Calculation of Thermal Neutron Flux in Two. Dimensional Structures with Periodic Moderators

Size: px
Start display at page:

Download "Calculation of Thermal Neutron Flux in Two. Dimensional Structures with Periodic Moderators"

Transcription

1 Apple Mhemcl Scences Vol. 8 no Clculon of Theml Neuon Flu n Two mensonl Sucues wh Peoc Moeos S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn In Unvesy of Scence n Technology Tehn In epmen of Nucle Physcs hossenmolgh@us.c. In Unvesy of Scence n Technology Tehn In epmen of Nucle Physcs Absc In hs ppe we compue he heml neuon ffuson flu s funcon of spce n me n wo-mensonl sucues wh peoc moeos compose of ccul os wh sque lces. The moeos e ssume o be C n HO. Ou compuons e gven n wo mn seps. Sep one: he moeos nse n ouse of he o e ssume h become C n HO especvely.sep wo: hs sep s he nvese of sep one. In such sucues mpng consn egons e efne s egons n whch heml neuon ffuson cnno e plce ppe. We efne hese mpng consn egons s ffuson bn gps. Keywos : neuon moeo ffuson flu bn gp. Inoucon The fel of neuon physcs hs become n negl p of nvesgons no n y of mpon ssues h spn fels s vese s nucle n pcle physcs funmenl symmees sophyscs n cosmology funmenl consns gvon n he nepeon of qunum mechncs. We efne heml neuons o be neuons wh enegy nely 5mev.Fs neuons ech he heml egme mos effcenly hough csce of oughly collsons wh me ch n hyogen o eueum. Col neuons e pouce by cyogenc neuon moeo jcen o he eco coe o spllon ge hel empeue of K. One genelly wns he moeo s col s possble o ncese he phse spce ensy of he neuons. As he neuon wvelenghs become lge compe o he omc spcng he ol sceng coss secons n

2 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn me e omne by elsc o quselsc pocesses n becomes moe ffcul fo he neuons o hemlze. Neuons e pouce fom fsson n esech eco n vege enegy of ppomely MeV. They e slowe o heml enegy n moeo such s hevy o lgh we gphe o beyllum suounng he fuel. Theml neuon ffuson hs ce much enon fo mny yes s one of he mos mpon poblems n nucle fsson [-] n fuson. In nucle fsson s mpon o conol heml neuon ffuson n nucle ecos. Fo emple he nhbon of heml neuon ffuson my pove novel pplcons n nucle ecos. In nucle fuson um whch s genee by he econ of lhum n heml neuons s neee. Theefoe he conol of heml neuons my lso pove novel pplcons n he geneon of um. Inee heml neuon ffuson s escbe by he ffuson equon..mhemclly howeve he ffuson equon wh cen mpng consn s nlogous o he wve equon wh cen fequency n heefoe sucues wh peoc moeos possess mpng consn egons n whch heml neuon ffuson cnno e plce le elecomgnec wves n phoonc bn gps.[ 7].In hs ppe we heoeclly emonse ffuson bn gps of heml neuon ffuson n heml neuon flu n wo-mensonl sucues wh peoc moeos compose of os wh sque lces. We o no conse heml neuon ffuson pepencul o wo-mensonl plnes. Moeos e ssume o be C n HO. ffuson bn gps sgnfcnly epen on he of os n he lce consns. Ths ppe s ve no 5 secons such h n secon I heoecl suggeson s gven n secon II we escbe he Foue nsfom of he ffuson coeffcen he bsopon coss-secon n he ffuson me especvely. In secon III by subsung hese Foue nsfoms no he neuon heml ffuson equon NTE wh some smplfcon we conve NTE o egenvlue poblem. In secon IV fom hs equon we eemne he egenvluesneuon mpng consns n egenfuncons neuon ffuson heml flu fo wo ffeen cses: cse moeos nse n ouse of he o e C n HO especvely cse moeos nse n ouse of he o e HO n C especvely. In fnl secon he obne esuls e gven.. Suggeson Theoy In fgue we show he schemc gm of wo mensonl sucues wh peoc moeos compose of os wh sque lces. []The egon embee by oe lnes nces he un cell. In fgue b we show he fs Blloun zone of sque lces wn by he she egon. As menone ele he fs Blloun zone s embee by he pepencul lnes whch ve equvlenly beween he ogn n he nees ecpocl pons o he ogn.the blc pons nce he nees ecpocl pons o he ogn. The oe lnes nce he pepencul lnes whch ve quvlenly beween he ogn n he nees

3 Clculon of heml neuon flu 9 ecpocl pons o he ogn n he Γ X n M pons e especvely. These pons nce hghly oonl symmec pons n he fs Blloun zone. Theefoe by he Bloch heoem wve vecos n gve he sme conon n we my nvesge only he fs Blloun zone n he wve veco spce. n Fgue. Schemc gm of wo-mensonl sucue wh peoc ffuson coeffcens. s he us of o s he lce consn of sque lces. b The fs Blloun zone of sque lces wn by he she egon. The blc pons nce he nees ecpocl pons o he ogn. The oe lnes nce he pepencul lnes whch ve equvlenly beween he ogn n he nees ecpocl pons o ogn n he Γ X n M pons e especvely. These pons nce symmec pons n he fs Bllon zone. Moeove ffuson bn sucues cn be obne by nvesgng wve vecos long he Γ X X M n M Γ segmens when sucues possess he C v symmey n he goup heoy. ffuson bn gps ppe wve vecos on oe lnes n fgue b. In he cse of unfom moeos ffuson bn gps o no ppe hese wve vecos. By openng of ffuson bn gps mpng consns ecese hese wve vecos whch cuses he ncese of elon me.e. he sblzon of he heml neuon flu. The econ of hs sble se nees cen eneges whch nces physcl menng of ffuson bn gps. Ths s sml o he cse of eleconc bn gps n sol ses [8-9].Any neuon souce cn be esgne o pouce lo of neuons. Howeve hgh neuon yel lone oes no epesen how useful hese neuons e. Flu s efne s he numbe of neuons cossng un e pe un me. I cn lso be

4 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn vewe n he followng wy: nv n s he neuon ensy v s he velocy of neuon. A neuon souce wh hgh yel mus lso hve hgh neuon ensy n oe o pove hgh neuon flu. When he neuon geneo s couple wh neuon geneo he volume of he souce nceses. As esul he neuon ensy nceses slowe hn he yel n he neuon flu wll no be mpove lnely wh he ue sysem mulplcon fco.[-] In oe o obn ffuson bn sucues we s wh he ffuson equon fo heml neuon fo wo-mensonl sucues { } s ν T Whee ν T b ν n e he ffuson coeffcen he bsopon coss- T secon he heml velocy n he ffuson me especvely n n especvely. We o no conse he heml neuon souce s e he heml neuon flu n he heml neuon souce s n nvesgng popees of wo-mensonl sucues wh peoc moeos. vng hus: equon by [ ] { } The ffuson coeffcen he ffuson me he bsopon coss-secon n e peoc wh espec o he lce veco genee by he pmve nslon n hey my be epne n Foue sees on he ecpocl veco ep ep b Whee n ep c n e he Foue coeffcens of especvely. In wo-mensonl peoc sucues wh sque lces he lce veco s: l l Whee l n l e ny wo neges n bsc vecos e 5

5 Clculon of heml neuon flu 9 b 5 s he lce consn of sque lces. On he ohe hn he ecpocl lce veco s: 6 hb hb Whee h n h e ny wo neges n bsc vecos of hs ecpocl lce e: b 7 b 7b Then he lce veco n ecpocl lce veco ssfy he followng elon: 8 nege Theefoe he ffuson coeffcen he ffuson me n he bsopon coss- s escbe by secon e nslonlly symmec wh espec o. ep λ 9 In vng equon 9 usng sepon of vbles meho on he equon.whee λ s mpng consn. Usng Bloch s heoem [8-] we my epn s ep{ } Whee s Foue coeffcen of nces he econ of neuon ffuson. Then elon: ep. n s he wve veco whch ssfes he followng By ffeenon elve o me fom he boh se of equon 9 we obn: λ λ e Subsung eq. no we fn: [. { } ] λ O [. ] λ Usng equons b n we obn;[]. e 5 [ ]. e 6

6 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn [ ] 7. e eplcng equons n -b no equon we obn: [ ] [ ]. ep [ ] [ ]. ep. [ ]. ep 8. e λ Now by mulplyng he boh se of bove elon on he e. fco n negon fom we wll hve: [ ] [ ]. [ ]. λ 9 Noe h n wng he bove equon we hve use he followng elon:[] { }. ep δ Whee s volume of un cell n δ s he Konee el funcon now usng he chnge of vble n he bove equon n we hve: [ ] λ [ ]. Also fo smplcy n hs equon we use he followng chnge of vbles: n heefoe he bove equon s convee o: K λ [ ]. K

7 Clculon of heml neuon flu 95 O λ K. K An: {. } λ In he fnl fom bove elon cn be wen n he followng m egenvlue poblem: λ Whee Φ 5 { } 6 Fom hs elon we see h fo fe wve veco of we wll hve one goup of soluons n fs Blloun zone hus by chngng wve veco of we hve nohe goup of soluons h e gven by ne n [9] whee hs ne epesene bn sucue.the eque conon fo hvng gp beween bns λ s [9]:.We cn nvesge hs conon n he followng fom: λ Fom equon 5 we hve: o hus by he mnus sgn n hs epesson some smplfcon we fn epesene h econ neuon wve veco s oppose he econ of ecpocl lce veco.e by ncesng he vlue of lce veco neuon wve veco s ecese.theefoe hs conon s ssfe n concluson ceon of he bn gp sucue s epece. In epesson 6 he m fom of cn be evlue n he followng meho: Clculon of Foue coeffcen of We now h: ep ou ou n n ou ou ep ep ep n n ep 7 ou ou

8 96 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn nces egon nse o. A The fome negl n equon 7 ep δ. 8 Whee δ s he Konece el. B The le negl n equon 7 ep ep 9 θ J l ep lθ l θ ep snθ J Whee J l s he l h-oe Bessel funcon. We use he followng elon[-]: ep { snθ } J ep{ lθ} l By usng he elon: { zj z } zj z z We cn obn: ep l J coeffcen of s gven by: ou ou n n Theefoe he Foue ou ou f J ou ou n n l f whee f.in he sml wy n e gven by : ou n ou { } f J ou n 5 f

9 Clculon of heml neuon flu 97 n { } { } 6 n ou n ou ou f J f The m fom of n e gven n he followng fom especvely: 7 Whee { } ou n ou 7 { } b J ou n 7 { } c J ou n 7 An: 8 Whee: { } ou n ou 8 { } b J ou n 8 { } c J ou n 8 Also;

10 98 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn 9 Whee ou ou n n ou ou 9 J n n ou ou 9 b { } J 9 n n ou ou { c. Numecl compuons: Ths secon s ve o wo mn ps: - eemnon of heml neuon flu wh conseng he moeos nse n ouse of he o s C n HO especvely. By nvesng hese mces we wll eemne he m fom of : Fo emple he fs elemen of m by he followng meho s eemne: '' We ssume h pons e he nees ecpocl pons o he ogn such h he componens e gven by :.Theefoe n n. n po po K K po The eque numecl vlues fo ffeen moeos C n H o n ou { } c cm C c.. compuons e gven by []: 8 cm. 7s n H O H o. 6cm. 97. s especvely. Une H o

11 Clculon of heml neuon flu 99 hese conons numecl vlue of m fom of n he econ of ΓX s gven by: 6.76e -.9e e - 6.9e -.9e - 6.7e -.9e e e - 6.9e - 6.7e -.9e -.9e e - 6.9e - 6.7e - Also he egenvecos of m e gven n he followng: The gonl fom of m s gven by: 9.67e - 7.e - 8.6e - 7.e - Noe h he gonl elemens of hs m e he egenvlue of m.we conclue h he neuon mpng consns h e ele o bn gp sucue e gven by: λ.67 λ 7. λ 8.6 n λ 7.. Now f we nse he egenfuncons of heml neuon flu no he Foue v nsfoms elon: j ep j. he pons: j.we fn:... e e e. e.... e e e e.... e e e e.... e e e e 5 Combnng eq. n 5 hus fnlly he obne esuls fo fou funcons s funcon of spce e gven n he below especvely: y e.5e.5.5e 5 y

12 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn y e.e.77.e 5 b y y y e.5e.99.5e 5 c y e.77e.77e 5 Fgues - o -show h he vons of y n s funcon of n y.fom hese fgues we see h heml neuon flu n hve ffeen pe pons lso n ffeen pons e negve n hee s no ccepble snce hs egon s nown s bn gp. Noe h fom Fg-we fn h some pons wh coones y he neuon heml flu s posve n ccepble n he ohe pons he numecl vlues of e negve h s nown s bn gp egon.[-5] Thus n ll pons of y e ccepble. Fg.-: The vons of cm s funcon of n y cm 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely. s Fg. -b: The vons of cm s funcon of n y 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely. s cm

13 Clculon of heml neuon flu 9 Fg.-c: The vons of cm s funcon of n 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely. s y cm Fg.-: The vons of cm s funcon of n y 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely. s cm Now by usng he elon ep λ we cn eemne he me epenence of n he obne esuls e gven n he fgues - o -. Noe h n ou compuons we e one of he pe pons on fgues - o - fo emple 5 n 5 especvely.fom hese fgues we see h by ncesng me he heml neuon flu s ecese n he numecl vlues of hese funcons epen on he pe pons songly. Fg-: The vons of me epenence of pe pon n 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely.

14 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn Fg-b: The vons of me epenence of 5cm /. 5 n when he moeos nse n ouse of he o e C n HO especvely. Fg-c: The vons of me epenence of 5cm /. 5 n 5 when he moeos nse n ouse of he o e C n HO especvely. Fg-: The vons of me epenence of 5cm /. 5 n 5 when he moeos nse n ouse of he o e C n HO especvely. Also he numecl vlues of vesus me e gven n he Tbles. Tble : numecl vlues of n vesus me efne pons 5 n 5 especvely 5cm /. 5 when he moeos nse n ouse of he o e C n HO especvely

15 Clculon of heml neuon flu 9 Fom hs ble we conclue h e no ccepble vlue becuse he pe pon 5 e plce n bn gp egon. -b eemnon of heml neuon flu wh conseng he moeos nse n ouse of he o s HO n C especvely. In hs p n sml wy he ol compuons of p e cheve ecep h we echnge he moeo nse of he o wh HO n ouse wh C. Theefoe he obne esuls e gven n he below.in hs cse we fn An s egenvecos e gven by The gonl fom of s gven by Such h. e. e. e e..... e e e e.... e e e e e e e e 9 Also pons.77.e.77 5 we fn:

16 9 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn y y.5e.5e.99.5e 5b y.5e.5e.5.5e 5c y e.77e.77e 5 Fgues - o -show h he vons of n s funcon of & y.fom hese fgues we see h heml neuon flu n hve ffeen pe pons only n ll ffeen pons e posve n ccepble bu n n ll pons e negve n e no ccepble snce hese egons conn bn gp sucue. AlsoFg.- shows h n some pons e negve n ohe pons e posve n ccepble. y y Fg.-: The vons of cm /. 5 especvely. s cm s funcon of n y cm when he moeos nse n ouse of he o e HO n C Fg. -b: The vons of cm s s funcon of n y cm cm /. 5 when he moeos nse n ouse of he o e HO n C especvely.

17 Clculon of heml neuon flu 95 Fg.-c: The vons of cm /. 5 especvely. s cm s funcon of n y cm when he moeos nse n ouse of he o e HO n C Fg.-: The vons of cm /. 5 especvely. s cm s funcon of n y cm when he moeos nse n ouse of he o e HO n C Now by usng he elon ep λ we cn eemne he me epenence of n he obne esuls e gven n he fgues 5- o 5-. Noe h n ou compuons we e one of he pe pons on fgues 5- o 5- fo emple 5 n 5 especvely.fom hese fgues we see h s no ccepble pon n by ncesng me e ecese pon 5 n 5. Fg5-: he vons of me epenence of cm /. 5 n when he moeos nse n ouse of he o e HO n C especvely.

18 96 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn Fg5-b: he vons of me epenence of cm /. 5 n when he moeos nse n ouse of he o e HO n C especvely Fg5-c: The vons of me epenence of cm /. 5 n 5 when he moeos nse n ouse of he o e HO n C especvely. Fg5-: The vons of me epenence of cm /. 5 n 5 when he moeos nse n ouse of he o e HO n C especvely. Also he numecl vlues of vesus me e gven n he Tbles. Tble:Numecl vlues of n vesus me efne pons 5 n 5 especvely cm /. 5 when he moeos nse n ouse of he o e HO n C especvely s Conclusons In mels connng oms of low omc mss neuons of ll eneges cn lose sgnfcn fcon of he enegy n sngle elsc collson n such

19 Clculon of heml neuon flu 97 mels e efee o s moeos. In hevy nucle ppecble enegy loss n collson s only possble hgh eneges whee nelsc sceng cn occu. We obn fom ou clculons hee mjo esuls such s :Fom ou gven suggeson heoy we cn conve he neuon heml ffuson equon o solvble egnvlue poblem by usng Foue nsfom echnque. We cn ble o clcule he heml neuon flu n neuon mpng consns n fs Blloun zone by usng he Mhemc Pogm n we fn h he heml neuon flu on hve connues sbuons n un cell..by nlyzng he suggeson heoy n scusson on he obne esuls we cn fn he physcl chcescs of bn gp sucues n wo followng seps: Sep one: when he moeos nse n ouse of he o e C n HO especvely. Sep wo: when he moeos nse n ouse of he o e HO n C especvely. In such sucues ffuson bn gps show h heml neuon ffuson cn no e plce ppe n mpng consns. ffuson bn gps ppe when C n HO e nse n ouse he os n vce ves. By compng he obne esuls fom sep one n wo we fn h he neuon mpng consns n heml neuon flu e no he sme becuse hese pmees e epen on he lce consn us of he o n choce of he suble moeos. Acnowlegmen Thns e ue o esech Councl of In Unvesy of Scence & Technology fo fnncl suppo of hs esech. efeences [] J.. Lmsh Inoucon o Nucle eco Theoy eng MA: Ason-Wesley 966. [] J.. Lmsh n A. B Inoucon o Nucle Engneeng Eon. []. ozon Inoucon o eco Knecs Polyechnque Inenonl Pess Monel 998. [] T. Hoyu n Y. Ksum J. Phys. : Appl. Phys. 6. [5] S. John Phys. ev. Le [6] E.Yblonovch Phys. ev. Le [7] H. Hym T. Hmno n Y. Aoyg Appl. Phys. Le

20 98 S. N. Hossenmolgh S. A. Agh L. Monzen S. Bsn [8] C. Kel Inoucon o Sol Se Physcs 6h en New Yo: Wley 986. [9] N.W. Ashcf n N.. Memn Sol Se Physcs. Hol neh n Wnson New Yo 976. [] E. Ks Aomc n Eleconc Sucue of Sols Cmbge Unvesy Pess. []. useppe n P.P. useppe Sol Se Physcs. Acemc Pess Sn ego Clf.. []. Afen n H. Webe Mhemcl Mehos fo Physcss 5h eon Acemc Pess Sn ego. [] C. Hpe Anlyc Mehos n Physcs. Wley-VCH Beln 999. []. Hempelmnn Quselsc Neuon Sceng n Sol Se ffuson Ofo Unv. Pess. [5]. L. Sques Inoucon o he Theoy of Theml Neuon Sceng ove Pubns 997. eceve: ecembe 8 7

Rotations.

Rotations. oons j.lbb@phscs.o.c.uk To s summ Fmes of efeence Invnce une nsfomons oon of wve funcon: -funcons Eule s ngles Emple: e e - - Angul momenum s oon geneo Genec nslons n Noehe s heoem Fmes of efeence Conse

More information

HERMITE SERIES SOLUTIONS OF LINEAR FREDHOLM INTEGRAL EQUATIONS

HERMITE SERIES SOLUTIONS OF LINEAR FREDHOLM INTEGRAL EQUATIONS Mhemcl nd Compuonl Applcons, Vol 6, o, pp 97-56, Assocon fo Scenfc Resech ERMITE SERIES SOLUTIOS OF LIEAR FREDOLM ITEGRAL EQUATIOS Slh Ylçınbş nd Müge Angül Depmen of Mhemcs, Fcul of Scence nd As, Cell

More information

5-1. 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 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 information

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )

Calculus 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 information

Chapter 6 Plane Motion of Rigid Bodies

Chapter 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 information

Go over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration

Go over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration Mh Csquee Go oe eco nd eco lgeb Dsplcemen nd poson n -D Aege nd nsnneous eloc n -D Aege nd nsnneous cceleon n -D Poecle moon Unfom ccle moon Rele eloc* The componens e he legs of he gh ngle whose hpoenuse

More information

Parameter Estimation and Hypothesis Testing of Two Negative Binomial Distribution Population with Missing Data

Parameter Estimation and Hypothesis Testing of Two Negative Binomial Distribution Population with Missing Data Avlble ole wwwsceceeccom Physcs Poce 0 475 480 0 Ieol Cofeece o Mecl Physcs Bomecl ee Pmee smo Hyohess es of wo Neve Boml Dsbuo Poulo wh Mss D Zhwe Zho Collee of MhemcsJl Noml UvesyS Ch zhozhwe@6com Absc

More information

Available online Journal of Scientific and Engineering Research, 2017, 4(2): Research Article

Available online   Journal of Scientific and Engineering Research, 2017, 4(2): Research Article Avlble onlne www.jse.com Jonl of Scenfc nd Engneeng Resech, 7, 4():5- Resech Acle SSN: 394-63 CODEN(USA): JSERBR Exc Solons of Qselsc Poblems of Lne Theoy of Vscoelscy nd Nonlne Theoy Vscoelscy fo echnclly

More information

Empirical equations for electrical parameters of asymmetrical coupled microstrip lines

Empirical equations for electrical parameters of asymmetrical coupled microstrip lines Epl equons fo elel petes of syel ouple osp lnes I.M. Bsee Eletons eseh Instute El-h steet, Dokk, o, Egypt Abstt: Epl equons e eve fo the self n utul nutne n ptne fo two syel ouple osp lnes. he obne ptne

More information

D zone schemes

D zone schemes Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic

More information

Modern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.

Modern 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 information

ME 141. Engineering Mechanics

ME 141. Engineering Mechanics ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics

More information

2 shear strain / L for small angle

2 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 information

Nanoparticles. Educts. Nucleus formation. Nucleus. Growth. Primary particle. Agglomeration Deagglomeration. Agglomerate

Nanoparticles. Educts. Nucleus formation. Nucleus. Growth. Primary particle. Agglomeration Deagglomeration. Agglomerate ucs Nucleus Nucleus omaon cal supesauaon Mng o eucs, empeaue, ec. Pmay pacle Gowh Inegaon o uson-lme pacle gowh Nanopacles Agglomeaon eagglomeaon Agglomeae Sablsaon o he nanopacles agans agglomeaon! anspo

More information

On Fractional Operational Calculus pertaining to the product of H- functions

On Fractional Operational Calculus pertaining to the product of H- functions nenonl eh ounl of Enneen n ehnolo RE e-ssn: 2395-56 Volume: 2 ue: 3 une-25 wwwene -SSN: 2395-72 On Fonl Oeonl Clulu enn o he ou of - funon D VBL Chu, C A 2 Demen of hem, Unve of Rhn, u-3255, n E-ml : vl@hooom

More information

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration Secion 1.4 Moion in Spce: Velociy nd Acceleion We e going o dive lile deepe ino somehing we ve ledy inoduced, nmely () nd (). Discuss wih you neighbo he elionships beween posiion, velociy nd cceleion you

More information

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt. 4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss

More information

PHY2053 Summer C 2013 Exam 1 Solutions

PHY2053 Summer C 2013 Exam 1 Solutions PHY053 Sue C 03 E Soluon. The foce G on o G G The onl cobnon h e '/ = doubln.. The peed of lh le 8fulon c 86,8 le 60 n 60n h 4h d 4d fonh.80 fulon/ fonh 3. The dnce eled fo he ene p,, 36 (75n h 45 The

More information

Chapter 4: Motion in Two Dimensions Part-1

Chapter 4: Motion in Two Dimensions Part-1 Lecue 4: Moon n Two Dmensons Chpe 4: Moon n Two Dmensons P- In hs lesson we wll dscuss moon n wo dmensons. In wo dmensons, s necess o use eco noon o descbe phscl qunes wh boh mnude nd decon. In hs chpe,

More information

Reinforcement learning

Reinforcement learning CS 75 Mchine Lening Lecue b einfocemen lening Milos Huskech milos@cs.pi.edu 539 Senno Sque einfocemen lening We wn o len conol policy: : X A We see emples of bu oupus e no given Insed of we ge feedbck

More information

SIMPLIFIED ROTATING TIRE MODELS BASED ON CYLINDRICAL SHELLS WITH FREE BOUNDARY CONDITIONS

SIMPLIFIED ROTATING TIRE MODELS BASED ON CYLINDRICAL SHELLS WITH FREE BOUNDARY CONDITIONS F1-NVH-8 SIMPLIFIED ROTATING TIRE MODELS BASED ON CYLINDRICAL SHELLS WITH FREE BOUNDARY CONDITIONS 1 Alujevc Neven * ; Cmpllo-Dvo Nu; 3 Knd Pee; 1 Pluymes Be; 1 Ss Pul; 1 Desme Wm; 1 KU Leuven PMA Dvson

More information

Technical Appendix for Inventory Management for an Assembly System with Product or Component Returns, DeCroix and Zipkin, Management Science 2005.

Technical Appendix for Inventory Management for an Assembly System with Product or Component Returns, DeCroix and Zipkin, Management Science 2005. Techc Appedx fo Iveoy geme fo Assemy Sysem wh Poduc o Compoe eus ecox d Zp geme Scece 2005 Lemm µ µ s c Poof If J d µ > µ he ˆ 0 µ µ µ µ µ µ µ µ Sm gumes essh he esu f µ ˆ > µ > µ > µ o K ˆ If J he so

More information

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis.

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis. Insucos: Fel/ce PYSICS DEPATET PY 48 Em Ocoe 3, 4 me pn, ls fs: Sgnue: On m ono, I e nee gen no ecee unuoe on s emnon. YOU TEST UBE IS TE 5-DIGIT UBE AT TE TOP OF EAC PAGE. Coe ou es nume on ou nswe see

More information

Introduction. Voice Coil Motors. Introduction - Voice Coil Velocimeter Electromechanical Systems. F = Bli

Introduction. Voice Coil Motors. Introduction - Voice Coil Velocimeter Electromechanical Systems. F = Bli UNIVERSITY O TECHNOLOGY, SYDNEY ACULTY O ENGINEERING 4853 Elecroechncl Syses Voce Col Moors Topcs o cover:.. Mnec Crcus 3. EM n Voce Col 4. orce n Torque 5. Mhecl Moel 6. Perornce Voce cols re wely use

More information

Supporting information How to concatenate the local attractors of subnetworks in the HPFP

Supporting information How to concatenate the local attractors of subnetworks in the HPFP n Effcen lgorh for Idenfyng Prry Phenoype rcors of Lrge-Scle Boolen Newor Sng-Mo Choo nd Kwng-Hyun Cho Depren of Mhecs Unversy of Ulsn Ulsn 446 Republc of Kore Depren of Bo nd Brn Engneerng Kore dvnced

More information

Lecture 5 Single factor design and analysis

Lecture 5 Single factor design and analysis Lectue 5 Sngle fcto desgn nd nlss Completel ndomzed desgn (CRD Completel ndomzed desgn In the desgn of expements, completel ndomzed desgns e fo studng the effects of one pm fcto wthout the need to tke

More information

EE 410/510: Electromechanical Systems Chapter 3

EE 410/510: Electromechanical Systems Chapter 3 EE 4/5: Eleomehnl Syem hpe 3 hpe 3. Inoon o Powe Eleon Moelng n Applon of Op. Amp. Powe Amplfe Powe onvee Powe Amp n Anlog onolle Swhng onvee Boo onvee onvee Flyb n Fow onvee eonn n Swhng onvee 5// All

More information

Name of the Student:

Name 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 information

MODEL SOLUTIONS TO IIT JEE ADVANCED 2014

MODEL SOLUTIONS TO IIT JEE ADVANCED 2014 MODEL SOLUTIONS TO IIT JEE ADVANCED Pper II Code PART I 6 7 8 9 B A A C D B D C C B 6 C B D D C A 7 8 9 C A B D. Rhc(Z ). Cu M. ZM Secon I K Z 8 Cu hc W mu hc 8 W + KE hc W + KE W + KE W + KE W + KE (KE

More information

Physics 120 Spring 2007 Exam #1 April 20, Name

Physics 120 Spring 2007 Exam #1 April 20, Name Phc 0 Spng 007 E # pl 0, 007 Ne P Mulple Choce / 0 Poble # / 0 Poble # / 0 Poble # / 0 ol / 00 In eepng wh he Unon College polc on cdec hone, ued h ou wll nehe ccep no pode unuhozed nce n he copleon o

More information

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:

Homework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is: . Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo

More information

Caputo Equations in the frame of fractional operators with Mittag-Leffler kernels

Caputo Equations in the frame of fractional operators with Mittag-Leffler kernels nvenon Jounl o Reseh Tehnoloy n nneen & Mnemen JRTM SSN: 455-689 wwwjemom Volume ssue 0 ǁ Ooe 08 ǁ PP 9-45 Cuo uons n he me o onl oeos wh M-ele enels on Qn Chenmn Hou* Ynn Unvesy Jln Ynj 00 ASTRACT: n

More information

Lecture 3 summary. C4 Lecture 3 - Jim Libby 1

Lecture 3 summary. C4 Lecture 3 - Jim Libby 1 Lecue su Fes of efeece Ivce ude sfoos oo of H wve fuco: d-fucos Eple: e e - µ µ - Agul oeu s oo geeo Eule gles Geec slos cosevo lws d Noehe s heoe C4 Lecue - Lbb Fes of efeece Cosde fe of efeece O whch

More information

_ J.. C C A 551NED. - n R ' ' t i :. t ; . b c c : : I I .., I AS IEC. r '2 5? 9

_ 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 information

Physics 201, Lecture 5

Physics 201, Lecture 5 Phsics 1 Lecue 5 Tod s Topics n Moion in D (Chp 4.1-4.3): n D Kinemicl Quniies (sec. 4.1) n D Kinemics wih Consn Acceleion (sec. 4.) n D Pojecile (Sec 4.3) n Epeced fom Peiew: n Displcemen eloci cceleion

More information

Chapter I Vector Analysis

Chapter I Vector Analysis . Chpte I Vecto nlss . Vecto lgeb j It s well-nown tht n vecto cn be wtten s Vectos obe the followng lgebc ules: scl s ) ( j v v cos ) ( e Commuttv ) ( ssoctve C C ) ( ) ( v j ) ( ) ( ) ( ) ( (v) he lw

More information

A Design Configuration and Optimization for a Multi Rotor UAV

A Design Configuration and Optimization for a Multi Rotor UAV UNCLSSIFIED/UNLIITED Desgn Confguon n Opmzon fo ul oo UV Els Cpello, Gogo Gugle, Fulv Quglo olecnco Tono DIS Coso Duc egl buzz 4 9 Tono (Ily) els.cpello@polo. -fulv.quglo@polo. - gogo.gugle@polo. STCT

More information

Chapter Linear Regression

Chapter Linear Regression Chpte 6.3 Le Regesso Afte edg ths chpte, ou should be ble to. defe egesso,. use sevel mmzg of esdul cte to choose the ght cteo, 3. deve the costts of le egesso model bsed o lest sques method cteo,. use

More information

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2 Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe

More information

Generalisation on the Zeros of a Family of Complex Polynomials

Generalisation on the Zeros of a Family of Complex Polynomials Ieol Joul of hemcs esech. ISSN 976-584 Volume 6 Numbe 4. 93-97 Ieol esech Publco House h://www.house.com Geelso o he Zeos of Fmly of Comlex Polyomls Aee sgh Neh d S.K.Shu Deme of hemcs Lgys Uvesy Fdbd-

More information

Physics 15 Second Hour Exam

Physics 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 information

Fast Algorithm for Walsh Hadamard Transform on Sliding Windows

Fast Algorithm for Walsh Hadamard Transform on Sliding Windows Fs Algohm fo Wlsh Hdmd Tnsfom on Sldng Wndows Wnl Oung W.K. Chm Asc Ths ppe poposes fs lgohm fo Wlsh Hdmd Tnsfom on sldng wndows whch cn e used o mplemen pen mchng mos effcenl. The compuonl equemen of

More information

THE EXISTENCE OF SOLUTIONS FOR A CLASS OF IMPULSIVE FRACTIONAL Q-DIFFERENCE EQUATIONS

THE EXISTENCE OF SOLUTIONS FOR A CLASS OF IMPULSIVE FRACTIONAL Q-DIFFERENCE EQUATIONS Europen Journl of Mhemcs nd Compuer Scence Vol 4 No, 7 SSN 59-995 THE EXSTENCE OF SOLUTONS FOR A CLASS OF MPULSVE FRACTONAL Q-DFFERENCE EQUATONS Shuyun Wn, Yu Tng, Q GE Deprmen of Mhemcs, Ynbn Unversy,

More information

Chebyshev Polynomial Solution of Nonlinear Fredholm-Volterra Integro- Differential Equations

Chebyshev Polynomial Solution of Nonlinear Fredholm-Volterra Integro- Differential Equations Çny Ünvee Fen-Edeby Füle Jounl of A nd Scence Sy : 5 y 6 Chebyhev Polynol Soluon of onlne Fedhol-Vole Inego- Dffeenl Equon Hndn ÇERDİK-YASA nd Ayşegül AKYÜZ-DAŞCIOĞU Abc In h ppe Chebyhev collocon ehod

More information

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf Objecie F s w Tnsfome Moionl To be ble o fin nsfome. moionl nsfome n moionl. 331 1 331 Mwell s quion: ic Fiel D: Guss lw :KV : Guss lw H: Ampee s w Poin Fom Inegl Fom D D Q sufce loop H sufce H I enclose

More information

EXACT SOLUTIONS FOR NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS BY USING THE EXTENDED MULTIPLE RICCATI EQUATIONS EXPANSION METHOD

EXACT SOLUTIONS FOR NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS BY USING THE EXTENDED MULTIPLE RICCATI EQUATIONS EXPANSION METHOD IJRRAS 9 () Deceme www.ess.com/volmes/vol9isse/ijrras_9.f EXACT SOUTIONS FOR NONINEAR PARTIA DIFFERENTIA EQUATIONS BY USING THE EXTENDED MUTIPE RICCATI EQUATIONS EXPANSION METHOD Mmo M. El-Bo Aff A. Zgo

More information

Uniform Circular Motion

Uniform Circular Motion Unfom Ccul Moton Unfom ccul Moton An object mong t constnt sped n ccle The ntude of the eloct emns constnt The decton of the eloct chnges contnuousl!!!! Snce cceleton s te of chnge of eloct:!! Δ Δt The

More information

Maximum likelihood estimate of phylogeny. BIOL 495S/ CS 490B/ MATH 490B/ STAT 490B Introduction to Bioinformatics April 24, 2002

Maximum likelihood estimate of phylogeny. BIOL 495S/ CS 490B/ MATH 490B/ STAT 490B Introduction to Bioinformatics April 24, 2002 Mmm lkelhood eme of phylogey BIO 9S/ S 90B/ MH 90B/ S 90B Iodco o Bofomc pl 00 Ovevew of he pobblc ppoch o phylogey o k ee ccodg o he lkelhood d ee whee d e e of eqece d ee by ee wh leve fo he eqece. he

More information

New Stability Condition of T-S Fuzzy Systems and Design of Robust Flight Control Principle

New Stability Condition of T-S Fuzzy Systems and Design of Robust Flight Control Principle 96 JOURNAL O ELECRONIC SCIENCE AND ECHNOLOGY, VOL., NO., MARCH 3 New Sably Conon of -S uzzy Sysems an Desgn of Robus lgh Conol Pncple Chun-Nng Yang, Ya-Zhou Yue, an Hu L Absac Unlke he pevous eseach woks

More information

( ) ( ) ( ) ( ) ( ) ( ) j ( ) A. b) Theorem

( ) ( ) ( ) ( ) ( ) ( ) j ( ) A. b) Theorem b) Theoe The u of he eco pojecon of eco n ll uull pependcul (n he ene of he cl poduc) decon equl o he eco. ( ) n e e o The pojecon conue he eco coponen of he eco. poof. n e ( ) ( ) ( ) e e e e e e e e

More information

Chapter 3: Vectors and Two-Dimensional Motion

Chapter 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

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes omewok # P7-3 ecngul loop of widh w nd heigh h is siued ne ve long wie cing cuen i s in Fig 7- ssume i o e ecngul pulse s shown in Fig 7- Find he induced cuen i in he ecngul loop whose self-inducnce is

More information

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006 Homewok 5 fo BST 63: Sisicl Theoy I Soluions, 9//6 Due Time: 5:PM Thusy, on 9/8/6. Polem ( oins). Book olem.8. Soluion: E = x f ( x) = ( x) f ( x) + ( x ) f ( x) = xf ( x) + xf ( x) + f ( x) f ( x) Accoing

More information

Solution in semi infinite diffusion couples (error function analysis)

Solution in semi infinite diffusion couples (error function analysis) Soluon n sem nfne dffuson couples (error funcon analyss) Le us consder now he sem nfne dffuson couple of wo blocks wh concenraon of and I means ha, n a A- bnary sysem, s bondng beween wo blocks made of

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

Numerical Analysis of Freeway Traffic Flow Dynamics under Multiclass Drivers

Numerical Analysis of Freeway Traffic Flow Dynamics under Multiclass Drivers Zuojn Zhu, Gng-len Chng nd Tongqng Wu Numecl Anlyss of Feewy Tffc Flow Dynmcs unde Mulclss Dves Zuojn Zhu, Gng-len Chng nd Tongqng Wu Depmen of Theml Scence nd Enegy Engneeng, Unvesy of Scence nd Technology

More information

Physics 201 Lecture 15

Physics 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 information

L4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3

L4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3 elave moon L4:1 To appl Newon's laws we need measuemens made fom a 'fed,' neal efeence fame (unacceleaed, non-oang) n man applcaons, measuemens ae made moe smpl fom movng efeence fames We hen need a wa

More information

The Shape of the Pair Distribution Function.

The Shape of the Pair Distribution Function. The Shpe of the P Dstbuton Functon. Vlentn Levshov nd.f. Thope Deptment of Phscs & stonom nd Cente fo Fundmentl tels Resech chgn Stte Unvest Sgnfcnt pogess n hgh-esoluton dffcton epements on powde smples

More information

Lecture 5. Plane Wave Reflection and Transmission

Lecture 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 information

September 20 Homework Solutions

September 20 Homework Solutions College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum

More information

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.

THIS 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 information

THIS PAGE DECLASSIFIED IAW EO 12958

THIS PAGE DECLASSIFIED IAW EO 12958 THIS PAGE DECLASSIFIED IAW EO 2958 THIS PAGE DECLASSIFIED IAW EO 2958 THIS PAGE DECLASSIFIED IAW E0 2958 S T T T I R F R S T Exhb e 3 9 ( 66 h Bm dn ) c f o 6 8 b o d o L) B C = 6 h oup C L) TO d 8 f f

More information

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions II The Z Trnsfor Tocs o e covered. Inroducon. The Z rnsfor 3. Z rnsfors of eleenry funcons 4. Proeres nd Theory of rnsfor 5. The nverse rnsfor 6. Z rnsfor for solvng dfference equons II. Inroducon The

More information

Answers to test yourself questions

Answers to test yourself questions Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E

More information

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3 DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl

More information

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis   2/3/2007 Physics 253 Science Adeisemen Inegoenmenl Pnel on Clime Chnge: The Phsicl Science Bsis hp://www.ipcc.ch/spmfeb7.pdf /3/7 Phsics 53 hp://www.fonews.com/pojecs/pdf/spmfeb7.pdf /3/7 Phsics 53 3 Sus: Uni, Chpe 3 Vecos

More information

6.6 The Marquardt Algorithm

6.6 The Marquardt Algorithm 6.6 The Mqudt Algothm lmttons of the gdent nd Tylo expnson methods ecstng the Tylo expnson n tems of ch-sque devtves ecstng the gdent sech nto n tetve mtx fomlsm Mqudt's lgothm utomtclly combnes the gdent

More information

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1. LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle

More information

e t dt e t dt = lim e t dt T (1 e T ) = 1

e t dt e t dt = lim e t dt T (1 e T ) = 1 Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie

More information

s = rθ Chapter 10: Rotation 10.1: What is physics?

s = 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 information

Field due to a collection of N discrete point charges: r is in the direction from

Field 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 information

2 dependence in the electrostatic force means that it is also

2 dependence in the electrostatic force means that it is also lectc Potental negy an lectc Potental A scala el, nvolvng magntues only, s oten ease to wo wth when compae to a vecto el. Fo electc els not havng to begn wth vecto ssues woul be nce. To aange ths a scala

More information

Physics 201 Lecture 2

Physics 201 Lecture 2 Physcs 1 Lecure Lecure Chper.1-. Dene Poson, Dsplcemen & Dsnce Dsngush Tme nd Tme Inerl Dene Velocy (Aerge nd Insnneous), Speed Dene Acceleron Undersnd lgebrclly, hrough ecors, nd grphclly he relonshps

More information

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM

PHYSICS 102. Intro PHYSICS-ELECTROMAGNETISM PHYS 0 Suen Nme: Suen Numbe: FAUTY OF SIENE Viul Miem EXAMINATION PHYSIS 0 Ino PHYSIS-EETROMAGNETISM Emines: D. Yoichi Miyh INSTRUTIONS: Aemp ll 4 quesions. All quesions hve equl weighs 0 poins ech. Answes

More information

ANSWERS TO ODD NUMBERED EXERCISES IN CHAPTER 2

ANSWERS TO ODD NUMBERED EXERCISES IN CHAPTER 2 Joh Rley Novembe ANSWERS O ODD NUMBERED EXERCISES IN CHAPER Seo Eese -: asvy (a) Se y ad y z follows fom asvy ha z Ehe z o z We suppose he lae ad seek a oado he z Se y follows by asvy ha z y Bu hs oads

More information

EEM 486: Computer Architecture

EEM 486: Computer Architecture EEM 486: Compuer Archecure Lecure 4 ALU EEM 486 MIPS Arhmec Insrucons R-ype I-ype Insrucon Exmpe Menng Commen dd dd $,$2,$3 $ = $2 + $3 sub sub $,$2,$3 $ = $2 - $3 3 opernds; overfow deeced 3 opernds;

More information

Chapter 2 Linear Mo on

Chapter 2 Linear Mo on Chper Lner M n .1 Aerge Velcy The erge elcy prcle s dened s The erge elcy depends nly n he nl nd he nl psns he prcle. Ths mens h prcle srs rm pn nd reurn bck he sme pn, s dsplcemen, nd s s erge elcy s

More information

The Characterization of Jones Polynomial. for Some Knots

The Characterization of Jones Polynomial. for Some Knots Inernon Mhemc Forum,, 8, no, 9 - The Chrceron of Jones Poynom for Some Knos Mur Cncn Yuuncu Y Ünversy, Fcuy of rs nd Scences Mhemcs Deprmen, 8, n, Turkey m_cencen@yhoocom İsm Yr Non Educon Mnsry, 8, n,

More information

Electrostatic/magnetostatic forces

Electrostatic/magnetostatic forces Eecsc/gnesc ces spes ppc: eneg e ec eneg ce (vec) ve (vec) en ( eneg ) ( snce) ne s cn gve e O ce (n pessue) u cn en snge sp cne s pe e ce spe epe: pe pes eecsc: ppe vge gnesc: cuen I Den. Nekk 00, s upe

More information

1 Constant Real Rate C 1

1 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 information

Addition & Subtraction of Polynomials

Addition & Subtraction of Polynomials Addiion & Sucion of Polynomil Addiion of Polynomil: Adding wo o moe olynomil i imly me of dding like em. The following ocedue hould e ued o dd olynomil 1. Remove enhee if hee e enhee. Add imil em. Wie

More information

Principle Component Analysis

Principle Component Analysis Prncple Component Anlyss Jng Go SUNY Bufflo Why Dmensonlty Reducton? We hve too mny dmensons o reson bout or obtn nsghts from o vsulze oo much nose n the dt Need to reduce them to smller set of fctors

More information

A Study on Root Properties of Super Hyperbolic GKM algebra

A Study on Root Properties of Super Hyperbolic GKM algebra Stuy on Root Popetes o Supe Hypebol GKM lgeb G.Uth n M.Pyn Deptment o Mthemts Phypp s College Chenn Tmlnu In. bstt: In ths ppe the Supe hypebol genelze K-Mooy lgebs o nente type s ene n the mly s lso elte.

More information

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes] ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,

More information

CHAPTER 10: LINEAR DISCRIMINATION

CHAPTER 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 information

X-Ray Notes, Part III

X-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 information

-HYBRID LAPLACE TRANSFORM AND APPLICATIONS TO MULTIDIMENSIONAL HYBRID SYSTEMS. PART II: DETERMINING THE ORIGINAL

-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 information

EVALUATION OF TEMPERATURE DISTRIBUTION AND FLUID FLOW IN FUSION WELDING PROCESSES

EVALUATION OF TEMPERATURE DISTRIBUTION AND FLUID FLOW IN FUSION WELDING PROCESSES Nume olume mch Jounl o Engneeng EALAION OF EMPERARE DISRIBION AND FLID FLOW IN FSION WELDING PROCESSES Ass. Po. D. Ihsn Y. Hussn Mech. Eng. Dep. College o Eng. nvesy o Bghdd Bghdd Iq Slh Seeh Aed - AlKeem

More information

The Feigel Process. The Momentum of Quantum Vacuum. Geert Rikken Vojislav Krstic. CNRS-France. Ariadne call A0/1-4532/03/NL/MV 04/1201

The Feigel Process. The Momentum of Quantum Vacuum. Geert Rikken Vojislav Krstic. CNRS-France. Ariadne call A0/1-4532/03/NL/MV 04/1201 The Fegel Pocess The Momenum of Quanum Vacuum a an Tggelen CNRS -Fance Laboaoe e Physque e Moélsaon es Mleux Complexes Unesé Joseph Foue/CNRS, Genoble, Fance Gee Ren Vosla Ksc CNRS Fance CNRS-Fance Laboaoe

More information

Electric Potential. and Equipotentials

Electric Potential. and Equipotentials Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil

More information

Physics 207, Lecture 3

Physics 207, Lecture 3 Physcs 7 Lecue 3 Physcs 7, Lecue 3 l Tody (Fnsh Ch. & s Ch. 3) Emne sysems wh non-zeo cceleon (ofen consn) Sole D poblems wh zeo nd consn cceleon (ncludng fee-fll nd moon on n nclne) Use Cesn nd pol coodne

More information

4.8 Improper Integrals

4.8 Improper Integrals 4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls

More information

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA WO INERFIL OLLINER GRIFFIH RS IN HERMO- ELSI OMOSIE MEDI h m MISHR S DS * Deme o Mheml See I Ie o eholog BHU V-5 I he oee o he le o he e e o eeg o o olle Gh e he ee o he wo ohoo mel e e e emee el. he olem

More information

Heat conduction in a composite sphere - the effect of fractional derivative order on temperature distribution

Heat conduction in a composite sphere - the effect of fractional derivative order on temperature distribution MATEC We of Confeence 57, 88 (8) MMS 7 hp://do.og/.5/mecconf/85788 He conducon n compoe phee - he effec of fconl devve ode on empeue duon Uzul Sedlec,*, Snłw Kul Inue of Mhemc, Czeochow Unvey of Technology,

More information

Electricity & Magnetism Lecture 6: Electric Potential

Electricity & Magnetism Lecture 6: Electric Potential Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why

More information

Chapter Direct Method of Interpolation More Examples Mechanical Engineering

Chapter Direct Method of Interpolation More Examples Mechanical Engineering Chpte 5 iect Method o Intepoltion Moe Exmples Mechnicl Engineeing Exmple Fo the pupose o shinking tunnion into hub, the eduction o dimete o tunnion sht by cooling it though tempetue chnge o is given by

More information

PHYS 2421 Fields and Waves

PHYS 2421 Fields and Waves PHYS 242 Felds nd Wves Instucto: Joge A. López Offce: PSCI 29 A, Phone: 747-7528 Textook: Unvesty Physcs e, Young nd Feedmn 23. Electc potentl enegy 23.2 Electc potentl 23.3 Clcultng electc potentl 23.4

More information

Macroscopic quantum effects generated by the acoustic wave in a molecular magnet

Macroscopic quantum effects generated by the acoustic wave in a molecular magnet Cudnovsky-Fes-09034 Mcroscopc qunum effecs genered by e cousc wve n moleculr mgne Gwng-Hee Km ejong Unv., Kore Eugene M. Cudnovksy Lemn College, CUNY Acknowledgemens D. A. Grnn Lemn College, CUNY Oulne

More information

COMP 465: Data Mining More on PageRank

COMP 465: Data Mining More on PageRank COMP 465: Dt Mnng Moe on PgeRnk Sldes Adpted Fo: www.ds.og (Mnng Mssve Dtsets) Powe Iteton: Set = 1/ 1: = 2: = Goto 1 Exple: d 1/3 1/3 5/12 9/24 6/15 = 1/3 3/6 1/3 11/24 6/15 1/3 1/6 3/12 1/6 3/15 Iteton

More information