Light scattering and absorption by atmospheric particulates. Part 2: Scattering and absorption by spherical particles.

Size: px
Start display at page:

Download "Light scattering and absorption by atmospheric particulates. Part 2: Scattering and absorption by spherical particles."

Transcription

1 Lctu. Light cattig ad abpti by atmphic paticulat. at : cattig ad abpti by phical paticl. Objctiv:. Maxwll quati. Wav quati. Dilctical ctat f a mdium.. Mi-Dby thy. 3. Vlum ptical ppti f a mbl f paticl. Rquid Radig: L: 5., 3.3. Additial/Advacd Radig: Bh, G.F., ad D.R. Huffma, Abpti ad cattig f light by mall paticl. Jh Wily&, 983 (Mi thy ivati i giv pp.8-, a hadcpy will b pvidd i cla). Maxwll quati. Wav quati. Dilctical ctat f a mdium. Maxwll quati cct th fiv baic quatiti th lctic vct, E, magtic vct, H, magtic iducti, B, lctic diplacmt, D, ad lctic cut dity, j : (i cg ytm) D π H + j c t c B E c t D πρ B wh c i a ctat (wav vlcity); ad ρ i th lctic chag dity. [.] T allw a uiqu dtmiati f th lctmagtic fild vct, th Maxwll quati mut b upplmtd by lati which dcib th bhavi f ubtac u th ifluc f lctmagtic fild. Thy a j σe D εe B µ H [.] wh σ i calld th pcific cductivity; ε i calld th dilctical ctat ( th pmittivity), ad µ i calld th magtic pmability.

2 Dpdig th valu f σ, th ubtac a dividd it: cduct: σ dilctic ( iulat: σ (i.., σ i NOT gligibly mall), (f itac, mtal) (i.., σ i gligibly mall), (f itac, ai, al ad clud paticulat) Lt ci th ppagati f EM wav i a mdium which i (a) uifm, that ε ha th am valu at all pit; (b) itpic, that ε i idpdt f th dicti f ppagati; (c) -cductig (dilctic), that σ ad thf j ; (d) f fm chag, that ρ. With th aumpti th Maxwll quati duc t ε E H c t µ H E c t E H [.3] Elimiatig E ad H i th fit tw quati i [.3] ad uig th vct thm, w hav εµ E E [.] c t εµ H H c t Th abv quati a tadad quati f wav mti f a wav ppagatig with a vlcity wh c i th pd f light i vacuum. c v [.5] εµ NOTE: f vacuum: µ ad ε i cg uit, but i I ytm µ ο ad ε a ctat uch that c / ε µ.

3 F mt ubtac (icludig th ai µ i uity. Thu, th lctical ppti f a mdium a chaactizd by th dilctical ctat ε. Rfactiv idx ( ptical ctat) f a mdium i dfid a m ε [.6] aumig that µ. NOTE: tictly pakig, ε i Eq.[.6] i th lativ pmittivity f mdium (h it i lativ t vacuum). Rfactiv idx: Th factiv idx mm - im i i cmmly xpd a a cmplx umb. Th z imagiay pat m i f th factiv idx i pibl f abpti f th wav a it ppagat thugh th mdium; wha th al pat m f th factiv idx lat t th vlcity f ppagati f th EM wav. Th factiv idx i a tg fucti f th wavlgth. Each ubtac ha a pcific pctum f th factiv idx ( figu , Lctu 5) aticl f difft iz, hap ad idic f facti will hav difft cattig ad abbig ppti. Al paticl ft cit f val chmical pci (calld th ital mixtu. Th a val appach (calld mixig ul) t calculat th ffctiv factiv idx m f th itally mixd paticl uig th factiv idic f th idividual pci ( Lctu 5) 3

4 cattig dmai: Rayligh cattig: π/ << ad m i abitay (appli t cattig by mlcul ad mall al paticl); π Rayligh-Ga cattig: m << ad m << (t uful f atmphic applicati); Mi-Dby cattig: π/ ad m a bth abitay but f ph ly (appli t cattig by al ad clud paticl) Gmtic ptic: π/ >> ad m i al (appli t cattig by lag clud plt). Figu. Rlatihip btw paticl iz, adiati wavlgth ad cattig bhavi f atmphic paticl. Diagal dahd li pt ugh budai btw cattig gim.

5 . Mi-Dby thy. NOTE: Mi-Dby thy i ft calld Mi thy Ltz-Mi thy Mi thy utli: Aumpti: i) aticl i a ph f adiu ii) aticl i hmgu (thf it i chaactizd by a factiv idx mm - im i at a giv wavlgth); NOTE: Mi thy qui th lativ factiv idx factiv idx f a paticl dividd by th factiv idx f a mdium. But f ai m i abut, d t kw th factiv idx f th paticl (i.., factiv idx f th matial f which th paticl i cmpd). NOTE: If a paticl ha cmplx chmical cmpiti, th ffctiv factiv idx mut b calculatd at a giv wavlgth. tatgy: ) k a luti f a vct wav quati (Eq.[.]) f E ad H ε E E c t with th buday cditi that th tagtial cmpt f E ad H b ctiuu ac th phical ufac f a paticl. Aumpti th phical ufac f a paticl allw lvig th vct quati aalytically. ) R-wit th wav quati i phical cdiat ad xp lctic fild iid ad utid ph i vct phical hamic xpai. NOTE: Mi thy calculat th lctmagtic fild at all pit i th paticl (calld ital fild) ad at all pit f th hmgu mdium i which th paticl i mbddd. F all pactical applicati i th atmph, light cattig bvati a caid ut i th fa-fild z (i.., at th lag ditac fm a ph: 3) Apply buday cditi match tav fild at ph ufac t btai cattd phical wav Mi cfficit a ad b which d t dpd th agl 5

6 but dpd iz paamt x π/ ( i th adiu f th paticl) ad vaiabl y x m (m i factiv idx f th paticl). ) U i ivlvig a ad b t btai xticti ad cattig fficici ( ad ). 5) U i i Mi agula fucti π ad t btai cattig amplitud fucti (Θ) ad (Θ), fm which th cattig pha fucti i ivd. NOTE: Full ivati f Mi thy a giv i L, cti 5. (ad Bh&Huffma 983, pp.8-). Mi cattig amplitud (al calld cattig fucti) ivd fm Mi thy a ( Eq i L) + [ a π (cθ) + b (cθ ] ( Θ) ) ( + ) + [ b (c Θ) + a (c Θ ] ( Θ) ) ( + ) π [.7] wh Mi cfficit a ad b a ( Eq.5..7 i L) y ( y) y ( x) my ( y) y ( x) my ( y) y ( x) y ( y) y ( x) a ( x, y) b ( x, y) [.8] y ( y) x ( x) my ( y) x ( x) my ( y) x ( x) y ( y) x ( x) h th pim dt difftiati; x π/ ad y x m; πρ ( ρ) J / ( ρ) ad πρ () ξ ( ρ) H + / ( ρ) wh J ) ( +/ ρ i th half-itgal- ψ + () phical Bl fucti ad H i th half-itgal- Hakl fucti f th cd kid; +/ ad π ad a th Mi agula fucti wh π (cθ) (cθ) i( Θ) d (cθ) (cθ) [.9] dθ a th aciatd Lg plymial ( Appdix E)

7 I th fa-fild z (i.., at th lag ditac R fm a ph, Mi thy giv th luti f th vct wav quati a E E l xp( ikr + ikz) ikr 3 E E i l i [.] Eq.[.] i a fudamtal quati f cattd adiati icludig plaizati i th fa fild. ( Θ) ( Θ) 3( Θ) ( Θ) i th amplitud cattig matix (uitl) F ph: 3 (Θ) (Θ) Thu, f ph Eq.[5.] duc t E E l xp( ikr + ikz) ikr wh xp(ikz) i th icidt pla wav, ad wav. E E xp( ikr) ikr i l i [.] i th utgig cattd Fudamtal xticti fmula ( ptical thm) giv th xticti c cti f a paticl π σ R[ ( )], [.] k But f th fwad dicti (i.. Θ ) fm Eq.[.7], w hav [.3] ( ) ( ) ( + )( a + b ) Thu, xticti c cti i latd t cattig i fwad dicti. 7

8 Efficici ( fficicy fact f xticti, cattig ad abpti a dfid a σ π π a a σ [.] π wh π i th paticl aa pjctd t th pla ppdicula t th icidt bam. Mi fficicy fact a ivd fm th Mi cattig amplitud [.5] x ( + ) R[ a + ] b [.6] x ( + )[ a + ] b ad th abpti fficicy ca b calculatd a a [.7] Figu. Exampl f ad a calculatd with Mi thy f val factiv idx. 8

9 cattig pha matix Rcall dfiiti f tk paamt ( Lctu 5), which uiquly chaactiz th lctmagtic wav. Lt I,, U ad V b th tk paamt f icidt fild ad I,, U ad V b th tk paamt f cattd adiati V U I R V U I π [.8] wh i th cattig pha matix [.9] wh ach lmt dpd th cattig agl (/R i fm lid agl) F ph: ad 33 NOTE: I gal, f a paticl f ay hap, th cattig pha matix cit f 6 idpdt lmt, but f a ph thi umb duc t fu. Thu f ph, Eq.[.8] duc t V U I R V U I π [.] wh ach lmt f th cattig pha matix i xpd via th cattig amplitud (Θ) ad (Θ) [ ] k + π [ ] k π [.] 9

10 [ ] 33 k + π [ ] 3 k π (Θ) (Θ) i th cattig pha fucti dfid i Lctu. Figu.3 Exampl f cattig pha fucti calculatd with Mi thy f val iz paamt f abbig ph. Nt icaig cillatig bhavi with icaig iz paamt.

11 m highlight f Mi cattig ult: Exticti fficicy v. iz paamt x (aumig NO ABORTION): ) mall i Rayligh limit: x ) lagt wh paticl ad wavlgth hav imila iz 3) -> i th gmtic limit ( x ) ) Ocillati ( Fig.5.3) fm itfc f tamittd ad diffactd wav id i x f itfc cillati dpd th factiv idx. Abpti duc itfc cillati ad kill ippl tuctu. cattig ad abpti fficici v. iz paamt with ABORTION: A x : ad, tig ay a abbd iid paticl. mall imagiay pat f th factiv idx qui lag paticl t fully abb ital ay. cattig pha fucti: fwad pak hight ica amatically with x. F igl paticl umb f cillati i (Θ) ica with x. 3. Vlum ptical ppti f a mbl f paticl. Mi thy giv th xticti, cattig ad abpti c-cti (ad fficici) ad th cattig pha matix f a igl phical paticl. NOTE: Rcall Lctu wh th paticl iz ditibuti w itducd f atmphic al ad clud. If th paticl chaactizd by a iz ditibuti N(, th vlum xticti, cattig ad abpti cfficit (i uit LENGTH - ) a calculatd a β max mi σ ( N( max β ( N( [.] mi β a max mi σ ( N( a

12 wh σ i th cpdig c cti f a paticl f adiu ad N( i th paticl iz ditibuti (.g., i uit m -3 µm - ). igl cattig albd (uitl) i dfid a ω β [.3] β Th igl cattig albd giv th pctag f light which will b cattd i a igl cattd vt. cattig pha fucti i [ + ] N( max ( Θ) π k β [.] mi ( Θ) max mi ( Θ) N( β [.5] Aymmty paamt i dfid a th fit mmt f th cattig pha fucti g (cθ)c( Θ) d(cθ) [.6] g f qual fwad ad backwad cattig; g f ttally fwad cattig Th Hyy-Gti cattig pha fucti i a mdl pha fucti, which i ft ud i adiativ taf calculati t appximat al cattig: g HG ( Θ) 3/ ( + g g cθ) [.7] wh g i th aymmty paamt.

13 Optical ppti f clud p: F may pactical applicati, th ptical ppti f wat clud a paamtizd a a fucti f th ffctiv adiu ad liquid wat ctt (LWC). Th ffctiv adiu i dfid a 3 N( N( wh N( i th paticl iz ditibuti (.g., i uit m -3 µm - ). Th liquid wat ctt (LWC) wa dfid i Lctu 5 ( Eq.[5.7]): 3 [.8] LWC w V w N( 3 π [.9] Uig that th xticti cfficit f clud plt i σ ( N( β π N( ) ad that f wat plt at la wavlgth, w hav LWC β 3 [.3] w Effctiv ptical ppti f a atmphic lay citig f ga, al ad/ clud paticl: Effctiv (al calld ttal) ptical dpth: wh M a, ad M M A A a, +, + a, +, [.3] M, a ptical dpth du t abpti by ga ad mlcula (Rayligh) cattig, pctivly; A A a, ad, a ptical dpth du t abpti ad cattig by al (ad/ clud) paticl, pctivly. 3

14 Effctiv igl cattig albd: ω A M,,, + [.3] Effctiv cattig pha fucti: A M A A M M,,,, ) ( ) ( ) ( + Θ + Θ Θ [.33] Effctiv aymmty paamt: A M A A g g,,, + [.3]

Light scattering and absorption by atmospheric particulates. Part 2: Scattering and absorption by spherical particles.

Light scattering and absorption by atmospheric particulates. Part 2: Scattering and absorption by spherical particles. Lctu Light catting and abptin by atmphic paticulat. at : catting and abptin by phical paticl. Objctiv:. Maxwll quatin. Wav quatin. Dilctical cntant f a mdium.. Mi-Dby thy. 3. Optical ppti f an nmbl f phical

More information

SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.

SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction. he 47 Lctu Fall 5 SFE OPERION OF UBULR (PFR DIBI REORS I a xthmic acti th tmatu will ctiu t is as mvs alg a lug flw act util all f th limitig actat is xhaust. Schmatically th aiabatic tmatu is as a fucti

More information

Analysis and Design of Basic Interconnects (Part 1)

Analysis and Design of Basic Interconnects (Part 1) Analysis and Dsign f Basic Intcnncts (Pat ) Outlin Tw-wi lins and caxial lins Stiplin Stiplin gmty and fild distibutin Chaactizing stiplins Micstip lin Micstip gmty and fild distibutin Chaactizing micstip

More information

Electrical field generated by a charged harmonic oscillator at thermodynamic equilibrium

Electrical field generated by a charged harmonic oscillator at thermodynamic equilibrium lctical fild gatd by a cagd aic scillat at tdyaic uilibiu STFANO GIODANO Dpatt f Bipysical ad lctic giig Uivsity f Ga Via Opa Pia A 65 Gva ITALY Abstact: - I tis pap w aalys t lctagtic fild gatd by a cagd

More information

Basic Interconnects at High Frequencies (Part 1)

Basic Interconnects at High Frequencies (Part 1) Basic Intcnncts at High Fquncis (Pat ) Outlin Tw-wi cabls and caxial cabls Stiplin Stiplin gmty and fild distibutin Chaactizing stiplins Micstip lin Micstip gmty and fild distibutin Chaactizing micstip

More information

Lectur 22. RF and Microwave Circuit Design Γ-Plane and Smith Chart Analysis. ECE 303 Fall 2005 Farhan Rana Cornell University

Lectur 22. RF and Microwave Circuit Design Γ-Plane and Smith Chart Analysis. ECE 303 Fall 2005 Farhan Rana Cornell University ctur RF ad Micrwav Circuit Dig -Pla ad Smith Chart Aalyi I thi lctur yu will lar: -pla ad Smith Chart Stub tuig Quartr-Wav trafrmr ECE 33 Fall 5 Farha Raa Crll Uivrity V V Impdac Trafrmati i Tramii i ω

More information

User s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube

User s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube U Guid Elctnic Cv Ntwk XM66 Vaiabl Fquncy XM9 24 db/ctav XM16 48 db/ctav XM44 24/48 db/ctav XM26 24 db/ctav Tub XM46 24 db/ctav Paiv Lin Lvl XM126 24 db/ctav Tub Machand Elctnic Inc. Rcht, NY (585) 423

More information

Lecture 14. Time Harmonic Fields

Lecture 14. Time Harmonic Fields Lcu 4 Tim amic Filds I his lcu u will la: Cmpl mahmaics f im-hamic filds Mawll s quais f im-hamic filds Cmpl Pig vc C 303 Fall 007 Faha aa Cll Uivsi Tim-amic Filds ad -filds f a pla wav a (fm las lcu:

More information

The Phase Probability for Some Excited Binomial States

The Phase Probability for Some Excited Binomial States Egypt. J. Sl., Vl. 5, N., 3 Th Pha Prbability fr S Excitd Biial Stat. Darwih Faculty f Educati, Suz Caal Uivrity at Al-Arih, Egypt. I thi papr, th pha prprti i Pgg-Bartt frali ar cidrd. Th pha ditributi

More information

The theory of relativistic spontaneous emission from hydrogen atom in Schwarzschild Black hole

The theory of relativistic spontaneous emission from hydrogen atom in Schwarzschild Black hole Amica Jual f Astmy ad Astphysics 01; (6): 66-71 Publishd li Dcmb 9, 01 (http://www.scicpublishiggup.cm/j/ajaa) di: 10.1168/j.ajaa.01006.1 IN: 76-678 (Pit); IN: 76-686 (Oli) Th thy f lativistic sptaus missi

More information

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What

More information

The tight-binding method

The tight-binding method Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i

More information

Handout 30. Optical Processes in Solids and the Dielectric Constant

Handout 30. Optical Processes in Solids and the Dielectric Constant Haut Otal Sl a th Dlt Ctat I th ltu yu wll la: La ut Ka-Kg lat Dlt tat l Itba a Itaba tbut t th lt tat l C 47 Sg 9 Faha Raa Cll Uty Chag Dl, Dl Mt, a lazat Dty A hag l t a gat a a t hag aat by ta: Q Q

More information

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes

Galaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds

More information

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh

More information

Ch. 6 Free Electron Fermi Gas

Ch. 6 Free Electron Fermi Gas Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio

More information

4.4 Linear Dielectrics F

4.4 Linear Dielectrics F 4.4 Lina Dilctics F stal F stal θ magntic dipol imag dipol supconducto 4.4.1 Suscptiility, mitivility, Dilctic Constant I is not too stong, th polaization is popotional to th ild. χ (sinc D, D is lctic

More information

Lecture 20. Transmission Lines: The Basics

Lecture 20. Transmission Lines: The Basics Lcu 0 Tansmissin Lins: Th Basics n his lcu u will lan: Tansmissin lins Diffn ps f ansmissin lin sucus Tansmissin lin quains Pw flw in ansmissin lins Appndi C 303 Fall 006 Fahan Rana Cnll Univsi Guidd Wavs

More information

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists

More information

Chapter 15: Mathematics More Fun With

Chapter 15: Mathematics More Fun With Pg 5 Chpt 15: Mthmtic M Fu With Numb. I thi chpt w will lk t m dditil mthmticl pt d fucti tht wk with umb. Tpic will b bk dw it fu cti: 1) w pt; ) w itg fucti, 3) w fltig pit fucti, d 4) tigmtic fucti.

More information

GUC (Dr. Hany Hammad)

GUC (Dr. Hany Hammad) Lct # Pl s. Li bdsid s with ifm mplitd distibtis. Gl Csidtis Uifm Bimil Optimm (Dlph-Tchbshff) Cicl s. Pl s ssmig ifm mplitd citti m F m d cs z F d d M COMM Lct # Pl s ssmig ifm mplitd citti F m m m T

More information

Dielectric Waveguide 1

Dielectric Waveguide 1 Dilctic Wavgui Total Ital Rflctio i c si c t si si t i i i c i Total Ital Rflctio i c i cos si Wh i t i si c si cos t j o cos t t o si i si bcoms pul imagia pul imagia i, al Total Ital Rflctio 3 i c i

More information

MODELING OF THE LASER METAL NANOPARTICLES FRAGMENTATION

MODELING OF THE LASER METAL NANOPARTICLES FRAGMENTATION MATHEMATICA MONTISNIGRI Vol XXXI (014) MODELING OF THE LASER METAL NANOPARTICLES FRAGMENTATION I.N. ZAVESTOVSKAYA 1,, A.P. KANAVIN 1, 1 P.N. Lbdv Phyical Ititut, RAS, Mocow, 119991, Ruia Natioal Rach Nucla

More information

Continuous-Time Fourier Transform. Transform. Transform. Transform. Transform. Transform. Definition The CTFT of a continuoustime

Continuous-Time Fourier Transform. Transform. Transform. Transform. Transform. Transform. Definition The CTFT of a continuoustime Ctiuus-Tim Furir Dfiiti Th CTFT f a ctiuustim sigal x a (t is giv by Xa ( jω xa( t jωt Oft rfrrd t as th Furir spctrum r simply th spctrum f th ctiuus-tim sigal dt Ctiuus-Tim Furir Dfiiti Th ivrs CTFT

More information

On Gaussian Distribution

On Gaussian Distribution Ppad b Çağata ada MU lctical gi. Dpt. Dc. documt vio. Gauia ditibutio i did a ollow O Gauia Ditibutio π h uctio i clal poitiv valud. Bo callig thi uctio a a pobabilit dit uctio w hould chc whth th aa ud

More information

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6

GRAVITATION. (d) If a spring balance having frequency f is taken on moon (having g = g / 6) it will have a frequency of (a) 6f (b) f / 6 GVITTION 1. Two satllits and o ound a plant P in cicula obits havin adii 4 and spctivly. If th spd of th satllit is V, th spd of th satllit will b 1 V 6 V 4V V. Th scap vlocity on th sufac of th ath is

More information

School of Electrical Engineering. Lecture 2: Wire Antennas

School of Electrical Engineering. Lecture 2: Wire Antennas School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/

More information

ELEC 372 LECTURE NOTES, WEEK 11 Dr. Amir G. Aghdam Concordia University

ELEC 372 LECTURE NOTES, WEEK 11 Dr. Amir G. Aghdam Concordia University ELEC 37 LECTURE NOTES, WEE Dr Amir Aghdam Cncrdia Univrity Part f th nt ar adaptd frm th matrial in th fllwing rfrnc: Mdrn Cntrl Sytm by Richard C Drf and Rbrt H Bihp, Prntic Hall Fdback Cntrl f Dynamic

More information

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th

More information

GUC (Dr. Hany Hammad) 11/2/2016

GUC (Dr. Hany Hammad) 11/2/2016 GUC (D. Han Hammad) //6 ctu # 7 Magntic Vct Ptntial. Radiatin fm an lmnta Dipl. Dictivit. Radiatin Rsistanc. Th ng Dipl Th half wavlngth Dipl Dictivit. Radiatin Rsistanc. Tavling wav antnna. Th lp antnna.

More information

LECTURE 5 Guassian Wave Packet

LECTURE 5 Guassian Wave Packet LECTURE 5 Guassian Wav Pact 1.5 Eampl f a guassian shap fr dscribing a wav pact Elctrn Pact ψ Guassian Assumptin Apprimatin ψ As w hav sn in QM th wav functin is ftn rprsntd as a Furir transfrm r sris.

More information

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY Ntil uvy f tudt Eggt, pig 11 T Uivity t Alby, UNY EXECUTIVE UMMARY Jl D. Bl, P.D. Dit f Adi At & uvy R I Fbuy d M 11, T Uivity t Alby ptiiptd i t Ntil uvy f tudt Eggt (NE) f t d ti, fllwig up u pviu ptiipti

More information

ANALYSIS OF SLOT COUPLED MICROSTRIP PATCH ANTENNAS

ANALYSIS OF SLOT COUPLED MICROSTRIP PATCH ANTENNAS AALYSIS OF SLOT COUPLED MICROSTRIP PATCH ATEAS A THESIS SUBMITTED TO THE GRADUATE SCHOOL OF ATURAL AD APPLIED SCIECES OF MIDDLE EAST TECHICAL UIVERSITY BY ELİF BALLIKAYA I PARTIAL FULFILLMET OF THE REUIREMETS

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

Acoustics and electroacoustics

Acoustics and electroacoustics coustics and lctoacoustics Chapt : Sound soucs and adiation ELEN78 - Chapt - 3 Quantitis units and smbols: f Hz : fqunc of an acoustical wav pu ton T s : piod = /f m : wavlngth= c/f Sound pssu a : pzt

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordiary Diffrtial Equatio Aftr radig thi chaptr, you hould b abl to:. dfi a ordiary diffrtial quatio,. diffrtiat btw a ordiary ad partial diffrtial quatio, ad. Solv liar ordiary diffrtial quatio with fid

More information

EE 119 Homework 6 Solution

EE 119 Homework 6 Solution EE 9 Hmwrk 6 Slutin Prr: J Bkr TA: Xi Lu Slutin: (a) Th angular magniicatin a tlcp i m / th cal lngth th bjctiv ln i m 4 45 80cm (b) Th clar aprtur th xit pupil i 35 mm Th ditanc btwn th bjctiv ln and

More information

Chapter 5. Root Locus Techniques

Chapter 5. Root Locus Techniques Chapter 5 Rt Lcu Techique Itrducti Sytem perfrmace ad tability dt determied dby cled-lp l ple Typical cled-lp feedback ctrl ytem G Ope-lp TF KG H Zer -, - Ple 0, -, - K Lcati f ple eaily fud Variati f

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

ARC Window System. General Information: Determine your window type and turn to the specific pages for the. Type #1 Arc. Windows. Type #2 Arc Windows

ARC Window System. General Information: Determine your window type and turn to the specific pages for the. Type #1 Arc. Windows. Type #2 Arc Windows I-1 ARC Wid Systm This systm quis a additial tip t th jb sit ad cdiati bt th km ad th istall. Tip #1- Masu th id. Tip #2- Fi-tu th fit t th id, th s th tatmt. Tip #3- Istall fial tatmt. As ith ay typ f

More information

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance.

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance. VISUAL PHYSICS ONLIN BOHR MODL OF TH ATOM Bhr typ mdls f th atm giv a ttally icrrct pictur f th atm ad ar f ly histrical sigificac. Fig.. Bhr s platary mdl f th atm. Hwvr, th Bhr mdls wr a imprtat stp

More information

An Unknown Physical Constant Missing from Physics

An Unknown Physical Constant Missing from Physics Applid Phyic Rach; Vol 7, No 5; 5 ISSN 96-9639 -ISSN 96-967 Publihd by Caadia Ct of Scic ad ducatio A Ukow Phyical Cotat Miig fom Phyic Chudaiji Buddhit Tmpl, Iaki, Japa Kohu Suto Copodc: Kohu Suto, Chudaiji

More information

WAVELENGTH TUNABLE DEVICES BASED ON HOLOGRAPHIC POLYMER DISPERSED LIQUID CRYSTALS. A dissertation Submitted to. Kent State University

WAVELENGTH TUNABLE DEVICES BASED ON HOLOGRAPHIC POLYMER DISPERSED LIQUID CRYSTALS. A dissertation Submitted to. Kent State University WAVELENGTH TUNABLE DEVICES BASED ON HOLOGRAPHIC POLYMER DISPERSED LIQUID CRYSTALS A disstatio Submittd to Kt Stat Uivsity i patial fulfillmt of th quimts fo th dg of DOCTOR OF PHILOSOPHY By Hailiag Zhag

More information

ENGO 431 Analytical Photogrammetry

ENGO 431 Analytical Photogrammetry EGO Altil Phtgmmt Fll 00 LAB : SIGLE PHOTO RESECTIO u t: vm 00 Ojtiv: tmi th Eti Oitti Pmts EOP f sigl ht usig lst squs justmt u. Giv:. Iti Oitti Pmts IOP f th m fm th Cm Cliti Ctifit CCC; Clit fl lgth

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

More information

Section 4.2 Radians, Arc Length, and Area of a Sector

Section 4.2 Radians, Arc Length, and Area of a Sector Sectin 4.2 Radian, Ac Length, and Aea f a Sect An angle i fmed by tw ay that have a cmmn endpint (vetex). One ay i the initial ide and the the i the teminal ide. We typically will daw angle in the cdinate

More information

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig.

( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig. HS Mathmatics Solutios Qustio.778.78 ( sig. fig.) (b) (c) ( )( + ) + + + + d d (d) l ( ) () 8 6 (f) + + + + ( ) ( ) (iii) β + + α α β αβ 6 (b) si π si π π π +,π π π, (c) y + dy + d 8+ At : y + (,) dy 8(

More information

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM

Physics 202, Lecture 5. Today s Topics. Announcements: Homework #3 on WebAssign by tonight Due (with Homework #2) on 9/24, 10 PM Physics 0, Lctu 5 Today s Topics nnouncmnts: Homwok #3 on Wbssign by tonight Du (with Homwok #) on 9/4, 10 PM Rviw: (Ch. 5Pat I) Elctic Potntial Engy, Elctic Potntial Elctic Potntial (Ch. 5Pat II) Elctic

More information

Note 6 Frequency Response

Note 6 Frequency Response No 6 Frqucy Rpo Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada. alyical Exprio

More information

Transmission Lines. Introduction to Transmission Lines (T.L.) Exercise Common Transmission Lines. Transmission Lines (TL) Don t worry about the

Transmission Lines. Introduction to Transmission Lines (T.L.) Exercise Common Transmission Lines. Transmission Lines (TL) Don t worry about the Tramii i Itrducti t Tramii i (T.. Hi frqucy r hi pwr rquir T.. TEM wav prpagat thru T.. W wi dvp T.. thry t hw wav prpagat thru thm Dr. Sadra CruzP ECE Dpt. UPRM Sm t b i para, but th ar t qua! Exrci 11.3

More information

Even/Odd Mode Analysis of the Wilkinson Divider

Even/Odd Mode Analysis of the Wilkinson Divider //9 Wilkinn Dividr Evn and Odd Md Analyi.dc / Evn/Odd Md Analyi f th Wilkinn Dividr Cnidr a matchd Wilkinn pwr dividr, with a urc at prt : Prt Prt Prt T implify thi chmatic, w rmv th grund plan, which

More information

E F. and H v. or A r and F r are dual of each other.

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

More information

Handout 32. Electronic Energy Transport and Thermoelectric Effects

Handout 32. Electronic Energy Transport and Thermoelectric Effects Haut lti y aspt a hmlti ts I is ltu yu will la: hmal y taspt by lts hmlti ts b t Plti t hmlti ls hmlti pw ts Las Osa (9-976) C 47 pi 9 aha Raa Cll Uisity Nt Ntati I is haut ulss stats wis w will assum

More information

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )

More information

If σis unknown. Properties of t distribution. 6.3 One and Two Sample Inferences for Means. What is the correct multiplier? t

If σis unknown. Properties of t distribution. 6.3 One and Two Sample Inferences for Means. What is the correct multiplier? t /8/009 6.3 Oe a Tw Samle Iferece fr Mea If i kw a 95% Cfiece Iterval i 96 ±.96 96.96 ± But i ever kw. If i ukw Etimate by amle taar eviati The etimate taar errr f the mea will be / Uig the etimate taar

More information

, University. 1and. y T. since. g g

, University. 1and. y T. since. g g UADPhilEc, Dp. f Ecmics,, Uivsi f Ahss Lcu: Nichlas J. hcaakis Dcmb 2 Ec Advacd Maccmic h I: Mdul : Gwh G ad Ccls Basic wh mah im vaiabls. 2. Disc vaiabls Scks (a a pi f im,.. labu fc) ad Flws ( i a pid

More information

Lossy Transmission Lines. EELE 461/561 Digital System Design. Module #7 Lossy Lines. Lossy Transmission Lines. Lossy Transmission Lines

Lossy Transmission Lines. EELE 461/561 Digital System Design. Module #7 Lossy Lines. Lossy Transmission Lines. Lossy Transmission Lines Topics EEE 46/56 Digital Systm Dsign. Skin Ect. Dilctic oss Modul #7 ossy ins ossy ins - Whn w divd Tlgaphs Equations, w mad an assumption that th was no loss in th quivalnt cicuit modl i.., =, = - This

More information

Sub-Wavelength Resonances in Metamaterial-Based Multi-Cylinder Configurations

Sub-Wavelength Resonances in Metamaterial-Based Multi-Cylinder Configurations Matrial 211, 4, 117-13; di:1.339/ma41117 Articl OPEN ACCESS matrial ISSN 1996-1944 www.mdpi.cm/jural/matrial Sub-Wavlgth Rac i Mtamatrial-Bad Multi-Cylidr Cfigurati Saml Arlaagić * ad Olav Bribjrg Dpartmt

More information

Sec. 9.1 Lines and Angles

Sec. 9.1 Lines and Angles Sec. 9. Line and Angle Leaning Objective:. Identify line, line egment, ay, and angle.. Claify angel a acute, igt, btue, taigt.. Identify cmplementay and upplementay angle. 4. Find meaue f angle. 5. Key

More information

Outline of the Three Multiprocessor Servers from the 2009 Sun Microsystems Grant

Outline of the Three Multiprocessor Servers from the 2009 Sun Microsystems Grant Outi f th Th Mutip Sv fm th 2009 Su Miytm Gt D E. P, http://futy.kutztw.u/p, CSC 402, F 2010 A (ik it) hh tb p k vy ik it, wig y th t tim it h bukt it. A g ut tt, th pbbiity f iig k -- whih ti witig --

More information

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident

Part I- Wave Reflection and Transmission at Normal Incident. Part II- Wave Reflection and Transmission at Oblique Incident Apl 6, 3 Uboudd Mda Gudd Mda Chap 7 Chap 8 3 mls 3 o 3 M F bad Lgh wavs md by h su Pa I- Wav Rlo ad Tasmsso a Nomal Id Pa II- Wav Rlo ad Tasmsso a Oblqu Id Pa III- Gal Rlao Bw ad Wavguds ad Cavy Rsoao

More information

GUC (Dr. Hany Hammad) 4/20/2016

GUC (Dr. Hany Hammad) 4/20/2016 GU (r. Hay Hamma) 4/0/06 Lctur # 0 Filtr sig y Th srti Lss Mth sig Stps Lw-pass prttyp sig. () Scalig a cvrsi. () mplmtati. Usig Stus. Usig High-Lw mpac Sctis. Thry f priic structurs. mag impacs a Trasfr

More information

MATH Midterm Examination Victor Matveev October 26, 2016

MATH Midterm Examination Victor Matveev October 26, 2016 MATH 33- Midterm Examiati Victr Matveev Octber 6, 6. (5pts, mi) Suppse f(x) equals si x the iterval < x < (=), ad is a eve peridic extesi f this fucti t the rest f the real lie. Fid the csie series fr

More information

Entire Solution of a Singular Semilinear Elliptic Problem

Entire Solution of a Singular Semilinear Elliptic Problem JOURNAL OF MATEMATICAL ANALYSIS AND APPLICATIONS 200, 498505 1996 ARTICLE NO 0218 Etie Sluti f a Sigula Semiliea Elliptic Pblem Ala V Lai ad Aihua W Shae Depatmet f Mathematics ad Statistics, Ai Fce Istitute

More information

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e 8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain

More information

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109 Th fa fl calculao: Appoa a ac oluo Pa K Novb 0h 005 B-09 Oul Novb 0h 005 Pa K Iouco Appoa oluo flco fo h gou ac oluo Cocluo Pla wav fo Ic fl: pla wav k ( ) jk H ( ) λ λ ( ) Polaao fo η 0 0 Hooal polaao

More information

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS

5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS 5.61 Fall 2007 Lctu #2 pag 1 Th DEMISE of CLASSICAL PHYSICS (a) Discovy of th Elcton In 1897 J.J. Thomson discovs th lcton and masus ( m ) (and inadvtntly invnts th cathod ay (TV) tub) Faaday (1860 s 1870

More information

Math 334 Fall 2011 Homework 10 Solutions

Math 334 Fall 2011 Homework 10 Solutions Nov. 5, Math 334 Fall Homework Solution Baic Problem. Expre the following function uing the unit tep function. And ketch their graph. < t < a g(t = < t < t > t t < b g(t = t Solution. a We

More information

STUDENT S t-distribution AND CONFIDENCE INTERVALS OF THE MEAN ( )

STUDENT S t-distribution AND CONFIDENCE INTERVALS OF THE MEAN ( ) STUDENT S t-distribution AND CONFIDENCE INTERVALS OF THE MEAN Suppoe that we have a ample of meaured value x1, x, x3,, x of a igle uow quatity. Aumig that the meauremet are draw from a ormal ditributio

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

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,

More information

Unit 3: Transistor at Low Frequencies

Unit 3: Transistor at Low Frequencies Unt 3: Tansst at Lw Fquncs JT Tansst Mdlng mdl s an qualnt ccut that psnts th chaactstcs f th tansst. mdl uss ccut lmnts that appxmat th ha f th tansst. Th a tw mdls cmmnly usd n small sgnal analyss f

More information

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10.

EE243 Advanced Electromagnetic Theory Lec # 22 Scattering and Diffraction. Reading: Jackson Chapter 10.1, 10.3, lite on both 10.2 and 10. Appid M Fa 6, Nuuth Lctu # V //6 43 Advancd ctomagntic Thoy Lc # Scatting and Diffaction Scatting Fom Sma Obcts Scatting by Sma Dictic and Mtaic Sphs Coction of Scatts Sphica Wav xpansions Scaa Vcto Rading:

More information

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii

More information

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

More information

MIL-HDBK OCTOBER 1984 MAINTAINABILITY ANALYSIS

MIL-HDBK OCTOBER 1984 MAINTAINABILITY ANALYSIS 5 CTBER 984 TABLE 5.3..-: VALUES F R z (t'i_ a ) MST CMMNLY USED IN MAINTAINABILITY ANALYSIS l-

More information

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain

More information

COMMUNITY LEGAL CLINIC OF YORK REGION 21 DUNLOP ST., SUITE 200 RICHMOND HILL, ON., L4C 2M6

COMMUNITY LEGAL CLINIC OF YORK REGION 21 DUNLOP ST., SUITE 200 RICHMOND HILL, ON., L4C 2M6 B T T D I G 1 0 D o u g l a s o a d U x b r i d g e, O. L 9 P 1 9 HHAngus & Associates Limited Consulting ngineers 1127 Leslie treet, Toronto, O, M3C 2J6 Canada GAL OT THI DAWIG I TH POPTY OF BTT DIG AOCIAT

More information

SIMPLIFICATIONS AND SOLUTIONS OF DIFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT

SIMPLIFICATIONS AND SOLUTIONS OF DIFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT ICSV Cain Autalia 9- July 7 SIMPLIFICATIONS AN SOLUTIONS OF IFFRACTION FUNCTIONS IN NONLINEAR ACOUSTIC PARAMETER MEASUREMENT jilali Koutich Launt Alliè Rachid Gula and Mutapha Nadi LIEN Nancy-Univité Faculté

More information

Chapter 3.1: Polynomial Functions

Chapter 3.1: Polynomial Functions Ntes 3.1: Ply Fucs Chapter 3.1: Plymial Fuctis I Algebra I ad Algebra II, yu ecutered sme very famus plymial fuctis. I this secti, yu will meet may ther members f the plymial family, what sets them apart

More information

m = Mass flow rate The Lonely Electron Example 0a:

m = Mass flow rate The Lonely Electron Example 0a: The Lel Elect Exaple 0a: Mass flw ate l Liea velcit Hw fa ut f ptial eeg iteacti? Hge ucleus Bh --- 93: Uest the etu ccept. Liea etu istace eeg ( l ) l F ( tie ) ( tie ) + Like t use the peples ieas (if

More information

Helping you learn to save. Pigby s tips and tricks

Helping you learn to save. Pigby s tips and tricks Hlpg yu lan t av Pigby tip and tick Hlpg vy littl av Pigby ha bn tachg hi find all abut ny and hw t av f what ty want. Tuffl i avg f a nw tappy bubbl d and Pi can t wait t b abl t buy nw il pat. Pigby

More information

3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers

3.46 PHOTONIC MATERIALS AND DEVICES Lecture 10: LEDs and Optical Amplifiers 3.46 PHOTONIC MATERIALS AND DEVICES Lctu 0: LEDs and Optical Amplifis Lctu Rfncs:. Salh, M. Tich, Photonics, (John-Wily, Chapts 5-6. This lctu will viw how lctons and hols combin in smiconductos and nat

More information

PD12 21 The Highlands East Sign Package

PD12 21 The Highlands East Sign Package PD12 21 The Highlands ast ign Package March 5, 2013 T T TAT: ALL CHAL LTT MUT B 3 DP (TH G LY) CHAL LTT BY TAT: 3 PFHD Y TU; WHT ACYLC FAC; 1 Y JWLT TM TALLY LLUM. w/wht LD; FT UFAC YL TAT PAL PTD. PAYLAT

More information

PREPARATORY MATHEMATICS FOR ENGINEERS

PREPARATORY MATHEMATICS FOR ENGINEERS CIVE 690 This qusti ppr csists f 6 pritd pgs, ch f which is idtifid by th Cd Numbr CIVE690 FORMULA SHEET ATTACHED UNIVERSITY OF LEEDS Jury 008 Emiti fr th dgr f BEg/ MEg Civil Egirig PREPARATORY MATHEMATICS

More information

COMPSCI 230 Discrete Math Trees March 21, / 22

COMPSCI 230 Discrete Math Trees March 21, / 22 COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /

More information

STRUCTURES IN MIKE 21. Flow over sluice gates A-1

STRUCTURES IN MIKE 21. Flow over sluice gates A-1 A-1 STRUCTURES IN MIKE 1 Fl ver luice gate Fr a give gemetry f the luice gate ad k ater level uptream ad dtream f the tructure, the fl rate, ca be determied thrugh the equati f eergy ad mmetum - ee B Pedere,

More information

ELEC9721: Digital Signal Processing Theory and Applications

ELEC9721: Digital Signal Processing Theory and Applications ELEC97: Digital Sigal Pocssig Thoy ad Applicatios Tutoial ad solutios Not: som of th solutios may hav som typos. Q a Show that oth digital filts giv low hav th sam magitud spos: i [] [ ] m m i i i x c

More information

Great Idea #4: Parallelism. CS 61C: Great Ideas in Computer Architecture. Pipelining Hazards. Agenda. Review of Last Lecture

Great Idea #4: Parallelism. CS 61C: Great Ideas in Computer Architecture. Pipelining Hazards. Agenda. Review of Last Lecture CS 61C: Gat das i Comput Achitctu Pipliig Hazads Gu Lctu: Jui Hsia 4/12/2013 Spig 2013 Lctu #31 1 Gat da #4: Paalllism Softwa Paalll Rqus Assigd to comput.g. sach Gacia Paalll Thads Assigd to co.g. lookup,

More information

RR-1B. r e Rd W BR O. Wy nd m e RR-1B IX TH. K nol l. r th LR-1A. F arm Rd D A K OTA A VE NG HI LL RD. Long. Lake LR-1A L A KE Y ZA E TR E L IN L UC

RR-1B. r e Rd W BR O. Wy nd m e RR-1B IX TH. K nol l. r th LR-1A. F arm Rd D A K OTA A VE NG HI LL RD. Long. Lake LR-1A L A KE Y ZA E TR E L IN L UC F a c 20 pl a v ac -1B 21 F B faytt -1-1 aag -1-1 iv t ig t P B-4-1-1-1 B P itka Z Bui h aw B B F P B-3 B-4-1B -1B B- PU - ighway cial catial ual idtial -1 - Faily ual idtial - 5 c haig -1-1 - Faily h

More information

Helping every little saver

Helping every little saver Spt th diffc d cut hw u c fid I c spt thigs! Hlpig v littl sv Hw d u p i? I ch Just pp it f u chs. T fid u lcl ch just visit s.c.uk/ch If u pig i chqu, it c tk ud 4 wkig ds t cl Ov th ph Just cll Tlph

More information

RADIO-FREQUENCY WALL CONDITIONING FOR STEADY-STATE STELLARATORS

RADIO-FREQUENCY WALL CONDITIONING FOR STEADY-STATE STELLARATORS RAIO-FREQUENCY WALL CONIIONING FOR SEAY-SAE SELLARAORS Yu. S. Kulyk, V.E.Moisko,. Wauts, A.I.Lyssoiva Istitut of Plasma Physics, Natioal Scic Ct Khakiv Istitut of Physics ad chology, 68 Khakiv, Ukai Laboatoy

More information

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication.

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication. STIPLINES A tiplin i a plana typ tanmiion lin hih i ll uitd fo mioav intgatd iuity and photolithogaphi faiation. It i uually ontutd y thing th nt onduto of idth, on a utat of thikn and thn oving ith anoth

More information

Topic 5:Discrete-Time Fourier Transform (DTFT)

Topic 5:Discrete-Time Fourier Transform (DTFT) ELEC64: Sigals Ad Systms Tpic 5:Discrt-Tim Furir Trasfrm DTFT Aishy Amr Ccrdia Uivrsity Elctrical ad Cmputr Egirig Itrducti DT Furir Trasfrm Sufficit cditi fr th DTFT DT Furir Trasfrm f Pridic Sigals DTFT

More information

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware LG 43 Lctur #6 Mrk Mirtnik, Ph.D. Prfssr Th Univrsity f Dlwr mil: mirtni@c.udl.du Wv Prpgtin nd Plritin TM: Trnsvrs lctrmgntic Wvs A md is prticulr fild cnfigurtin. Fr givn lctrmgntic bundry vlu prblm,

More information

2. SIMPLE SOIL PROPETIES

2. SIMPLE SOIL PROPETIES 2. SIMPLE SOIL PROPETIES 2.1 EIGHT-OLUME RELATIONSHIPS It i oft rquir of th gotchical gir to collct, claify a ivtigat oil ampl. B it for ig of fouatio or i calculatio of arthork volum, trmiatio of oil

More information

Solutions. Definitions pertaining to solutions

Solutions. Definitions pertaining to solutions Slutis Defiitis pertaiig t slutis Slute is the substace that is disslved. It is usually preset i the smaller amut. Slvet is the substace that des the disslvig. It is usually preset i the larger amut. Slubility

More information

The Hydrogen Atom. Chapter 7

The Hydrogen Atom. Chapter 7 Th Hyog Ato Chapt 7 Hyog ato Th vy fist pobl that Schöig hislf tackl with his w wav quatio Poucig th oh s gy lvls a o! lctic pottial gy still plays a ol i a subatoic lvl btw poto a lcto V 4 Schöig q. fo

More information

TECHNICAL INFORMATION MANUAL

TECHNICAL INFORMATION MANUAL TCICAL IFMATI MAUAL MB/MB Blowers Models listed on page 3 efer to ervice Manual 60000 for installation, operation, and troubleshooting information. All safety information must be followed as provided in

More information

ANOVA- Analyisis of Variance

ANOVA- Analyisis of Variance ANOVA- Aalii of Variac CS 700 Comparig altrativ Comparig two altrativ u cofidc itrval Comparig mor tha two altrativ ANOVA Aali of Variac Comparig Mor Tha Two Altrativ Naïv approach Compar cofidc itrval

More information