LOW ORDER POLYNOMIAL EXPANSION NODAL METHOD FOR A DeCART AXIAL SOLUTION
|
|
- Gabriel Anthony
- 5 years ago
- Views:
Transcription
1 9 Inenaona Nucea Aanc Confeence - INAC 9 Ro de JaneoRJ az epembe7 o Ocobe 9 AOCIAÇÃO RAILEIRA DE ENERGIA NUCLEAR - AEN IN: LOW ORDER POLYNOMIAL EXPANION NODAL METHOD FOR A DeCART AXIAL OLUTION Jn-Young Cho Jae-eung ong and Hyun-Chu Lee Koea Aomc Enegy Reeach Inue 5 Deokjn-dong Yueong-gu Daejon 5-5 Koea jyoung@kae.e.k Koea Aomc Enegy Reeach Inue 5 Deokjn-dong Yueong-gu Daejon 5-5 Koea jong@kae.e.k Koea Aomc Enegy Reeach Inue 5 Deokjn-dong Yueong-gu Daejon 5-5 Koea hc@kae.e.k ATRACT Th pape appe a ow ode poynoma expanon noda (LPEN) mehod o he mpfed Pn (Pn) anpo equaon fo he DeCART (Deemnc Coe Anay baed on Ray Tacng) axa ouon. Fo a pefomance examnaon of he mpemened LPWN mehod he C5G7MOC -D benchmak and he C5G7 hexagona vaaon pobem ae oved. LPEN mehod expand he angua fux momen by ung up o he econd ode Legende poynoma. In he C5G7MOC -D benchmak DeCART how e han 4 pcm egenvaue and e % -D pn powe dbuon eo whch ae ma a he hghe ode noda mehod uch a NEM o ANM. In C5G7 hexagona vaaon pobem DeCART how he ma eo eve a n he C5G7MOX benchmak. Ao LPEN mehod eque e compung me and e memoy ze han he hghe ode noda mehod. Theefoe concuded ha he LPEN mehod moe appcabe o he DeCART ce baed axa ove han he hghe ode noda mehod n apec of accuacy and pefomance.. INTRODUCTION DeCART (Deemnc Coe Anay baed on Ray Tacng) [] a whoe-coe anpo code whch poduce ub-pn eve fux dbuon by ovng he anvee eakage couped ada and axa equaon [4]. The ada ouon of he DeCART code obaned by pefomng he pana ay acng cacuaon fo he MOC anpo equaon by ung axa anvee eakage whou paa homogenzaon. The axa ouon obaned by ovng he P N anpo equaon fo a homogenzed ce by ung ada anvee eakage. The cuen DeCART veon ove he axa mpfed Pn (P N ) equaon by noducng he hghe ode noda mehod uch a NEM [5] and ANM [6]. Ao DeCART noduce a ub-pane cheme whch dvde a hck MOC pane no evea ub-pane o educe he noda effec of he axa kene. The ada anvee eakage appoxmaon and he axa ouon ae cacuaed baed on hee ub-pane. The hghe ode noda mehod uch a NEM and ANM poduce a vey accuae ouon wh a eavey age meh ze by noducng he hghe ode poynoma o he anayc funcon. Howeve fo an effcen cacuaon hoe mehod pe-cacuae and oe he
2 coupng coeffcen befoe he man egenvaue cacuaon. Ao a hown n Fg. n cona o he mooh hape n he aemby baed noda cacuaon he axa anvee eakage n he ce baed cacuaon vae hapy a he odded pane bounday. Theefoe n he DeCART code he hghe ode noda mehod keep a ma meh ze by noducng he ub-pane cheme o ea he anvee eakage hape accuaey whch oe he me of he age meh ze of hee mehod. In h pape a owe ode poynoma expanon noda (LPEN) mehod noduced baed on he ub-pane cheme. The LPEN mehod appoxmae he neuon fux by he econd-ode poynoma and ue fa anvee eakage appoxmaon. Though LPEN eque moe numbe of ub-pane han he hghe ode noda mehod doe no eque pe-cacuaon of he coupng coeffcen due o mpcy. Theefoe h mehod eove boh he accuacy and he memoy pobem. In he nex econ he LPEN mehod decbed accuaey fo he P N equaon. In he foowng econ he C5G7MOX -D benchmak [78] and he C5G7 hexagona vaaon pobem [] ae oved and he accuacy and he pefomance of he LPEN mehod ae dcued. Rada Tanvee Leakage Unodded Regon Rodded Regon Refeco Regon Fne Meh (.484 cm) Noda Meh (.7 cm) Eevaon cm Fgue. Axa hape of Rada Tanvee Leakage. Low Ode Poynoma Expanon Noda Mehod fo P Tanpo Equaon In he LPEN mehod he one-dmenona angua fux momen ae expanded by ung he Legende poynoma a: ( u) ˆ φ ( u) φ ( u) + φ ( u a P () ) INAC 9 Ro de Janeo RJ az.
3 ( u) ˆ φ ( u) φ ( u c P ) whee φ and φ ae he zeo-h and he econd momen fo he angua fux. P (u) he Legende poynoma and a and c ae he expanon coeffcen. The expanon coeffcen of Eq. () can be obaned by ung he noda aveaged and he uface aveaged angua momen a: a φˆ c φˆ ( ˆ ˆ φ φ ) ( ˆ φ φˆ ) a c c ˆ ˆ ˆ φ + φ φ a ( ˆ φ ˆ + φ ) ˆ φ ( ) () whee ˆ φ ˆ φ ˆ φ and ˆ φ ˆ φ ˆ φ ae he node aveaged vaue and he vaue a he gh and ef uface fo he zeo-h and he econd angua fux momen epecvey. The cuen equaon a he gh uface can be expeed n em of he node aveaged momen and he uface momen a: J ˆ + ˆ 6 ˆ β 4φ φ φ J ˆ + ˆ 6 ˆ β 4φ φ φ () whee J and J ae he f and he hd angua momen a he gh uface and β and β ae defned a: D β D and D. h Σ 7 Σ z The noda neuon baance equaon fo he even ode angua momen can be wen a: ( Σ + γ ) ˆ φ Σ ˆ φ + 6γ ( ˆ φ ˆ + φ ) Σ ˆ φ + ( Σ + γ ) ˆ φ + 6γ ( ˆ φ + ˆ φ ) (4) whee Σ Σ + + h N ad ~ ( D Dˆ ) h N ad ~ ( D + Dˆ ) N ad ~ Σ Σ + D h N ad ˆ φ + h β γ hz ~ D ˆ φ INAC 9 Ro de Janeo RJ az.
4 ~ ~ and D and D ae he cuen coupng coeffcen n he odnay fne dffeence mehod ˆ he cuen coecve coeffcen n he coae meh fne dffeence mehod. D Fom he noda baance equaon of Eq. (4) he node aveaged even ode angua momen can be expeed n he max fom a: ˆ φ ˆ φ ˆ + ˆ. (5) φ φ 8 ˆ φ + ˆ φ y neng Eq. (5) o Eq. () he cuen equaon can be wen n he max fom a: J ˆ ˆ (6) Φ + Φ + whee J ˆ J Φˆ φ ˆ Φˆ φ J ˆ φ ˆ φ b b b8 b b b 6 b8 b b4 b5 7 b9 b ( ) b β 6 4 b β ( 6 ) b 6β4 b4 6β b5 6β b 6 β ( 6 8 4) b 7 β ( 6 8 ) b8 6β 7 b9 6β 5 b 6β 6. y ung Eq. (6) he cuen connuy condon a he neface beween node k and k+ can be wen n em of he uface fuxe and he ouce a: k k+ k k+ k+ k k+ ( + ) Φˆ + Φ Φˆ + ˆ. (7) k k In he P appoxmaon he cuen a he pobem bounday can be expeed n em of he uface fux and he ncomng paa cuen a: J αφ ˆ (8) jn whee and J and j 4 jn α j 8 7 J ae he f and he hd ncomng angua momen a he gh uface y ung he wo expeon of Eq. (6) and (8) he cuen connuy condon a he pobem bounday can be wen a: INAC 9 Ro de Janeo RJ az.
5 k k k k ( αφ ) ˆ + ˆ. (9) k k Φ jn The yem equaon fo a pn can be eabhed by coecng a he connuy condon of Eq. (7) and (9) a: whee α + + O O O K K K K + b K K α + K K Φˆ Φˆ Φˆ Φˆ L Φˆ [ ] T Φ ˆ () K K K K [ ] T jn L and K he oa numbe of node n he pobem doman. The yem equaon of Eq. () ncudng he hee bock dagona max of can be oved eay by appyng he bock LU facozaon cheme. If he uface fuxe ae obaned fom Eq. () he node aveaged fuxe of a he node can be obaned by ung Eq. (5). The ougong paa cuen a he pobem bounday whch ued a an ncomng paa cuen of he nex axa pane can be obaned a: jn J Ko αφ ˆ J. () Ko K In he LPEN mehod he coupng coeffcen ae no oed becaue hey can be poduced eay. Ao he anvee eakage hape no mpoan becaue he LPEN mehod ue he fa anvee eakage cheme fo a hn pane ze. Fuhemoe ony he node aveaged fuxe and he ougong paa cuen ae eaed a unknown. Theefoe he LPEN mehod eque vey ma compue memoy compaed o he NEM and ANM. Howeve he LPEN mehod eque abou hee me moe axa node o acheve he accuacy of he NEM and ANM.. Examnaon of he LPEN ouon To examne he ouon accuacy and he compuaona pefomance of he LPEN mehod he C5G7MOX -D benchmak fo ecangua coe and C5G7 hexagona vaaon benchmak fo hexagona coe ae oved. Theee -D benchmak con of pobem of one unodded and wo odded confguaon. The efeence ouon fo he ecangua and hexagona geomee ae gven by MCNP and he McCARD [9] code epecvey. Fg. how he DeCART ce mode fo C5G7MOX enchmak and fo he C5G7 hexagona vaaon pobem. The fue ce f dvded no 8 unfom co econ ng (5 fo fue and fo cooan egon) and hen each unfom co econ ng azmuhay INAC 9 Ro de Janeo RJ az.
6 dvded no 8 o 6 fa ouce egon fo ecangua and hexagona pobem. The efeco ce dvded no oa 8 and 5 fa ouce egon fo ecangua and hexagona pobem. The gap ce exng a he bounday of he hexagona aemby ae f dvded no 4 fa ouce egon and hen chopped by he aemby bounday ne. In ovng he benchmak pobem 4 azmuha ange fo 9± and 6± eco fo he ecangua and he hexagona geomey epecvey and opmzed poa ange and.5 cm ay pacng ae ued. In he coe cacuaon he 45± aemby edge ymmey opon fo he ecangua coe and he ± aemby cene ymmey opon fo he hexagona coe ae ued. (a) Fue Ce Mode (b) Refeco Ce Mode (c) Fue Ce Mode (d) Refeco Ce Mode (e) Aemby Gap Mode Fgue. DeCART Ce Mode fo C5G7MOX and Hexagona Vaaon Pobem. DeCART ove he -D pobem by empoyng he CMFD fomuaon baed on he homogenzed ce and MOC pane. The ada and he axa cuen coecve em of he -D CMFD fomuaon ae uppoed by he pana MOC and he LPEN kene whch pefom he pana MOC cacuaon and he cewe ub-pane cacuaon epecvey. In he MOC cacuaon he axa anvee eakage geneaed by he -D CMFD cacuaon ued. In he axa kene he ada CMFD and axa LPEN couped cacuaon pefomed baed on he homogenzed ce. The cuen geneaed n he MOC and he LPEN kene ae ued fo he cuen coecve em of he -D CMFD fomuaon. Tabe and how he ouon accuacy of he DeCART code accodng o he numbe of ub-pane fo he C5G7MOX -D benchmak and C5G7 hexagona vaaon pobem. The egenvaue and he pn powe dbuon eo appoach o a cean eo eve wh he INAC 9 Ro de Janeo RJ az.
7 nceae of he numbe of ub-pane and each he NEM accuacy when ung ubpane. In he C5G7MOX -D benchmak DeCART how abou and 5 pcm of egenvaue eo and abou.8 %.9 % and.5 % of -D oca pn powe eo fo he unodded odded A and confguaon. In he C5G7 hexagona vaaon pobem DeCART how abou and 5 of pcm egenvaue eo and abou.8 %.7 % and. % of -D oca pn powe eo fo he unodded odded A and confguaon. In he axay negaed - D powe dbuon DeCART how e han. % and abou.5 % eo fo he C5G7MOX -D benchmak and he C5G7 hexagona vaaon pobem. Pobem Unodded Rodded A Rodded Tabe. LPEN ouon Eo fo C5G7MOX enchmak Mehod NEM LPEN Np 5 5 ε k a pcm ε pp b % ε pd c % ε k a pcm ε p b % ε pd c % ε k a pcm ε p b % ε pd c % a Egenvaue Eo Refeence ae and 7777 fo Unodded Rodded A and wh e han 6 pcm of andad Devaon. b Maxmum D Pn Powe Eo c Maxmum D Pn Powe Eo Tabe. LPEN ouon Eo fo C5G7 Hexagona Vaaon Pobem Pobem Np 5 5 ε k a pcm Unodded ε pp b % ε pd c % ε k a pcm Rodded ε A p b % ε pd c % Rodded ε k a pcm ε p b % ε pd c % a Egenvaue Eo Refeence ae.7.89 and 6 fo Unodded Rodded A and wh e han pcm of andad Devaon. b Maxmum D Pn Powe Eo c Maxmum D Pn Powe Eo INAC 9 Ro de Janeo RJ az.
8 Fg. and how he axay negaed pn powe eo fo he Rodded confguaon. The neo pn powe dbuon how eavey e eo han he exeo one and he maxmum eo appea a he coe efeco bounday. In he ecangua pobem DeCART emae a hghe pn powe n he UO aembe and oppoey n he MOX aembe. In he hexagona pobem DeCART emae eavey hghe powe dbuon n he MOX aembe han n he UO aembe. Tabe ummaze he compung me beakup of he DeCART code fo he unodded confguaon accodng o he numbe of ub-pane. The compung me equed fo he MOC kene no eaed o he numbe of ub-pane and hey ae uned ou o be abou 8 and econd fo he ecangua and fo he hexagona coe. The compung me equed fo he -D CMFD and fo he axa LPEN kene nceae neay wh he numbe of ub-pane and hey ae uned ou o be abou 4 and econd fo he ecangua and fo he hexagona coe when ung ub-pane pe MOC pane. Theefoe concuded ha he LPEN mehod we deveoped and he LPEN kene we mpemened o he DeCART code pdecart pef 5 4 e - pef Fgue. Pn Powe Eo fo C5G7MOX Rodded Confguaon. INAC 9 Ro de Janeo RJ az.
9 p e DeCART p ef p ef Fgue. Pn Powe Eo fo C5G7 Hexagona Rodded Confguaon. Tabe. Compung Tme of LPEN Mehod fo C5G7MOX Unodded Pobem (INTEL QUAD(TM) QUAD. GHz econd) Pobem Np 5 5 Toa C5G7MOX CMFD+Axa enchmak MOC C5G7 Hex. Vaaon Toa CMFD+Axa MOC CONCLUION In h pape a ow ode poynoma expanon noda (LPEN) mehod whch expand he angua fux momen up o econd ode Legende poynoma fo he mpfed Pn (Pn) anpo equaon wa deveoped fo he DeCART axa ouon. In he pefomance examnaon DeCART howed e han 4 pcm egenvaue eo and e han % -D pn powe dbuon eo wh abou mnue of compung me when ung ub-pane pe MOC pane. Theefoe concuded ha he LPEN mehod we apped o he DeCART axa kene and poduce a good ouon whn an affodabe compung me. INAC 9 Ro de Janeo RJ az.
10 ACKNOWLEDGMENT Th wok wa uppoed by he Inenaona Nucea Enegy Reeach Inave (INERI) pogam jony funded by he Mny of Educaon cence and Technoogy of Koea and he Depamen of Enegy of he Uned ae. REFERENCE. H-G. Joo J-Y. Cho K-. Km C-C. Lee and -Q. Zee "Mehod and Pefomance of a Thee-Dmenona Whoe-Coe Tanpo Code DeCART" PHYOR 4 Chcago UA Ap. 5-9 (4).. J-Y. Cho K-. Km H-J. hm J-. ong C-C. Lee and H-G. Joo Whoe Coe Tanpo Cacuaon Empoyng Hexagona Modua Ray Tacng and CMFD Fomuaon" Jouna of Nucea cence and Technoogy 45 no (8).. N-Z Cho e a. Refnemen of he -D/-D Fuon Mehod fo -D Whoe-Coe Tanpo Cacuaon Tan. Am. Nuc. oc (). 4.. Koaka and T. Takeda Dffuon-Lke -D Heeogeneou Coe Cacuaon wh -D Chaacec Tanpo Coecon by Non-Lnea Ieaon Technque In. Conf. Nucea Mahemaca and Compuaon cence (M&C ) Ganbug Ap 6- CD-ROM AN (). 5. J-Y Cho K-. Km C-C. Lee -Q. Zee and H-G.. Joo "Axa PN and Rada MOC Couped Whoe Coe Tanpo Cacuaon" Jouna of Nucea cence and Technoogy 44 no (7). 6. J-Y. Cho K-. Km C-C. Lee -Q. Zee and H-G.. Joo "ub-pane cheme fo a Rada Tanpo and Axa Dffuon Code ICAPP 7 Nce Fance May -8 (7). 7. M. A. mh e a. "enchmak on Deemnc Tanpo cacuaon whou paa Homogenzaon (MOX Fue Aemby -D Exenon Cae)" OECD NEA Repo NEA/NC/DOC(5)6 (6). 8. M. A. mh e a. "enchmak on Deemnc -D MOX Fue Aemby Tanpo Cacuaon whou paa Homogenzaon" Poge n Nuc. Enegy 48 8 (6). 9. H-J. hm and C-H. Km "oppng Cea of Inacve Cyce Mone Cao Cacuaon" Nucea cence and Engneeng 57 no. -4 (7). INAC 9 Ro de Janeo RJ az.
Numerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs)
USOD 005 uecal Sudy of Lage-aea An-Reonan Reflecng Opcal Wavegude (ARROW Vecal-Cavy Seconduco Opcal Aplfe (VCSOA anhu Chen Su Fung Yu School of Eleccal and Eleconc Engneeng Conen Inoducon Vecal Cavy Seconduco
More informationSeveral Intensive Steel Quenching Models for Rectangular and Spherical Samples
Recen Advances n Fud Mecancs and Hea & Mass ansfe Sevea Inensve See Quencng Modes fo Recangua and Speca Sampes SANDA BLOMKALNA MARGARIA BUIKE ANDRIS BUIKIS Unvesy of Lava Facuy of Pyscs and Maemacs Insue
More informationOutline. GW approximation. Electrons in solids. The Green Function. Total energy---well solved Single particle excitation---under developing
Peenaon fo Theoecal Condened Mae Phyc n TU Beln Geen-Funcon and GW appoxmaon Xnzheng L Theoy Depamen FHI May.8h 2005 Elecon n old Oulne Toal enegy---well olved Sngle pacle excaon---unde developng The Geen
More informationChapter 6 Plane Motion of Rigid Bodies
Chpe 6 Pne oon of Rd ode 6. Equon of oon fo Rd bod. 6., 6., 6.3 Conde d bod ced upon b ee een foce,, 3,. We cn ume h he bod mde of e numbe n of pce of m Δm (,,, n). Conden f he moon of he m cene of he
More information5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )
5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma
More informationField due to a collection of N discrete point charges: r is in the direction from
Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc
More informationESS 265 Spring Quarter 2005 Kinetic Simulations
SS 65 Spng Quae 5 Knec Sulaon Lecue une 9 5 An aple of an lecoagnec Pacle Code A an eaple of a knec ulaon we wll ue a one denonal elecoagnec ulaon code called KMPO deeloped b Yohhau Oua and Hoh Mauoo.
More information1 Constant Real Rate C 1
Consan Real Rae. Real Rae of Inees Suppose you ae equally happy wh uns of he consumpon good oday o 5 uns of he consumpon good n peod s me. C 5 Tha means you ll be pepaed o gve up uns oday n eun fo 5 uns
More informationName of the Student:
Engneeng Mahemacs 05 SUBJEC NAME : Pobably & Random Pocess SUBJEC CODE : MA645 MAERIAL NAME : Fomula Maeal MAERIAL CODE : JM08AM007 REGULAION : R03 UPDAED ON : Febuay 05 (Scan he above QR code fo he dec
More informationOn Probability Density Function of the Quotient of Generalized Order Statistics from the Weibull Distribution
ISSN 684-843 Joua of Sac Voue 5 8 pp. 7-5 O Pobaby Dey Fuco of he Quoe of Geeaed Ode Sac fo he Webu Dbuo Abac The pobaby dey fuco of Muhaad Aee X k Y k Z whee k X ad Y k ae h ad h geeaed ode ac fo Webu
More informationLecture 5. Plane Wave Reflection and Transmission
Lecue 5 Plane Wave Reflecon and Tansmsson Incden wave: 1z E ( z) xˆ E (0) e 1 H ( z) yˆ E (0) e 1 Nomal Incdence (Revew) z 1 (,, ) E H S y (,, ) 1 1 1 Refleced wave: 1z E ( z) xˆ E E (0) e S H 1 1z H (
More information2 shear strain / L for small angle
Sac quaons F F M al Sess omal sess foce coss-seconal aea eage Shea Sess shea sess shea foce coss-seconal aea llowable Sess Faco of Safe F. S San falue Shea San falue san change n lengh ognal lengh Hooke
More informationThen the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
More informationMatrix Elements of Many-Electron Wavefunctions. noninteger principal quantum number. solutions to Schröd. Eq. outside sphere of radius r
30 - Matx Eements of Many-Eecton Wavefunctons Last tme: ν = R En, f ( ν, ) g ( ν, ) need both f and g to satsfy bounday condton fo E < 0 as ν = n µ πµ s phase shft of f ( ν, ) nonntege pncpa quantum numbe
More informationTHIS PAGE DECLASSIFIED IAW E
THS PAGE DECLASSFED AW E0 2958 BL K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW E0 2958 B L K THS PAGE DECLASSFED AW E0 2958 THS PAGE DECLASSFED AW EO 2958 THS PAGE DECLASSFED AW EO 2958 THS
More informationJackson 4.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 4.7 Homewok obem Soution D. Chistophe S. Baid Univesity of Massachusetts Lowe ROBLEM: A ocaized distibution of chage has a chage density ρ()= 6 e sin θ (a) Make a mutipoe expansion of the potentia
More informationNumerical Integration
MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationExcellent web site with information on various methods and numerical codes for scattering by nonspherical particles:
Lectue 5. Lght catteng and abopton by atmophec patcuate. at 3: Scatteng and abopton by nonpheca patce: Ray-tacng, T- Matx, and FDTD method. Objectve:. Type of nonpheca patce n the atmophee.. Ray-tacng
More informationThree-dimensional systems with spherical symmetry
Thee-dimensiona systems with spheica symmety Thee-dimensiona systems with spheica symmety 006 Quantum Mechanics Pof. Y. F. Chen Thee-dimensiona systems with spheica symmety We conside a patice moving in
More informationChapter 3: Vectors and Two-Dimensional Motion
Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon
More information_ J.. C C A 551NED. - n R ' ' t i :. t ; . b c c : : I I .., I AS IEC. r '2 5? 9
C C A 55NED n R 5 0 9 b c c \ { s AS EC 2 5? 9 Con 0 \ 0265 o + s ^! 4 y!! {! w Y n < R > s s = ~ C c [ + * c n j R c C / e A / = + j ) d /! Y 6 ] s v * ^ / ) v } > { ± n S = S w c s y c C { ~! > R = n
More informationCalculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )
Clculu 4, econ Lm/Connuy & Devve/Inel noe y Tm Plchow, wh domn o el Wh we hve o : veco-vlued uncon, ( ) ( ) ( ) j ( ) nume nd ne o veco The uncon, nd A w done wh eul uncon ( x) nd connuy e he componen
More informationObjectives. We will also get to know about the wavefunction and its use in developing the concept of the structure of atoms.
Modue "Atomic physics and atomic stuctue" Lectue 7 Quantum Mechanica teatment of One-eecton atoms Page 1 Objectives In this ectue, we wi appy the Schodinge Equation to the simpe system Hydogen and compae
More informationDevelopment of Model Reduction using Stability Equation and Cauer Continued Fraction Method
Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More information= ρ. Since this equation is applied to an arbitrary point in space, we can use it to determine the charge density once we know the field.
Gauss s Law In diffeentia fom D = ρ. ince this equation is appied to an abita point in space, we can use it to detemine the chage densit once we know the fied. (We can use this equation to ve fo the fied
More informationLECTURE 14. m 1 m 2 b) Based on the second law of Newton Figure 1 similarly F21 m2 c) Based on the third law of Newton F 12
CTU 4 ] NWTON W O GVITY -The gavity law i foulated fo two point paticle with ae and at a ditance between the. Hee ae the fou tep that bing to univeal law of gavitation dicoveed by NWTON. a Baed on expeiental
More informationPhysics 201 Lecture 15
Phscs 0 Lecue 5 l Goals Lecue 5 v Elo consevaon of oenu n D & D v Inouce oenu an Iulse Coens on oenu Consevaon l oe geneal han consevaon of echancal eneg l oenu Consevaon occus n sses wh no ne eenal foces
More informationSupport Vector Machines
Suppo Veco Machine CSL 3 ARIFICIAL INELLIGENCE SPRING 4 Suppo Veco Machine O, Kenel Machine Diciminan-baed mehod olean cla boundaie Suppo veco coni of eample cloe o bounday Kenel compue imilaiy beeen eample
More informationASTR415: Problem Set #6
ASTR45: Poblem Set #6 Cuan D. Muhlbege Univesity of Mayland (Dated: May 7, 27) Using existing implementations of the leapfog and Runge-Kutta methods fo solving coupled odinay diffeential equations, seveal
More informationP 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 informationSCIENCE CHINA Technological Sciences
SIENE HINA Technologcal Scences Acle Apl 4 Vol.57 No.4: 84 8 do:.7/s43-3-5448- The andom walkng mehod fo he seady lnea convecondffuson equaon wh axsymmec dsc bounday HEN Ka, SONG MengXuan & ZHANG Xng *
More informationChapter Eight Notes N P U1C8S4-6
Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that
More information! -., THIS PAGE DECLASSIFIED IAW EQ t Fr ra _ ce, _., I B T 1CC33ti3HI QI L '14 D? 0. l d! .; ' D. o.. r l y. - - PR Pi B nt 8, HZ5 0 QL
H PAGE DECAFED AW E0 2958 UAF HORCA UD & D m \ Z c PREMNAR D FGHER BOMBER ARC o v N C o m p R C DECEMBER 956 PREPARED B HE UAF HORCA DVO N HRO UGH HE COOPERAON O F HE HORCA DVON HEADQUARER UAREUR DEPARMEN
More informationTRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the
Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection
More informationRevision of Lecture Eight
Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection
More informations = rθ Chapter 10: Rotation 10.1: What is physics?
Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous
More informationA. Inventory model. Why are we interested in it? What do we really study in such cases.
Some general yem model.. Inenory model. Why are we nereed n? Wha do we really udy n uch cae. General raegy of machng wo dmlar procee, ay, machng a fa proce wh a low one. We need an nenory or a buffer or
More information(,,, ) (,,, ). In addition, there are three other consumers, -2, -1, and 0. Consumer -2 has the utility function
MACROECONOMIC THEORY T J KEHOE ECON 87 SPRING 5 PROBLEM SET # Conder an overlappng generaon economy le ha n queon 5 on problem e n whch conumer lve for perod The uly funcon of he conumer born n perod,
More informationLecture 1. time, say t=0, to find the wavefunction at any subsequent time t. This can be carried out by
Lectue The Schödinge equation In quantum mechanics, the fundamenta quantity that descibes both the patice-ike and waveike chaacteistics of patices is wavefunction, Ψ(. The pobabiity of finding a patice
More informationASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.
ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae
More informationMaximum Likelihood Estimation
Mau Lkelhood aon Beln Chen Depaen of Copue Scence & Infoaon ngneeng aonal Tawan oal Unvey Refeence:. he Alpaydn, Inoducon o Machne Leanng, Chape 4, MIT Pe, 4 Saple Sac and Populaon Paaee A Scheac Depcon
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Fne Dffeence Mehod fo Odnay Dffeenal Eqaons Afe eadng hs chape, yo shold be able o. Undesand wha he fne dffeence mehod s and how o se o solve poblems. Wha s he fne dffeence mehod? The fne dffeence
More informationModern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.
Moden Enegy Funconal fo Nucle and Nuclea Mae By: lbeo noosa Teas &M Unvesy REU Cycloon 008 Meno: D. Shalom Shlomo Oulne. Inoducon.. The many-body poblem and he aee-fock mehod. 3. Skyme neacon. 4. aee-fock
More informationJackson 3.3 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 3.3 Homewok Pobem Soution D. Chistophe S. Baid Univesity of Massachusetts Lowe POBLEM: A thin, fat, conducting, cicua disc of adius is ocated in the x-y pane with its cente at the oigin, and is
More informationc- : r - C ' ',. A a \ V
HS PAGE DECLASSFED AW EO 2958 c C \ V A A a HS PAGE DECLASSFED AW EO 2958 HS PAGE DECLASSFED AW EO 2958 = N! [! D!! * J!! [ c 9 c 6 j C v C! ( «! Y y Y ^ L! J ( ) J! J ~ n + ~ L a Y C + J " J 7 = [ " S!
More informationMerging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)
Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationThe Solutions of the Classical Relativistic Two-Body Equation
T. J. of Physics (998), 07 4. c TÜBİTAK The Soutions of the Cassica Reativistic Two-Body Equation Coşkun ÖNEM Eciyes Univesity, Physics Depatment, 38039, Kaysei - TURKEY Received 3.08.996 Abstact With
More informationClassical Electrodynamics
A Fst Look at Quantum Physcs Cassca Eectodynamcs Chapte 4 Mutpoes, Eectostatcs of Macoscopc Meda, Deectcs Cassca Eectodynamcs Pof. Y. F. Chen Contents A Fst Look at Quantum Physcs 4. Mutpoe Expanson 4.
More informationChapter 2: Descriptive Statistics
Chapte : Decptve Stattc Peequte: Chapte. Revew of Uvaate Stattc The cetal teecy of a oe o le yetc tbuto of a et of teval, o hghe, cale coe, ofte uaze by the athetc ea, whch efe a We ca ue the ea to ceate
More informationCHAPTER 10: LINEAR DISCRIMINATION
HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g
More informationΣr2=0. Σ Br. Σ br. Σ r=0. br = Σ. Σa r-s b s (1.2) s=0. Σa r-s b s-t c t (1.3) t=0. cr = Σ. dr = Σ. Σa r-s b s-t c t-u d u (1.4) u =0.
0 Powe of Infinite Seie. Multiple Cauchy Poduct The multinomial theoem i uele fo the powe calculation of infinite eie. Thi i becaue the polynomial theoem depend on the numbe of tem, o it can not be applied
More informationPHYS 705: Classical Mechanics. Central Force Problems I
1 PHYS 705: Cassica Mechanics Centa Foce Pobems I Two-Body Centa Foce Pobem Histoica Backgound: Kepe s Laws on ceestia bodies (~1605) - Based his 3 aws on obsevationa data fom Tycho Bahe - Fomuate his
More informationLINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE
LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization
More informationPHYS 301 HOMEWORK #10 (Optional HW)
PHYS 301 HOMEWORK #10 (Optional HW) 1. Conside the Legende diffeential equation : 1 - x 2 y'' - 2xy' + m m + 1 y = 0 Make the substitution x = cos q and show the Legende equation tansfoms into d 2 y 2
More information-HYBRID LAPLACE TRANSFORM AND APPLICATIONS TO MULTIDIMENSIONAL HYBRID SYSTEMS. PART II: DETERMINING THE ORIGINAL
UPB Sc B See A Vo 72 I 3 2 ISSN 223-727 MUTIPE -HYBRID APACE TRANSORM AND APPICATIONS TO MUTIDIMENSIONA HYBRID SYSTEMS PART II: DETERMININ THE ORIINA Ve PREPEIŢĂ Te VASIACHE 2 Ace co copeeă oă - pce he
More informationMonetary policy and models
Moneay polcy and odels Kes Næss and Kes Haae Moka Noges Bank Moneay Polcy Unvesy of Copenhagen, 8 May 8 Consue pces and oney supply Annual pecenage gowh. -yea ovng aveage Gowh n oney supply Inflaon - 9
More informationTwo-Pion Exchange Currents in Photodisintegration of the Deuteron
Two-Pion Exchange Cuens in Phoodisinegaion of he Deueon Dagaa Rozędzik and Jacek Goak Jagieonian Univesiy Kaków MENU00 3 May 00 Wiiasbug Conen Chia Effecive Fied Theoy ChEFT Eecoagneic cuen oeaos wihin
More informationAlgebra-based Physics II
lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of
More informationCptS 570 Machine Learning School of EECS Washington State University. CptS Machine Learning 1
ps 57 Machne Leann School of EES Washnon Sae Unves ps 57 - Machne Leann Assume nsances of classes ae lneal sepaable Esmae paamees of lnea dscmnan If ( - -) > hen + Else - ps 57 - Machne Leann lassfcaon
More informationDymore User s Manual Two- and three dimensional dynamic inflow models
Dymoe Use s Manual Two- and thee dimensional dynamic inflow models Contents 1 Two-dimensional finite-state genealized dynamic wake theoy 1 Thee-dimensional finite-state genealized dynamic wake theoy 1
More informationA Bijective Approach to the Permutational Power of a Priority Queue
A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation
More informationUniversity of California, Davis Date: June xx, PRELIMINARY EXAMINATION FOR THE Ph.D. DEGREE ANSWER KEY
Unvesy of Calfona, Davs Dae: June xx, 009 Depamen of Economcs Tme: 5 hous Mcoeconomcs Readng Tme: 0 mnues PRELIMIARY EXAMIATIO FOR THE Ph.D. DEGREE Pa I ASWER KEY Ia) Thee ae goods. Good s lesue, measued
More informationMutual Inductance. If current i 1 is time varying, then the Φ B2 flux is varying and this induces an emf ε 2 in coil 2, the emf is
Mutua Inductance If we have a constant cuent i in coi, a constant magnetic fied is ceated and this poduces a constant magnetic fux in coi. Since the Φ B is constant, thee O induced cuent in coi. If cuent
More informationLow-complexity Algorithms for MIMO Multiplexing Systems
Low-complexiy Algoihms fo MIMO Muliplexing Sysems Ouline Inoducion QRD-M M algoihm Algoihm I: : o educe he numbe of suviving pahs. Algoihm II: : o educe he numbe of candidaes fo each ansmied signal. :
More informationTheorem 2: Proof: Note 1: Proof: Note 2:
A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method
More informationX-Ray Notes, Part III
oll 6 X-y oe 3: Pe X-Ry oe, P III oe Deeo Coe oupu o x-y ye h look lke h: We efe ue of que lhly ffee efo h ue y ovk: Co: C ΔS S Sl o oe Ro: SR S Co o oe Ro: CR ΔS C SR Pevouly, we ee he SR fo ye hv pxel
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More informationHomework 1 Solutions CSE 101 Summer 2017
Homewok 1 Soutions CSE 101 Summe 2017 1 Waming Up 1.1 Pobem and Pobem Instance Find the smaest numbe in an aay of n integes a 1, a 2,..., a n. What is the input? What is the output? Is this a pobem o a
More informationCOMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS
ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More information( n x ( ) Last Time Exam 3 results. Question. 3-D particle in box: summary. Modified Bohr model. 3-D Hydrogen atom. r n. = n 2 a o
Last Time Exam 3 esults Quantum tunneling 3-dimensional wave functions Deceasing paticle size Quantum dots paticle in box) This week s honos lectue: Pof. ad histian, Positon Emission Tomogaphy Tue. Dec.
More informationDetection and Estimation Theory
ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu
More informationTopic 4a Introduction to Root Finding & Bracketing Methods
/8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline
More informationLecture Principles of scattering and main concepts.
Lectue 15. Light catteing and aboption by atmopheic paticuate. Pat 1: Pincipe of catteing. Main concept: eementay wave, poaization, Stoke matix, and catteing phae function. Rayeigh catteing. Objective:
More informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More informationOH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9
OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at
More informationV V The circumflex (^) tells us this is a unit vector
Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude
More informationExponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.
Eponenial and Logaihmic Equaions and Popeies of Logaihms Popeies Eponenial a a s = a +s a /a s = a -s (a ) s = a s a b = (ab) Logaihmic log s = log + logs log/s = log - logs log s = s log log a b = loga
More informationPhysics 15 Second Hour Exam
hc 5 Second Hou e nwe e Mulle hoce / ole / ole /6 ole / ------------------------------- ol / I ee eone ole lee how ll wo n ode o ecee l ced. I ou oluon e llegle no ced wll e gen.. onde he collon o wo 7.
More informationRotor Power Feedback Control of Wind Turbine System with Doubly-Fed Induction Generator
Poceedn of he 6h WSEAS Inenaonal Confeence on Smulaon Modelln and Opmzaon Lbon Poual Sepembe -4 6 48 Roo Powe Feedback Conol of Wnd Tubne Syem wh Doubly-Fed Inducon Geneao J. Smajo Faculy of Eleccal Enneen
More informationOn The Estimation of Two Missing Values in Randomized Complete Block Designs
Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.
More informationCoarse Mesh Radiation Transport Code COMET Radiation Therapy Application*
Coase Mesh Radiation Tanspot Code COMT Radiation Theapy Application* Fazad Rahnema Nuclea & Radiological ngineeing and Medical Physics Pogams Geogia Institute of Technology Computational Medical Physics
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationScienceDirect. Behavior of Integral Curves of the Quasilinear Second Order Differential Equations. Alma Omerspahic *
Avalable onlne a wwwscencedeccom ScenceDec oceda Engneeng 69 4 85 86 4h DAAAM Inenaonal Smposum on Inellgen Manufacung and Auomaon Behavo of Inegal Cuves of he uaslnea Second Ode Dffeenal Equaons Alma
More informationPhysics 121 Hour Exam #5 Solution
Physics 2 Hou xam # Solution This exam consists of a five poblems on five pages. Point values ae given with each poblem. They add up to 99 points; you will get fee point to make a total of. In any given
More informationComputational Methods of Solid Mechanics. Project report
Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate
More informationAn o5en- confusing point:
An o5en- confusing point: Recall this example fom last lectue: E due to a unifom spheical suface chage, density = σ. Let s calculate the pessue on the suface. Due to the epulsive foces, thee is an outwad
More information4. Compare the electric force holding the electron in orbit ( r = 0.53
Electostatics WS Electic Foce an Fiel. Calculate the magnitue of the foce between two 3.60-µ C point chages 9.3 cm apat.. How many electons make up a chage of 30.0 µ C? 3. Two chage ust paticles exet a
More informationPrecision Spectrophotometry
Peciion Spectophotomety Pupoe The pinciple of peciion pectophotomety ae illutated in thi expeiment by the detemination of chomium (III). ppaatu Spectophotomete (B&L Spec 20 D) Cuvette (minimum 2) Pipet:
More information1.2 Differential cross section
.2. DIFFERENTIAL CROSS SECTION Febuay 9, 205 Lectue VIII.2 Diffeential coss section We found that the solution to the Schodinge equation has the fom e ik x ψ 2π 3/2 fk, k + e ik x and that fk, k = 2 m
More informationLecture 7: Angular Momentum, Hydrogen Atom
Lectue 7: Angula Momentum, Hydogen Atom Vecto Quantization of Angula Momentum and Nomalization of 3D Rigid Roto wavefunctions Conside l, so L 2 2 2. Thus, we have L 2. Thee ae thee possibilities fo L z
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationA PATRA CONFERINŢĂ A HIDROENERGETICIENILOR DIN ROMÂNIA,
A PATRA ONFERINŢĂ A HIDROENERGETIIENILOR DIN ROMÂNIA, Do Pael MODELLING OF SEDIMENTATION PROESS IN LONGITUDINAL HORIZONTAL TANK MODELAREA PROESELOR DE SEPARARE A FAZELOR ÎN DEANTOARE LONGITUDINALE Da ROBESU,
More informationAuchmuty High School Mathematics Department Advanced Higher Notes Teacher Version
The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!
More information