Proceedings of the 7th IASME / WSEAS International Conference on HEAT TRANSFER, THERMAL ENGINEERING and ENVIRONMENT (HTE '09)

Size: px
Start display at page:

Download "Proceedings of the 7th IASME / WSEAS International Conference on HEAT TRANSFER, THERMAL ENGINEERING and ENVIRONMENT (HTE '09)"

Transcription

1 athmatal modlng of forst fr sprad VALEIY PEINOV Dpartmnt of athmats and Natural Sn Blovo Branh of Kmrovo Stat Unvrsty Sovtskaya Strt Blovo Kmrovo rgon 6600 USSIA Abstrat: - Ths papr s dvotd a problm of dvlopmnt of a mathmatal modl for dsrpton of hat and mass transfr prosss at rown forst fr ntaton and sprad. athmatal modl of forst fr was basd on an analyss of xprmntal data and usng onpt and mthods from ratv mda mhans. Ths study gvs a two dmnsonal avragd mathmatal sttng and mthod of numral soluton of a problm of a forst fr sprad. Th boundary-valu problm s solvd numrally usng th mthod of splttng aordng to physal prosss. It was basd on numral soluton of two dmnsonal ynolds quatons for th dsrpton of turbulnt flow takng nto aount for dffuson quatons hmal omponnts and quatons of nrgy onsrvaton for gasous and ondnsd phass. In ths ontxt a study - mathmatal modlng - of th ondtons of forst fr spradng that would mak t possbl to obtan a dtald ptur of th hang n th vloty tmpratur and omponnt onntraton flds wth tm and dtrmn as wll as th lmtng ondtons of forst fr propagaton s of ntrst.. Ky-Words: athmatal modl forst fr gnton ombuston ontrol volum dsrt analogu. Introduton A grat dal of work has bn don on th thortal problm of forst fr ntaton. Crown frs ar ntatd by onvtv and radatv hat transfr from surfa frs. Howvr onvton s th man hat transfr mhansm. Th frst xplanaton of ths pross was gvn by Van Wagnr []. Th thory proposd thr dpnds on thr smpl rown proprts: rown bas hght bulk dnsty and mostur ontnt of forst ful. Also rown fr ntaton and hazard hav bn studd and modld n dtal (s for xampl Alxandr []; Van Wagnr []; Xanthopoulos []; othrml []; Cruz and othrs [6]; Albn and othrs [7]; Sott and nhardt [8]).Th mor omplt dsusson of th problm of modlng forst frs s provdd by a yl of works produd by a group of oworkrs at Tomsk Unvrsty (Grshn [9]; Grshn and Prmnov [0]; Prmnov []). In partular a mathmatal modl of forst frs was obtand by Grshn [9] basd on an analyss of known and orgnal xprmntal data (Grshn [9]; Konv [] and usng onpts and mthods from ratv mda mhans. Th physal two-phas modls usd by orvan and Dupuy [] may b onsdrd as a ontnuaton and xtnson of th formulaton proposd n [9]. Problm Formulaton Th bas assumptons adoptd durng th dduton of quatons and boundary and ntal ondtons: ) th forst rprsnts a mult-phas multstord spatally htrognous mdum; ) n th fr zon th forst s a porous-dsprsd two-tmpratur sngl-vloty ratv mdum; ) th forst anopy s supposd to b non - dformd mdum (trunks larg branhs small twgs and ndls) whh affts only th magntud of th for of rsstan n th quaton of onsrvaton of momntum n th gas phas.. th mdum s assumd to b quas-sold (almost non-dformabl durng wnd gusts); ) lt thr b a so-alld vntlatd forst massf n whh th volum of fratons of ondnsd forst ful phass onsstng of dry organ mattr watr n lqud stat sold pyrolyss produts and ash an b ngltd ompard to th volum fraton of gas phas (omponnts of ar and gasous pyrolyss produts); ) th flow has a dvlopd turbulnt natur and molular transfr s ngltd; 6) gasous phas dnsty dosn t dpnd on th prssur baus of th low vlots of th flow n omparson wth th vloty of th sound. Lt th oordnat rfrn pont x x x = 0 b stuatd at th ntr of th surfa forst fr sour at th hght of th roughnss lvl axs 0x drtd paralll to th Earth s surfa to th rght n th drton of th unprturbd wnd spd axs 0x drtd prpndular to 0x and axs 0x drtd upward (Fg. ). Fgur ISSN: ISBN:

2 Baus of th horzontal szs of forst massf mor than hght of forst h systm of quatons of gnral mathmatal modl of forst fr [9] was ntgratd btwn th lmts from hght of th roughnss lvl - 0 to h. Bsds suppos that h 0 φ dx =φ h & φ & - avrag valu of φ. Th problm formulatd abov s rdud to a soluton of th followng systm of quatons: ρ + + ( ρv ) = Q ( m& m& ) / h = ; t x dv p r ρ = + ( ρv v ) ρsd v v ρg dt x x ρ p d ρ dt x = dt dt + Qv + ( τ τ ) / h = ; = ( ρ v T p ) + q v ( T Ts ) + x = x k ρ p ( q T + q ) / h; T + ( ρv ) + Q + ( J J ) / h = ; U k( U x TS ϕ = q t + ( T T V S ); ϕ ϕ ρ = ρ t t ϕ ρ = C t C σt S ) + ( q q q + k( U = ϕ ρ t = 0; + ) / h = 0; σt r r = p = ρ T v = ( v v v) g = (00 g). = = Th systm of quatons () (7) must b solvd takng nto aount th ntal and boundary ondtons t = 0 : v = 0 v = 0 v = 0 T = T = T = T ϕ = ϕ ; s v x = x v = V v = = T = T = : 0 0 x U + U /= 0; k x v v S ) = x : = 0 = 0 = 0 = 0 x x x x x T U = 0 + U = 0 ; x k x v (8) (9) v v v x = x0: = 0 = 0 = 0 = 0 x x x x (0) T U = 0 + U = 0 ; x k x () () () () () (6) (7) v v v x = x : = 0 = 0 = 0 = 0 x x x x () T U = 0 + U = 0. x k x U x = 0 : v = 0 v = 0 0 U 0 x = k x + = () v = v0 T = Tg x Δ x Δ v = 0 T = T x >Δ x >Δ; v v v x = x : = 0 = 0 = 0 = 0 x x x x () T U = 0 + U = 0. x k x Hr and abov d s th symbol of th t otal (subs tantal) dt drvatv; v s th offnt of phas xhang; ρ - dnsty of gas dsprsd phas t s tm; v - th vloty omponnts; T T S - tmpraturs of gas and sold phass U - dnsty of radaton nrgy k - offnt of radaton attnuaton P - prssur; p onstant prssur spf hat of th gas phas p ρ ϕ spf hat dnsty and volum of fraton of ondnsd phas ( dry organ substan mostur ondnsd pyrolyss produts mnral part of forst ful) th mass rats of hmal ratons q thrmal ffts of hmal ratons; k g k S - radaton absorpton offnts for gas and ondnsd phass; T - th ambnt tmpratur; - mass onntratons of - omponnt of gas - dsprsd mdum ndx = whr orrsponds to th dnsty of oxygn - to arbon monoxd CO - to arbon doxd and nrt omponnts of ar; unvrsal gas onstant; C and molular mass of - omponnts of th gas phas arbon and ar mxtur; g s th gravty alraton; d s an mpral offnt of th rsstan of th vgtaton s s th spf surfa of th forst ful n th gvn forst stratum. To dfn sour trms whh haratrz nflow (outflow of mass) n a volum unt of th gas-dsprsd phas th followng formula wr usd for th rat of formulaton of th gasdsprsd mxtur m& outflow of oxygn hangng arbon monoxd. Q = ( ) + + = = ν ( ) = 0. g Hr ν g mass fraton of gas ombustbl produts of pyrolyss and mpral onstants. aton rats of ths varous ontrbutons (pyrolyss vaporaton ombuston of ok and volatl ombustbl produts of pyrolyss) ar approxmatd by Arrhnus laws whos paramtrs (pr-xponntal onstant k and atvaton ISSN: ISBN:

3 nrgy E ) ar valuatd usng data for mathmatal modls [9]. E 0. E = kρϕ xp = kρϕ T s xp Ts Ts E. E = kρϕsσ xp = k T xp. Ts T Th ntal valus for volum of fratons of ondnsd phass ar dtrmnd usng th xprssons: d( ν z ) Wd ϕ ρ ϕ = ϕ = ϕ = ρ ρ ρ 0. whr d -bulk dnsty for surfa layr ν z offnt of ashs of forst ful W forst ful mostur ontnt. It s supposd that th optal proprts of a mdum ar ndpndnt of radaton wavlngth (th assumpton that th mdum s gry ) and th so-alld dffuson approxmaton for radaton flux dnsty wr usd for a mathmatal dsrpton of radaton transport durng forst frs. To los th systm () (7) th omponnts of th tnsor of turbulnt strsss and th turbulnt hat and mass fluxs ar dtrmnd usng th loal-qulbrum modl of turbuln (Grshn [9]). Th systm of quatons () (7) ontans trms assoatd wth turbulnt dffuson thrmal onduton and onvton and nds to b losd. Th omponnts of th tnsor of turbulnt strsss ρ v as v wll as th turbulnt fluxs of hat and mass ρ vt p ρ v ar wrttn n trms of th gradnts of th avrag flow proprts usng th formulas ρv v v μ v = t + Kδ x x T ρvpt = λ t ρv = ρdt x x λ = μ / Pr ρ D = μ / S μ μ ρ K t t p t t t t t = / ε whr μ t λ t D t ar th offnts of turbulnt vsosty thrmal ondutvty and dffuson rsptvly; Pr t S t ar th turbulnt Prandtl and Shmdt numbrs whh wr assumd to b qual to. In dmnsonal form th offnt of dynam turbulnt vsosty s dtrmnd usng loal qulbrum modl of turbuln [9]. Th thrmodynam thrmophysal and strutural haratrsts orrspond to th forst fuls n th anopy of a dffrnt (for xampl pn [9]) typ of forst. Th systm of quatons () (7) must b solvd takng nto aount th ntal and boundary ondtons. Th thrmodynam thrmophysal and strutural haratrsts orrspond to th forst fuls n th anopy of a dffrnt typ of forst; for xampl pn forst (Grshn Prmnov []). Calulaton thod and sults Th boundary-valu problm () (7) s solvd numrally usng th mthod of splttng aordng to physal prosss (Prmnov []). In th frst stag th hydrodynam pattrn of flow and dstrbuton of salar funtons was alulatd. Th systm of ordnary dffrntal quatons of hmal knts obtand as a rsult of splttng was thn ntgratd. A dsrt analog was obtand by mans of th ontrol volum mthod usng th SIPLE lk algorthm (Patankar [6] ) Th auray of th program was hkd by th mthod of nsrtd analytal solutons. Analytal xprssons for th unknown funtons wr substtutd n () (7) and th losur of th quatons wr alulatd. Ths was thn tratd as th sour n ah quaton. Nxt wth th ad of th algorthm dsrbd abov th valus of th funtons usd wr nfrrd wth an auray of not lss than %. Th fft of th dmnsons of th ontrol volums on th soluton was studd by dmnshng thm. Th tm stp was sltd automatally. Flds of tmpratur vloty omponnt mass fratons and volum fratons of phass wr obtand numrally. Th dstrbuton of bas funtons shows that th pross of rown forst fr ntaton gos through th nxt stags. Th frst stag s rlatd to nrasng maxmum tmpratur n th ground ovr wth th rsult that a surfa fr sour appars. At ths pross stag ovr th fr sour a thrmal wnd s formd a zon of hatd forst fr pyrolyss produts whh ar mxd wth ar float up and pntrat nto th rowns of trs. As a rsult forst fuls n th tr rowns ar hatd mostur vaporats and gasous and dsprsd pyrolyss produts ar gnratd. Ignton of gasous pyrolyss produts of th ground ovr ours at th nxt stag and that of gasous pyrolyss produts n th forst anopy ours at th last stag. As a rsult of hatng of forst ful lmnts of rown mostur vaporats and pyrolyss ours aompand by th rlas of gasous produts whh thn gnt and burn away n th forst anopy. At th momnt of gnton th gas ombustbl produts of pyrolyss burns away and th onntraton of oxygn s rapdly rdud. Th tmpraturs of both phass rah a maxmum valu at th pont of gnton. Th gnton prosss s of a gas - phas natur. Not also that th transfr of nrgy from th fr sour taks pla du to radaton; th valu of radaton hat flux dnsty s small ompard to that of th onvtv hat flux. In th vnty of th sour of hat and mass rlas hatd ar masss and produts of pyrolyss and ombuston float up. At V 0 th wnd fld n th forst anopy ntrats wth th gas-t obstal that forms from th surfa forst fr sour and from th gntd forst anopy bas and burn away n th forst anopy. In th vnty of th sour of hat and mass rlas hatd ar masss and produts of pyrolyss and ombuston float up. At V 0 th wnd fld n th ISSN: ISBN:

4 forst anopy ntrats wth th gas-t obstal that forms from th surfa forst fr sour and from th gntd forst anopy bas. On th wndward sd th movmnt of th ar flowng past th gnton rgon alrats. Fgurs ab ab and ab prsnt th dstrbuton of tmpratur T ( T = T / T T = 00K) (-...) for gas phas oxygn ( ) volatl ombustbl produts of pyrolyss onntratons ( ) ( = с / с = 0. ) for wnd vloty V = 0 m/s: and a) t= s. b) t= s. W an not that th sothrms s movd n th forst anopy and dformd by th aton of wnd. Smlarly th flds of omponnt onntratons ar dformd. It s onludd that th forst fr bgns to sprad. Fgur. a. Fgur.a Fgur b. Fgur.b Fgur a. ISSN: ISBN:

5 Th rsults obtand agr wth th laws of physs and xprmntal data. frns Conluson Fgur b. Th rsults of alulaton gv an opportunty to valuat rtal ondton of th forst fr sprad whh allows applyng th gvn modl for prvntng frs. It ovrstmats th rown forst fr sprad that dpnds on rown proprts: bulk dnsty mostur ontnt of forst ful and t. Th modl proposd thr gv a dtald ptur of th hang n th vloty tmpratur and omponnt onntraton flds wth tm and dtrmn as wll as th nflun of dffrnt ondtons on th rown forst fr ntaton. Th rsults obtand agr wth th laws of physs and xprmntal data (Grshn [9]; Konv []). From an analyss of alulatons and xprmntal data t was found that for th ass n quston th mnmum total nndary hat puls s 600 kj/m (Grshn [9]).. Fgur 8 llustrats th tmpratur dpndn of tm gnton of rown for dffrnt bulk dnsts of surfa layr ( d=0 and - 0 kg/m - numral alulatons; - d=0 and x 0 kg/m xprmntal rsults (orshn [7]). Fgur 8. ostur ontnt of FF n rown s W=0% and d=0. kg/m. [] Van Wagnr C.E. Condtons for th start and sprad of rown fr. Canadan Journal of Forst sarh No pp. -. [] Alxandr.E. Crown fr thrsholds n xot pn plantatons of Australasa. PhD thss Dpartmnt of Forstry Australan Natonal Unvrsty 998. [] Van Wagnr C. E. Prdton of rown fr bhavor n onfr stands. In '0th onfrn on fr and forst mtorology'. Ottawa Ontaro. (Eds D. C. aivr H. Auld and. Whtwood) pp [] Xanthopoulos G. Dvlopmnt of a wldland rown fr ntaton modl. PhD thss Unvrsty of ontana 990. [] othrml.c. Crown fr analyss and ntrprtaton. In th Intrnatonal onfrn on fr and forst mtorology. ssoula ontana USA 99. [6] Cruz.G. t al Prdtng rown fr bhavor to support forst fr managmnt dson-makng. In 'IV Intrnatonal onfrn on forst fr rsarh'. Luso- Combra Portugal. (Ed. D. X. Vgas) [CD-O]. (llprss) 00. [7] Albn F.A. t al odlng gnton and burnng rat of larg woody natural fuls. Int. Journal of Wldland fr Vol. No. 99 pp [8] Sott J.H. t al Assssng rown fr potntal by lnkng modls of surfa and rown fr bhavor. USDA Forst Srv oky ountan Forst and ang Exprmnt Staton. Fort Collns: S-P-9 (Colorado USA) 00. [9] Grshn A.. athmatal odlng Forst Fr and Nw thods Fghtng Thm. Tomsk Publshng Hous of Tomsk Unvrsty ussa [0] Grshn A.. Prmnov V.A. athmatal modlng of th gnton of tr rowns. Combuston Exploson and Shok Wavs Vol. 998 pp [] Prmnov V.A. athmatal odlng of Crown and ass Forst Frs Intaton Wth th Allowan for th adatv - Convtv Hat and ass Transfr and Two Tmpraturs of dum Ph.D Thss Tomsk Stat Unvrsty ussa 99. [] Prmnov V.A. athmatal modlng of rown forst fr ntaton. In 'III Intrnatonal onfrn on forst fr rsarh and th onfrn on fr and forst mtorology'. Luso Portugal. (Ed. D.X.Vgas) 998 pp. 9-. [] Konv E.V. Th physal foundaton of vgtatv matrals ombuston.. Novosbrsk Nauka ussa [] orvan D. Dupuy J.L. odlng of fr sprad ISSN: ISBN:

6 through a forst ful bd usng a multphas formulaton. Combuston and Flam Vol pp [] orvan D. Dupuy J.L. odlng th propagaton of wldfr through a dtrranan shrub usng a multphas formulaton. Combuston and Flam Vol pp [6] Patankar S.V. Numral Hat Transfr and Flud Flow. Nw York: Hmsphr Publshng Corporaton 98. [7] orshn V.N. [986]. Calulaton mthod of th thn vgtabl partl gnton by onvtv flux LTA Lnngrad (ussa). ISSN: ISBN:

Mathematical modeling of the crown forest fires impact on buildings

Mathematical modeling of the crown forest fires impact on buildings INTENATIONAL JOUNAL OF ATHEATIC AND COPUTE IN IULATION Volum 07 athmatal modlng of th rown forst frs mpat on buldngs Valry Prmno Abstrat Th mathmatal modlng of forst frs atons on buldngs and struturs has

More information

Advances in the study of intrinsic rotation with flux tube gyrokinetics

Advances in the study of intrinsic rotation with flux tube gyrokinetics Adans n th study o ntrns rotaton wth lux tub gyroknts F.I. Parra and M. arns Unrsty o Oxord Wolgang Paul Insttut, Vnna, Aprl 0 Introduton In th absn o obous momntum nput (apart rom th dg), tokamak plasmas

More information

The gravitational field energy density for symmetrical and asymmetrical systems

The gravitational field energy density for symmetrical and asymmetrical systems Th ravtatonal ld nry dnsty or symmtral and asymmtral systms Roald Sosnovsy Thnal Unvrsty 1941 St. Ptrsbur Russa E-mal:rosov@yandx Abstrat. Th rlatvst thory o ravtaton has th onsdrabl dults by dsrpton o

More information

MATHEMATICAL MODELING OF FOREST FIRES INITIATION, SPREAD AND IMPACT ON ENVIRONMENT

MATHEMATICAL MODELING OF FOREST FIRES INITIATION, SPREAD AND IMPACT ON ENVIRONMENT Intrnational Journal of GEOATE, July, 07, Vol., Issu 5, pp.9-99 Got., Const. at. & Env., IN:86-990, Japan, DOI: http://dx.doi.org/0.660/07.5.670 Intrnational Journal of GEOATE, July, 07, Vol., Issu 5,

More information

Electrochemical reaction mechanisms

Electrochemical reaction mechanisms Eltrohmal raton mhansms Exampl: oppr rduton (): Cu + + Cu + slow (): Cu + + Cu fast Coppr also undrgos a dsproportonaton raton: Cu + Cu + + Cu Its qulbrum onstant s K. 6. As th frst stp s slow ompard to

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added 4.3, 4.4 Phas Equlbrum Dtrmn th slops of th f lns Rlat p and at qulbrum btwn two phass ts consdr th Gbbs functon dg η + V Appls to a homognous systm An opn systm whr a nw phas may form or a nw componnt

More information

Matched Quick Switching Variable Sampling System with Quick Switching Attribute Sampling System

Matched Quick Switching Variable Sampling System with Quick Switching Attribute Sampling System Natur and Sn 9;7( g v, t al, Samlng Systm Mathd Quk Swthng Varabl Samlng Systm wth Quk Swthng Attrbut Samlng Systm Srramahandran G.V, Palanvl.M Dartmnt of Mathmats, Dr.Mahalngam Collg of Engnrng and Thnology,

More information

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.

More information

APPLICATION OF FLOW-THROUGH THREE-DIMENSIONAL ELECTRODES FOR REGENERATION OF PLATING IRON ELECTROLYTES: 1. MATHEMATICAL MODEL

APPLICATION OF FLOW-THROUGH THREE-DIMENSIONAL ELECTRODES FOR REGENERATION OF PLATING IRON ELECTROLYTES: 1. MATHEMATICAL MODEL hmstry Journal of oldova. Gnral, Industral and Eologal hmstry. 4, 9, 3-4 APPLIATION O LOW-THROUGH THREE-DIENSIONAL ELETRODES OR REGENERATION O PLATING IRON ELETROLYTES:. ATHEATIAL ODEL Alandr Kоshv a,

More information

Research Note A 1D Model for Erosion Through Submerged, Prone Vegetation

Research Note A 1D Model for Erosion Through Submerged, Prone Vegetation Rsarh Not A 1D Modl for Eroson Through Submrgd, Pron Vgtaton J. M.V. Saman Asso. Prof. of Agrultur Faulty, Tarbat Modarrs Unv. P.O.Box: 14115-336. saman_j@modars.a.r (Rvd: Sp. 3, Aptd: Ds. 4) Abstrat-Vgtaton

More information

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 6: Heat Conduction: Thermal Stresses

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 6: Heat Conduction: Thermal Stresses 16.512, okt Proulon Prof. Manul Martnz-Sanhz Ltur 6: Hat Conduton: Thrmal Str Efft of Sold or Lqud Partl n Nozzl Flow An u n hhly alumnzd old rokt motor. 3 2Al + O 2 Al 2 O 2 3 m.. 2072 C, b.. 2980 C In

More information

EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In the absence of or in between ELMs)

EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In the absence of or in between ELMs) I. EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In th absnc of or n btwn ELMs) Abstract W. M. Stacy (Gorga Tch) and R. J. Grobnr (Gnral Atomcs) A constrant on th on prssur gradnt s mposd by momntum

More information

THE PRINCIPLE OF HARMONIC COMPLEMENTARITY IN EVALUATION OF A SPECIFIC THRUST JET ENGINE

THE PRINCIPLE OF HARMONIC COMPLEMENTARITY IN EVALUATION OF A SPECIFIC THRUST JET ENGINE U.P.B. S. Bull., Srs D, Vol. 76, Iss., 04 ISSN 454-358 THE PRINCIPLE OF HARMONIC COMPLEMENTARITY IN EVALUATION OF A SPECIFIC THRUST JET ENGINE Vrgl STANCIU, Crstna PAVEL Th fundamntal da of ths papr s

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

Kinetics of Release from Polydisperse Core Particles Coated with Layers of Fine Soluble Particles

Kinetics of Release from Polydisperse Core Particles Coated with Layers of Fine Soluble Particles Intrnatonal Journal of Chmal Engnrng and Applatons Vol. No. 4 August 011 Knts of Rlas from Polydsprs Cor Partls Coatd wth Layrs of Fn Solubl Partls Bors Golman Mmbr APCBEES Abstrat Th knts of rlas of atv

More information

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces C465/865, 26-3, Lctur 7, 2 th Sp., 26 lctrochmcal qulbrum lctromotv Forc Rlaton btwn chmcal and lctrc drvng forcs lctrochmcal systm at constant T and p: consdr G Consdr lctrochmcal racton (nvolvng transfr

More information

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is

ANALYSIS: The mass rate balance for the one-inlet, one-exit control volume at steady state is Problm 4.47 Fgur P4.47 provds stady stat opratng data for a pump drawng watr from a rsrvor and dlvrng t at a prssur of 3 bar to a storag tank prchd 5 m abov th rsrvor. Th powr nput to th pump s 0.5 kw.

More information

First looking at the scalar potential term, suppose that the displacement is given by u = φ. If one can find a scalar φ such that u = φ. u x.

First looking at the scalar potential term, suppose that the displacement is given by u = φ. If one can find a scalar φ such that u = φ. u x. 7.4 Eastodynams 7.4. Propagaton of Wavs n East Sods Whn a strss wav travs throgh a matra, t ass matra parts to dspa by. It an b shown that any vtor an b wrttn n th form φ + ra (7.4. whr φ s a saar potnta

More information

Stability of an Exciton bound to an Ionized Donor in Quantum Dots

Stability of an Exciton bound to an Ionized Donor in Quantum Dots Stablty of an Exton bound to an Ionzd Donor n Quantum Dots by S. Baskoutas 1*), W. Shommrs ), A. F. Trzs 3), V. Kapakls 4), M. Rth 5), C. Polts 4,6) 1) Matrals Sn Dpartmnt, Unvrsty of Patras, 6500 Patras,

More information

1- Summary of Kinetic Theory of Gases

1- Summary of Kinetic Theory of Gases Dr. Kasra Etmad Octobr 5, 011 1- Summary of Kntc Thory of Gass - Radaton 3- E4 4- Plasma Proprts f(v f ( v m 4 ( kt 3/ v xp( mv kt V v v m v 1 rms V kt v m ( m 1/ v 8kT m 3kT v rms ( m 1/ E3: Prcntag of

More information

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS COMPUTTION FUID DYNMICS: FVM: pplcatons to Scalar Transport Prolms ctur 3 PPICTIONS OF FINITE EEMENT METHOD TO SCR TRNSPORT PROBEMS 3. PPICTION OF FEM TO -D DIFFUSION PROBEM Consdr th stady stat dffuson

More information

IV. First Law of Thermodynamics. Cooler. IV. First Law of Thermodynamics

IV. First Law of Thermodynamics. Cooler. IV. First Law of Thermodynamics D. Applcatons to stady flow dvcs. Hat xchangrs - xampl: Clkr coolr for cmnt kln Scondary ar 50 C, 57,000 lbm/h Clkr? C, 5 ton/h Coolr Clkr 400 C, 5 ton/h Scondary ar 0 C, 57,000 lbm/h a. Assumptons. changs

More information

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

More information

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D Comp 35 Introducton to Machn Larnng and Data Mnng Fall 204 rofssor: Ron Khardon Mxtur Modls Motvatd by soft k-mans w dvlopd a gnratv modl for clustrng. Assum thr ar k clustrs Clustrs ar not rqurd to hav

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

Heating of a solid cylinder immersed in an insulated bath. Thermal diffusivity and heat capacity experimental evaluation.

Heating of a solid cylinder immersed in an insulated bath. Thermal diffusivity and heat capacity experimental evaluation. Hatng of a sold cylndr mmrsd n an nsulatd bath. Thrmal dffusvty and hat capacty xprmntal valuaton. Žtný R., CTU FE Dpartmnt of Procss Engnrng, arch. Introducton Th problm as ntatd by th follong E-mal from

More information

Review - Probabilistic Classification

Review - Probabilistic Classification Mmoral Unvrsty of wfoundland Pattrn Rcognton Lctur 8 May 5, 6 http://www.ngr.mun.ca/~charlsr Offc Hours: Tusdays Thursdays 8:3-9:3 PM E- (untl furthr notc) Gvn lablld sampls { ɛc,,,..., } {. Estmat Rvw

More information

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D Comp 35 Machn Larnng Computr Scnc Tufts Unvrsty Fall 207 Ron Khardon Th EM Algorthm Mxtur Modls Sm-Suprvsd Larnng Soft k-mans Clustrng ck k clustr cntrs : Assocat xampls wth cntrs p,j ~~ smlarty b/w cntr

More information

Theory about cathode arc root: a review

Theory about cathode arc root: a review IOP Confrn Srs: Matrals Sn and Engnrng Thory about athod ar root: a rvw To t ths artl: A Lfort and M Abbaou 1 IOP Conf. Sr.: Matr. S. Eng. 9 16 Vw th artl onln for updats and nhanmnts. Rlatd ontnt - Vauum

More information

An analytical solution to predict axial load along fully grouted bolts in an elasto-plastic rock mass

An analytical solution to predict axial load along fully grouted bolts in an elasto-plastic rock mass An analytal soluton to prdt axal load along fully groutd bolts n an lasto-plast rok mass by H. Jalalfar* T h n a l Synopss Nowadays, fully napsulatd rokbolts hav bom a ky lmnt n th dsgn of ground ontrol

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

Magneto-elastic coupling model of deformable anisotropic superconductors

Magneto-elastic coupling model of deformable anisotropic superconductors Magnto-last ouplng modl of dformabl ansotrop suprondutors Yngu L, Guohng Kang, and Yuanwn Gao,4 ppld Mhans and Strutur Safty Ky Laboratory of Shuan Provn, Shool of Mhans and Engnrng, Southwst Jaotong Unvrsty,

More information

From Structural Analysis to FEM. Dhiman Basu

From Structural Analysis to FEM. Dhiman Basu From Structural Analyss to FEM Dhman Basu Acknowldgmnt Followng txt books wr consultd whl prparng ths lctur nots: Znkwcz, OC O.C. andtaylor Taylor, R.L. (000). Th FntElmnt Mthod, Vol. : Th Bass, Ffth dton,

More information

Multiple-Choice Test Runge-Kutta 4 th Order Method Ordinary Differential Equations COMPLETE SOLUTION SET

Multiple-Choice Test Runge-Kutta 4 th Order Method Ordinary Differential Equations COMPLETE SOLUTION SET Multpl-Co Tst Rung-Kutta t Ordr Mtod Ordnar Drntal Equatons COMPLETE SOLUTION SET. To solv t ordnar drntal quaton sn ( Rung-Kutta t ordr mtod ou nd to rwrt t quaton as (A sn ( (B ( sn ( (C os ( (D sn (

More information

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas Shool of roa Engnrng Equl. Prort of Ratng Ga Mxtur So far hav lookd at Stattal Mhan rult for a ngl (ur) rft ga hown how to gt ga rort (,, h, v,,, ) from artton funton () For nonratng rft ga mxtur, gt mxtur

More information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

CHAPTER 4. The First Law of Thermodynamics for Control Volumes

CHAPTER 4. The First Law of Thermodynamics for Control Volumes CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst

More information

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.

Utilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice. Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl

More information

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges Physcs of Vry Hgh Frquncy (VHF) Capactvly Coupld Plasma Dschargs Shahd Rauf, Kallol Bra, Stv Shannon, and Kn Collns Appld Matrals, Inc., Sunnyval, CA AVS 54 th Intrnatonal Symposum Sattl, WA Octobr 15-19,

More information

Finite Element Based Implementation of Fiala s Thermal Manikin in THESEUS-FE

Finite Element Based Implementation of Fiala s Thermal Manikin in THESEUS-FE Fnt Elmnt Basd Implmntaton of Fala s hrmal Mankn n HESEUS-FE Author: Dr. Stfan Paulk (chncal Managr) VMS, 3.05.007 Global Modllng Mankn Implmntaton Global Human Hat Fluxs Human mpratur Valdaton Global

More information

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS ACOUSTIC WAE EQUATION Contnts INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS INTRODUCTION As w try to vsualz th arth ssmcally w mak crtan physcal smplfcatons that mak t asr to mak and xplan our obsrvatons.

More information

Polytropic Process. A polytropic process is a quasiequilibrium process described by

Polytropic Process. A polytropic process is a quasiequilibrium process described by Polytropc Procss A polytropc procss s a quasqulbrum procss dscrbd by pv n = constant (Eq. 3.5 Th xponnt, n, may tak on any valu from to dpndng on th partcular procss. For any gas (or lqud, whn n = 0, th

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

:2;$-$(01*%<*=,-./-*=0;"%/;"-*

:2;$-$(01*%<*=,-./-*=0;%/;-* !"#$%'()%"*#%*+,-./-*+01.2(.*3+456789*!"#$%"'()'*+,-."/0.%+1'23"45'46'7.89:89'/' ;8-,"$4351415,8:+#9' Dr. Ptr T. Gallaghr Astrphyscs Rsarch Grup Trnty Cllg Dubln :2;$-$(01*%

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

Lecture 3: Phasor notation, Transfer Functions. Context

Lecture 3: Phasor notation, Transfer Functions. Context EECS 5 Fall 4, ctur 3 ctur 3: Phasor notaton, Transfr Functons EECS 5 Fall 3, ctur 3 Contxt In th last lctur, w dscussd: how to convrt a lnar crcut nto a st of dffrntal quatons, How to convrt th st of

More information

3.4 Properties of the Stress Tensor

3.4 Properties of the Stress Tensor cto.4.4 Proprts of th trss sor.4. trss rasformato Lt th compots of th Cauchy strss tsor a coordat systm wth bas vctors b. h compots a scod coordat systm wth bas vctors j,, ar gv by th tsor trasformato

More information

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP ISAHP 00, Bal, Indonsa, August -9, 00 COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP Chkako MIYAKE, Kkch OHSAWA, Masahro KITO, and Masaak SHINOHARA Dpartmnt of Mathmatcal Informaton Engnrng

More information

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions 9 Strss-Basd Fnt Elmnt Mthods for Dynamcs Analyss of Eulr-Brnoull Bams wth Varous Boundary Condtons Abstract In ths rsarch, two strss-basd fnt lmnt mthods ncludng th curvatur-basd fnt lmnt mthod (CFE)

More information

New solution to the cosmological constant problem and cosmological model with superconductivity

New solution to the cosmological constant problem and cosmological model with superconductivity Alksandr V Bukalo DC 53:547:539:5454:530 w soluton to th osmologal onstant probl and osmologal modl wth suprondutty Th Cntr of hysal and Spa Rsarhs, IIS, Mlnkoa str,, K-050, 04050, kran -mal: bukalophyss@soonnfo

More information

An Overview of Markov Random Field and Application to Texture Segmentation

An Overview of Markov Random Field and Application to Texture Segmentation An Ovrvw o Markov Random Fld and Applcaton to Txtur Sgmntaton Song-Wook Joo Octobr 003. What s MRF? MRF s an xtnson o Markov Procss MP (D squnc o r.v. s unlatral (causal: p(x t x,

More information

Guo, James C.Y. (1998). "Overland Flow on a Pervious Surface," IWRA International J. of Water, Vol 23, No 2, June.

Guo, James C.Y. (1998). Overland Flow on a Pervious Surface, IWRA International J. of Water, Vol 23, No 2, June. Guo, Jams C.Y. (006). Knmatc Wav Unt Hyrograph for Storm Watr Prctons, Vol 3, No. 4, ASCE J. of Irrgaton an Dranag Engnrng, July/August. Guo, Jams C.Y. (998). "Ovrlan Flow on a Prvous Surfac," IWRA Intrnatonal

More information

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 1: Introduction. - Depending on gas acceleration mechanism/force on vehicle mechanism.

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 1: Introduction. - Depending on gas acceleration mechanism/force on vehicle mechanism. 6.5, Rokt Propulson Prof. Manul Martnz-Sanhz Ltur : Introduton Typs of Rokts (Engns) - Dpndng on gas alraton mhansm/for on vhl mhansm. Thrmal Gas pushs drtly on walls by P (prssur) fors Nozzl alrats gas

More information

Chapter 3: Energy Band and Charge Carriers Semiconductor

Chapter 3: Energy Band and Charge Carriers Semiconductor Chaptr 3: nrgy Band and Charg Carrrs Smondutor 3. Bondng Fors and nrgy bands n Sold Th bas dffrn btwn th as of an ltron n a sold and that of an ltron n an solatd atom s that n th sold th ltron has a rang,

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

Physics 256: Lecture 2. Physics

Physics 256: Lecture 2. Physics Physcs 56: Lctur Intro to Quantum Physcs Agnda for Today Complx Numbrs Intrfrnc of lght Intrfrnc Two slt ntrfrnc Dffracton Sngl slt dffracton Physcs 01: Lctur 1, Pg 1 Constructv Intrfrnc Ths wll occur

More information

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline Introucton to Ornar Dffrntal Equatons Sptmbr 7, 7 Introucton to Ornar Dffrntal Equatons Larr artto Mchancal Engnrng AB Smnar n Engnrng Analss Sptmbr 7, 7 Outln Rvw numrcal solutons Bascs of ffrntal quatons

More information

Outlier-tolerant parameter estimation

Outlier-tolerant parameter estimation Outlr-tolrant paramtr stmaton Baysan thods n physcs statstcs machn larnng and sgnal procssng (SS 003 Frdrch Fraundorfr fraunfr@cg.tu-graz.ac.at Computr Graphcs and Vson Graz Unvrsty of Tchnology Outln

More information

Multiple Choice Questions

Multiple Choice Questions B S. M. CHINCHOLE Multpl Co Qustons L. V. H. ARTS, SCIENCE AND COMMERCE COLLEGE, PANCHAVATI, NSAHIK - Pag B S. M. CHINCHOLE L. V. H. ARTS, SCIENCE AND COMMERCE COLLEGE, PANCHAVATI, NSAHIK - Pag B S. M.

More information

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density

Radial Cataphoresis in Hg-Ar Fluorescent Lamp Discharges at High Power Density [NWP.19] Radal Cataphorss n Hg-Ar Fluorscnt Lamp schargs at Hgh Powr nsty Y. Aura, G. A. Bonvallt, J. E. Lawlr Unv. of Wsconsn-Madson, Physcs pt. ABSTRACT Radal cataphorss s a procss n whch th lowr onzaton

More information

Discrete Shells Simulation

Discrete Shells Simulation Dscrt Shlls Smulaton Xaofng M hs proct s an mplmntaton of Grnspun s dscrt shlls, th modl of whch s govrnd by nonlnar mmbran and flxural nrgs. hs nrgs masur dffrncs btwns th undformd confguraton and th

More information

FEFF and Related Codes

FEFF and Related Codes FEFF and Rlatd Cods Anatoly Frnl Profssor Physcs Dpartmnt, Yshva Unvrsty, w Yor, USA Synchrotron Catalyss Consortum, Broohavn atonal Laboratory, USA www.yu.du/faculty/afrnl Anatoly.Frnl@yu.du FEFF: John

More information

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION CHAPTER 7d. DIFFERENTIATION AND INTEGRATION A. J. Clark School o Engnrng Dpartmnt o Cvl and Envronmntal Engnrng by Dr. Ibrahm A. Assakka Sprng ENCE - Computaton Mthods n Cvl Engnrng II Dpartmnt o Cvl and

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Advanced Queueing Theory. M/G/1 Queueing Systems

Advanced Queueing Theory. M/G/1 Queueing Systems Advand Quung Thory Ths slds ar rad by Dr. Yh Huang of Gorg Mason Unvrsy. Sudns rgsrd n Dr. Huang's ourss a GMU an ma a sngl mahn-radabl opy and prn a sngl opy of ah sld for hr own rfrn, so long as ah sld

More information

3: Interaction of ionizing radiation with tissue

3: Interaction of ionizing radiation with tissue 3: Intraton o onzng radaton wth tssu 1. What s th bass o ontrast or x-ray magng?. By whh mhansms dos onzng radaton ntrat wth mattr? Raylgh sattrng Compton sattrng Photoltr t Par produton 3. How dos ths

More information

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint Optmal Ordrng Polcy n a Two-Lvl Supply Chan wth Budgt Constrant Rasoul aj Alrza aj Babak aj ABSTRACT Ths papr consdrs a two- lvl supply chan whch consst of a vndor and svral rtalrs. Unsatsfd dmands n rtalrs

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES 13 th World Confrnc on Earthquak Engnrng Vancouvr, B.C., Canada August 1-6, 4 Papr No. 485 ORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WIT VARIABLE PROPERTIES Mngln Lou 1 and Wnan Wang Abstract:

More information

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h For t BWR oprating paramtrs givn blow, comput and plot: a) T clad surfac tmpratur assuming t Jns-Lotts Corrlation b) T clad surfac tmpratur assuming t Tom Corrlation c) T clad surfac tmpratur assuming

More information

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering Last Lcturs: Polaraton of Elctromagntc Wavs Phys 774: Nonlnar Spctroscopy: SHG and Scattrng Gnral consdraton of polaraton Jons Formalsm How Polarrs work Mullr matrcs Stoks paramtrs Poncar sphr Fall 7 Polaraton

More information

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time.

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time. Elctroncphalography EEG Dynamc Causal Modllng for M/EEG ampltud μv tm ms tral typ 1 tm channls channls tral typ 2 C. Phllps, Cntr d Rchrchs du Cyclotron, ULg, Blgum Basd on slds from: S. Kbl M/EEG analyss

More information

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs.

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs. Ttl Autor(s) Two-Tmpratur Plasma Modlng of Argon Gas Tungstn Arcs Tasro, Snc; Tanaa, Manabu Ctaton Transactons of JWRI. 37(1) P.7-P.11 Issu Dat 2008-07 Txt Vrson publsr URL ttp://dl.andl.nt/11094/8887

More information

IV. Transport Phenomena Lecture 35: Porous Electrodes (I. Supercapacitors)

IV. Transport Phenomena Lecture 35: Porous Electrodes (I. Supercapacitors) IV. Transort Phnomna Lctur 35: Porous Elctrods (I. Surcaactors) MIT Studnt (and MZB) 1. Effctv Equatons for Thn Doubl Layrs For surcaactor lctrods, convcton s usually nglgbl, and w dro out convcton trms

More information

A Humanoid Robot Gait Planning and Its Stability Validation

A Humanoid Robot Gait Planning and Its Stability Validation Journal of Computr and Communatons, 204, 2, 68-74 Publshd Onln Sptmbr 204 n SRs. http://www.srp.org/journal/j http://dx.do.org/0.4236/j.204.2009 A Humanod Robot Gat Plannng and Its Stablt Valdaton Jan

More information

Chapter 2: The Photosphere

Chapter 2: The Photosphere 3 Chaptr : Th Photosphr Outr Atmosphr Cor - Enrgy Gnraton Zon.3R.7R Radaton Zon Convcton Zon Photosphr 3 km Fg -: Th Sun - Ovrall Structur.: Th Larg Scal Structur of th Photosphr Th photosphr, th vsbl

More information

Add sodium hydroxide solution

Add sodium hydroxide solution , :::.l9 &30 ~!fjrkh:+l. ~ S/::T..:=4... A studnt has four solutons lablld A, B, C and D. Each soluton contans on compound from th followng lst: FCh Th studnt dos som smpl tsts to dntfy th compounds prsnt.

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

SCIENCE CHINA Chemistry. Signatures of shear thinning-thickening transition in steady shear flows of dense non-brownian yield stress systems

SCIENCE CHINA Chemistry. Signatures of shear thinning-thickening transition in steady shear flows of dense non-brownian yield stress systems SCIENCE CHINA Chmstry ARICES do: 10.1007/s1146-015-5335-8 do: 10.1007/s1146-015-5335-8 Sgnaturs of shar thnnng-thknng transton n stady shar flows of dns non-brownan yld strss systms Wn Zhng, Yu Sh & Nng

More information

Dyna ISSN: Universidad Nacional de Colombia Colombia

Dyna ISSN: Universidad Nacional de Colombia Colombia yna ISSN: 1-7353 dyna@unalmd.du.o Unvrsdad Naonal d Colomba Colomba Vangas-Ush, Lbardo V.; Abdl-Wahab, Magd M.; Parkr, Graham A. trmnaton of th Raylgh dampng offnts of stl brstls and lustrs of brstls of

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

Gravitation as Geometry or as Field

Gravitation as Geometry or as Field Journal of Appld Mathmatcs and Physcs, 7, 5, 86-87 http://wwwscrporg/journal/jamp ISSN Onln: 37-4379 ISSN Prnt: 37-435 Gravtaton as Gomtry or as Fld Waltr Ptry Mathmatcal Insttut of th Unvrsty Dussldorf,

More information

Reliability of time dependent stress-strength system for various distributions

Reliability of time dependent stress-strength system for various distributions IOS Joural of Mathmatcs (IOS-JM ISSN: 78-578. Volum 3, Issu 6 (Sp-Oct., PP -7 www.osrjourals.org lablty of tm dpdt strss-strgth systm for varous dstrbutos N.Swath, T.S.Uma Mahswar,, Dpartmt of Mathmatcs,

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

Random Process Part 1

Random Process Part 1 Random Procss Part A random procss t (, ζ is a signal or wavform in tim. t : tim ζ : outcom in th sampl spac Each tim w rapat th xprimnt, a nw wavform is gnratd. ( W will adopt t for short. Tim sampls

More information

Chapter 2 Theoretical Framework of the Electrochemical Model

Chapter 2 Theoretical Framework of the Electrochemical Model Chaptr 2 Thortcal Framwork of th Elctrochmcal Modl Th basc prncpls of th lctrochmcal modl for L on battry s dvlopd from fundamntals of thrmodynamcs and transport phnomna. Th voluton of th lctrochmcal modl

More information

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach Unv.Prof. r. J. FrankVbach WS 067: Intrnatonal Economcs ( st xam prod) Unvrstät Sgn Fakultät III Unv.Prof. r. Jan FrankVbach Exam Intrnatonal Economcs Wntr Smstr 067 ( st Exam Prod) Avalabl tm: 60 mnuts

More information

Development of an Incremental Model for Fatigue Crack Growth Predictions

Development of an Incremental Model for Fatigue Crack Growth Predictions Dvlopmnt of an nrmntal Modl for Fatgu Crak Growth Prdtons S. Pommr To t ths vrson: S. Pommr. Dvlopmnt of an nrmntal Modl for Fatgu Crak Growth Prdtons. Arospa- Lab, 05, p. -. .

More information

Self-interaction mass formula that relates all leptons and quarks to the electron

Self-interaction mass formula that relates all leptons and quarks to the electron Slf-intraction mass formula that rlats all lptons and quarks to th lctron GERALD ROSEN (a) Dpartmnt of Physics, Drxl Univrsity Philadlphia, PA 19104, USA PACS. 12.15. Ff Quark and lpton modls spcific thoris

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

Problem 22: Journey to the Center of the Earth

Problem 22: Journey to the Center of the Earth Problm : Journy to th Cntr of th Earth Imagin that on drilld a hol with smooth sids straight through th ntr of th arth If th air is rmod from this tub (and it dosn t fill up with watr, liquid rok, or iron

More information

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University Statc/Dynamc Dormaton wth Fnt Elmnt Mthod Graphcs & Mda Lab Sol Natonal Unvrsty Statc/Dynamc Dormaton Statc dormaton Dynamc dormaton ndormd shap ntrnal + = nrta = trnal dormd shap statc qlbrm dynamc qlbrm

More information

Real-time Clothoid Approximation by Rational Bezier Curves

Real-time Clothoid Approximation by Rational Bezier Curves 008 IEEE Intrnatonal onfrn on Robots and Automaton Pasadna A USA May 9-3 008 Ral-tm lothod Approxmaton by Ratonal Bzr urvs olás Montés Alvaro Hrraz Lopoldo Armsto* and Josp Tornro* *Mmbr IEEE Abstrat-

More information

Lecture 21. Boltzmann Statistics (Ch. 6)

Lecture 21. Boltzmann Statistics (Ch. 6) Lctur. oltzmann tatstcs (Ch. 6) W hav followd th followng logc:. tatstcal tratmnt of solatd systms: multplcty ntropy th nd Law.. hrmodynamc tratmnt of systms n contact wth th hat rsrvor th mnmum fr nrgy

More information

Space-time Clutter Model and Simulation for Space-based Radar

Space-time Clutter Model and Simulation for Space-based Radar Spa-tm Cluttr Modl and Smulaton for Spa-basd Radar Shool of Eltron Engnrng, Unvrsty of Eltron Sn and Thnology of Chna, Chngdu 610054, Chna E-mal:ltang827@yahoo.om Abstrat Th prforman of Spa-Basd Radar

More information