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 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 paticl. Rquid Rading: L: 5. Additinal/Advancd Rading: Bhn, G.F., and D.R. Huffmn, Abptin and catting f light by mall paticl. Jhn Wily&n, 983. Excllnt wb it n Th ptic f a wat dp: Mi catting Maxwll quatin. Wav quatin. Dilctical cntant f a mdium. Maxwll quatin cnnct th fiv baic quantiti th lctic vct, E, magntic vct, H, magntic inductin, B, lctic diplacmnt, D, and lctic cunt dnity, j : (in cg ytm) D H + c t B E c t D πρ B wh c i a cntant (wav vlcity); and ρ i th lctic chag dnity. π c j [.]

2 T allw a uniqu dtminatin f th lctmagntic fild vct, th Maxwll quatin mut b upplmntd by latin which dcib th bhavi f ubtanc und th influnc f lctmagntic fild. Thy a j E D E [.] B µ E wh i calld th pcific cnductivity; i calld th dilctical cntant ( th pmittivity), and µ i calld th magntic pmability. Dpnding n th valu f, th ubtanc a dividd int: cnduct: dilctic ( inulat): (i.., i NOT ngligibly mall), (f intanc, mtal) (i.., i ngligibly mall), (f intanc, ai al and clud paticulat) Lt cnid th ppagatin f EM wav in a mdium which i (a) unifm, that ha th am valu at all pint; (b) itpic, that i indpndnt f th dictin f ppagatin; (c) nn-cnducting (dilctic), that and thf j ; (d) f fm chag, that ρ. With th aumptin th Maxwll quatin duc t E H c t µ H E c t E H [.3] Eliminating E and H in th fit tw quatin in [.3] and uing th vct thm, w hav

3 µ E E c t µ H H c t [.] Th abv quatin a tandad quatin f wav mtin f a wav ppagating with a vlcity v c µ [.5] wh c i th pd f light in vacuum. NOTE: f vacuum: µ and in cg unit, but in I ytm µ ο and a cntant uch that c / µ. F mt ubtanc (including th ai) µ i unity. Thu, th lctical ppti f a mdium i chaactizd by th dilctical cntant. Rfactiv indx ( ptical cntant) f a mdium i dfind a m [.6] auming that µ. NOTE: tictly paking, in Eq.[.6] i th lativ pmittivity f mdium (h it i lativ t vacuum). Th factiv indx mm +im i in a cmplx numb. Th nnz imaginay pat m i f th factiv indx i pnibl f abptin f th wav a it ppagat thugh th mdium; wha th al pat m f th factiv indx lat t th vlcity f ppagatin f th EM wav. Th factiv indx i a tng functin f th wavlngth. Each ubtanc ha a pcific pctum f th factiv indx. 3

4 aticl f diffnt iz, hap and indic f factin will hav diffnt catting and abbing ppti. Rfactiv indic f wat, ic and m al pci Figu. Ral and imaginay pat f th factiv indx f wat and ic in th IR.

5 Figu. Ral and imaginay pat f th factiv indx f wat and ic in th viibl and na-ir. NOTE: wat ha lw imaginay pat in th viibl > ngligibl abptin by wat dp in th viibl 5

6 Figu.3 Imaginay pat f th factiv indx f m al matial (Bhn and Huffman, Fig.5.6). NOTE: Main abbing pci in th W a black cabn (t) and hmatit (dut), but in th LW vaiu pci hav high imaginay pat f th factiv indx. But vall abptin (i.., abptin cfficint) i al cntlld by paticl iz. 6

7 Al paticl ftn cnit f val chmical pci (calld th intnal mixtu). Th a val appach (calld mixing ul) t calculat th ffctiv factiv indx m f th intnally mixd paticl uing th factiv indic f th individual pci: A) Vlum ( ma) wightd mixing: m m f [.7] wh m j i th factiv indx f j-pci and f j i it vlum factin. B) Buggman appximatin f tw andmly mixd pci: f j j j + f [.8] + + wh i a th dilctic cntant f tw matial and f i a thi vlum factin. Rcall that th factiv indx i m C) Maxwll-Gantt appximatin f tw pciu whn n i a matix (ht matial) with th dilctic cntant and anth i an incluin with : [.9] f + + f + + NOTE: B) and C) appach can b xtndd f th n-cmpnnt mixtu. catting dmain: Rayligh catting: π/λ << and m i abitay (appli t catting by mlcul and mall al paticl); π Rayligh-Gan catting: m << and m << (nt uful f atmphic λ applicatin); Mi-Dby catting: π/λ and m a bth abitay but f ph nly (appli t catting by al and clud paticl) Gmtic ptic: π/λ >> and m i al (appli t catting by lag clud dplt). 7

8 . Mi-Dby thy. NOTE: Mi-Dby thy i ftn calld Mi thy Lntz-Mi thy. Mi thy utlin: Aumptin: i) aticl i a ph f adiu a; ii) aticl i hmgnu (thf it i chaactizd by a ingl factiv indx mm + im i at a givn wavlngth); NOTE: Mi thy qui th lativ factiv indx factiv indx f a paticl/factiv indx f a mdium. But f ai m i abut, n nd t knw th factiv indx f th paticl (i.., factiv indx f th matial f which th paticl i cmpd). NOTE: If a paticl ha cmplx chmical cmpitin, th ffctiv factiv indx mut b calculatd at a givn wavlngth. tatgy: ) k a lutin f a vct wav quatin (Eq.[.]) f E and H E c E t with th bunday cnditin that th tangntial cmpnnt f E and H b cntinuu ac th phical ufac f a paticl. Aumptin n th phical ufac f a paticl allw lving th vct quatin analytically. ) R-wit th wav quatin in phical cdinat and xp lctic fild inid and utid ph in a vct phical hamnic xpanin. NOTE: Mi thy calculat th lctmagntic fild at all pint in th paticl (calld intnal fild) and at all pint f th hmgnu mdium in which th paticl i mbddd. F all pactical applicatin in th atmph, light catting bvatin a caid ut in th fa-fild zn (i.., at th lag ditanc fm a ph): 3) Apply bunday cnditin match tanv fild at ph ufac t btain cattd phical wav Mi cfficint a n and b n which dn t dpnd n th angl 8

9 but dpnd n iz paamt x πa/λ (a i th adiu f th paticl) and vaiabl y x m (m i factiv indx f th paticl). Th xpin f a n and b n a givn by Eq.[5..7] in L. ) U i invlving a n and b n t btain xtinctin and catting fficinci ( and ). 5) U i in Mi angula functin π n and τ n t btain catting amplitud functin (Θ) and (Θ), fm which th catting pha functin i divd. Mi catting amplitud (al calld catting functin) a intducd a n + [ a n π (c Θ ) + b τ (c Θ ] ( Θ ) n n n ) n n ( n + ) n + [ b n (c Θ ) + a τ (c Θ ] ( Θ ) n n n ) n n ( n + ) wh π n and τ n a Mi angula functin π [.] π (c n Θ ) in( Θ ) n (c Θ ) wh d τ n (c Θ ) n (c Θ ) [.] dθ n a th aciatd Lgnd plynmial. In th fa-fild zn (i.., at th lag ditanc fm a ph), th lutin f th vct wav quatin can b btaind a E E l xp( ik + ikz ) ik 3 E E i l i [.] Eq.[.] i a fundamntal quatin f cattd adiatin including plaizatin in th fa fild. ( Θ) ( Θ) 3 ( Θ) ( Θ) i th amplitud catting matix (unitl) F ph: 3 (Θ) (Θ) 9

10 Thu, f ph Eq.[.] duc t wh xp( ikz ) wav. E E l xp( ik + ikz ) ik i th incidnt plan wav, and E E xp( ik ) ik i l i [.3] i th utging cattd Fundamntal xtinctin fmula ( ptical thm) giv th xtinctin c ctin f a paticl π R[ ( )], [.] k But f th fwad dictin (i.. Θ ) fm Eq.[.], w hav [.5] ( ) ( ) (n + )( a n + b n ) n Thu, xtinctin c ctin i latd t catting in fwad dictin. Efficinci ( fficincy fact) f xtinctin, catting and abptin a dfind a a a π a π a [.6] π a wh πa i th paticl aa pjctd nt th plan ppndicula t th incidnt bam. Mi fficincy fact a divd fm th Mi catting amplitud [.7] x ( n + ) R[ a + ] n b n n [.8] x ( n + )[ a + ] n b n n and th abptin fficincy can b calculatd a a [.9]

11 Figu. Exampl f calculatd with Mi thy f val factiv indx. (m in Lab 7). catting pha matix Rcall dfinitin f tk paamt ( Lctu 3), which uniquly chaactiz th lctmagntic wav. Lt I,, U and V b th tk paamt f incidnt fild and I,, U and V b th tk paamt f cattd adiatin V U I V U I π [.] wh i th catting pha matix.

12 [.] wh ach lmnt dpnd n th catting angl (/ i fm lid angl) F ph: and 33 NOTE: In gnal, f a paticl f any hap, th catting pha matix cnit f 6 indpndnt lmnt, but f a ph thi numb duc t fu. Thu f ph, Eq.[.] duc t V U I V U I π [.] wh ach lmnt f th catting pha matix i xpd via th catting amplitud (Θ) and (Θ) [ ] k + π [ ] k π [.3] [ ] 33 k + π [ ] 3 k π (Θ) (Θ) i th catting pha functin dfind in Lctu 3.

13 Figu.5 Exampl f catting pha functin calculatd with Mi thy f val iz paamt f nnabbing ph (m in Lab 7). m highlight f Mi catting ult Extinctin fficincy v. iz paamt x (auming NO ABORTION): ) mall in Rayligh limit: x ) lagt whn paticl and wavlngth hav imila iz 3) --> in gmtic limit ( x ) ) Ocillatin ( Fig..) fm intfnc f tanmittd and diffactd wav id in x f intfnc cillatin dpnd n th factiv indx. Abptin duc intfnc cillatin and kill ippl tuctu. catting and abptin fficinci v. iz paamt with ABORTION: A x : and, nting ay a abbd inid paticl. mall imaginay pat f th factiv indx qui lag paticl t fully abb intnal ay. catting pha functin: fwad pak hight inca damatically with x. F ingl paticl numb f cillatin in (Θ) inca with x. 3

14 3. Optical ppti f an nmbl f phical paticl. Mi thy giv th xtinctin, catting and abptin c-ctin and th catting pha matix f a ingl phical paticl. Rcall Lctu wh th al paticl iz ditibutin w intducd. If th paticl chaactizd by a iz ditibutin N(), th vlum xtinctin, catting and abptin cfficint (in unit LENGTH - ) a calculatd a max min ( ) N ( ) d max ( ) N ( ) d [.] a min max min ( ) N ( ) d ingl catting albd (unitl) if dfind a ω a [.5] Th ingl catting albd giv th pcntag f light which will b cattd in a ingl cattd vnt. catting pha functin i ( Θ ) k ( Θ ) π max [ ] N ( ) d + [.6] min max min ( Θ ) N ( ) d [.6a] Aymmty paamt i fit mmnt f th catting pha functin and i dfind a g (c Θ) c( Θ) d (c Θ) [.6b] g f qual fwad and backwad; g f ttally fwad F many pactical applicatin, th ptical ppti f wat clud a paamtizd a a functin f th ffctiv adiu and liquid wat cntnt (LWC).

15 Th ffctiv adiu i dfind a 3 N ( ) d N ( ) d wh N() i th dplt iz ditibutin (.g., in unit m -3 µm - ). Th liquid wat cntnt (LWC) wa dfind in Lctu : [.7] 3 LWC ρ w V ρ w N ( ) d 3 π [.8] Uing that th xtinctin cfficint f clud dplt i N d N d ( ) ( ) π ( ) and that f wat dplt at la wavlngth, w hav 3 LWC ρ [.9] w Figu.6 Exampl f ptical ppti f typical cumulu and tatu clud (f a clud dplt iz ditibutin ff 6 µm). H th nmalizd xtinctin cfficint i ( λ ) / (.5 m ) and (.5 ).8km. µm µ 5

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 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.

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

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

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

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

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

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

which represents a straight line whose slope is C 1.

which represents a straight line whose slope is C 1. hapte, Slutin 5. Ye, thi claim i eanable ince in the abence any heat eatin the ate heat tane thugh a plain wall in teady peatin mut be cntant. But the value thi cntant mut be ze ince ne ide the wall i

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

Propagation of Light About Rapidly Rotating Neutron Stars. Sheldon Campbell University of Alberta

Propagation of Light About Rapidly Rotating Neutron Stars. Sheldon Campbell University of Alberta Ppagatin f Light Abut Rapily Rtating Nutn Stas Shln Campbll Univsity f Albta Mtivatin Tlscps a nw pcis nugh t tct thmal spcta fm cmpact stas. What flux is masu by an bsv lking at a apily tating lativistic

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

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

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

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

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

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

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

Solutions to Supplementary Problems

Solutions to Supplementary Problems Solution to Supplmntay Poblm Chapt Solution. Fomula (.4): g d G + g : E ping th void atio: G d 2.7 9.8 0.56 (56%) 7 mg Fomula (.6): S Fomula (.40): g d E ping at contnt: S m G 0.56 0.5 0. (%) 2.7 + m E

More information

Gas Exchange Process. Gas Exchange Process. Internal Combustion Engines MAK 493E. Prof.Dr. Cem Soruşbay Istanbul Technical University

Gas Exchange Process. Gas Exchange Process. Internal Combustion Engines MAK 493E. Prof.Dr. Cem Soruşbay Istanbul Technical University Intnal Cmbustin Engins MAK 493E Gas Exchang Pcss Pf.D. Cm Suşbay Istanbul Tchnical Univsity Intnal Cmbustin Engins MAK 493E Gas Exchang Pcss Intductin Valv mchanisms Inductin in ngins Scavnging in -stk

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

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

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

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble

Q Q N, V, e, Quantum Statistics for Ideal Gas and Black Body Radiation. The Canonical Ensemble Quantum Statistics fo Idal Gas and Black Body Radiation Physics 436 Lctu #0 Th Canonical Ensmbl Ei Q Q N V p i 1 Q E i i Bos-Einstin Statistics Paticls with intg valu of spin... qi... q j...... q j...

More information

Chapter 6: Polarization and Crystal Optics

Chapter 6: Polarization and Crystal Optics Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar

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

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLMNTARY INFORMATION. Dtmin th gat inducd bgap cai concntation. Th fild inducd bgap cai concntation in bilay gaphn a indpndntly vaid by contolling th both th top bottom displacmnt lctical filds D t

More information

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have

CHAPTER 17. Solutions for Exercises. Using the expressions given in the Exercise statement for the currents, we have CHATER 7 Slutin f Execie E7. F Equatin 7.5, we have B gap Ki ( t ) c( θ) + Ki ( t ) c( θ 0 ) + Ki ( t ) c( θ 40 a b c ) Uing the expein given in the Execie tateent f the cuent, we have B gap K c( ωt )c(

More information

Duct Efficiency under Full-Load or Modulating Conditions: Implications for Heat Pump Performance

Duct Efficiency under Full-Load or Modulating Conditions: Implications for Heat Pump Performance Duct Efficincy und Full-Lad Mdulating Cnditin: Imlicatin f Hat Pum Pfmanc Lay Palmit and Ein Ku, Ect Inc. Paul Fancic, Univity f Illini, Building Rach Cuncil ABSTRACT Ductwk in uncnditind ac ult in annual

More information

STATISTICAL MECHANICS OF DIATOMIC GASES

STATISTICAL MECHANICS OF DIATOMIC GASES Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific

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

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 301 Signls & Systms Pf. Mk Fwl Discussin #1 Cmplx Numbs nd Cmplx-Vlud Functins Rding Assignmnt: Appndix A f Kmn nd Hck Cmplx Numbs Cmplx numbs is s ts f plynmils. Dfinitin f imginy # j nd sm sulting

More information

Ch. 3: Inverse Kinematics Ch. 4: Velocity Kinematics. The Interventional Centre

Ch. 3: Inverse Kinematics Ch. 4: Velocity Kinematics. The Interventional Centre Ch. : Invee Kinemati Ch. : Velity Kinemati The Inteventinal Cente eap: kinemati eupling Apppiate f ytem that have an am a wit Suh that the wit jint ae ae aligne at a pint F uh ytem, we an plit the invee

More information

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

AIR FORCE RESEARCH LABORATORY

AIR FORCE RESEARCH LABORATORY AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base

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

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

Theoretical Study of Electromagnetic Wave Propagation: Gaussian Bean Method

Theoretical Study of Electromagnetic Wave Propagation: Gaussian Bean Method Applid Mathmatics, 3, 4, 466-47 http://d.doi.og/.436/am.3.498 Publishd Onlin Octob 3 (http://www.scip.og/jounal/am) Thotical Study of Elctomagntic Wav Popagation: Gaussian Ban Mthod E. I. Ugwu, J. E. Ekp,

More information

1. Radiation from an infinitesimal dipole (current element).

1. Radiation from an infinitesimal dipole (current element). LECTURE 3: Radiation fom Infinitsimal (Elmntay) Soucs (Radiation fom an infinitsimal dipol. Duality in Maxwll s quations. Radiation fom an infinitsimal loop. Radiation zons.). Radiation fom an infinitsimal

More information

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals

Hydrogen atom. Energy levels and wave functions Orbital momentum, electron spin and nuclear spin Fine and hyperfine interaction Hydrogen orbitals Hydogn atom Engy lvls and wav functions Obital momntum, lcton spin and nucla spin Fin and hypfin intaction Hydogn obitals Hydogn atom A finmnt of th Rydbg constant: R ~ 109 737.3156841 cm -1 A hydogn mas

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

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics

Aakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)

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

Name Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes.

Name Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes. Name Student ID II. [25 pt] Thi quetin cnit f tw unrelated part. Part 1. In the circuit belw, bulb 1-5 are identical, and the batterie are identical and ideal. Bxe,, and cntain unknwn arrangement f linear

More information

Chapter 9 Compressible Flow 667

Chapter 9 Compressible Flow 667 Chapter 9 Cmpreible Flw 667 9.57 Air flw frm a tank thrugh a nzzle int the tandard atmphere, a in Fig. P9.57. A nrmal hck tand in the exit f the nzzle, a hwn. Etimate (a) the tank preure; and (b) the ma

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

MOS transistors (in subthreshold)

MOS transistors (in subthreshold) MOS tanito (in ubthhold) Hitoy o th Tanito Th tm tanito i a gnic nam o a olid-tat dvic with 3 o mo tminal. Th ild-ct tanito tuctu wa it dcibd in a patnt by J. Lilinld in th 193! t took about 4 ya bo MOS

More information

Lecture 2: Frequency domain analysis, Phasors. Announcements

Lecture 2: Frequency domain analysis, Phasors. Announcements EECS 5 SPRING 24, ctu ctu 2: Fquncy domain analyi, Phao EECS 5 Fall 24, ctu 2 Announcmnt Th cou wb it i http://int.c.bkly.du/~5 Today dicuion ction will mt Th Wdnday dicuion ction will mo to Tuday, 5:-6:,

More information

Lecture 35. Diffraction and Aperture Antennas

Lecture 35. Diffraction and Aperture Antennas ctu 35 Dictin nd ptu ntnns In this lctu u will ln: Dictin f lctmgntic ditin Gin nd ditin pttn f ptu ntnns C 303 Fll 005 Fhn Rn Cnll Univsit Dictin nd ptu ntnns ptu ntnn usull fs t (mtllic) sht with hl

More information

Topic 5: Discrete-Time Fourier Transform (DTFT)

Topic 5: Discrete-Time Fourier Transform (DTFT) ELEC36: Signals And Systms Tpic 5: Discrt-Tim Furir Transfrm (DTFT) Dr. Aishy Amr Cncrdia Univrsity Elctrical and Cmputr Enginring DT Furir Transfrm Ovrviw f Furir mthds DT Furir Transfrm f Pridic Signals

More information

CHAPTER 24 GAUSS LAW

CHAPTER 24 GAUSS LAW CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and

More information

ME 3600 Control Systems Frequency Domain Analysis

ME 3600 Control Systems Frequency Domain Analysis ME 3600 Cntl Systems Fequency Dmain Analysis The fequency espnse f a system is defined as the steady-state espnse f the system t a sinusidal (hamnic) input. F linea systems, the esulting utput is itself

More information

Lecture 2a. Crystal Growth (cont d) ECE723

Lecture 2a. Crystal Growth (cont d) ECE723 Lctur 2a rystal Grwth (cnt d) 1 Distributin f Dpants As a crystal is pulld frm th mlt, th dping cncntratin incrpratd int th crystal (slid) is usually diffrnt frm th dping cncntratin f th mlt (liquid) at

More information

Another Explanation of the Cosmological Redshift. April 6, 2010.

Another Explanation of the Cosmological Redshift. April 6, 2010. Anthr Explanatin f th Csmlgical Rdshift April 6, 010. Jsé Francisc García Juliá C/ Dr. Marc Mrncian, 65, 5. 4605 Valncia (Spain) E-mail: js.garcia@dival.s h lss f nrgy f th phtn with th tim by missin f

More information

(( ) ( ) ( ) ( ) ( 1 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek

(( ) ( ) ( ) ( ) ( 1 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek Two ag ampling and andom ffct 8- Two Stag Clu Sampling and Random Effct Ed Stank FTE POPULATO Fam Labl Expctd Rpon Rpon otation and tminology Expctd Rpon: y = and fo ach ; t = Rpon: k = y + Wk k = indx

More information

Lecture 27: The 180º Hybrid.

Lecture 27: The 180º Hybrid. Whits, EE 48/58 Lctur 7 Pag f 0 Lctur 7: Th 80º Hybrid. Th scnd rciprcal dirctinal cuplr w will discuss is th 80º hybrid. As th nam implis, th utputs frm such a dvic can b 80º ut f phas. Thr ar tw primary

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

Radiation Resistance of System G( Iron Torus is not used as we can see ) ( ) 2

Radiation Resistance of System G( Iron Torus is not used as we can see ) ( ) 2 THE FNAL NVESTGATON ON TORS EXPERMENT N AQNO S SET P n the llwing invetigatin, we ae ging t exaine the equatin Syte G, accding t Pe Aquin clai. THE EQATONS FOR THE TORS EXPERMENT ARE THE FOLLOW: Velcity

More information

Modeling of a Dielectric Barrier Discharge Lamp for UV Production

Modeling of a Dielectric Barrier Discharge Lamp for UV Production Excpt fom th Pocding of th COMSOL Confnc 28 Hannov Modling of a Dilctic Bai Dichag Lamp fo UV Poduction S Bhol* 1, R Diz 1, H Piqut 1, D L Thanh 1, B Rahmani 1, D Buo 1 1 Univité d Toulou - LAPLACE UMR5213-3162

More information

On orthonormal Bernstein polynomial of order eight

On orthonormal Bernstein polynomial of order eight Oen Science Junal f Mathematic and Alicatin 2014; 22): 15-19 Publihed nline Ail 20, 2014 htt://www.enciencenline.cm/junal/jma) On thnmal Bentein lynmial f de eight Suha N. Shihab, Tamaa N. Naif Alied Science

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

UNIFORM PLANE WAVES (PROPAGATION IN FREE SPACE)

UNIFORM PLANE WAVES (PROPAGATION IN FREE SPACE) D. Na Abu-Zaid; Lcu n in lcmagnic h ; Rfncd ngining lcmagnic b a, 8 h diin 0; D. Na Abu-Zaid Pag 7//0 UNIFORM PLAN WAVS (PROPAGATION IN FR SPAC) Saing wih pin fm f Mawll quain f im vaing fild in f pac:

More information

Effect of a radial magnetic field on the stability of Dean flow

Effect of a radial magnetic field on the stability of Dean flow Indian.l unal f Engining & M atials Scincs Vl. 9, Octb 02, pp. 344-350 Effct f a adial magntic fild n th stability f Dan flw MAAli Uni vsity f Bahain, Dpatmnt f M athmatics, PO Bx 338, Bahain Rcivd N vmb

More information

Using Multiwavelength Spectroscopy. Alicia C. Garcia-Lopez

Using Multiwavelength Spectroscopy. Alicia C. Garcia-Lopez Hybid Modl fo Chaactization of Submicon Paticls Using Multiwavlngth Spctoscopy by Alicia C. Gacia-Lopz A disstation submittd in patial fulfillmnt of th quimnts fo th dg of Docto of Philosophy Dpatmnt of

More information

CHAPTER 2 ELECTRIC FIELD

CHAPTER 2 ELECTRIC FIELD lecticity-mgnetim Tutil (QU PROJCT) 9 CHAPTR LCTRIC FILD.. Intductin If we plce tet chge in the pce ne chged d, n electttic fce will ct n the chge. In thi ce we pek f n electic field in thi pce ( nlgy

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

1 st VS 2 nd Laws of Thermodynamics

1 st VS 2 nd Laws of Thermodynamics t VS nd Law f hemdynamic he fit Law Enegy cneatin Quantity pint f iew - In tem f Enegy Enegy cannt be ceated detyed, but it alway cnee - If nt, it ilate t law f themdynamic Enegy input Enegy utput Enegy

More information

Lecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o.

Lecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o. ecture 13 - Bt C-C Cnverter Pwer Electrnic Step-Up r Bt cnverter eliver C pwer frm a lwer vltage C level ( ) t a higher la vltage. i i i + v i c T C (a) + R (a) v 0 0 i 0 R1 t n t ff + t T i n T t ff =

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

International Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN

International Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN Intntinl Junl f Scintific & Engining Rsch, Vlum, Issu 9, Sptmb- bstct: Jcbin intgl nd Stbility f th quilibium psitin f th cnt f mss f n xtnsibl cbl cnnctd stllits systm in th lliptic bit. Vijy Kum ssistnt

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

Theoretical Extension and Experimental Verification of a Frequency-Domain Recursive Approach to Ultrasonic Waves in Multilayered Media

Theoretical Extension and Experimental Verification of a Frequency-Domain Recursive Approach to Ultrasonic Waves in Multilayered Media ECNDT 006 - Post 99 Thotical Extnsion and Expimntal Vification of a Fquncy-Domain Rcusiv Appoach to Ultasonic Wavs in Multilayd Mdia Natalya MANN Quality Assuanc and Rliability Tchnion- Isal Institut of

More information

6. Negative Feedback in Single- Transistor Circuits

6. Negative Feedback in Single- Transistor Circuits Lctur 8: Intrductin t lctrnic analg circuit 36--366 6. Ngativ Fdback in Singl- Tranitr ircuit ugn Paprn, 2008 Our aim i t tudy t ffct f ngativ fdback n t mall-ignal gain and t mall-ignal input and utput

More information

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll

Q Q N, V, e, Quantum Statistics for Ideal Gas. The Canonical Ensemble 10/12/2009. Physics 4362, Lecture #19. Dr. Peter Kroll Quantum Statistics fo Idal Gas Physics 436 Lctu #9 D. Pt Koll Assistant Pofsso Dpatmnt of Chmisty & Biochmisty Univsity of Txas Alington Will psnt a lctu ntitld: Squzing Matt and Pdicting w Compounds:

More information

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function

More information

Chapter 2 Linear Waveshaping: High-pass Circuits

Chapter 2 Linear Waveshaping: High-pass Circuits Puls and Digital Circuits nkata Ra K., Rama Sudha K. and Manmadha Ra G. Chaptr 2 Linar Wavshaping: High-pass Circuits. A ramp shwn in Fig.2p. is applid t a high-pass circuit. Draw t scal th utput wavfrm

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

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD

II.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD II.3. DETEMINTION OF THE ELETON SPEIFI HGE Y MENS OF THE MGNETON METHOD. Wok pupos Th wok pupos is to dtin th atio btwn th absolut alu of th lcton chag and its ass, /, using a dic calld agnton. In this

More information

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL

GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL GAUSS PLANETARY EQUATIONS IN A NON-SINGULAR GRAVITATIONAL POTENTIAL Ioannis Iaklis Haanas * and Michal Hany# * Dpatmnt of Physics and Astonomy, Yok Univsity 34 A Pti Scinc Building Noth Yok, Ontaio, M3J-P3,

More information

Partial Fraction Expansion

Partial Fraction Expansion Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

PHYS 272H Spring 2011 FINAL FORM B. Duration: 2 hours

PHYS 272H Spring 2011 FINAL FORM B. Duration: 2 hours PHYS 7H Sing 11 FINAL Duation: hous All a multil-choic oblms with total oints. Each oblm has on and only on coct answ. All xam ags a doubl-sidd. Th Answ-sht is th last ag. Ta it off to tun in aft you finish.

More information

PHYS 272H Spring 2011 FINAL FORM A. Duration: 2 hours

PHYS 272H Spring 2011 FINAL FORM A. Duration: 2 hours PHYS 7H Sing 11 FINAL Duation: hous All a multil-choic oblms with total oints. Each oblm has on and only on coct answ. All xam ags a doubl-sidd. Th Answ-sht is th last ag. Ta it off to tun in aft you finish.

More information

Free carriers in materials

Free carriers in materials Lctu / F cais in matials Mtals n ~ cm -3 Smiconductos n ~ 8... 9 cm -3 Insulatos n < 8 cm -3 φ isolatd atoms a >> a B a B.59-8 cm 3 ϕ ( Zq) q atom spacing a Lctu / "Two atoms two lvls" φ a T splitting

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

. This is made to keep the kinetic energy at outlet a minimum.

. This is made to keep the kinetic energy at outlet a minimum. Runnr Francis Turbin Th shap th blads a Francis runnr is cmplx. Th xact shap dpnds n its spciic spd. It is bvius rm th quatin spciic spd (Eq.5.8) that highr spciic spd mans lwr had. This rquirs that th

More information

Example

Example hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a

More information

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set WYSE Academic Challenge Sectinal 006 Slutin Set. Cect answe: e. mph is 76 feet pe minute, and 4 mph is 35 feet pe minute. The tip up the hill takes 600/76, 3.4 minutes, and the tip dwn takes 600/35,.70

More information

Chapter 1 The Dawn of Quantum Theory

Chapter 1 The Dawn of Quantum Theory Chapt 1 Th Dawn of Quantum Thoy * By th Lat 18 s - Chmists had -- gnatd a mthod fo dtmining atomic masss -- gnatd th piodic tabl basd on mpiical obsvations -- solvd th stuctu of bnzn -- lucidatd th fundamntals

More information

Sources. My Friends, the above placed Intro was given at ANTENTOP to Antennas Lectures.

Sources. My Friends, the above placed Intro was given at ANTENTOP to Antennas Lectures. ANTENTOP- 01-008, # 010 Radiation fom Infinitsimal (Elmntay) Soucs Fl Youslf a Studnt! Da finds, I would lik to giv to you an intsting and liabl antnna thoy. Hous saching in th wb gav m lots thotical infomation

More information

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007 Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting

More information

Chapter 4 Motion in Two and Three Dimensions

Chapter 4 Motion in Two and Three Dimensions Chapte 4 Mtin in Tw and Thee Dimensins In this chapte we will cntinue t stud the mtin f bjects withut the estictin we put in chapte t me aln a staiht line. Instead we will cnside mtin in a plane (tw dimensinal

More information

FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC B. M. Jovanović, B. Živković

FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC B. M. Jovanović, B. Živković FACTA UNIVERSITATIS Sris: Physics, Chmistry and Tchnlgy Vl., N 5, 3, pp. 45-51 FUNDAMENTAL AND SECOND HARMONIC AMPLITUDES IN A COLLISIONAL MAGNETOACTIVE PLASMA UDC 533.9 B. M. Jvanvić, B. Živkvić Dpartmnt

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

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)

(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4) ots lctu Th IS/LM modl fo an opn conomy is basd on a fixd pic lvl (vy sticky pics) and consists of a goods makt and a mony makt. Th goods makt is Y C+ I + G+ X εq (.) E SEK wh ε = is th al xchang at, E

More information

ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIVE HEAT TRANSFER

ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIVE HEAT TRANSFER ROLE OF FLUCTUATIONAL ELECTRODYNAMICS IN NEAR-FIELD RADIATIE HEAT TRANSFER Mathiu Fancou and M. Pina Mngüç Radiativ Tansf Laboatoy, Dpatmnt of Mchanical Engining Univsity of Kntucky, Lington, KY 456-53,

More information

ELECTROSTATIC FIELDS IN MATERIAL MEDIA

ELECTROSTATIC FIELDS IN MATERIAL MEDIA MF LCTROSTATIC FILDS IN MATRIAL MDIA 3/4/07 LCTURS Materials media may be classified in terms f their cnductivity σ (S/m) as: Cnductrs The cnductivity usually depends n temperature and frequency A material

More information

Electric Charge. Electric charge is quantized. Electric charge is conserved

Electric Charge. Electric charge is quantized. Electric charge is conserved lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne

More information

N J of oscillators in the three lowest quantum

N J of oscillators in the three lowest quantum . a) Calculat th fractinal numbr f scillatrs in th thr lwst quantum stats (j,,,) fr fr and Sl: ( ) ( ) ( ) ( ) ( ).6.98. fr usth sam apprach fr fr j fr frm q. b) .) a) Fr a systm f lcalizd distinguishabl

More information

Chapter 3. Electric Flux Density, Gauss s Law and Divergence

Chapter 3. Electric Flux Density, Gauss s Law and Divergence Chapter 3. Electric Flu Denity, Gau aw and Diergence Hayt; 9/7/009; 3-1 3.1 Electric Flu Denity Faraday Eperiment Cncentric phere filled with dielectric material. + i gien t the inner phere. - i induced

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