burghozr Outi! Photoacoustic Imagig! Acoustic attuatio! Stoks quatio! Attuatio i tissu: powr aw dpdc! Ivrsio! Hat diffusio quatio! Soutio i k-spac! Ivrsio! Rguarizatio mthods! Etropy productio ad iformatio oss! Cocusio ad Outook Sit RECENDT 9 Ptr Burghozr

2 Imagig tchiqus X-ray utrasoud ight Sit 3 RECENDT 9 Ptr Burghozr Sit 4 RECENDT 9 Ptr Burghozr

3 Sit 5 RECENDT 9 Ptr Burghozr Mod basd tim rvrsa mthod P. Burghozr, G. J. Matt, M. Hatmir, ad G. Patauf, Exact ad approximativ imagig mthods for photoacoustic tomography usig a arbitrary dtctio surfac, Physica Rviw E 75, 7 Sit 6 RECENDT 9 Ptr Burghozr 3

4 Stoks quatio i! Kx% $ t" ikx % i$ t %# x " pa wavs: p & p & p " With compx K(!) = k(!) + i "(!) =!/c(!) + i "(!) " k(!), "(!) hav to satisfy Kramrs-Kröig-Ratios ".g. Stoks quatio: dsity chag foows prssur chag with a raxatio tim # ( p % c ' ' t p ) ' p ( & ' t p c '* ( ' t Stoks quatio + Rxatio tim # $ 3 # & c k $ 3 & c %. A A / ). A A / with A - ) $ + for $+,, : $ + # 4 c $ % k $ +. c 8 / Sit 7 RECENDT 9 Ptr Burghozr Photoacoustic imagig with tim rvrsa accoutig for acoustic attuatio " (a) Prssur simuatio rsuts for # =. ad c= " (b), (c) Rcostructios with tim rvrsa without ad with compsatio of attuatio " (d) Rcostructio profi aog horizota dashd i P. Burghozr t a., Compsatio of acoustic attuatio for high-rsoutio photoacoustic imagig with i dtctors usig tim rvrsa Proc. SPIE , Photoics Wst, BIOS 7 Sit 8 RECENDT 9 Ptr Burghozr 4

5 Examp for Stoks quatio: Oi # = 7 ps Micha J. Buckigham., Causaity, Stoks wav quatio, ad acoustic pus propagatio i a viscous fuid, Phys. Rv. E 7, 5 Sit 9 RECENDT 9 Ptr Burghozr PA sigas i oi mm from icusio $ ~ 5 6 ick ( ) t p( r, $ ) & pida! r, t" $ c K % 6 ( $ ) dt Rivir, Zhag, ad Aastasio, Optics Lttrs (6). Diamtr. mm c t p ( r ) p( r, 3D Sit RECENDT 9 Ptr Burghozr 5

6 Ivrsio: rguarizatio with SVD for oisy sigas % ois.% ois.% ois.% ois Sit RECENDT 9 Ptr Burghozr Tim dampd soutios Two possib soutios of th wav quatio ar: "! ra, K(!) = k(!) + i "(!) =!/c(!) + i "(!) compx, dscribs a statioary wav dampd i spac. " k ra, $ (k) =!(k) - i!(k) compx, dscribs a stadig wav (.g. i a asr rsoator) dampd i tim. p ( r ) p( r, Ra spac FT IFT pˆ ( r) Tim t pˆ ( r) % i$ t %7 t Fourir spac Sit RECENDT 9 Ptr Burghozr 6

7 Exprimta Dtrmiatio of Attuatio Sit 3 RECENDT 9 Ptr Burghozr Attuatio i tissu " For tissu: # y! $ " 8 # $ with y 8 Kda R. Watrs, Micha S. Hughs, Jo Moby & Jams G. Mir; Diffrtia Forms of th Kramrs-Kröig Disprsio Ratios; IEEE Trasactios o Utrasoics, Frroctrics, ad Frqucy Cotro, Vo. 5, No., Jauary 3, c! $ " c! $ " y% y! $ % $ " 3 9 % & ) # ta y. / for y= c & c % # $ $! $ "! $ " 9 Sit 4 RECENDT 9 Ptr Burghozr 7

8 Ifuc of Attuatio i D, D ad 3D Attuatio i huma fat:.6 db MHz - cm - ; dtctor distac is mm (3 db MHz - cm - i huma drmis) p ( x ) Layr with thickss. mm k x p ( r ) Diamtr. mm Diamtr. mm c t p ( r ) c t D c t p( x, p( r, D p( r, 3D Sit 5 RECENDT 9 Ptr Burghozr Acoustic attuatio i various dimsios D D 3D Sit 6 RECENDT 9 Ptr Burghozr 8

9 Th ifuc of disprsio! Iitia prssur distributio: sphrica absorbr (diamtr.mm)! Simuatio rsuts at a distac of mm i huma fat gctig disprsio (gr) ad takig disprsio ito accout (rd)! Rcostructio of th iitia prssur distributio from abov dtctor sigas gctig disprsio (gr) ad takig disprsio ito accout (rd) Sit 7 RECENDT 9 Ptr Burghozr Ivrsio: rguarizatio with SVD for oisy sigas % ois.% ois.% ois thrma ois Sit 8 RECENDT 9 Ptr Burghozr 9

10 D hat diffusio quatio ' T & # ( T ' t Fourir 83, or.g. Madis t a. "..thrma diffusivity Iitia vaus: T ( x, t & ) & T ( x) ' Numa boudary coditios: T & for x & ad x & ' x Usuay sovd by tmpora Fourir trasform # Hmhotz quatio with soutios: < cos( ; x % $ # or spatia Fourir trasform, (costrasform).g. by Brosti: T ( x, & : b cos( kx), with 6 % k # t k b & 5 T ( x dx ) & b & 5T ( x)cos( kx) dx, &,,3,... $ x # T ~ $! 9 & Sit 9 RECENDT 9 Ptr Burghozr T ( x, t & ) & T ( x) T ( x, Costrasform b Tim t A U b Ivrs Cos-trasform % k # t 9, with k & T ( x &, & T ( S Sit RECENDT 9 Ptr Burghozr

11 D hat diffusio quatio: tim rvrsa T ( x, t & ) & T ( x) T ( x, Ivrs Cos-trasform b ) k # t 9, with k & Iv(U) Tim t Iv(A) b Costrasform Sit RECENDT 9 Ptr Burghozr SVD ad Tikhoov rguarizatio mthod i k-spac k # t b t & % ( ) b (), with k & bt & Atb A & diag(xp( % k SVD: = C b () & B =A 9 ) k # t b (, for D i? s => t # ) Tikhoov: t t mi(( A t b % b t ) ) 7b ) At bt & ( At At ) 7E) b % k # t b ( ) & b ( % k # t ) 7 Sit RECENDT 9 Ptr Burghozr

12 SVD ad Tikhoov rguarizatio mthod i k-spac () (b Tmpratur (ad aso prssur) ar ma vaus Statistica fuctuatios: (( T ) & kbt C Sit 3 RECENDT 9 Ptr Burghozr Cocusios Dissipatio causs: $ Etropy productio $ Fuctuatios: usig ths as ois v th rcostructd imag shows a oss of iformatio which is qua to th tropy productio (at ast for th D hat diffusio quatio). Sit 4 RECENDT 9 Ptr Burghozr

13 Outook! Hat diffusio quatio: D ad 3D! Prssur wavs takig acoustic attuatio ito accout! fuctuatio dissipatio thorm from statistica physics dscribs i a vry gra way how fuctuatios ad tropy productio ar ratd. Thrfor it shoud b possib to graiz th rsuts foud for D tmpratur profis. Sit 5 RECENDT 9 Ptr Burghozr Ackowdgmts This work has b supportd by th Austria Scic Fud (FWF), projct umbrs S53-N ad S5-N, by th Europa Rgioa Dvopmt Fud (EFRE) i th framwork of th EU-programm Rgio 3, ad th fdra stat Uppr Austria. Sit 6 RECENDT 9 Ptr Burghozr 3

14 thak you for your atttio Sit 7 RECENDT 9 Ptr Burghozr 4

Zero Point Energy: Thermodynamic Equilibrium and Planck Radiation Law

Zero Point Energy: Thermodynamic Equilibrium and Planck Radiation Law Gaug Institut Journa Vo. No 4, Novmbr 005, Zro Point Enrgy: Thrmodynamic Equiibrium and Panck Radiation Law Novmbr, 005 vick@adnc.com Abstract: In a rcnt papr, w provd that Panck s radiation aw with zro

More information

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

Solid State Device Fundamentals

Solid State Device Fundamentals 8 Biasd - Juctio Solid Stat Dvic Fudamtals 8. Biasd - Juctio ENS 345 Lctur Cours by Aladr M. Zaitsv aladr.zaitsv@csi.cuy.du Tl: 718 98 81 4N101b Dartmt of Egirig Scic ad Physics Biasig uiolar smicoductor

More information

Ideal crystal : Regulary ordered point masses connected via harmonic springs

Ideal crystal : Regulary ordered point masses connected via harmonic springs Statistical thrmodyamics of crystals Mooatomic crystal Idal crystal : Rgulary ordrd poit masss coctd via harmoic sprigs Itratomic itractios Rprstd by th lattic forc-costat quivalt atom positios miima o

More information

Quasi-Supercontinuum Interband Lasing Characteristics of Quantum Dot Nanostructures

Quasi-Supercontinuum Interband Lasing Characteristics of Quantum Dot Nanostructures USOD 008 ottiha UK Quasi-Suprcotiuu Itrbad Lasi Charactristics of Quatu Dot aostructurs C. L. a Y. Wa H. S. Di B. S. Ooi Ctr for Optica choois ad Dpartt of ctrica ad Coputr iri Lhih Uivrsity Bthh Psyvaia

More information

S- AND P-POLARIZED REFLECTIVITIES OF EXPLOSIVELY DRIVEN STRONGLY NON-IDEAL XENON PLASMA

S- AND P-POLARIZED REFLECTIVITIES OF EXPLOSIVELY DRIVEN STRONGLY NON-IDEAL XENON PLASMA S- AND P-POLARIZED REFLECTIVITIES OF EXPLOSIVELY DRIVEN STRONGLY NON-IDEAL XENON PLASMA Zaporozhts Yu.B.*, Mitsv V.B., Gryazov V.K., Riholz H., Röpk G. 3, Fortov V.E. 4 Istitut of Problms of Chmical Physics

More information

Intro to QM due: February 8, 2019 Problem Set 12

Intro to QM due: February 8, 2019 Problem Set 12 Intro to QM du: Fbruary 8, 9 Prob St Prob : Us [ x i, p j ] i δ ij to vrify that th anguar ontu oprators L i jk ɛ ijk x j p k satisfy th coutation rations [ L i, L j ] i k ɛ ijk Lk, [ L i, x j ] i k ɛ

More information

Control systems (Lecture #11)

Control systems (Lecture #11) .5 Cotro sstms (Lctur #) Last tim, Cotroabiit ad obsrvabiit (Chaptr ) Two approachs to stat fdback dsig (Chaptr 8) Usig cotroab caoica form B sovig matri quatios Toda, w cotiu to work o fdback dsig (Chaptr

More information

ERROR CONTROL FOR TIME-SPLITTING SPECTRAL APPROXIMATIONS OF THE SEMICLASSICAL SCHRÖDINGER EQUATION. 1. Introduction

ERROR CONTROL FOR TIME-SPLITTING SPECTRAL APPROXIMATIONS OF THE SEMICLASSICAL SCHRÖDINGER EQUATION. 1. Introduction ERROR CONTROL FOR TME-SPLTTNG SPECTRAL APPROXMATONS OF THE SEMCLASSCAL SCHRÖDNGER EQUATON RENE KYZA, CHARALAMBOS MAKRDAKS, AND MCHAEL PLEXOUSAKS Abstract. W prov a postriori rror stimats of optima ordr

More information

Figure 2-18 Thevenin Equivalent Circuit of a Noisy Resistor

Figure 2-18 Thevenin Equivalent Circuit of a Noisy Resistor .8 NOISE.8. Th Nyquist Nois Thorm W ow wat to tur our atttio to ois. W will start with th basic dfiitio of ois as usd i radar thory ad th discuss ois figur. Th typ of ois of itrst i radar thory is trmd

More information

Discrete Fourier Transform (DFT)

Discrete Fourier Transform (DFT) Discrt Fourir Trasorm DFT Major: All Egirig Majors Authors: Duc guy http://umricalmthods.g.us.du umrical Mthods or STEM udrgraduats 8/3/29 http://umricalmthods.g.us.du Discrt Fourir Trasorm Rcalld th xpotial

More information

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting

Mixed Mode Oscillations as a Mechanism for Pseudo-Plateau Bursting Mixd Mod Oscillatios as a Mchaism for Psudo-Platau Burstig Richard Brtram Dpartmt of Mathmatics Florida Stat Uivrsity Tallahass, FL Collaborators ad Support Thodor Vo Marti Wchslbrgr Joël Tabak Uivrsity

More information

Introduction to Quantum Information Processing. Overview. A classical randomised algorithm. q 3,3 00 0,0. p 0,0. Lecture 10.

Introduction to Quantum Information Processing. Overview. A classical randomised algorithm. q 3,3 00 0,0. p 0,0. Lecture 10. Itroductio to Quatum Iformatio Procssig Lctur Michl Mosca Ovrviw! Classical Radomizd vs. Quatum Computig! Dutsch-Jozsa ad Brsti- Vazirai algorithms! Th quatum Fourir trasform ad phas stimatio A classical

More information

= (3) family of spreading sequences. The dimension of an Oppermann set with the code length of N is determined by

= (3) family of spreading sequences. The dimension of an Oppermann set with the code length of N is determined by (EUSIPCO Europa Siga Procssig Cofrc, Gasgow, Aug. 9 Improv Corratio of Graiz DFT with oiar Phas for OFD a CDA Commuicatios Ai. Aasu a Haa Agirma-Tosu w Jrsy Istitut of Tchoogy Dpartmt of Ectrica & Computr

More information

ECE594I Notes set 6: Thermal Noise

ECE594I Notes set 6: Thermal Noise C594I ots, M. odwll, copyrightd C594I Nots st 6: Thrmal Nois Mark odwll Uivrsity of Califoria, ata Barbara rodwll@c.ucsb.du 805-893-344, 805-893-36 fax frcs ad Citatios: C594I ots, M. odwll, copyrightd

More information

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms Math Sci Ltt Vol No 8-87 (0) adamard Exotial al Matrix, Its Eigvalus ad Som Norms İ ad M bula Mathmatical Scics Lttrs Itratioal Joural @ 0 NSP Natural Scics Publishig Cor Dartmt of Mathmatics, aculty of

More information

Chapter Discrete Fourier Transform

Chapter Discrete Fourier Transform haptr.4 Dscrt Fourr Trasform Itroducto Rcad th xpota form of Fourr srs s Equatos 8 ad from haptr., wt f t 8, h.. T w t f t dt T Wh th abov tgra ca b usd to comput, h.., t s mor prfrab to hav a dscrtzd

More information

MILLIKAN OIL DROP EXPERIMENT

MILLIKAN OIL DROP EXPERIMENT 11 Oct 18 Millika.1 MILLIKAN OIL DROP EXPERIMENT This xprimt is dsigd to show th quatizatio of lctric charg ad allow dtrmiatio of th lmtary charg,. As i Millika s origial xprimt, oil drops ar sprayd ito

More information

Discrete Fourier Series and Transforms

Discrete Fourier Series and Transforms Lctur 4 Outi: Discrt Fourir Sris ad Trasforms Aoucmts: H 4 postd, du Tus May 8 at 4:3pm. o at Hs as soutios wi b avaiab immdiaty. Midtrm dtais o t pag H 5 wi b postd Fri May, du foowig Fri (as usua) Rviw

More information

15/03/1439. Lectures on Signals & systems Engineering

15/03/1439. Lectures on Signals & systems Engineering Lcturs o Sigals & syms Egirig Dsigd ad Prd by Dr. Ayma Elshawy Elsfy Dpt. of Syms & Computr Eg. Al-Azhar Uivrsity Email : aymalshawy@yahoo.com A sigal ca b rprd as a liar combiatio of basic sigals. Th

More information

RÉSONATEURS NANOMÉCANIQUES DANS LE RÉGIME QUANTIQUE NANOMECHANICAL RESONATORS IN QUANTUM REGIME

RÉSONATEURS NANOMÉCANIQUES DANS LE RÉGIME QUANTIQUE NANOMECHANICAL RESONATORS IN QUANTUM REGIME Chair d Physiqu Mésoscopiqu Michl Dvort Aé 01, 15 ai - 19 ju RÉSONATEURS NANOMÉCANIQUES DANS LE RÉGIME QUANTIQUE NANOMECHANICAL RESONATORS IN QUANTUM REGIME Cquiè lço / Fifth lctur This Collg d Frac docut

More information

April 1980 TR/96. Extrapolation techniques for first order hyperbolic partial differential equations. E.H. Twizell

April 1980 TR/96. Extrapolation techniques for first order hyperbolic partial differential equations. E.H. Twizell TR/96 Apri 980 Extrapoatio techiques for first order hyperboic partia differetia equatios. E.H. Twize W96086 (0) 0. Abstract A uifor grid of step size h is superiposed o the space variabe x i the first

More information

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels LUR 3 illig th bads Occupacy o Availabl rgy Lvls W hav dtrmid ad a dsity o stats. W also d a way o dtrmiig i a stat is illd or ot at a giv tmpratur. h distributio o th rgis o a larg umbr o particls ad

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE57 - Pasma Physics ad Appicatios Lecture 9 Prof. Jorge Rocca ad r. Ferado Tomase epartmet of Eectrica ad Computer Egieerig Low temperature pasmas Low temperature pasmas are a very iterestig subject

More information

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 12

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 12 REVIEW Lctur 11: Numrical Fluid Mchaics Sprig 2015 Lctur 12 Fiit Diffrcs basd Polyomial approximatios Obtai polyomial (i gral u-qually spacd), th diffrtiat as dd Nwto s itrpolatig polyomial formulas Triagular

More information

RETAILER S INVENTORY POLICY UNDER SUPPLIER S PARTIAL TRADE CREDIT POLICY

RETAILER S INVENTORY POLICY UNDER SUPPLIER S PARTIAL TRADE CREDIT POLICY Joura of th Opratios Rsarch Socity of Japa 005, Vo. 48, No. 3, 173-18 005 Th Opratios Rsarch Socity of Japa RETAILER S INVENTORY POLICY UNDER SUPPLIER S PARTIAL TRADE CREDIT POLICY Yug-Fu Huag Chaoyag

More information

DFT: Discrete Fourier Transform

DFT: Discrete Fourier Transform : Discrt Fourir Trasform Cogruc (Itgr modulo m) I this sctio, all lttrs stad for itgrs. gcd m, = th gratst commo divisor of ad m Lt d = gcd(,m) All th liar combiatios r s m of ad m ar multils of d. a b

More information

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted? All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody

More information

Chemistry 342 Spring, The Hydrogen Atom.

Chemistry 342 Spring, The Hydrogen Atom. Th Hyrogn Ato. Th quation. Th first quation w want to sov is φ This quation is of faiiar for; rca that for th fr partic, w ha ψ x for which th soution is Sinc k ψ ψ(x) a cos kx a / k sin kx ± ix cos x

More information

Spatial channeling of energy and momentum of energetic ions by destabilized Alfvén eigenmodes

Spatial channeling of energy and momentum of energetic ions by destabilized Alfvén eigenmodes Spatial channling of nrgy and momntum of nrgtic ions by dstabilizd Alfvén ignmods Ya.I. Kolsnichnko 1,V.V. Lutsnko 1, R.B. Whit, Yu.V. Yakovnko 1 1 Institut for Nuclar Rsarch, Kyiv, Ukrain Princton Plasma

More information

Self-Consistent Simulations of Beam and Plasma Systems Final Exam ( take-home )

Self-Consistent Simulations of Beam and Plasma Systems Final Exam ( take-home ) Sef-Cosistet Simuatios of Beam ad Pasma Systems Fia Exam ( take-home ) S. M. Lud, J.-L. Vay, R. Lehe, ad D. Wikeher Thursday, Jue 16 th, 2016 Probem 1 - Maxwe s equatios ad redudat iformatio. a) Show that

More information

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.

More information

Power Spectrum Estimation of Stochastic Stationary Signals

Power Spectrum Estimation of Stochastic Stationary Signals ag of 6 or Spctru stato of Stochastc Statoary Sgas Lt s cosr a obsrvato of a stochastc procss (). Ay obsrvato s a ft rcor of th ra procss. Thrfor, ca say:

More information

Class #24 Monday, April 16, φ φ φ

Class #24 Monday, April 16, φ φ φ lass #4 Moday, April 6, 08 haptr 3: Partial Diffrtial Equatios (PDE s First of all, this sctio is vry, vry difficult. But it s also supr cool. PDE s thr is mor tha o idpdt variabl. Exampl: φ φ φ φ = 0

More information

1D Heat Propagation Problems

1D Heat Propagation Problems Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2

More information

Stat 543 Exam 3 Spring 2016

Stat 543 Exam 3 Spring 2016 Stat 543 Exam 3 Sprig 06 I have either give or received uauthorized assistace o this exam. Name Siged Date Name Prited This exam cosists of parts. Do at east 8 of them. I wi score aswers at 0 poits apiece

More information

A Review of Complex Arithmetic

A Review of Complex Arithmetic /0/005 Rviw of omplx Arithmti.do /9 A Rviw of omplx Arithmti A omplx valu has both a ral ad imagiary ompot: { } ad Im{ } a R b so that w a xprss this omplx valu as: whr. a + b Just as a ral valu a b xprssd

More information

A Simple Proof that e is Irrational

A Simple Proof that e is Irrational Two of th most bautiful ad sigificat umbrs i mathmatics ar π ad. π (approximatly qual to 3.459) rprsts th ratio of th circumfrc of a circl to its diamtr. (approximatly qual to.788) is th bas of th atural

More information

Chapter 4 - The Fourier Series

Chapter 4 - The Fourier Series M. J. Robrts - 8/8/4 Chaptr 4 - Th Fourir Sris Slctd Solutios (I this solutio maual, th symbol,, is usd for priodic covolutio bcaus th prfrrd symbol which appars i th txt is ot i th fot slctio of th word

More information

Chp6. pn Junction Diode: I-V Characteristics I

Chp6. pn Junction Diode: I-V Characteristics I 147 C6. uctio Diod: I-V Caractristics I 6.1. THE IDEAL DIODE EQUATION 6.1.1. Qualitativ Drivatio 148 Figur rfrc: Smicoductor Dvic Fudamtals Robrt F. Pirrt, Addiso-Wsly Publicig Comay 149 Figur 6.1 juctio

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

More information

Available online at Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10

Available online at   Energy Procedia 4 (2011) Energy Procedia 00 (2010) GHGT-10 Availabl oli at www.scicdirct.com Ergy Procdia 4 (01 170 177 Ergy Procdia 00 (010) 000 000 Ergy Procdia www.lsvir.com/locat/procdia www.lsvir.com/locat/xxx GHGT-10 Exprimtal Studis of CO ad CH 4 Diffusio

More information

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1

DTFT Properties. Example - Determine the DTFT Y ( e ) of n. Let. We can therefore write. From Table 3.1, the DTFT of x[n] is given by 1 DTFT Proprtis Exampl - Dtrmi th DTFT Y of y α µ, α < Lt x α µ, α < W ca thrfor writ y x x From Tabl 3., th DTFT of x is giv by ω X ω α ω Copyright, S. K. Mitra Copyright, S. K. Mitra DTFT Proprtis DTFT

More information

Problem Session (3) for Chapter 4 Signal Modeling

Problem Session (3) for Chapter 4 Signal Modeling Pobm Sssio fo Cht Sig Modig Soutios to Pobms....5. d... Fid th Pdé oimtio of scod-od to sig tht is giv by [... ] T i.. d so o. I oth wods usig oimtio of th fom b b b H fid th cofficits b b b d. Soutio

More information

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted?

Blackbody Radiation. All bodies at a temperature T emit and absorb thermal electromagnetic radiation. How is blackbody radiation absorbed and emitted? All bodis at a tmpratur T mit ad absorb thrmal lctromagtic radiatio Blackbody radiatio I thrmal quilibrium, th powr mittd quals th powr absorbd How is blackbody radiatio absorbd ad mittd? 1 2 A blackbody

More information

What Is the Difference between Gamma and Gaussian Distributions?

What Is the Difference between Gamma and Gaussian Distributions? Applid Mahmaics,,, 85-89 hp://ddoiorg/6/am Publishd Oli Fbruary (hp://wwwscirporg/joural/am) Wha Is h Diffrc bw Gamma ad Gaussia Disribuios? iao-li Hu chool of Elcrical Egirig ad Compur cic, Uivrsiy of

More information

Higher-Order Discrete Calculus Methods

Higher-Order Discrete Calculus Methods Highr-Ordr Discrt Calculus Mthods J. Blair Prot V. Subramanian Ralistic Practical, Cost-ctiv, Physically Accurat Paralll, Moving Msh, Complx Gomtry, Slid 1 Contxt Discrt Calculus Mthods Finit Dirnc Mimtic

More information

Bipolar Junction Transistors

Bipolar Junction Transistors ipolar Juctio Trasistors ipolar juctio trasistors (JT) ar activ 3-trmial dvics with aras of applicatios: amplifirs, switch tc. high-powr circuits high-spd logic circuits for high-spd computrs. JT structur:

More information

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2

Review Exercises. 1. Evaluate using the definition of the definite integral as a Riemann Sum. Does the answer represent an area? 2 MATHEMATIS --RE Itgral alculus Marti Huard Witr 9 Rviw Erciss. Evaluat usig th dfiitio of th dfiit itgral as a Rima Sum. Dos th aswr rprst a ara? a ( d b ( d c ( ( d d ( d. Fid f ( usig th Fudamtal Thorm

More information

Construction of Mimetic Numerical Methods

Construction of Mimetic Numerical Methods Construction of Mimtic Numrical Mthods Blair Prot Thortical and Computational Fluid Dynamics Laboratory Dltars July 17, 013 Numrical Mthods Th Foundation on which CFD rsts. Rvolution Math: Accuracy Stability

More information

A Mathematical Study of Electro-Magneto- Thermo-Voigt Viscoelastic Surface Wave Propagation under Gravity Involving Time Rate of Change of Strain

A Mathematical Study of Electro-Magneto- Thermo-Voigt Viscoelastic Surface Wave Propagation under Gravity Involving Time Rate of Change of Strain Thortical Mathmatics & Applicatios vol.3 o.3 3 87-6 ISSN: 79-9687 (prit) 79-979 (oli) Sciprss Ltd 3 A Mathmatical Study of Elctro-Magto- Thrmo-Voigt Viscolastic Surfac Wav Propagatio udr Gravity Ivolvig

More information

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 116C. Problem Set 4. Benjamin Stahl. November 6, 2014

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 116C. Problem Set 4. Benjamin Stahl. November 6, 2014 UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 6C Problem Set 4 Bejami Stahl November 6, 4 BOAS, P. 63, PROBLEM.-5 The Laguerre differetial equatio, x y + ( xy + py =, will be solved

More information

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei.

They must have different numbers of electrons orbiting their nuclei. They must have the same number of neutrons in their nuclei. 37 1 How may utros ar i a uclus of th uclid l? 20 37 54 2 crtai lmt has svral isotops. Which statmt about ths isotops is corrct? Thy must hav diffrt umbrs of lctros orbitig thir ucli. Thy must hav th sam

More information

EE 570: Location and Navigation: Theory & Practice

EE 570: Location and Navigation: Theory & Practice EE 570: Locatio ad Naigatio: Thory & Practic Naigatio Ssors ad INS Mchaizatio NMT EE 570: Locatio ad Naigatio: Thory & Practic Slid 1 of 13 Naigatio Ssors ad INS Mchaizatio Naigatio Equatios Cas 3: Na

More information

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering

Chapter 11.00C Physical Problem for Fast Fourier Transform Civil Engineering haptr. Physical Problm for Fast Fourir Trasform ivil Egirig Itroductio I this chaptr, applicatios of FFT algorithms [-5] for solvig ral-lif problms such as computig th dyamical (displacmt rspos [6-7] of

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

c 1999 Society for Industrial and Applied Mathematics

c 1999 Society for Industrial and Applied Mathematics SIAM J. NUMER. ANAL. Vo. 37, No. 2, pp. 423 442 c 1999 Socity for Idustria ad Appid Mathmatics SOLUTION OF PARABOLIC EQUATIONS BY BACKWARD EULER-MIXED FINITE ELEMENT METHODS ON A DYNAMICALLY CHANGING MESH

More information

Numerical Methods in Geophysics: Implicit Methods

Numerical Methods in Geophysics: Implicit Methods Numerical Methods i Geophysics: What is a implicit scheme? Explicit vs. implicit scheme for Newtoia oolig rak-nicholso Scheme (mixed explicit-implicit Explicit vs. implicit for the diffusio equatio Relaxatio

More information

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors 3 Lightwav Dvics Lctur 3: Basic Smicoductor Physics ad Optical Procsss Istructor: Mig C. Wu Uivrsity of Califoria, Brly lctrical girig ad Computr Scics Dpt. 3 Lctur 3- Optical Proprtis of Smicoductors

More information

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz risic formuaio for asic i form o a surfac by a xra fi i h psuo-aia spac Nvi ürbüz Eskişhir Osmaazi Uivrsiy Mahmaics a Compur Scics Dparm urbuz@ouur Absrac: his papr w riv irisic formuaio for asic i form

More information

The polarization preservation of partially coherent Hermite-Gaussian. beams for multiple-degrees-of-freedom free-space communication

The polarization preservation of partially coherent Hermite-Gaussian. beams for multiple-degrees-of-freedom free-space communication The poarizatio preservatio of partia coheret Hermite-Gaussia beams for mutipe-degrees-of-freedom free-space commuicatio Lig Ji 1,, Ai-Li Yag 1,, Xiao-Feg Li 1,, Xia-Mi Ji 1,* 1 State Ke Laborator of Advaced

More information

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET Ray Optics Theory ad Mode Theory Dr. Mohammad Faisal Dept. of, BUT Optical Fiber WG For light to be trasmitted through fiber core, i.e., for total iteral reflectio i medium, > Ray Theory Trasmissio Ray

More information

Exercises for lectures 23 Discrete systems

Exercises for lectures 23 Discrete systems Exrciss for lcturs 3 Discrt systms Michal Šbk Automatické říí 06 30-4-7 Stat-Spac a Iput-Output scriptios Automatické říí - Kybrtika a robotika Mols a trasfrs i CSTbx >> F=[ ; 3 4]; G=[ ;]; H=[ ]; J=0;

More information

A NOVEL 3-D MODEL FOR THE WATER CRESTING IN HORIZONTAL WELLS *

A NOVEL 3-D MODEL FOR THE WATER CRESTING IN HORIZONTAL WELLS * 79 008,0(6:79-755 A NOVEL 3- MOEL FOR THE WATER CRESTNG N HORZONTAL WELLS * LUO Wa-jig, ZHOU Yig-fag, WANG Xiao-dog School of Ergy Rsourcs, Chia Uirsity of Goscics, Bijig 00083, Chia, E-mail: luoajig@6.com

More information

On the Diophantine equation x 2 2 ˆ y n

On the Diophantine equation x 2 2 ˆ y n Arch. Math. 74 (000) 50±55 000-889/00/05050-06 $.70/0 Birkhäuser Verag, Base, 000 Archiv der Mathematik O the Diohatie equatio x ˆ y By B. SURY Abstract. We give a eemetary roof of the fact that the oy

More information

Numerical Modeling of Laser Ablation

Numerical Modeling of Laser Ablation Nmrica Moding of Lasr Abation Xianfan X, Associat Profssor Cntr for Lasr Micro-Fabrication Schoo of Mchanica Enginring Prd Univrsity Cntr for Lasr Micro-Fabrication Fndd by th Prd Acadmic Rinvstmnt Program,

More information

Statistics 3858 : Likelihood Ratio for Exponential Distribution

Statistics 3858 : Likelihood Ratio for Exponential Distribution Statistics 3858 : Liklihood Ratio for Expotial Distributio I ths two xampl th rjctio rjctio rgio is of th form {x : 2 log (Λ(x)) > c} for a appropriat costat c. For a siz α tst, usig Thorm 9.5A w obtai

More information

(Reference: sections in Silberberg 5 th ed.)

(Reference: sections in Silberberg 5 th ed.) ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists

More information

H2 Mathematics Arithmetic & Geometric Series ( )

H2 Mathematics Arithmetic & Geometric Series ( ) H Mathmatics Arithmtic & Gomtric Sris (08 09) Basic Mastry Qustios Arithmtic Progrssio ad Sris. Th rth trm of a squc is 4r 7. (i) Stat th first four trms ad th 0th trm. (ii) Show that th squc is a arithmtic

More information

PURE MATHEMATICS A-LEVEL PAPER 1

PURE MATHEMATICS A-LEVEL PAPER 1 -AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio

More information

DISCRETE-TIME RANDOM PROCESSES

DISCRETE-TIME RANDOM PROCESSES DISCRT-TIM RNDOM PROCSSS Rado Pocsss Dfiitio; Ma ad vaiac; autocoatio ad autocovaiac; Ratiosip btw ado vaiabs i a sig ado pocss; Coss-covaiac ad coss-coatio of two ado pocsss; Statioa Rado Pocsss Statioait;

More information

Probability & Statistics,

Probability & Statistics, Probability & Statistics, BITS Pilai K K Birla Goa Campus Dr. Jajati Kshari Sahoo Dpartmt of Mathmatics BITS Pilai, K K Birla Goa Campus Poisso Distributio Poisso Distributio: A radom variabl X is said

More information

CIVE322 BASIC HYDROLOGY Hydrologic Science and Engineering Civil and Environmental Engineering Department Fort Collins, CO (970)

CIVE322 BASIC HYDROLOGY Hydrologic Science and Engineering Civil and Environmental Engineering Department Fort Collins, CO (970) CVE322 BASC HYDROLOGY Hydrologic Scic ad Egirig Civil ad Evirotal Egirig Dpartt Fort Collis, CO 80523-1372 (970 491-7621 MDERM EXAM 1 NO. 1 Moday, Octobr 3, 2016 8:00-8:50 AM Haod Auditoriu You ay ot cosult

More information

Velocity and Temperature Boundary- Layer Modeling Using Averaged Molecule cluster Transport Equations

Velocity and Temperature Boundary- Layer Modeling Using Averaged Molecule cluster Transport Equations IUVSTA 011 Leiseiler, May 16 th 011 Velocity ad Temperature Boudary- Layer Modelig Usig Averaged Molecule cluster Trasport Equatios R. Groll Uiversity of Breme, Am Fallturm, D-859 Breme R. Groll 1 Micro

More information

A Novel Approach to Recovering Depth from Defocus

A Novel Approach to Recovering Depth from Defocus Ssors & Trasducrs 03 by IFSA http://www.ssorsportal.com A Novl Approach to Rcovrig Dpth from Dfocus H Zhipa Liu Zhzhog Wu Qiufg ad Fu Lifag Collg of Egirig Northast Agricultural Uivrsity 50030 Harbi Chia

More information

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti

More information

CATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A. Ήχος Πα. to os se e e na aș te e e slă ă ă vi i i i i

CATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A. Ήχος Πα. to os se e e na aș te e e slă ă ă vi i i i i CATAVASII LA NAȘTEREA DOMNULUI DUMNEZEU ȘI MÂNTUITORULUI NOSTRU, IISUS HRISTOS. CÂNTAREA I-A Ήχος α H ris to os s n ș t slă ă ă vi i i i i ți'l Hris to o os di in c ru u uri, în tâm pi i n ți i'l Hris

More information

ECE 599/692 Deep Learning

ECE 599/692 Deep Learning ECE 599/69 Dp Lari Lctur Autocors Hairo Qi Goal Family Profssor Elctrical Eiri a Computr Scic Uivrsity of ss Kovill http://www.cs.ut.u/faculty/qi Email: hqi@ut.u A loo ac i tim INPU 33 C: fatur maps 6@88

More information

Frequency Measurement in Noise

Frequency Measurement in Noise Frqucy Masurmt i ois Porat Sctio 6.5 /4 Frqucy Mas. i ois Problm Wat to o look at th ct o ois o usig th DFT to masur th rqucy o a siusoid. Cosidr sigl complx siusoid cas: j y +, ssum Complx Whit ois Gaussia,

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

0 : Recap of last two classes

0 : Recap of last two classes Cass 12 : Superova cosmoogy ad the acceeratio of the Uiverse This cass Redshift-distace reatio as a probe of the cosmoogica mode Type-1A superovae Superovae ad cosmoogy Discovery of acceeratio It a fits

More information

PHY 410. Final Examination, Spring May 4, 2009 (5:45-7:45 p.m.)

PHY 410. Final Examination, Spring May 4, 2009 (5:45-7:45 p.m.) PHY ina amination, Spring 9 May, 9 5:5-7:5 p.m. PLAS WAIT UTIL YOU AR TOLD TO BGI TH XAM. Wi waiting, carfuy fi in t information rqustd bow Your am: Your Studnt umbr: DO OT TUR THIS PAG UTIL TH XAM STARTS

More information

Alternative Orthogonal Polynomials. Vladimir Chelyshkov

Alternative Orthogonal Polynomials. Vladimir Chelyshkov Aterative Orthogoa oyomias Vadimir Cheyshov Istitute of Hydromechaics of the NAS Uraie Georgia Souther Uiversity USA Abstract. The doube-directio orthogoaizatio agorithm is appied to costruct sequeces

More information

Session : Plasmas in Equilibrium

Session : Plasmas in Equilibrium Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

Also, recall that the radiative transfer (excluding scattering, formally) is given by ( ) ( )

Also, recall that the radiative transfer (excluding scattering, formally) is given by ( ) ( ) 16. Lin shaps Rmmbr that (dimnsionss) = S (cm) N (cm - ) (cm); N = coumn dnsity, = in shap. Th quivant width W S N. Aso, rca that th radiativ transfr (xcuding scattring, formay) is givn by ( ) ( ) I( )

More information

Solution evolutionary method of compressible boundary layers stability problems

Solution evolutionary method of compressible boundary layers stability problems S. A. Gapoov A. N. Smov Itratioal Joural o Mathmatical ad Computatioal Mthods http:www.iaras.orgiarasjouralsijmcm Solutio volutioary mthod o comprssibl boudary layrs stability problms S. A. GAPONOV A.

More information

Engineering Differential Equations Practice Final Exam Solutions Fall 2011

Engineering Differential Equations Practice Final Exam Solutions Fall 2011 9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.

More information

Physics of the Interstellar and Intergalactic Medium

Physics of the Interstellar and Intergalactic Medium PYA0 Sior Sophistr Physics of th Itrstllar ad Itrgalactic Mdium Lctur 7: II gios Dr Graham M. arpr School of Physics, TCD Follow-up radig for this ad t lctur Chaptr 5: Dyso ad Williams (lss dtaild) Chaptr

More information

Bayesian approach to image reconstruction in photoacoustic tomography

Bayesian approach to image reconstruction in photoacoustic tomography Bayesian approach to image reconstruction in photoacoustic tomography Jenni Tick a, Aki Pulkkinen a, and Tanja Tarvainen a,b a Department of Applied Physics, University of Eastern Finland, P.O. Box 167,

More information

Traveling Salesperson Problem and Neural Networks. A Complete Algorithm in Matrix Form

Traveling Salesperson Problem and Neural Networks. A Complete Algorithm in Matrix Form Procdigs of th th WSEAS Itratioal Cofrc o COMPUTERS, Agios Nikolaos, Crt Islad, Grc, July 6-8, 7 47 Travlig Salsprso Problm ad Nural Ntworks A Complt Algorithm i Matrix Form NICOLAE POPOVICIU Faculty of

More information

Statistical Thermodynamics Essential Concepts. (Boltzmann Population, Partition Functions, Entropy, Enthalpy, Free Energy) - lecture 5 -

Statistical Thermodynamics Essential Concepts. (Boltzmann Population, Partition Functions, Entropy, Enthalpy, Free Energy) - lecture 5 - Statstcal Thrmodyamcs sstal Cocpts (Boltzma Populato, Partto Fuctos, tropy, thalpy, Fr rgy) - lctur 5 - uatum mchacs of atoms ad molculs STATISTICAL MCHANICS ulbrum Proprts: Thrmodyamcs MACROSCOPIC Proprts

More information

Indexed Search Tree (Trie)

Indexed Search Tree (Trie) Indxd Sarch Tr (Tri) Fawzi Emad Chau-Wn Tsng Dpartmnt of Computr Scinc Univrsity of Maryand, Cog Park Indxd Sarch Tr (Tri) Spcia cas of tr Appicab whn Ky C can b dcomposd into a squnc of subkys C 1, C

More information

Design of Dynamic Reconfigurable Structure Based on Integrated Filter Banks

Design of Dynamic Reconfigurable Structure Based on Integrated Filter Banks It J Commuicatios, Ntwor ad Systm Scics, 27,, 236-245 http://wwwscirporg/joural/ijcs ISSN Oli: 93-3723 ISSN Prit: 93-375 Dsig of Dyamic Rcofigurabl Structur Basd o Itgratd Filtr Bas Wxu Zhag, Chgqu Zhou,

More information

Recovering multiscale buried anomalies in a two-layered medium

Recovering multiscale buried anomalies in a two-layered medium Hom Sarch Collctios Jourals About Cotact us M IOPscic Rcovrig multiscal burid aomalis i a twolard mdium This cott has b dowloadd from IOPscic. Plas scroll dow to s th full tt. 5 Ivrs Problms 3 56 (http://iopscic.iop.org/6656/3//56

More information

The Pennsylvania State University. The Graduate School. College of Engineering MODELING OF DISPERSED FLOW FILM BOILING WITH TWO FLOW, FIVE

The Pennsylvania State University. The Graduate School. College of Engineering MODELING OF DISPERSED FLOW FILM BOILING WITH TWO FLOW, FIVE Th Psyaia Stat Uirsity Th Graduat Schoo Cog of Egirig MODELING OF DISPERSED FLOW FILM BOILING WITH TWO FLOW, FIVE FIELD EULERIAN- EULERIAN APPROACH AND EFFECTS OF SPACER GRIDS ON HEAT TRANSFER A Thsis

More information

Chapter (8) Estimation and Confedence Intervals Examples

Chapter (8) Estimation and Confedence Intervals Examples Chaptr (8) Estimatio ad Cofdc Itrvals Exampls Typs of stimatio: i. Poit stimatio: Exampl (1): Cosidr th sampl obsrvatios, 17,3,5,1,18,6,16,10 8 X i i1 17 3 5 118 6 16 10 116 X 14.5 8 8 8 14.5 is a poit

More information

APPENDIX: STATISTICAL TOOLS

APPENDIX: STATISTICAL TOOLS I. Nots o radom samplig Why do you d to sampl radomly? APPENDI: STATISTICAL TOOLS I ordr to masur som valu o a populatio of orgaisms, you usually caot masur all orgaisms, so you sampl a subst of th populatio.

More information

arxiv: v2 [math.nt] 9 May 2017

arxiv: v2 [math.nt] 9 May 2017 arxiv:6.42v2 [math.nt] 9 May 27 Itegral Represetatios of Equally Positive Iteger-Idexed Harmoic Sums at Ifiity Li Jiu Research Istitute for Symbolic Computatio Johaes Kepler Uiversity 44 Liz, Austria ljiu@risc.ui-liz.ac.at

More information

Diffraction of SH Waves by an Elliptic Inclusion with Partially Debonded Region in Bi-Material Half Space Ding xiaohao, Qi hui

Diffraction of SH Waves by an Elliptic Inclusion with Partially Debonded Region in Bi-Material Half Space Ding xiaohao, Qi hui Diffractio of SH Waves by a Eiptic Icusio with Partiay Deboded Regio i Bi-Materia Haf Space Dig xiaohao, Qi hui Coege of erospace ad Civi Egieerig,Harbi Egieerig Uiversity,Harbi, Chia Keywords: bi-ateria

More information