NOVEL DEVELOPMENTS AND FINDINGS FOR THE SAFETY ASSESSMENT OF EARTHQUAKE-EXCITED DAM-RESERVOIR SYSTEMS

Size: px
Start display at page:

Download "NOVEL DEVELOPMENTS AND FINDINGS FOR THE SAFETY ASSESSMENT OF EARTHQUAKE-EXCITED DAM-RESERVOIR SYSTEMS"

Transcription

1 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia NOVEL DEVELOPMENTS AND FINDINGS FOR TE SAFET ASSESSMENT OF EARTQUAKE-EXCITED DAM-RESERVOIR SSTEMS N. Bouaaai, F. Lu, C. Pault 3, M.A. Chago, ad I. Gogoi 4 Associat Pofsso ail: aib.bouaaai@oltl.ca, Rsach Gaduat Assistat, 3 Rsach Assistat Datt. of Civil, Gological ad Miig Egiig, Écol Poltchiu d Motéal, Caada 4 Lctu, Datt of Civil Egiig, Assa Egiig Istitut, Guwahati, Idia ABSTRACT : Ma das woldwid hav b i svic ov 5 as ad a locatd i high sisicit aas. Th iitial sisic dsig of ths citical stuctus was gall coductd usig silifid thods that do ot full ta ito accout of th daic atu of athua citatio ad th col fluid-stuctu itactio. Although sigificat wo has b do to valuat th sisic sos of das, th is still a d to iov cool usd silifid thods ad to accuatl assss th fficic of o sohisticatd os. Th fist at of this a ooss w actical foulas to valuat athua-iducd hdodaic loadig o coct das. This oigial tchiu galizs th classical addd-ass foulatio b icludig th ffcts of da flibilit ad svoi botto absotio. Fuc sos fuctios of hdodaic ssus withi th svoi a coad to aaltical solutios. It is show that th thod accuatl dicts hdodaic loads ad that it ca b asil iltd i a cout oga o a sadsht. Th scod at of th a ivstigats fiit lt odlig ascts to assss th sisic foac of coct das. Sval fiit lt odls of da-svoi ssts with vaious disios a usd to coduct fuc ad ti doai aalss. Pottial-basd fluid lts ad viscous bouda coditios a validatd agaist aaltical solutios ad th a show to fo aduatl fo actical sisic aalsis of da-svoi ssts. KEWORDS: Da saft, dodaic loadig, Sisic ffcts, Nuical odlig.. INTRODUCTION Da failus a sult i catastohic cosucs, causig cosidabl loss of lif ad ot. Rsach dalig with da saft has b tsivl activ duig th last 5 as to iov udstadig of th col bhavio of da-svoi ssts ad ilt o liabl aoachs ito th cods of actic. Rigoous tchius to ivstigat daic da-svoi itactios a lativl w coad to o stablishd static da aalsis tools. Th ilsto of such igoous tatt dats bac to th ioig wo of Wstgaad 933, who oosd to odl wat actio o a da subctd to hoizotal goud acclatios as a uivalt addd ass hight-wis distibutio alid o th da fac. Although Wstgaad s aaltical solutio glctd da flibilit ad wat cossibilit, it has b widl usd fo a dcads to dsig athua sistat coct das. Daic itactios i da-svoi ssts a col hoa uiig advacd athatical ad uical odlig. Although availabl sohisticatd tchius ca hadl a ascts of ths hoa, silifid ocdus a usful ad still dd to globall valuat th ffcts of da-svoi itactio. This sctio of th a ooss a oigial ad actical ocdu to valuat athua iducd da-svoi itactios, icludig th ffcts of da flibilit, wat cossibilit ad svoi botto wav absotio. I a vious wo, th fist autho of th st a oosd a silifid closd-fo foulatio to valuat athua-iducd hdodaic ssus o coct das Bouaaai t al. 3. Th thod icluds th ffcts of wat cossibilit ad svoi botto wav absotio. Th ifluc of da dfoabilit was howv glctd ad thfo th total hdodaic ssu td o a da duig a athua could ot b dtid. Th fist at of this a ooss a wl iovd ad actical foulatio wh th igid da stictig assutio is waivd.

2 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia O th oth had, tsiv wo has b ddicatd to th dvlot of solid ad fluid fiit lt foulatios, ad thi iltatio i fluid-stuctu itactio obls. Aog ths tchius, Eulia-basd foulatios st sval advatags ad w succssfull alid to tasit wav oagatio obls Nilso t al. 98; Evsti t al. 983, Olso ad Bath 985. I th scod at of this a, a ottial-basd foulatio is adatd to ivstigat da-svoi ssts. Th foulatio is validatd agaist aaltical solutios obtaid ov a wid fuc ag.. SIMPLIFIED FORMULATION.. Thotical bacgoud Th silifid got of a da-svoi sst is show i Figu. Th da has a total hight s ad it iouds a si-ifiit svoi of costat dth. Sdits that a b dositd at svoi botto a also cosidd. A Catsia coodiat sst with as ad with oigi at th hl of th stuctu is adotd ad th followig ai assutios a ad: i th da ad th wat a assud to hav a lia bhavio; ii th wat i th svoi is cossibl ad iviscid, with its otio iotatioal ad liitd to sall alituds; ad iii gavit sufac wavs a glctd. Ud ths assutios, th hdodaic ssu,,t i th svoi i css of th hdostatic ssu obs th wav uatio C t.. wh is th Lalac difftial oato, t th ti vaiabl; ρ th ass dsit of wat ad C th cossio wav vlocit giv b C μ ρ.. i which μ dots th bul odulus of wat. Figu. Da-svoi sst with a silifid got. Cosidig haoic goud otios, hdodaic ssu i th svoi ca th b ssd i fuc doai as t,, t,, i wh th suscit dots th o athua dictio, th citig fuc, ad,, a col-valud fuc sos fuctio. Itoducig this tasfoatio ito E... ilds th classical lholtz uatio

3 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia, C + ;..3 Th col valud ssu fuc sos fuctios alog dictios, ca b ssd as Fvs ad Choa 984,,, Z,,,, ; s..4 wh is th fuc sos fuctio fo th hdodaic ssu at igid da fac du to goud acclatio alog, dictio, is th fuc sos fo hdodaic ssu du to hoizotal acclatio, ψ ψ of th da usta fac, Z is th galizd coodiat alog athua citatio dictio, ad s th total ub of od shas icludd i th aalsis. Thoughout this a, hdodaic ssus ad will b fd to as th igid ad th flibl ats of th total hdodaic ssu, sctivl. Th bouda coditios to b satisfid b hdodaic fuc sos fuctios taslat coatibilit of ssus ad dislacts at da-svoi itfac ad wav absotio at svoi botto Fvs ad Choa 984. Bouda coditios to odl f sufac, gavit wavs o th sc of a ic cov at svoi sufac w also oosd Bouaaai t al. 3. Th col fuc sos fuctios of hdodaic ssus ad ca th b ssd as th suatio of sos fuctios ad cosodig ach to a svoi od g, I a,,,, β ρ..5, I,,,, β ρ..6 wh ad a col-valud fuc ddt igvalus ad othogoal igfuctios satisfig, fo ach svoi od + i..7 [ ] [ ], i i ad wh th ts β,, I ad I a giv b [ ] ; i β + C..9 ; d, I d, I ψ.... Silifid ssios Th coot of th stuctual od sha ψ ca b aoiatd as a oloial fuctio a s ψ.. wh is th coodiat vaig ov th hight of th stuctu asud fo th botto. W show th that

4 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia th igid ad flibl hdodaic ssus at acoustical od a latd b,, G,, F +.. ag I i which l Λ l l Λ l+ F a + a+..3 l Λ s l Λ + s i i G F + a a +..4 Λ s Λ + s ad wh th col-valud fuctio Λ is dfid b z Λ z..5! fo col ad itg ubs, z ad, sctivl. This iotat ad oigial latio lats th flibl ad igid ats of hdodaic ssu fo a giv svoi acoustical od to th vibatio of th stuctu alog a giv od sha. Th igid ssu ca th b dtid usig closd-fo ssios siila to thos dvlod b th fist autho of this a Bouaaai t al. 3. Ths ssios ta accout of wat cossibilit ad wav absotio at svoi botto ad th w show valid fo a wid fuc ag..3. Nuical alicatio Th silifid thod std i th vious sctio is alid to a silifid tiagula da coss-sctio with got isid fo th tallst o-ovflow oolith of Pi Flat da Fvs ad Choa 984. Th da has a hight s.9, a dowsta slo of.8 ad a vtical usta da fac. Th followig da atial otis a slctd: a Poisso s atio ν s. ad a ass dsit ρ s 4 g/ 3. Two valus of odulus of lasticit E s 5 MPa ad E s 35 MPa a cosidd. Th wat is assud cossibl, with a vlocit of ssu wavs C 44 /s, a ass dsit ρ g/ 3 ad a bul odulus ν. 3 MPa. A cubic ofil is chos to aoiat th fist stuctual od sha ψ. Es...3,..4 ad.. a usd to dti th sos fuctios F, G ad. E...4 is th usd to cout th hdodaic ssu fuc sos fuctios illustatd i Figu. Fuc soss a lottd agaist th fuc atio / wh is th fudatal vibatio fuc of th da o igid foudatio with a t svoi. A sufficit ub of svoi ods N 5 is icludd i th aalsis. Th figu shows a cllt agt btw th silifid foulatio ad th aaltical solutio. W also obsv that th ualit of th aoiatio dos ot dca as wav flctio cofficit dcass. 3. FINITE ELEMENT MODELING 3.. Pottial-basd foulatio Th aaltical foulatio std abov icluds th cobid ffcts of wat cossibilit, da flibilit ad wav absotio at svoi botto. It is howv staid b th silifid ctagula got of th ioudd svoi. I this sctio a φ U ottial-basd foulatio is usd to ivstigat da-svoi-foudatio ssts with igula gotis. Assuig a iotatioal wat otio ad ifiitsial vlocit ad dsit chags, ilis th istc of a vlocit ottial φ,, t satisfig th uatios of cotiuit ad g cosvatio Ladau ad Lifshitz 959 φ φ 3.. C t

5 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia Figu. Absolut valu of fuc sos fuctios of oalizd hdodaic ssu at da hl: a α.95 ad E s 5 MPa; b α.95 ad E s 35 MPa; c α.65 ad E s 5 MPa; d α.65 ad E s 35 MPa; Aaltical solutio; -- Silifid foulatio. E. 3.. is associatd to th sstial bouda coditio φ 3.. o th f sufac ad igid boudais, ad to th atual bouda coditio φ u& 3..3 o ovig fluid-stuctu itfacs with ositiv oal vlocit u&, cosodig to uit sufac oal vcto oitig ito th fluid ad out of th stuctu. Usig stadad tchius, th wa vaiatioal fo of E. 3.. ca b obtaid ρ & d + d + d φ δφ V ρ u& δφ S ρ φ δφ V 3..4 C V S V i which V idicats th svoi doai, ad S a svoi bouda wh oal vlocit is scibd. Ud athua citatio, th daic sos of th da ad th svoi a could though coatibilit of vlocit ottial s. hdodaic ssu ad scibd oal vlocit s. oal acclatio at da-svoi itfac. Da-svoi itactio is cotaid i th scod t of E Figu 3 shows a fiit lt sh of a da oolith ioudig a svoi with a igula sha. Usig classical Gali disctizatio, th coulig btw th da ad svoi sub-stuctus ilds th sst of uatios M ss U&& Css Cs U& K ss U - Mss u&& g t M Φ && Cs C & Φ - K Φ - Cs u& g t wh vctos U ad Φ cotai th odal dislacts lativ to th goud ad th odal vlocit ottials, sctivl.

6 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia Figu 3. Fiit lt odl a da-svoi sst ad cosodig bouda coditios. Sub-atics M ss ad K ss st th ass ad stiffss atics fo th da substuctu, ad M ad K thos fo th svoi. A Raligh daig ati C ss is cosidd fo th da substuctu ad sub-atics C s ad C s accout fo da-svoi itactio though focd uilibiu ad coatibilit at fluid-stuctu itfac as illustatd i Figu 3. Sub-ati C accouts fo daig du to g dissiatio at th botto ad/o at th fa usta bouda of th svoi ad is giv b T C ρ N NdS 3..6 S i which N is a stadad isoaatic sha fuctio ati fo fluid lts ad S s dots sufac of th svoi botto bouda. Usig th tchiu oosd b Ls ad Kuhl 969, th absotiv coditio at svoi botto ca b aoiatd b a sis of viscous das lacd at th svoi-foudatio itfac. To su coatibilit btw fluid ad da lts ad abl fluid-stuctu itactio, isoaatic ba lts a istd alog svoi-foudatio itfac. Da lts a th built b coctig ba lt ods to th goud. Da ad ba lt ods a costaid to ov ol diculal to th svoi botto bouda. I th t sctio, th ottial-basd foulatio ad bouda coditios dscibd viousl a cofotd agaist aaltical solutios wh availabl o bouda lt solutios othwis. 3.. Nuical sults Gavit da ooliths ioudig svois with difft shas w aalsd usig th ottial-basd foulatio std abov. Rsults a show fo th sa tiagula da coss-sctio dscibd i sctio.3. Th fiit lt odls a built usig th softwa ADINA 6. Th da ad svoi a odld usig 9-od isoaatic la stss fiit lts icludig icoatibl ods ad 9-od ottial-basd fiit lts, sctivl. Aaltical ad fiit lt solutios a std i Figu 4 fo a ctagula svoi lgth L s ad hight s. W cosid fuc sw atios / vaig fo to 4 wh πc / dots th atual fuc of th full svoi. Th figu illustats a cllt agt btw th sults of ottial-basd fluid lts ad th aaltical solutio is cllt fo th igid cas. It is s that da flibilit ad stuctual daig affcts th accuac of th sults with so slight discacis aaig at high fucis lag tha 3. Figu 5 illustats th ffcts of svoi sha ad wav absotio at svoi botto. Th viscous bouda coditio dscibd i th vious sctio is alid alog th svoi botto usig cosistt luig.

7 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia Figu 4. Absolut valu of fuc sos cuvs of oalizd hdodaic ssus at th hl of th da ioudig a ctagula svoi with α.: a ad b Rigid da; c ad d Flibl da with 5% stuctual daig. Aaltical solutio; -- Pottial-basd fiit lt solutio. Figu 5. Absolut valu of fuc sos cuvs of oalizd hdodaic ssus at th hl of th da: a ad b Rctagula svoi with α.6; c ad d Tiagula svoi with α.6. Aaltical solutio; -- Pottial-basd fiit lt solutio.

8 Th 4 th Wold Cofc o Eathua Egiig Octob -7, 8, Biig, Chia Fo th tiagula svoi Figs. 5 c ad d, fiit lt sults a coad to a bouda lt solutio obtaid usig a oga dvlod b th fist autho Bouaaai ad Pault 5. Figu 5 clal shows that th ottial-basd fiit lt foulatio cobid with th viscous bouda coditio giv cllt sults fo wid fuc ad wav absotio ags. This ottial-basd foulatio ca also b fficitl usd with oth bouda coditios to accout fo g dissiatio at th svoi fa usta o fo daic itactio with a ic sht covig th svoi Bouaaai ad Chago CONCLUSIONS This a std silifid ssios ad o advacd fiit lt tchius to assss th ffct of fluid-stuctu itactio i sisicall citd da-svoi ssts. Sval da-svoi ssts with vaious shas w usd. Th hdodaic fuc sos cuvs obtaid usig th oosd thods w validatd agaist aaltical solutios wh availabl ad bouda lt solutios othwis. Ecllt agt is obtaid ov actical fuc ad wav absotio ags. Th oosd tchius a show to fo aduatl fo actical sisic aalsis of da-svoi ssts i fuc ad ti doais. ACKNOWLEDGEMENTS Fiacial suot fo th Natual Scics ad Egiig Rsach Coucil of Caada ad th Qubc Fud fo Rsach o Natu ad Tcholog is gatfull acowldgd. REFERENCES ADINA Tho ad Modlig Guid. Rot ARD ADINA R & D, Ic. Bouaaai, N. Pault, P., ad Poul, J. 3. A closd-fo foulatio fo athua-iducd hdodaic ssu o gavit das. Joual of Soud ad Vibatio, 33, Bouaaai, N. ad Pault, P. 5. A w bouda coditio fo g adiatio i covd svois usig BEM. Egiig aalsis with bouda lts, 9: 9, Bouaaai, N. ad Chago, M-A. 6. Sisic aalsis of Ic-Da-Rsvoi ssts. st Itatioal Stuctual Scialt Cofc - Caadia Socit of Civil Egiig, Calga, Ma 3-6, Pa ST-. Fvs, G. ad Choa, A.K EAGD-84, a cout oga fo athua aalsis of coct gavit das. Rot No. UCB/EERC-84/, Uivsit of Califoia, Bl, Califoia. Ls, J. ad Kuhl, R.L Fiit daic odl fo ifiit dia. Joual of th Egiig Mchaics Divisio, ASCE, 95, Nilso,.C., Evsti, G.C., ad Wag,.F. 98. Tasit sos of a subgd fluid-could doubl-walld shll stuctu to a ssu uls. Joual of th Acoustical Socit of Aica, 7, Evsti, G.C., Macus, M.S., ad Quzo, A.J Fiit lt aalsis of fluid-filld lastic iig ssts. Elvth Nasta Us's Collouiu, Ma, 4-6. Ladau, L.D. ad Lifshitz, E.M Fluid chaics. Pgao Pss. Olso, L.G. ad Bath, K.J Aalsis of fluid-stuctu itactios: a dict stic could foulatio basd o th fluid vlocit ottial. Couts ad Stuctus, :/, -3.

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

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

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

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

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

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

STATISTICAL PARAMETER ESTIMATION FROM MODAL DATA USING A VARIABLE TRANSFORMATION AND TWO WEIGHTING MATRICES

STATISTICAL PARAMETER ESTIMATION FROM MODAL DATA USING A VARIABLE TRANSFORMATION AND TWO WEIGHTING MATRICES SAISICAL PARAMEER ESIMAION FROM MODAL DAA USING A VARIABLE RANSFORMAION AND WO WEIGHING MARICES Haddad Khodapaast, H., Mottshad, J. E., Badcock, K. J. ad Mas, C. Dpatt of Egiig, Uivsity of Livpool, Livpool

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

Study of the Balance for the DHS Distribution

Study of the Balance for the DHS Distribution Itatioal Mathmatical Foum, Vol. 7, 01, o. 3, 1553-1565 Study of th Balac fo th Distibutio S. A. El-Shhawy Datmt of Mathmatics, Faculty of scic Moufiya Uivsity, Shbi El-Kom, Egyt Cut addss: Datmt of Mathmatics,

More information

DISCRETE-TIME RANDOM PROCESSES

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

More information

Improving the Predictive Capability of Popular SWCCs by Incorporating Maximum Possible Suction

Improving the Predictive Capability of Popular SWCCs by Incorporating Maximum Possible Suction Itatioal Joual of Gocic, 2011, 2, 468-475 doi:10.4236/ijg.2011.24049 Publihd Oli Novb 2011 (http://www.scirp.og/joual/ijg) Ipovig th Pdictiv Capabilit of Popula SWCC b Icopoatig Maxiu Poibl Suctio Abtact

More information

Homework 1: Solutions

Homework 1: Solutions Howo : Solutos No-a Fals supposto tst but passs scal tst lthouh -f th ta as slowss [S /V] vs t th appaac of laty alty th path alo whch slowss s to b tat to obta tavl ts ps o th ol paat S o V as a cosquc

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

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

EXACT MODEL MATCHING AND DISTURBANCE REJECTION FOR GENERAL LINEAR TIME DELAY SYSTEMS VIA MEASUREMENT OUTPUT FEEDBACK

EXACT MODEL MATCHING AND DISTURBANCE REJECTION FOR GENERAL LINEAR TIME DELAY SYSTEMS VIA MEASUREMENT OUTPUT FEEDBACK EXACT ODEL ATCHIN AND DISTURBANCE REJECTION FOR ENERAL LINEAR TIE DELAY SYSTES VIA EASUREENT OUTUT FEEDBACK Fotis N. Kouboulis Halkis Istitut of Tchology Dpatt of Autoatio saha Evoia Halki 344, c kouboulis@tihal.g

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

A Manipulated Deformable Object as an Underactuated Mechanical System

A Manipulated Deformable Object as an Underactuated Mechanical System Maipulatd Dfoabl Obct as a Udactuatd Mchaical Syst Hbt G. a Kostas. Kyiaopoulos bstact. Dfoabl obcts ud aipulatio ca b odld usig fiit lts. h sultig odl is i fact a udactuatd chaical syst. h cosucs of ay

More information

Chapter 6 Perturbation theory

Chapter 6 Perturbation theory Ct 6 Ptutio to 6. Ti-iddt odgt tutio to i o tutio sst is giv to fid solutios of λ ' ; : iltoi of si stt : igvlus of : otool igfutios of ; δ ii Rlig-Södig tutio to ' λ..6. ; : gl iltoi ': tutio λ : sll

More information

MODELLING THE THREE-DIMENSIONAL TIDAL FLOW STRUCTURE IN SEMI-ENCLOSED BASINS. Olav van Duin

MODELLING THE THREE-DIMENSIONAL TIDAL FLOW STRUCTURE IN SEMI-ENCLOSED BASINS. Olav van Duin MODELLIG THE THREE-DIMESIOAL TIDAL FLOW STRUCTURE I SEMI-ECLOSED BASIS Olav va Dui Modllig th th-dimsioal flow stuctu i smi-closd basis Olav va Dui MODELLIG THE THREE-DIMESIOAL TIDAL FLOW STRUCTURE I SEMI-ECLOSED

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

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

Non-Relativistic Limit of Neutron Beta-Decay Cross-Section in the Presence of Strong Magnetic Field

Non-Relativistic Limit of Neutron Beta-Decay Cross-Section in the Presence of Strong Magnetic Field Joual of Scics, Islaic Rublic of Ia 9(): 81-86 (18) Uivsity of Tha, ISSN 116-114 htt://jscics.ut.ac.i No-Rlativistic iit of Nuto Bta-Dcay Coss-Sctio i th Psc of Stog Magtic ild M. Sidi * Datt of hysics,

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

A A A. p mu E mc K mc E p c m c. = d /dk. c = 3.00 x 10 8 m/s e = 1.60 x C 1 ev = 1.60 x J 1 Å = m M Sun = 2 x kg

A A A. p mu E mc K mc E p c m c. = d /dk. c = 3.00 x 10 8 m/s e = 1.60 x C 1 ev = 1.60 x J 1 Å = m M Sun = 2 x kg Physics 9HE-Mod Physics Fial Examiatio Mach 1, 14 (1 poits total) You may ta off this sht. ---------------------------------------------------------------------------------------------- Miscllaous data

More information

The Real Hydrogen Atom

The Real Hydrogen Atom T Ra Hydog Ato ov ad i fist od gt iddt of :.6V a us tubatio toy to dti: agti ffts si-obit ad yfi -A ativisti otios Aso av ab sift du to to sfitatio. Nd QD Dia q. ad dds o H wavfutio at sou of ti fid. Vy

More information

Chapter 3 Higher Order Linear ODEs

Chapter 3 Higher Order Linear ODEs ht High Od i ODEs. Hoogous i ODEs A li qutio: is lld ohoogous. is lld hoogous. Tho. Sus d ostt ultils of solutios of o so o itvl I gi solutios of o I. Dfiitio. futios lld lil iddt o so itvl I if th qutio

More information

A New Method of Estimating Wave Energy from Ground Vibrations

A New Method of Estimating Wave Energy from Ground Vibrations Gomatials, 215, 5, 45-55 Publishd Oli Apil 215 i SciRs. http://www.scip.o/joual/m http://dx.doi.o/1.4236/m.215.525 A Nw Mthod of stimati Wav fom Goud Vibatios K. Ram Chada *, V. R. Sast Dpatmt of Mii ii,

More information

On Jackson's Theorem

On Jackson's Theorem It. J. Cotm. Math. Scics, Vol. 7, 0, o. 4, 49 54 O Jackso's Thom Ema Sami Bhaya Datmt o Mathmatics, Collg o Educatio Babylo Uivsity, Babil, Iaq mabhaya@yahoo.com Abstact W ov that o a uctio W [, ], 0

More information

2012 GCE A Level H2 Maths Solution Paper Let x,

2012 GCE A Level H2 Maths Solution Paper Let x, GCE A Level H Maths Solutio Pape. Let, y ad z be the cost of a ticet fo ude yeas, betwee ad 5 yeas, ad ove 5 yeas categoies espectively. 9 + y + 4z =. 7 + 5y + z = 8. + 4y + 5z = 58.5 Fo ude, ticet costs

More information

( ) L = D e. e e. Example:

( ) L = D e. e e. Example: xapl: A Si p juctio diod av acoss sctioal aa of, a accpto coctatio of 5 0 8 c -3 o t p-sid ad a doo coctatio of 0 6 c -3 o t -sid. T lif ti of ols i -gio is 47 s ad t lif ti of lctos i t p-gio is 5 s.

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

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Basic Science and Humanities

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Basic Science and Humanities P E PESIT Bglo South Cpus Hosu od, k bfo Elctoic Cit, Bgluu -00 Dptt of Bsic Scic d Huitis INTERNAL ASSESSMENT TEST Dt : 0/0/07 Mks: 0 Subjct & Cod : Egiig Mthtics I 5MAT Sc : ALL N of fcult : GVR,GKJ,RR,SV,NHM,DN,KR,

More information

A 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 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 information

Exponential Atomic Decomposition in Generalized Weighted Lebesgue Spaces

Exponential Atomic Decomposition in Generalized Weighted Lebesgue Spaces Joual of Mathatics Rsach; Vol 6 No 4; 4 ISSN 96-9795 E-ISSN 96-989 Publish by Caaia Ct of Scic a Eucatio Exotial Atoic Dcoosio i Galiz Wight Lbsgu Sacs Nasibova NP Istut of Mathatics a Mchaics of NAS of

More information

ln x = n e = 20 (nearest integer)

ln x = n e = 20 (nearest integer) H JC Prlim Solutios 6 a + b y a + b / / dy a b 3/ d dy a b at, d Giv quatio of ormal at is y dy ad y wh. d a b () (,) is o th curv a+ b () y.9958 Qustio Solvig () ad (), w hav a, b. Qustio d.77 d d d.77

More information

A novel analytic potential function applied to neutral diatomic molecules and charged lons

A novel analytic potential function applied to neutral diatomic molecules and charged lons Vol., No., 84-89 (00 http://dx.doi.o/0.46/s.00.08 Natual Scic A ovl aalytic pottial fuctio applid to utal diatomic molculs ad chad los Cha-F Yu, Cha-Ju Zhu, Cho-Hui Zha, Li-Xu So, Qiu-Pi Wa Dpatmt of physics,

More information

International Journal of Mathematics Trends and Technology (IJMTT) Volume 47 Number 1 July 2017

International Journal of Mathematics Trends and Technology (IJMTT) Volume 47 Number 1 July 2017 Iteatioal Joual of Matheatics Teds ad Techology (IJMTT) Volue 47 Nube July 07 Coe Metic Saces, Coe Rectagula Metic Saces ad Coo Fixed Poit Theoes M. Sivastava; S.C. Ghosh Deatet of Matheatics, D.A.V. College

More information

T h e C S E T I P r o j e c t

T 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

DFT: Discrete Fourier Transform

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

More information

Low frequency sound transmission of double plates. in an impedance tube

Low frequency sound transmission of double plates. in an impedance tube INTER-NOISE 6 ow fequec soud tasissio of double lates i a iedace tube Hu-Sil KI ; Jae-Seug KI ; Seog-Hu EE 3 ; Yu-Ho SEO 4 ; Pug-Sik A 5 Acoustics ad Noise Reseach Tea Koea Istitute of achie ad ateials,

More information

Problem Session (3) for Chapter 4 Signal Modeling

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

More information

P a g e 3 6 of R e p o r t P B 4 / 0 9

P a g e 3 6 of R e p o r t P B 4 / 0 9 P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J

More information

Output Control of Nonlinear Systems with Unmodelled Dynamics 1

Output Control of Nonlinear Systems with Unmodelled Dynamics 1 Ppits of th 9th Wold Cogss h Itatioal Fdatio of Autoatic Cotol Cap ow South Afica. August -9 Output Cotol of Nolia Systs with Uodlld Dyaics Alxy A. Bobtsov *;** Sgy A. Kolyubi *** Ato A. Pyki * Alksad

More information

Improved Soil-Water Characteristic Curves and Permeability Functions for Unsaturated Soils

Improved Soil-Water Characteristic Curves and Permeability Functions for Unsaturated Soils Ipovd SoilWat haactitic uv ad Pailit Fuctio fo Uatuatd Soil Shada H. Kihapillai, Nadaajah Ravichada ivil Egiig Dpatt lo Uivit, lo, S, USA ABSTRAT Soilwat chaactitic cuv (SW) which pt th oituuctio latio

More information

Magnetic effects and the peculiarity of the electron spin in Atoms

Magnetic effects and the peculiarity of the electron spin in Atoms Magtic ffcts ad t pculiaity of t lcto spi i Atos Pit Za Hdik otz Nobl Piz 90 Otto t Nobl 9 Wolfgag Pauli Nobl 95 ctu Nots tuctu of Matt: Atos ad Molculs; W. Ubacs T obital agula otu of a lcto i obit iclassical

More information

Previous knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators

Previous knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators // vious owg ui phica haoics a so o thi poptis Goup thoy Quatu chaics pctoscopy H. Haga 8 phica haoics Rcs Bia. iv «Iucib Tso thos A Itouctio o chists» Acaic ss D.A. c Quai.D. io «hii hysiu Appoch oécuai»

More information

Quantization of Atomic Energy Levels

Quantization of Atomic Energy Levels Quatizatio o Atomic Egy Lvls Atomic Scta Th ist al clus to th tu atu ad stuctu o atoms 1 w ovidd by atomic scta Dcads bo uthod dvlod his modl o th atom ad Plack advacd his quatum thoy o blackbody adiatio,

More information

PURE MATHEMATICS A-LEVEL PAPER 1

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

More information

Quantum Mechanics Lecture Notes 10 April 2007 Meg Noah

Quantum Mechanics Lecture Notes 10 April 2007 Meg Noah The -Patice syste: ˆ H V This is difficut to sove. y V 1 ˆ H V 1 1 1 1 ˆ = ad with 1 1 Hˆ Cete of Mass ˆ fo Patice i fee space He Reative Haitoia eative coodiate of the tota oetu Pˆ the tota oetu tota

More information

Zeroth moment of the Boltzmann Equation The Equation of Continuity (Particle conservation)

Zeroth moment of the Boltzmann Equation The Equation of Continuity (Particle conservation) Plasas as Fluids At this poit w d to us a ub of basi quatios that dsib plasas as fluids. Whil it is possibl to alulat ths quatios fo fist piipls, usig Maxwll s ltoagti fild quatios ad Maxwll s vloity distibutio

More information

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r.

a) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r. Solutios to MAML Olympiad Level 00. Factioated a) The aveage (mea) of the two factios is halfway betwee them: p ps+ q ps+ q + q s qs qs b) The aswe is yes. Assume without loss of geeality that p

More information

TYRE NOISE HORN EFFECT ON AN ABSORBING ROAD SURFACE SEMI-ANALYTICAL MODELLING USING THE MULTIPOLE SYNTHESIS

TYRE NOISE HORN EFFECT ON AN ABSORBING ROAD SURFACE SEMI-ANALYTICAL MODELLING USING THE MULTIPOLE SYNTHESIS TYRE NOISE HORN EFFECT ON AN ABSORBING ROAD SURFACE SEMI-ANALYTICAL MODELLING USING THE MULTIPOLE SYNTHESIS PACS REFERENCE: NUM- Philippe Klei INRETS 5 aveue Façois Mittead Case 4 BRON FRANCE Tel: +33

More information

Rectangular Waveguides

Rectangular Waveguides Rtgulr Wvguids Wvguids tt://www.tllguid.o/wvguidlirit.tl Uss To rdu ttutio loss ig rquis ig owr C ort ol ov rti rquis Ats s ig-ss iltr Norll irulr or rtgulr W will ssu losslss rtgulr tt://www..surr..u/prsol/d.jris/wguid.tl

More information

Digital Signal Processing, Fall 2006

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

More information

Probability & Statistics,

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

More information

2011 HSC Mathematics Extension 1 Solutions

2011 HSC Mathematics Extension 1 Solutions 0 HSC Mathmatics Etsio Solutios Qustio, (a) A B 9, (b) : 9, P 5 0, 5 5 7, si cos si d d by th quotit ul si (c) 0 si cos si si cos si 0 0 () I u du d u cos d u.du cos (f) f l Now 0 fo all l l fo all Rag

More information

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

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

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

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

The Reign of Grace and Life. Romans 5:12-21 (5:12-14, 17 focus)

The Reign of Grace and Life. Romans 5:12-21 (5:12-14, 17 focus) Th Rig of Gc d Lif Rom 5:12-21 (5:12-14, 17 focu) Th Ifluc of O h d ud Adolph H J o ph Smith B i t l m t Fid Idi Gdhi Ci Lu Gu ich N itz y l M d i M ch Nlo h Vig T L M uhmmd B m i o t T Ju Chit w I N h

More information

DESIGN AND ANALYSIS OF HORN ANTENNA AND ITS ARRAYS AT C BAND

DESIGN AND ANALYSIS OF HORN ANTENNA AND ITS ARRAYS AT C BAND Itatioal Joual of lctoics, Commuicatio & Istumtatio giig Rsach ad Dvlopmt (IJCIRD) ISS(P): 49-684X; ISS(): 49-795 Vol. 5, Issu 5, Oct 5, -4 TJPRC Pvt. Ltd. DSIG AD AALYSIS OF HOR ATA AD ITS ARRAYS AT C

More information

Classical Theory of Fourier Series : Demystified and Generalised VIVEK V. RANE. The Institute of Science, 15, Madam Cama Road, Mumbai

Classical Theory of Fourier Series : Demystified and Generalised VIVEK V. RANE. The Institute of Science, 15, Madam Cama Road, Mumbai Clssil Thoy o Foi Sis : Dmystii Glis VIVEK V RANE Th Istitt o Si 5 Mm Cm Ro Mmbi-4 3 -mil ss : v_v_@yhoooi Abstt : Fo Rim itgbl tio o itvl o poit thi w i Foi Sis t th poit o th itvl big ot how wh th tio

More information

MA 1201 Engineering Mathematics MO/2017 Tutorial Sheet No. 2

MA 1201 Engineering Mathematics MO/2017 Tutorial Sheet No. 2 BIRLA INSTITUTE OF TECHNOLOGY, MESRA, RANCHI DEPARTMENT OF MATHEMATICS MA Egieeig Matheatis MO/7 Tutoia Sheet No. Modue IV:. Defie Beta futio ad Gaa futio.. Pove that,,,. Pove that, d. Pove that. & whee

More information

Technical Report: Bessel Filter Analysis

Technical Report: Bessel Filter Analysis Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we

More information

Narayana IIT Academy

Narayana IIT Academy INDIA Sc: LT-IIT-SPARK Dat: 9--8 6_P Max.Mars: 86 KEY SHEET PHYSIS A 5 D 6 7 A,B 8 B,D 9 A,B A,,D A,B, A,B B, A,B 5 A 6 D 7 8 A HEMISTRY 9 A B D B B 5 A,B,,D 6 A,,D 7 B,,D 8 A,B,,D 9 A,B, A,B, A,B,,D A,B,

More information

Temperature Distribution Control of Reactor Furnace by State Space Method using FEM Modeling

Temperature Distribution Control of Reactor Furnace by State Space Method using FEM Modeling Mmois of th Faculty of Egiig, Okayama ivsity, Vol. 4, pp. 79-90, Jauay 008 Tmpatu Distibutio Cotol of Racto Fuac by Stat Spac Mthod usig FEM Modlig Tadafumi NOTS Divisio of Elctoic ad Ifomatio Systm Egiig

More information

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane. CBSE CBSE SET- SECTION. Gv tht d W d to fd 7 7 Hc, 7 7 7. Lt,. W ow tht.. Thus,. Cosd th vcto quto of th pl.. z. - + z = - + z = Thus th Cts quto of th pl s - + z = Lt d th dstc tw th pot,, - to th pl.

More information

MATH 2300 review problems for Exam 2

MATH 2300 review problems for Exam 2 MATH 2300 review problems for Exam 2. A metal plate of costat desity ρ (i gm/cm 2 ) has a shape bouded by the curve y = x, the x-axis, ad the lie x =. (a) Fid the mass of the plate. Iclude uits. Mass =

More information

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

(Reference: sections in Silberberg 5 th ed.)

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

More information

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist

More information

y = f x x 1. If f x = e 2x tan -1 x, then f 1 = e 2 2 e 2 p C e 2 D e 2 p+1 4

y = f x x 1. If f x = e 2x tan -1 x, then f 1 = e 2 2 e 2 p C e 2 D e 2 p+1 4 . If f = e ta -, the f = e e p e e p e p+ 4 f = e ta -, so f = e ta - + e, so + f = e p + e = e p + e or f = e p + 4. The slope of the lie taget to the curve - + = at the poit, - is - 5 Differetiate -

More information

Week 03 Discussion. 30% are serious, and 50% are stable. Of the critical ones, 30% die; of the serious, 10% die; and of the stable, 2% die.

Week 03 Discussion. 30% are serious, and 50% are stable. Of the critical ones, 30% die; of the serious, 10% die; and of the stable, 2% die. STAT 400 Wee 03 Discussio Fall 07. ~.5- ~.6- At the begiig of a cetai study of a gou of esos, 5% wee classified as heavy smoes, 30% as light smoes, ad 55% as osmoes. I the five-yea study, it was detemied

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

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines

School of Aerospace Engineering Origins of Quantum Theory. Measurements of emission of light (EM radiation) from (H) atoms found discrete lines Ogs of Quatu Thoy Masuts of sso of lght (EM adato) fo (H) atos foud dsct ls 5 4 Abl to ft to followg ss psso ν R λ c λwavlgth, νfqucy, cspd lght RRydbg Costat (~09,7677.58c - ),,, +, +,..g.,,.6, 0.6, (Lya

More information

A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS

A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS A NEW SOLUTION FOR SHALLOW AND DEEP TUNNELS BY CONSIDERING THE GRAVITATIONAL LOADS MOHAMMAD REZA ZAREIFARD and AHMAD FAHIMIFAR about th authos Mohammad Rza Zaifad Amikabi Univsity of Tchnology Than, Ian

More information

Loss factor for a clamped edge circular plate subjected to an eccentric loading

Loss factor for a clamped edge circular plate subjected to an eccentric loading ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut

More information

Masses and orbits of minor planets with the GAIA mission

Masses and orbits of minor planets with the GAIA mission asses ad obits of io laets with the GAIA issio Sege ouet Suevisos : F.igad D.Hestoffe PLAN Itoductio Puose of the PhD Iotace of asses The diffeet ethods to estiate these asses Descitio of close aoach Diffeet

More information

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables Sogklaaka J. Sc. Tchol. 4 () 4-48 Ma. -. 8 Ogal tcl Nw bouds o Posso aomato to th dstbuto of a sum of gatv bomal adom vaabls * Kat Taabola Datmt of Mathmatcs Faculty of Scc Buaha Uvsty Muag Chobu 3 Thalad

More information

Structure and Some Geometric Properties of Nakano Difference Sequence Space

Structure and Some Geometric Properties of Nakano Difference Sequence Space Stuctue ad Soe Geoetic Poeties of Naao Diffeece Sequece Sace N Faied ad AA Baey Deatet of Matheatics, Faculty of Sciece, Ai Shas Uivesity, Caio, Egyt awad_baey@yahooco Abstact: I this ae, we exted the

More information

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

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

More information

New Advanced Higher Mathematics: Formulae

New Advanced Higher Mathematics: Formulae Advcd High Mthmtics Nw Advcd High Mthmtics: Fomul G (G): Fomul you must mmois i od to pss Advcd High mths s thy ot o th fomul sht. Am (A): Ths fomul giv o th fomul sht. ut it will still usful fo you to

More information

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120 Tim : hr. Tst Papr 8 D 4//5 Bch - R Marks : SINGLE CORRECT CHOICE TYPE [4, ]. If th compl umbr z sisfis th coditio z 3, th th last valu of z is qual to : z (A) 5/3 (B) 8/3 (C) /3 (D) o of ths 5 4. Th itgral,

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

Discussion 02 Solutions

Discussion 02 Solutions STAT 400 Discussio 0 Solutios Spig 08. ~.5 ~.6 At the begiig of a cetai study of a goup of pesos, 5% wee classified as heavy smoes, 30% as light smoes, ad 55% as osmoes. I the fiveyea study, it was detemied

More information

3D Viewing. Vanishing Points. Two ways Intersection of transformed lines Transformation of points at infinity. Y VP z. VP x

3D Viewing. Vanishing Points. Two ways Intersection of transformed lines Transformation of points at infinity. Y VP z. VP x Vaishig Poits Two ways Itsctio of tasfomd lis Tasfomatio of oits at ifiity Y Y VP z X VP x X Z Pla Gomtic Pojctios Paalll Pscti Othogahic Axoomtic Obliq Sigl Poit Timtic Dimtic Isomtic Caali Cabit Two

More information

The Dynamics of Shock Amplification

The Dynamics of Shock Amplification Pocdigs of th Wold Cogss o Egiig Vol II WCE, July -,, Lodo, UK Th Dyaics of Shock Aplificatio Bya Rodgs, Sush Goyal, Gad Klly, ad Michal Shhy Abstact W xai th dyaics of vlocity aplificatio though pai-wis

More information

Math 7409 Homework 2 Fall from which we can calculate the cycle index of the action of S 5 on pairs of vertices as

Math 7409 Homework 2 Fall from which we can calculate the cycle index of the action of S 5 on pairs of vertices as Math 7409 Hoewok 2 Fall 2010 1. Eueate the equivalece classes of siple gaphs o 5 vetices by usig the patte ivetoy as a guide. The cycle idex of S 5 actig o 5 vetices is 1 x 5 120 1 10 x 3 1 x 2 15 x 1

More information

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor Cotol Syt ctu 8 Root ocu Clacal Cotol Pof. Eugo Schut hgh Uvty Root ocu Cotoll Plat R E C U Y - H C D So Y C C R C H Wtg th loo ga a w a ttd tackg th clod-loo ol a ga va Clacal Cotol Pof. Eugo Schut hgh

More information

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms

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

More information

OH 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! 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 information

Software Process Models there are many process model s in th e li t e ra t u re, s om e a r e prescriptions and some are descriptions you need to mode

Software Process Models there are many process model s in th e li t e ra t u re, s om e a r e prescriptions and some are descriptions you need to mode Unit 2 : Software Process O b j ec t i ve This unit introduces software systems engineering through a discussion of software processes and their principal characteristics. In order to achieve the desireable

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

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna

Born-Oppenheimer Approximation and Nonadiabatic Effects. Hans Lischka University of Vienna Bo-Oppeheie Appoxiatio ad Noadiabatic Effects Has Lischa Uivesity of Viea Typical situatio. Fac-Codo excitatio fo the iiu of the goud state. Covetioal dyaics possibly M* ad TS 3. Coical itesectio fuel

More information

Consider that special case of a viscous fluid near a wall that is set suddenly in motion as shown in Figure 1. The unsteady Navier-Stokes reduces to

Consider that special case of a viscous fluid near a wall that is set suddenly in motion as shown in Figure 1. The unsteady Navier-Stokes reduces to Exact Solutios to the Navier-Stokes Equatio Ustead Parallel Flows (Plate Suddel Set i Motio) Cosider that special case of a viscous fluid ear a wall that is set suddel i motio as show i Figure. The ustead

More information

Fourier Series and the Wave Equation

Fourier Series and the Wave Equation Fourier Series ad the Wave Equatio We start with the oe-dimesioal wave equatio u u =, x u(, t) = u(, t) =, ux (,) = f( x), u ( x,) = This represets a vibratig strig, where u is the displacemet of the strig

More information

6.Optical and electronic properties of Low

6.Optical and electronic properties of Low 6.Optical and lctonic poptis of Low dinsional atials (I). Concpt of Engy Band. Bonding foation in H Molculs Lina cobination of atoic obital (LCAO) Schoding quation:(- i VionV) E find a,a s.t. E is in a

More information

Potential Energy of the Electron in a Hydrogen Atom and a Model of a Virtual Particle Pair Constituting the Vacuum

Potential Energy of the Electron in a Hydrogen Atom and a Model of a Virtual Particle Pair Constituting the Vacuum Applid Physics Rsach; Vol 1, No 4; 18 ISSN 1916-9639 -ISSN 1916-9647 Publishd by Caadia Ct of Scic ad ducatio Pottial gy of th lcto i a Hydog Atom ad a Modl of a Vitual Paticl Pai Costitutig th Vacuum

More information

SHEET BENDING THEORY APPLIED TO A THREE ROLL PROCESS

SHEET BENDING THEORY APPLIED TO A THREE ROLL PROCESS SHT BNDING THORY APPLID TO A THR ROLL PROCSS João Baisa d Aguia, Galdo Magla Baosa ad Gila Fia Baalha Uivsi of Sao Paulo Polchic School D. of Mchaoics ad Mchaical Sss giig Av. Pof. Mllo Moas, 05508.900

More information