MHD CASSON VISCOUS DISSIPATIVE FLUID FLOW PAST A VERTICALLY INCLINED PLATE IN PRESENCE OF HEAT AND MASS TRANSFER: A FINITE ELEMENT TECHNIQUE

Size: px
Start display at page:

Download "MHD CASSON VISCOUS DISSIPATIVE FLUID FLOW PAST A VERTICALLY INCLINED PLATE IN PRESENCE OF HEAT AND MASS TRANSFER: A FINITE ELEMENT TECHNIQUE"

Transcription

1 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Glbal Dgtal Cntral ISSN: Frntrs n Hat and Mass Transfr Avalabl at.thrmalfludscntral.rg MHD CASSON VISCOUS DISSIPATIVE FLUID FLOW PAST A VERTICALLY INCLINED PLATE IN PRESENCE OF HEAT AND MASS TRANSFER: A FINITE ELEMENT TECHNIQUE R. Srnvasa Rau a,*, G. Jthndr Rdd b, G. Antha a a Dpartmnt f Mathmatcs, GITAM Unvrst, Hdrabad Campus, Rudraram, 5039, Tlangana Stat, Inda b Dpartmnt f Mathmatcs, VNR Vgnana Jth Insttut f Engnrng and Tchnlg, Hdrabad, Ranga Rdd (Dt), , Tlangana Stat, Inda ASTRACT In th prsnt stud, cnsdr an nflunc f chmcal ractn n an unstad MHD fr cnvctv, vscus dsspatv Cassn flud fl vr a vrtcall nclnd plat n prsnc f magntc fld, hat and mass transfr. Th mdlng quatns ar cnvrtd t dmnsnlss quatns, thn slvd thrugh fnt lmnt tchnqu. Cmputatns r prfrmd t analz th bhavr f flud vlct, tmpratur, cncntratn and nducd magntc fld n th nclnd vrtcal plat th th varatn f mrgng phscal paramtrs. Cmpard th prsnt rsults th arlr rprtd studs fr crrctnss and applcablt f fnt lmnt tchnqu. Ths mdl ma b usful n v f lab prmntal rsults fr crrctnss and applcablt and usful t analz th flud bhavr n thrmal ngnrng ndustrs th th nflunc f th thrmal, magntc and chmcal ractn ffcts tc. rds: Magntc Fld, Cassn Flud Fl, Fr Cnvctn, Hat and Mass transfr, Fnt Elmnt Mthd.. INTRODUCTION Nn-Ntnan flud thr s a part f flud mchancs basd n th cntnuum thr that a flud partcl ma b cnsdrd as cntnuus n a structur. On f th nn-ntnan fluds s a Psud plastc tm ndpndnt flud hs bhavur s that Vscst dcrass th ncrasng vlct gradnt.g. bld, plmr slutns, tc. Cassn flud s n f th psudplastc fluds that mans shar thnnng fluds (Cassn, 959). At l shar rats th shar thnnng flud s mr vscus than th Ntnan flud, and at hgh shar rats t s lss vscus. S, MHD fl th Cassn flud s rcntl ll-knn. Harnath Rdd t al. (06) studd th nflunc f radatn absrptn and chmcal ractn n unstad magnthdrdnamc fr cnvctv hat and mass transfr Cassn flud past an scllatng vrtcal plat mbddd n a prus mdum n th prsnc f cnstant all tmpratur and cncntratn fl usng fnt dffrnc mthd. Vnkatsarlu and Sata Naraana (06) studd th cmbnd ffct f Srt and Dufur n MHD fl f a Cassn flud past a strtchng sht n th prsnc f vscus dsspatn, chmcal ractn and varabl thrmal cnductvt usng shtng mthd. Rammhan Rdd t al. (06) fund th analtcal slutns f MHD cnvctv fl f a ncmprssbl, vsclastc, radatv, chmcall ractv, lctrcall cnductng and rtatng flud thrugh a prus mdum flld n a vrtcal channl n th prsnc f thrmal dffusn usng prturbatn tchnqu. hattachara (03) fund th numrcal slutns f stad bundar lar stagnatn-pnt fl f Cassn flud and hat transfr tards a shrnkng/strtchng sht usng vr ffcnt shtng mthd. Mustafa and han (05) nvstgatd magntc fld ffcts n Cassn nanflud vr nnlnarl strtchng sht. Nadm t al. (0) analzd th stad stagnatn pnt fl f a nn-ntnan flud (Cassn mdl) tards a strtchng surfac th hat transfr and Nan partcls. Nadm t al. (03) plrd thr dmnsnal lctrcall cnductng bundar lar fl f Cassn flud vr strtchng sht saturatd n a prus mdum. hald t al. (05) nvstgatd th ffcts f magntc fld n fr cnvctn fl f Cassn flud vr scllatng plat mbddd n prus mdum. Sharadha and Shankar (05) studd bundar lar fl f Cassn flud vr pnntall strtchng sht. In th bundar lar, th nflunc f thrmal radatn s rlvant n man ngnrng prblms bcaus f ts applcatns spcall n hgh tmpratur ngnrng prcsss. Th ffct f hat radatn s mprtant n cntrllng th qualt f th fnal prduct as t affcts th rat clng. Du t th abv fact, sm f th authrs hav studd th ffct f thrmal radatn n thr rks, vz., Pal t al. (03), Mukhpadha t al. (0), Akbar t al. (03), hattachara and hs c-rkrs (03) and (0), Rashd t al. (0), Su t al. (0). Ahmd and Mahd (06) dlbratd th magnthdrdnamc rtatng fl f a lamnar ncmprssbl vscus lctrcall cnductng flud n th stagnatn rgn f an mpulsvl rtatng sphr n th prsnc f thrmal radatn, hat and mass transfr ffcts. Prakash t al. (0) studd th cmbnd ffcts f nducd magntc fld and radatn n MHD hat and mass transfr fl f vscus, ncmprssbl, Ntnan flud vr a prus vrtcal plat n th prsnc f vscus and magntc dsspatn usng prturbatn tchnqu. Rapts t al. (003) studd th ffct f radatn n an ptcall thn gra gas flng past a vrtcal nfnt plat n th prsnc f a magntc fld. Ahmd (00) fund th analtcal slutns f nducd magntc fld th radatng flud vr a prus vrtcal plat usng Prturbatn tchnqu. Thrfr ths rk can b cnsdrd as tnsn f Prakash t al. (0). S Nvlt f ths papr s dscussn f numrcal slutns * Crrspndng authr. Emal: srvass999@gmal.cm

2 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 usng fnt lmnt tchnqu f th unstad natural cnvctv Cassn flud fl past vr an vrtcall nclnd plat n th prsnc f a thrmal radatn, chmcal ractn, magntc and vscus dsspatns th nducd magntc fld. Als, th stud f grd ndpndnc f fnt lmnt tchnqu s dscussd thrugh tabular frm. Th bhavrs f dffrnt prtnnt paramtrs n vlct, nducd magntc fld, tmpratur and cncntratn prfls as ll as Skn-frctn, Rat f hat and mass transfr cffcnts s dscussd n dtal. Fg. Crdnat sstm and phscal cnfguratn. MATHEMATICAL FORMULATION In ths prblm, cnsdr th ffcts f magntc and vscus dsspatn n stad t-dmnsnal magnthdrdnamc md cnvctv Cassn flud fl f a nn-ntnan and vscus ncmprssbl radatv flud vr a vrtcal plat th nducd magntc fld and hat and mass transfr. Th crdnat sstm and th phscal mdl f th prblm ar shn n Fg.. Fr ths prsnt rsarch rk, mad th fllng assumptns: ). In th flud rgn, th plat s takn alng as n vrtcall upard drctn and as s nrmal t t. ). It s assumd that th all s prsrvd at an unvarng tmpratur T and cncntratn C hghr than th ambnt tmpratur T and cncntratn C rspctvl. ). A unfrm magntc fld f strngth s assumd t b appld nrmal t th drctn f fl. v). Th magntc Rnlds numbr f th fl s nt takn t b small and hnc th nducd magntc fld s nt nsgnfcant. v). Th thrmal dffusn and dffusn thrm ffcts ar nglctd du t th cncntratn f th dffusng spcs s assumd t b vr small n cmparsn th th thr chmcal spcs. v). All th flud prprts ar assumd t b cnstant cpt th ffct f th prssur gradnt n th bd frc trm. v). Thr s a frst rdr chmcal ractn btn th dffusng spcs and th flud. v). Snc th fl s assumd t b n th drctn f as, thrfr all th phscal quantts ar functns f spac crdnats n nl. Glbal Dgtal Cntral ISSN: ). Cnsdr vscus dsspatn n th nrg quatn. Th rhlgcal quatn f stat fr th Cauch strss tnsr f Cassn flud (Dash t al. (996)) s rttn as * 0 () p, c quvalntl () p, c c hr s shar strss, 0 s Cassn ld strss, s dnamc * vscst, s shar rat, and s th, th cmpnnt f dfrmatn rat, s th prduct basd n th nn-ntnan flud, c s a crtcal valu f ths prduct, s plastc dnamc vscst f th nn-ntnan flud, p (3) dnt th ld strss f flud. Sm fluds rqur a graduall ncrasng shar strss t mantan a cnstant stran rat and ar calld Rhpctc, n th cas f Cassn flud (Nn-Ntnan) fl hr c p () Substtutng Eq. (3) nt Eq. (), thn, th knmatc vscst can b rttn as (5) Fnall s th Cassn flud paramtr and as, th gvrnng quatns f th Cassn flud mdl ( ) gvn b Eqs. (8)-() bcm th gvrnng quatns f th Ntnan flud mdl ( ). Thn undr usual ussnsq s apprmatn alng th th assumptns cnsdrd t th fl, th fundamntal gvrnng partal dffrntal quatns that llustrat th phscal stuatn ar gvn b Equatn f Cnsrvatn f Elctrc Charg: J 0 hr J J, J, J z (6) Gauss La f Magntsm: H 0 H (a cnstant) (7) Equatn f Cnsrvatn f Mmntum: u u v g T T cs (8) * H g C C cs Equatn f Cnsrvatn f Enrg: T T qr u v C p C p C p (9) H C p Equatn f Cnsrvatn f Magntc Inductn: H H u v (0)

3 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Spcs Dffusn Equatn: C C v D k C C r () subct t th apprprat bundar cndtns (Prakash t al. 0) u 0, v V, T T, C C, H 0 at 0 () u U T T,, C C, H 0 as In cas f an ptcall thn gra gas, th prssn fr lcal radant (Prakash t al. 0) s gvn b q r * a T T (3) It s assumd that th tmpratur dffrncs thn th fl ar suffcntl small and that T ma b prssd as a lnar functn f th tmpratur. Ths s btand b pandng T n a Talr srs abut T and nglctng th hghr rdr trms, thus gt (Prakash t al. 0) 3 T T T 3T () Usng th fllng nn-dmnsnal quantts (5) u V H T T C C u,,,,, U U T T C C g T T g C C M, Gr, Gm, (5) V U V U V C p U Pr, Sc, R, Pr m D and th th hlp f Eqs. (3) and (), th gvrnng Eqs. (8)-() rduc t d u du d M Grcs cs 0 Gc (6) d d d d d Pr EcPr Pr m d d d d d d R 0 du d Pr EcPr d d M Pr m Pr m 0 du d (7) (8) d d Sc rsc 0 (9) d d th asscatd ntal and bundar cndtns u 0,,, 0 at 0 (0) u, 0, 0, 0 as All th smbls ar dfnd n nmnclatur. Th mathmatcal statmnt f th prblm s n cmplt and mbds th slutn f Eqs. (6), (7), (8) and (9) subct t bundar cndtns (0). Fr practcal ngnrng applcatns and th dsgn f chmcal ngnrng sstms, th lcal skn-frctn, Nusslt numbr and Shrd numbr ar mprtant phscal paramtrs fr ths tp f bundar lar fl. Th Skn-frctn at th plat, hch n th nndmnsnal frm s gvn b u C f () U 0 Th rat f hat transfr cffcnt, hch n th nn-dmnsnal frm n trms f th Nusslt numbr s gvn b T Nu T T 0 Nu R 0 Glbal Dgtal Cntral ISSN: () Th rat f mass transfr cffcnt, hch n th nndmnsnal frm n trms f th Shrd numbr, s gvn b C 0 Sh ShR (3) C C 0 3. NUMERICAL SOLUTIONS Y FEM 3.. Fnt Elmnt Mthd (FEM): Th fnt lmnt mthd (FEM) s a numrcal and cmputr basd tchnqu f slvng a vart f practcal ngnrng prblms that ars n dffrnt flds such as, n hat transfr, flud mchancs (Srnvasa Rau t al. 05; hargava and Rana, 0; Shr and Rau, 05, Shr and Rau, 06, Svaah and Rau, 03; Srnvasa Rau t al. 06), chmcal prcssng (Ln and L, 003)), rgd bd dnamcs (Dttmr and Prc, 006), sld mchancs (Hansb and Hansb, 003), and man thr flds. It s rcgnzd b dvlprs and usrs as n f th mst prful numrcal analss tls vr dvsd t analz cmpl prblms f ngnrng. Th sphstcatn f th mthd, ts accurac, smplct, and cmputablt all mak t a dl usd tl n th ngnrng mdlng and dsgn prcss. It has bn appld t a numbr f phscal prblms, hr th gvrnng dffrntal quatns ar slvd b transfrmng thm nt a matr quatn. Th prmar fatur f FEM s ts ablt t dscrb th gmtr r th mda f th prblm bng analzd th grat flblt. Ths s bcaus th dscrtzatn f th dman f th prblm s prfrmd usng hghl flbl unfrm r nn unfrm patchs r lmnts that can asl dscrb cmpl shaps. Th mthd ssntall cnssts, assumng th pcs cntnuus functn fr th slutn and btanng th paramtrs f th functns n a mannr that rducs th rrr n th slutn. An cllnt dscrptn f fnt lmnt frmulatns s avalabl n ath (996) and Rdd (985). Th stps nvlvd n th fnt lmnt analss aras flls Dscrtzatn f th Dman: Th basc cncpt f th FEM s t dvd th dman r rgn f th prblm nt small cnnctd patchs, calld fnt lmnts. Th cllctn f lmnts s calld th fnt lmnt msh. Ths fnt lmnts ar cnnctd n a nn vrlappng mannr, such that th cmpltl cvr th ntr spac f th prblm Gnratn f th Elmnt Equatns: A tpcal lmnt s slatd frm th msh and th varatnal frmulatn f th gvn prblm s cnstructd vr th tpcal lmnt. Ovr an lmnt, an apprmat slutn f th varatnal prblm s suppsd, and b substtutng ths n th sstm, th lmnt quatns ar gnratd. Th lmnt matr, hch s als knn as stffnss matr, s cnstructd b usng th lmnt ntrplatn functns. Ths stps rsult n a matr quatn f th frm u F hch dfns th fnt lmnt mdl f th rgnal quatn Assmbl f th Elmnt Equatns: Th algbrac quatns s btand ar assmbld b mpsng th ntr lmnt cntnut cndtns. Ths lds a larg numbr f algbrac quatns knn as th glbal fnt lmnt mdl, hch gvrns th hl dman. 3

4 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt Impstn f th undar Cndtns: On th assmbld quatns, th Drchlt's and Numann bundar cndtns (0) ar mpsd Slutn f Assmbld Equatns: Th assmbld quatns s btand can b slvd b an f th numrcal tchnqus, naml, Gauss lmnatn mthd, LU dcmpstn mthd, and th fnal matr quatn can b slvd b a drct r ndrct (tratv) mthd. Fr cmputatnal purpss, th crdnat s vard frm 0 t ma = 9, hr ma rprsnts nfnt.., trnal t th mmntum, nrg and cncntratn bundar lars. Th hl dman s dvdd nt a st f 90 ln sgmnts f qual dth 0., ach lmnt bng t-ndd. 3. Varatnal frmulatn: Th varatnal frmulatn asscatd th Eqs. (6)-(9) vr a tpcal t-ndd lnar lmnt, s gvn b d u du d M Grcs d d d d 0 () Gccs d d Prm PrmPr PrmR Pr d d d 0 (5) du d PrmEcPr EcPr d d d du d 3 M Pr m Pr m 0 d (6) d d d d d Sc rsc 0 d (7) d d Whr,, 3, ar arbtrar tst functns and ma b vd as th varatn n u,, and rspctvl. Aftr rducng th rdr f ntgratn and nn-lnart, arrv at th fllng sstm f quatns du d du d M d d d d d cs cs Gr Gc (8) u 0 Pr mpr Pr m Pr mec Pr Ec Pr Pr mpr R u u Pr m 0 d (9) d d3 M 3 d d d Prm 3 d d d d d rsc Prm Sc du d d d d d 0 3 Glbal Dgtal Cntral ISSN: (30) (3) 3.3 Fnt Elmnt frmulatn: Th fnt lmnt mdl ma b btand frm Eqs. (8)-(3) b substtutng fnt lmnt apprmatns f th frm: u,,,, (3) u Wth 3 (,) hr u,, and ar th Vlct, tmpratur, nducd magntc fld and cncntratn rspctvl at th th nd f tpcal th lmnt, and, and ar takn as: ar th shap functns fr ths lmnt and, Th fnt lmnt mdl f th quatns fr s gvn b 3 u M M M M u 3 M M M M M M M M 3 M M M M b b 3 b b mn mn Whr, M, u,,,, u, m, and b, n,, 3,,, (33) th lmnt thus frmd (3) m ar th st f matrcs dfnd as flls: d d, M 3 d, Gr Gc d, ,

5 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 M M M 3 M M M 3 3 M M M 33 3 M M M Pr mpr M M Pr m d, 3 b d, 3 d Pr mprr d, Pr mecpr M M EcPr d, 3 3 b d M Pr m d, d 3 0, d Pr m d, Sc d, rsc d, b, Pr 3 m, b, In n - dmnsnal spac, lnar lmnt, quadratc lmnt, r lmnt f hghr rdr can b takn. Th hl dman s dvdd nt a st f 90 ntrvals f qual lngth 0.. At ach nd functns ar t b valuatd. Hnc aftr assmbl f th lmnts btan a st f 36 quatns hch ar nnlnar. Thrfr, an tratv schm must b utlzd n th slutn. Aftr mpsng th bundar cndtns, a sstm f quatns has bn btand hch s slvd b th Gauss lmnatn mthd hl mantanng an accurac f A cnvrgnc crtrn basd n th rlatv dffrnc btn th currnt and prvus tratns s mpld. Whn ths dffrncs satsf th dsrd accurac, th slutn s assumd t hav bn cnvrgd and tratv prcss s trmnatd. Th Gaussan quadratur s mplmntd fr slvng th ntgratns. Th cd f th algrthm has bn cutd n MATLA runnng n a PC. Ecllnt cnvrgnc as achvd fr all th rsults.. STUDY OF GRID INDEPENDENCE OF FINITE ELEMENT METHOD In gnral, t stud th grd ndpndnc/dpndnc, th msh sz shuld b vard n rdr t chck th slutn at dffrnt msh (grd) Glbal Dgtal Cntral ISSN: szs and gt a rang at hch thr s n varatn n th slutn. Th numrcal valus f vlct (u), Inducd magntc fld (), tmpratur (θ) and cncntratn (ϕ) fr dffrnt valus f msh (grd) sz ar shn n tabl. Frm ths tabl, th authrs bsrvd that, thr s n varatn n th valus f vlct (u), Inducd magntc fld (), tmpratur (θ) and cncntratn (ϕ) fr dffrnt valus f msh (grd) sz. Hnc, t s cncludd that th rsults ar ndpndnt f msh (grd) sz. Tabl-. Th numrcal valus f u,, θ and ϕ fr varatn f msh szs Msh (Grd) Sz = u θ ϕ Msh (Grd) Sz = 0.00 u θ ϕ Msh (Grd) Sz = 0.0 u θ ϕ CODE VALIDATION Fr prgram cd valdatn, th authr cmpard th prsnt numrcal rsults th analtcal rsults f Prakash t al. (0), Rapts t al. (003) and Ahmd (00) n tabls, 3 and rspctvl hch ar avalabl n ltratur. Frm ths tabls, th authr bsrvd that th rsults ar n gd agrmnt th thr stud. Tabl-: Cmparsn btn th prsnt Vlct, Inducd magntc fld and Tmpratur rsults th th rsults f Prakash t al. (0) fr Prm << M. Rsults f Prakash t al. (0) Prsnt numrcal rsults u θ u θ M = 0.5 M = 0.5 R = 0.5 M = 0.5 M = 0.5 R =

6 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Tabl-3: Cmparsn btn th prsnt vlct rsults th th vlct rsults f Prakash t al. (0), Rapts t al. (003) and Ahmd (00) fr Prm = 0. < M = 0.5, Gr = 5.0, γ = 0.0, ψ = 0.0 and Gc = 0.0. Rsults f Rapts t al. (003) Rsults f Prakash t al. (0) Rsults f Ahmd (00) Prsnt vlct rsults R = 0. R = 0. R = 0. R = Glbal Dgtal Cntral ISSN: th vlct, nducd magntc fld, tmpratur and cncntratn prfls can b apprachd t th rlvant fr stram vlct. Th varatn f numrcal valus f thrmal Grashf numbr r Grashf numbr fr hat transfr (Gr) n vlct prfls at th bundar lar s as shn n th Fg.. It s bsrvd that an ncras n Gr lads t ncras n th flud vlct du t nhancmnt n buanc frc. Hr, th pstv valus f Gr crrspnd t clng f th plat. In addtn, t s bsrvd that th vlct ncrass sharpl nar th all as Gr ncrass and thn dcas t th fr stram valu. Tabl-: Cmparsn btn th prsnt Inducd magntc fld rsults th th rsults f Prakash t al. (0), Rapts t al. (003) and Ahmd (00) fr Prm = 0. < M = 0.5, Gr = 5.0, γ = 0.0, ψ = 0.0 and Gc = 0.0. Rsults f Rapts t al. (003) Rsults f Prakash t al. (0) Rsults f Ahmd (00) Prsnt Inducd Magntc fld rsults R = 0. R = 0. R = 0. R = Fg. 3 Influnc f Gc n vlct prfls 6. RESULTS AND DISCUSSION Fg. Influnc f M n vlct prfls Fg. Influnc f Gr n vlct prfls Numrcal slutns f nn-lnar cupld partal dffrntal quatns (6)-(9) undr bundar cndtns (0) ar btand thrugh fnt lmnt Galrkn tchnqu fr flud vlct, tmpratur, cncntratn and nducd magntc fld. Th bhavur f th flud (.., flud vlct, tmpratur, nducd magntc fld and cncntratn) as analzd and als Skn-frctn, Nusslt numbr and Shrd numbr th varus phscal paramtrs at =.0 thrugh th Fgs. ()-(0). In ths stud th bundar cndtn fr s rplacd b ma = 9 s a suffcntl larg valu f, hr Fg. 3 shs th nflunc f Grashf numbr fr mass transfr (Gc) n th vlct prfl at th bundar lar. Th vlct dstrbutn attans a dstnctv mamum valu n th vcnt f th plat and thn dcrass prprl t apprach a fr stram valu. As pctd, th flud vlct ncrass and th pak valu bcms mr dstnctv du t ncras n th buanc frc rprsntd b Gc. Th ffct f th Hartmann numbr (r) Magntc fld paramtr s shn n Fg.. It s bsrvd that th vlct f th flud dcrass th th ncras f th magntc fld paramtr valus. Th dcras n th vlct as th Magntc fld paramtr ncrass s bcaus th prsnc f a magntc fld n an lctrcall cnductng flud ntrducs a frc calld th Lrntz frc, hch acts aganst th fl f th magntc fld s appld n th nrmal drctn, as n th prsnt stud. Ths rsstv frc sls dn th flud vlct cmpnnt. Fgs. 5 and 6 6

7 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Glbal Dgtal Cntral ISSN: sh th bhavur f flud vlct and flud tmpratur rspctvl th an nflunc f Prandtl numbr. Flud vlct and tmpratur dcrass as ncrasng f Prandtl numbr du t nhancmnt f th thrmal cnductvt. Snc Prandtl numbr s th rat f mmntum dffusvt t thrmal cnductvt. Fr small Prandtl numbr, thrmal cnductvt s hgh and mmntum dffusvt s l, bcaus f that flud vscst s l. Thrfr rduc th hat transfr fr small Prandtl numbr. Fg. 7 Influnc f Sc n vlct prfls Fg. 5 Influnc f Pr n vlct prfls Fg. 8 Influnc f Sc n cncntratn prfls Fg. 6 Influnc f Pr n tmpratur prfls Fgurs 7 and 8 sh that, nflunc f Schmdt numbr (Sc) n vlct prfl and tmpratur prfl. It s bsrvd that, Schmdt numbr (Sc) s n th cncntratn and t s cupld n th mmntum quatn. Incrasng f Schmdt numbr (Sc) th mmntum bundar lar thcknss s ncrasng as ll as flud vlct and flud cncntratn s dcrasng n th ntr bundar f th rgn. Th ffct f th vscus dsspatn paramtr.., th Eckrt numbr Ec n th vlct and tmpratur ar shn n Fgs. 9 and 0 rspctvl. Th Eckrt numbr Ec prsss th rlatnshp btn th kntc nrg n th fl and th nthalp. It mbds th cnvrsn f kntc nrg nt ntrnal nrg b rk dn aganst th vscus flud strsss. Gratr vscus dsspatv hat causs a rs n th tmpratur, as ll as th vlct and crss fl vlct. Ths bhavur s vdnt frm Fgs. 9 and 0. 7 Fg. 9 Influnc f Ec n vlct prfls Fgs. and sh th nflunc f magntc Prandtl numbr Prm n th vlct f flud and tmpratur f flud. th flud vlct and tmpratur dcras as ncrasng f magntc Prandtl numbr Prm. Th ffcts f th thrmal radatn paramtr R n th vlct and tmpratur prfls n th bundar lar ar llustratd n

8 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Fgs. 3 and rspctvl. Incrasng th thrmal radatn paramtr prducs sgnfcant ncras n th thrmal cndtn f th flud and ts thrmal bundar lar. Ths ncras n th flud tmpratur nducs mr fl n th bundar lar causng th vlct f th flud thr t ncras. As pctd, th prsnc f th chmcal ractn sgnfcantl affcts th cncntratn prfls as ll as th vlct prfls frm Fgs. 5 and 6. It shuld b mntnd that th studd cas s bth fr dstructv and gnratv chmcal ractn. In fact, as chmcal ractn ncrass, th cnsdrabl rductn n th vlct prfls s prdctd, and th prsnc f th pak ndcats that th mamum valu f th vlct ccurs n th bd f th flud cls t th surfac but nt at th surfac. Als, th an ncras n th chmcal ractn paramtr, th cncntratn dcrass. It s vdnt that th ncras n th chmcal ractn sgnfcantl altrs th cncntratn bundar lar thcknss but ds nt altr th mmntum bundar lars. Glbal Dgtal Cntral ISSN: Fg. 9 fr ak buanc and arfl. Clarl, as Hartmann numbr ncrass, th nducd magntc fld rducs. Th ffct f magntc Prandtl numbr Prm n th nducd magntc fld s prsntd n th Fg. 0. In ths fgur magntc Prandtl numbr Prm s st as lss than unt, hch mpls that th magntc dffusn rat cds th vscus dffusn rat. As such Prm ncrass, mmntum dffusvt ll ncras. Thrfr, Prm ncrass frm 0. t.5, th nducd magntc fld s fund t ncras abslutl n th bundar lar 0 6, but ths trnd s ppst fr th rgn 6 9. Gratr flu rvrsal arss n th bundar lar rgn 0, 6 and fr Prm = 0. (magntc dffusn rat cds th vscus dffusn 6, 9. rat); but ths trnd s rvrsd fr th rgn Fg. Influnc f Prm n tmpratur prfls Fg. 0 Influnc f Ec n tmpratur prfls Fg. Influnc f Prm n vlct prfls Fg. 7 shs th flud vlct th an nflunc f Cassn flud paramtr. Wth an ncrasng Cassn paramtr, th flud vlct dcrass n th ntr bundar rgn. Snc flud vscst ll b hgh th ncras f Cassn paramtr, mmntum bundar lar thcknss dcrass. An nflunc f angl f nclnatn f th plat n th vlct prfl s shn n th Fg. 8. It s bsrvd that flud vlct dcrass th ncrasng nclnatn paramtr (ψ). Th rspns f nducd magntc fld t Hartmann numbr s shn n th 8 Fg. 3 Influnc f R n vlct prfls Tabls 5 and 6 rprsnt th varatns f Ec, R, γ and Prm, r, ψ n skn-frctn cffcnt rspctvl. Th skn-frctn cffcnt s ncrasng th ncrasng valus f Ec and dcrasng th ncrasng valus f R and γ. Th nfluncs f R, Pr and Ec n rat f hat transfr cffcnt r Nusslt numbr ar dscussd n tabl 7 th th hlp f numrcal valus. Th rat f hat transfr cffcnt s ncrasng th ncrasng valus f Ec and th rvrs ffct s bsrvd th ncrasng valus f R and Pr. Th cmbnd nflunc f Sc and r n rat f mass transfr cffcnt r Shrd numbr s dscussd n tabl 8. Frm ths tabl, th authrs bsrvd that th rat f mass transfr cffcnt s dcrasng th ncrasng valus f Sc and r.

9 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Glbal Dgtal Cntral ISSN: Fg. Influnc f R n tmpratur prfls Fg. 6 Influnc f r n cncntratn prfls Fg. 5 Influnc f r n vlct prfls Fg. 7 Influnc f γ n vlct prfls Tabl-5: Skn-frctn valus fr varatn f Ec, R and γ Ec R γ Cf Tabl-6: Skn-frctn valus fr varatn f Prm, r and ψ Prm r ψ Cf Fg. 8 Influnc f ψ n vlct prfls 9

10 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Fg. 9 Influnc f M n nducd magntc fld Glbal Dgtal Cntral ISSN: Th numrcal slutns hav bn dvlpd fr vlct, nducd magntc fld, tmpratur, cncntratn, Skn-frctn, Rat f hat and mass transfr cffcnts. Th faturs f th fl charactrstcs r analzd b plttng graphs and dscussd n dtal. Th nflunc f Grashf numbr fr hat and mass transfr stablzs th mmntum bundar lar grth. Incrasng th valus f Cassn flud paramtr, Hartmann numbr and Angl f nclnatn f th plat rtards th vlct f th fl fld at all pnts. A grng Prandtl numbr dcrass tmpratur f th fl fld at all pnts and ncrass th ncrasng thrmal radatn and vscus dsspatn paramtrs. Inducd Magntc fld dcrass th th ncrasng Hartmann numbr. Magntc Prandtl numbr dpl nflunc n th nducd magntc fld n th thrmal bundar lar.. nducd magntc fld dcrass th th ncras n th Magntc Prandtl numbr. Th cncntratn rducs th rsng f Schmdt numbr. Th vlct as ll as cncntratn rducs th an nlargmnt n th chmcal ractn paramtr. Th numrcal rsults ar btand and cmpard th frmrl rprtd cass avalabl n th pn ltratur and th ar fund t b n vr gd cncurrnc. Th prsnt stud has bn cnfnd t nn-ntnan vscus mdl. Futur nvstgatns ll cnsdr vsclastc and pr-la rhlgcal flud mdls and ll b cmmuncatd n th nar futur. ACNOWLEDGEMENT Authrs ar gratful t th rvrs fr thr valuabl cmmnts and suggstns hch hlpd thm t mprv th qualt f ths rsarch papr. Als th authrs ar thankful t Dr.. Tasan, GITAM Unvrst, Hdrabad campus, fr hr nputs. Fg. 0 Influnc f Prm n nducd magntc fld Tabl-7: Nusslt numbr valus fr varatn f Ec, R and Pr Ec R Pr Nu Tabl-8: Shrd numbr valus fr varatn f Sc and r Sc r Sh CONCLUSIONS Th prsnt stud addrssd th charactrstcs f hat and mass transfr n unstad magnthdrdnamc fr cnvctv Cassn flud fl f an ptcall thck flud vr an nclnd vrtcal plat th magntc and vscus dsspatns. Th st f fundamntal gvrnng quatns hav bn slvd numrcall usng fnt lmnt mthd. 0 C NOMENCLATURE Cncntratn f th flud far aa frm th plat 3 ( g m ) 3 C Cncntratn f th plat ( g m ) Dmnsnlss dsplacmnt ( m ) Gc Grashf numbr fr mass transfr u Nn-dmnsnal flud vlct ( m s ) Sh Th lcal Shrd numbr T Flud tmpratur aa frm th plat v Vlct cmpnnt ( m s ) u Vlct cmpnnt n drctn ( m s ) g Acclratn f gravt, 9.8 ( m s ) a A Cnstant r Chmcal ractn paramtr Crdnat as alng th plat ( m ) C-rdnat as nrmal t th plat ( m ) J Currnt dnst vctr ( A. s. m ) k r Dmnsnal Chmcal ractn paramtr Ec Eckrt numbr (Vscus Dsspatn paramtr) C 3 Flud Cncntratn ( g m ) T Flud Tmpratur ( ) T Flud tmpratur at th all

11 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 Gr Grashf numbr fr hat transfr Inducd Magntc fld (Tsla) H Inducd Magntc fld alng drctn (Tsla) H Inducd Magntc fld alng drctn (Tsla) M Magntc fld paramtr (r) Hartmann numbr Pr m Magntc Prandtl numbr Pr Prandtl numbr q r Radatv hat transfr cffcnt U Rfrnc vlct at th plat ( m s ) R Rnlds numbr J, J, J ) Scalar Cmpnnts f J ( z Sc Schmdt numbr D Slut mass dffusvt ( m s ) C Spcfc hat at cnstant prssur J g p Nu Th lcal Nusslt numbr C Th lcal skn-frctn ( N m ) f 0 Unfrm magntc fld (Tsla) Grk Smbls: Thrmal cnductvt f th flud ( W m ) Nn dmnsnal flud tmpratur Shar strss ( N m ) * Vlumtrc Cffcnt f thrmal pansn th 3 cncntratn ( m g ) Angl f nclnatn f plat ( dg rs ) Cassn flud paramtr Elctrc cnductvt f th flud ( s m ) nmatc vscst ( m s ) Magntc Prmablt ( N. A ) 3 Spcs cncntratn ( g m ) * Stfan ltzmann Cnstant ( W. m. ) 3 Th cnstant dnst ( g m ) Suprscrpts: / Subscrpts: p Vlumtrc cffcnt f thrmal pansn ( ) Dmnsnlss Prprts Fr stram cndtns Plat Cndtns n th all REFERENCES Ahmd, S., 00, "Inducd Magntc Fld th Radatng Flud vr a Prus Vrtcal Plat: Analtcal Stud," J. Navl f Arch. Marn Eng., 7, 6-7. Glbal Dgtal Cntral ISSN: Ahmd, S., and Mahd, A., 06, "Unstad MHD Dubl Dffusv Cnvctn n th Stagnatn Rgn f an Impulsvl Rtatng Sphr n th Prsnc f Thrmal Radatn Effct," J. Taan Inst. Chm. Eng., 58, Akbar, N.S., Nadm, S., Haq, R.U., and han, Z.H., 03, "Radatn Effcts n MHD Stagnatn Pnt Fl f Nanflud Tards a Strtchng Surfac th Cnvctv undar Cndtn," Chn. J. Arnaut., 6, ath,.j., 996, "Fnt Elmnt Prcdurs," Prntc-Hall, N Jrs. hargava, R., and Rana, P., 0, "Fnt Elmnt Slutn t Md Cnvctn n MHD Fl f Mcrplar Flud alng a Mvng Vrtcal Clndr th Varabl Cnductvt," Int. J. Appl. Math. Mch., 7, 9-5. hattachara,., 03, "undar Lar Stagnatn-Pnt Fl f Cassn Flud and Hat Transfr Tards a Shrnkng/Strtchng Sht," Frnt. Hat Mass Transf.,, hattachara,., 03, "MHD Stagnatn-Pnt Fl f Cassn Flud and Hat Transfr vr a Strtchng Sht th Thrmal Radatn," J. Thrmdn., 03, hattachara,., Mukhpadha, S., Lak, G.C., and Pp, I., 0, "Effcts f Thrmal Radatn n Mcrplar Flud Fl and Hat Transfr vr a Prus Shrnkng Sht," Int. J. Hat Mass Transf., 55, Cassn, M., 959, "A Fl Equatn fr Pgmnt-Ol Suspnsns f th Prntng Ink Tp,". In: C. C. Mlls (d.), Rhlg f dsprs sstms, Nrk, Ofrd: Prgamn Chamkha, A.J., and Camll, I., 000, "Effcts f Hat Gnratn/Absrptn and Thrmphrss n Hdrmagntc Fl th Hat and Mass Transfr vr a Flat Surfac," Int. J. Numr. Mthds Hat Flud Fl, 0, Dash, R.., Mhta,.N., and Jaaraman, G., 996, "Cassn Flud Fl n a Pp Flld th a Hmgnus Prus Mdum," Int. J. Eng. Sc., 3, Dttmr, W., and Prc, D., 006, "A Cmputatnal Framrk fr Flud-Rgd d Intractn: Fnt Elmnt Frmulatn and Applcatns," Cmput. Mthds Appl. Mch. Eng., 95, Hansb, A., and Hansb, P., 00, "A Fnt Elmnt Mthd fr th Smulatn f Strng and Wak Dscntnuts n Sld Mchancs," Cmput. Mthds Appl. Mch. Eng., 93, Harnath Rdd, S., Rau, M. C., and shava Rdd, E., 06, "Radatn Absrptn and Chmcal Ractn Effcts n MHD Fl f Hat Gnratng Cassn Flud Past Oscllatng Vrtcal Prus Plat," Frnt. Hat Mass Transf., 7,.

12 Frntrs n Hat and Mass Transfr (FHMT), 8, 7 (07) DOI: /hmt.8.7 hald, A., han, I., han, A., and Shaf, S., 05, "Unstad MHD Fr Cnvctn Fl f Cassn Flud Past vr an Oscllatng Vrtcal Plat Embddd n a Prus Mdum," Eng. Sc. Tchnl. Int. J., 80, Ln, Y-Y., and L, S-P., 003, "Fnt Elmnt Mdlng fr Chmcal Mchancal Plshng Prcss undr Dffrnt ack Prssurs," J. Matr. Prcssng Tchnl., 0, Mukhpadha, S., hattachara,., and Lak, G.C., 0, "Stad undar Lar Fl and Hat Transfr vr a Prus Mvng Plat n Prsnc f Thrmal Radatn," Int. J. Hat Mass Transf., 5, Mustafa, M., and han, J.A., 05, "Mdl fr L f Cassn Nanflud Past a Nnlnarl Strtchng Sht Cnsdrng Magntc Fld Effcts," AIP Adv., 5, Nadm, S., Haq, R.U., Akbar, N.S., and han, Z.H., 03, "MHD Thr-Dmnsnal Cassn Flud Fl Past a Prus Lnarl Strtchng Sht," Alandra Eng. J., 5, Nadm, S., Mhmd, R., and Akbar, N.S., 0, "Oblqu Stagnatn Pnt Fl f a Cassn Nanflud Tards a Strtchng Surfac th Hat Transfr," J. Cmp. Thr. Nansc.,, Pal, D., Mandal, G., and Varavlu,., 03, "MHD Cnvctn- Dsspatn Hat Transfr vr a Nn-Lnar Strtchng and Shrnkng Shts n Nanfluds th Thrmal Radatn," Int. J. Hat Mass Transf., 65, Prakash, J., Vaa umar, A.G., Rush umar,., and Varma, S.V.., 0, "Th Effcts f Inducd Magntc Fld and Radatn n MHD Md Cnvctv Fl vr a Prus Vrtcal Plat n th Prsnc f Vscus and Magntc Dsspatns," Int. Cnfrnc n Adv. Marn, Industral and Mch. Eng., 5-6. Ramamhan Rdd, L., Rau, M. C., Rau, G.S.S., and Rdd, N.A., 06, "Thrmal Dffusn and Rtatnal Effcts n Magnthdrdnamc Md Cnvctn Fl f Hat Absrbng/Gnratng Vsc-Elastc Flud Thrugh a Prus Channl," Frnt. Hat Mass Transf., 7, 0. Rapts, A.A., Prdks, C., and Lnttss, A., 003, "Effcts f Radatn n an Optcall Thn Gra Gas Flng Past a Vrtcal Infnt Plat n th Prsnc f a Magntc Fld," Hat Mass Transf., 39, Rashd, M.M., Al, M., Frdnmhr, N., Rstam,., and Hssan, M.A., 0, "Md Cnvctv Hat Transfr fr MHD Vsclastc Glbal Dgtal Cntral ISSN: Flud Fl vr a Prus Wdg th Thrmal Radatn," Adv. Mch. Eng., Rdd, J.N., 985, "An Intrductn t th Fnt Elmnt Mthd," McGra - Hll, N Yrk. Sharada,., and Shankar,., 05, "MHD Md Cnvctn Fl f a Cassn Flud vr an Epnntall Strtchng Surfac th th Effcts f Srt, Dufur, Thrmal Radatn and Chmcal Ractn," Wrld J. Mch., 5, Sva Rdd Shr, and Srnvasa Rau, R., 05, "Srt Effct n Unstad MHD Fr Cnvctv Fl Past a Sm-Infnt Vrtcal Plat n th Prsnc f Vscus Dsspatn," Int. J. Cmput. Mthds Eng. Sc. Mch., 6, Sva Rdd Shr, and Srnvasa Rau, R., 06, "Transnt MHD Fr Cnvctv Fl Past an Infnt Vrtcal Plat Embddd n a Prus Mdum th Vscus Dsspatn," Mccanca, 5, Svaah, S., and Srnvasa Rau, R., 03, "Fnt Elmnt Slutn f Hat and Mass Transfr Fl th Hall Currnt, Hat Surc and Vscus Dsspatn," Appl. Math. Mch. Englsh Edtn, 3, Srnvasa Rau, R., Jthndr Rdd, G., Anand Ra, J., Rashd, M.M., and Grla, R.S.R., 06, "Analtcal and Numrcal Stud f Unstad MHD Fr Cnvctn Fl vr an Epnntall Mvng Vrtcal Plat th Hat Absrptn," Int. J. Thrmal Sc., 07, Srnvasa Rau, R., Mahsh Rdd,., Rashd, M.M., and Grla, R.S.R., 06, "Applcatn f Fnt Elmnt Mthd t Unstad MHD Fr Cnvctn Fl Past a Vrtcall Inclnd Prus Plat Includng Thrmal Dffusn and Dffusn Thrm Effcts," J. Prus Mda, 9, Su, X., Zhng, L., Zhang, X., and Zhang, J., 0, "MHD Md Cnvctv Hat Transfr vr a Prmabl Strtchng Wdg th Thrmal Radatn and Ohmc Hatng," Chm. Eng. Sc., 78, Vnkatsarlu,., and Sata Naraana, P.V., 06, "Influnc f Varabl Thrmal Cnductvt n MHD Cassn Flud Fl vr a Strtchng Sht th Vscus Dsspatn, Srt and Dufur Effcts," Frnt. Hat Mass Transf., 7, 6. Zuc, J., ég, O.A., Takhar, H.S., and Prasad, V.R., 009, "Thrmphrtc Hdrmagntc Dsspatv Hat and Mass Transfr th Latral Mass Flu, Hat Surc, Ohmc Hatng and Thrmal Cnductvt Effcts: Ntrk Smulatn Numrcal Stud," Appl. Thrmal Eng., 9,

: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

Magnetohydrodynamic Stability of Self-Gravitating Fluid Layer Embedded into Different Fluid

Magnetohydrodynamic Stability of Self-Gravitating Fluid Layer Embedded into Different Fluid Australan Jurnal f Basc and Appld Scncs, 3(4): 46-466, 009 ISSN 99-878 Magnthydrdynamc Stablty f Slf-Gravtatng Flud Layr Embddd nt Dffrnt Flud Ahmd E. Radwan and AbdlTawab A.A. Shalaby Dpartmnt f Mathmatcs,

More information

9.5 Complex variables

9.5 Complex variables 9.5 Cmpl varabls. Cnsdr th funtn u v f( ) whr ( ) ( ), f( ), fr ths funtn tw statmnts ar as fllws: Statmnt : f( ) satsf Cauh mann quatn at th rgn. Statmnt : f ( ) ds nt st Th rrt statmnt ar (A) nl (B)

More information

Math 656 Midterm Examination March 27, 2015 Prof. Victor Matveev

Math 656 Midterm Examination March 27, 2015 Prof. Victor Matveev Math 656 Mdtrm Examnatn March 7, 05 Prf. Vctr Matvv ) (4pts) Fnd all vals f n plar r artsan frm, and plt thm as pnts n th cmplx plan: (a) Snc n-th rt has xactly n vals, thr wll b xactly =6 vals, lyng n

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

Computer graphics III Rendering equation and its solution. Jaroslav Křivánek, MFF UK

Computer graphics III Rendering equation and its solution. Jaroslav Křivánek, MFF UK Cmputr graphcs III Rndrng quatn and ts slutn Jarslav Křvánk MFF UK Jarslav.Krvank@mff.cun.cz Glbal llumnatn GI Drct llumnatn 2 Rvw: Rflctn quatn Sum ntgral f cntrbutns vr th hmsphr: r d cs H f r d n r

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

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

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY

Study of Dynamic Aperture for PETRA III Ring K. Balewski, W. Brefeld, W. Decking, Y. Li DESY Stud of Dnamc Aprtur for PETRA III Rng K. Balws, W. Brfld, W. Dcng, Y. L DESY FLS6 Hamburg PETRA III Yong-Jun L t al. Ovrvw Introducton Dnamcs of dampng wgglrs hoc of machn tuns, and optmzaton of stupol

More information

Equivalent Voice-coil Models for Real-time Computation in Electromagnetic Actuation and Sensor Applications

Equivalent Voice-coil Models for Real-time Computation in Electromagnetic Actuation and Sensor Applications Equvalnt Vc-cl Mdls fr Ral-tm Cmputatn n Elctrmagntc Actuatn and nsr Applcatns Kk-Mng L*, Fllw, IEEE and Hungsun n Abstract Ths papr prsnts a mthd t drv quvalnt mdls t charactrz th magntc fld f a mult-layr

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

Analytical Modeling and Equivalent Electromechanical Loading Techniques for Adaptive Laminated Piezoelectric Structures

Analytical Modeling and Equivalent Electromechanical Loading Techniques for Adaptive Laminated Piezoelectric Structures Analtcal Mdlng and Eqvalnt Elctrmchancal Ladng Tchnqs fr Adaptv Lamnatd Plctrc Strctrs b Clatn L. Smth Thss sbmttd t th faclt f th Vrgna Pltchnc Insttt and Stat Unvrst n partal flfllmnt f th rqrmnts fr

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

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

Variational Approach in FEM Part II

Variational Approach in FEM Part II COIUUM & FIIE ELEME MEHOD aratonal Approach n FEM Part II Prof. Song Jn Par Mchancal Engnrng, POSECH Fnt Elmnt Mthod vs. Ralgh-Rtz Mthod On wants to obtan an appromat solton to mnmz a fnctonal. On of th

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

On the Hydrodynamic Long Journal Bearing Theory

On the Hydrodynamic Long Journal Bearing Theory Prcdngs f th Wrld Cngrss n Engnrng Vl II, WCE, July -,, Lndn, U.K. On th Hydrdynamc Lng Jurnal Barng Thry Marc Tul C. Fara Abstract Ths wrk dals wth th dvlmnt f a fnt lmnt rcdur fr th stady-stat and dynamc

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

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

Finite Element Solution of MHD Transient Flow past an Impulsively Started Infinite Horizontal Porous Plate in a Rotating Fluid with Hall Current

Finite Element Solution of MHD Transient Flow past an Impulsively Started Infinite Horizontal Porous Plate in a Rotating Fluid with Hall Current Jurnal f Appled Flud Mechancs, Vl. 5,. 3, pp. 105-11, 01. Avalable nlne at www.afmnlne.net, ISS 1735-357, EISS 1735-3645. Fnte Element Slutn f MHD Transent Flw past an Impulsvel Started Infnte Hrzntal

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

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

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

Adsorption. (CHE 512) M.P. Dudukovic Chemical Reaction Engineering Laboratory (CREL), Washington University, St. Louis, MO

Adsorption. (CHE 512) M.P. Dudukovic Chemical Reaction Engineering Laboratory (CREL), Washington University, St. Louis, MO dsrptn (CHE 5) M.P. Dudukvc Chmcal Ractn Engnrng Labratry (CREL), Washngtn Unvrsty, St. Lus, MO bruary 8, 005 ChE 5 CHPTER 3 DSORPTION BSIC NOTION dsrptn s a prcss by whch a chmcal cmpnnt (spcs) frm a

More information

Large Deformation Behaviour of Continuum Compliant Systems

Large Deformation Behaviour of Continuum Compliant Systems Intrnatnal Jurnal f Engnrng and chnlgy Vlum 3 N. 2, Fbruary, 2013 Larg Dfrmatn Bhavur f Cntnuum Cmplant Systms hddus. Akan, Omtay A. Faknld Dpartmnt f Systms Engnrng, Unvrsty f Lags, Akka, Lags. Ngra ABSRAC

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

TOPOLOGY OPTIMIZATION UNDER THERMO-ELASTIC BUCKLING

TOPOLOGY OPTIMIZATION UNDER THERMO-ELASTIC BUCKLING OPOLOGY OPIMIZAION UNDER HERMO-ELASIC BUCKLING Shguang Dng, Graduat Studnt Krshnan Sursh, Prfssr, ksursh@wsc.du Mchancal Engnrng, Unvrsty f Wscnsn, Madsn, USA ABSRAC * h fcus f s papr s n tplgy ptmzatn

More information

Analyzing Frequencies

Analyzing Frequencies Frquncy (# ndvduals) Frquncy (# ndvduals) /3/16 H o : No dffrnc n obsrvd sz frquncs and that prdctd by growth modl How would you analyz ths data? 15 Obsrvd Numbr 15 Expctd Numbr from growth modl 1 1 5

More information

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

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

More information

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

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

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM Avalabl onln at www.scncdrct.com Procda Engnrng 9 () 373 377 Intrnatonal Workshop on Informaton and Elctroncs Engnrng (IWIEE) Thr-Nod Eulr-Brnoull Bam Elmnt Basd on Postonal FEM Lu Jan a *,b, Zhou Shnj

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

Supplementary. Mode division multiplexing using an orbital angular momentum mode. sorter and MIMO-DSP over a graded-index few-mode optical fibre

Supplementary. Mode division multiplexing using an orbital angular momentum mode. sorter and MIMO-DSP over a graded-index few-mode optical fibre Supplntary Md dvsn ultplxng usng an rbtal angular ntu d srtr and MIMO-DSP vr a gradd-ndx fw-d ptcal fbr Ha Huang 1,*, Gvann Mln 2,3,4,5,*, Martn P. J. Lavry 6,*, Gudng X 1, Yngxng Rn 1, Ynwn Ca 1, Nsar

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

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

LECTURE 5 Guassian Wave Packet

LECTURE 5 Guassian Wave Packet LECTURE 5 Guassian Wav Pact 1.5 Eampl f a guassian shap fr dscribing a wav pact Elctrn Pact ψ Guassian Assumptin Apprimatin ψ As w hav sn in QM th wav functin is ftn rprsntd as a Furir transfrm r sris.

More information

ECE542, Fall 2004 Homework 7 Solutions

ECE542, Fall 2004 Homework 7 Solutions EECE54: Dgtal Cmmuncatns Thry Prf. M. Hayat ECE54, Fall 004 Hmwrk 7 Slutns Prblm. Unn Bund: Ρ Ρ annunc, 0 { snt} dy Q But Ρ{ annunc snt} f ( y ( (Assum ( If

More information

Influence of Fiber Orientation on the Natural Frequencies of Laminated Composite Beams

Influence of Fiber Orientation on the Natural Frequencies of Laminated Composite Beams Intrnatonal Journal of Engnrng Rsarch And Advancd Tchnology (IJERAT) DOI: http://d.do.org/.74/ijerat.7.5 E-ISS : 454-65 Vol. (9) Sp -7 Influnc of Fbr Orntaton on th atural Fruncs of Lamnatd Compost Bams

More information

Transient Conduction: Spatial Effects and the Role of Analytical Solutions

Transient Conduction: Spatial Effects and the Role of Analytical Solutions Transent Cnductn: Spatal Effects and the Rle f Analytcal Slutns Slutn t the Heat Equatn fr a Plane Wall wth Symmetrcal Cnvectn Cndtns If the lumped capactance apprxmatn can nt be made, cnsderatn must be

More information

Role of Viscosity Ratio in Liquid-Liquid Jets under Radial Electric Field

Role of Viscosity Ratio in Liquid-Liquid Jets under Radial Electric Field Intrnatnal Jurnal f Chmcal and Blgcal Engnrng 6 01 Rl f Vscsty Rat n Lqud-Lqud Jts undr Radal Elctrc Fld Sddharth Gadkar and Rchsh Thakar Abstract Th ffct f vscsty rat (λ, dfnd as vscsty f surrundng mdum/vscsty

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

EFFECTS OF INCLINED CUTOFFS AND SOIL FOUNDATION CHARACTERISTICS ON SEEPAGE BENEATH HYDRAULIC STRUCTURES

EFFECTS OF INCLINED CUTOFFS AND SOIL FOUNDATION CHARACTERISTICS ON SEEPAGE BENEATH HYDRAULIC STRUCTURES Twlft Intrnatonal Watr Tcnology Confrnc, IWTC2 28, Alandra, Egypt 597 EFFECTS OF INCLINED CUTOFFS AND SOIL FOUNDATION CHARACTERISTICS ON SEEPAGE BENEATH HYDRAULIC STRUCTURES Kald Fadl Alsnous and Hasan

More information

CONNECTIVITY OF FRACTURE NETWORKS: THE EFFECTS OF ANISOTROPY AND SPATIAL CORRELATION ABSTRACT 1. INTRODUCTION

CONNECTIVITY OF FRACTURE NETWORKS: THE EFFECTS OF ANISOTROPY AND SPATIAL CORRELATION ABSTRACT 1. INTRODUCTION CONNECTIVITY OF FRACTURE NETWORKS: THE EFFECTS OF ANISOTROPY AND SPATIAL CORRELATION MOHSEN MASIHI 1, P. R. KING 1, P. R. NURAFZA 1 1 Dpartmnt f Earth Scnc & Engnrng, Impral Cllg, Ehbtn Rad, Lndn, SW7

More information

CHAPTER-2 MIXED CONVECTION FLOW OF MICROPOLAR FLUID OVER A POROUS SHRINKING SHEET WITH THERMAL RADIATION 2.1 INTRODUCTION

CHAPTER-2 MIXED CONVECTION FLOW OF MICROPOLAR FLUID OVER A POROUS SHRINKING SHEET WITH THERMAL RADIATION 2.1 INTRODUCTION CHAPTER- MIXED CONVECTION FLOW OF MICROPOLAR FLUID OVER A POROUS SHRINING SHEET WITH THERMAL RADIATION. INTRODUCTION Bounary layr flow of ncomprssbl flu ovr a shrnkng sht has attract th ntrst of many rsarchrs

More information

Lecture 26: Quadrature (90º) Hybrid.

Lecture 26: Quadrature (90º) Hybrid. Whits, EE 48/58 Lctur 26 Pag f Lctur 26: Quadratur (9º) Hybrid. Back in Lctur 23, w bgan ur discussin f dividrs and cuplrs by cnsidring imprtant gnral prprtis f thrand fur-prt ntwrks. This was fllwd by

More information

Finite element discretization of Laplace and Poisson equations

Finite element discretization of Laplace and Poisson equations Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization

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

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016

Self-Adjointness and Its Relationship to Quantum Mechanics. Ronald I. Frank 2016 Ronald I. Frank 06 Adjoint https://n.wikipdia.org/wiki/adjoint In gnral thr is an oprator and a procss that dfin its adjoint *. It is thn slf-adjoint if *. Innr product spac https://n.wikipdia.org/wiki/innr_product_spac

More information

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS Cênca/Scnc APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF D DIFFUSION IN SOLIDS E C Romão a, M D d Campos c, J A Martns b, and L F M d Moura a Unvrsdad Estadual d Campnas Faculdad d Engnhara

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

15. Stress-Strain behavior of soils

15. Stress-Strain behavior of soils 15. Strss-Strain bhavior of soils Sand bhavior Usually shard undr draind conditions (rlativly high prmability mans xcss por prssurs ar not gnratd). Paramtrs govrning sand bhaviour is: Rlativ dnsity Effctiv

More information

Chapter 3, Solution 1C.

Chapter 3, Solution 1C. COSMOS: Cmplete Onlne Slutns Manual Organzatn System Chapter 3, Slutn C. (a If the lateral surfaces f the rd are nsulated, the heat transfer surface area f the cylndrcal rd s the bttm r the tp surface

More information

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

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

More information

University of Tripoli / Tripoli - Libya. ** Centre for Solar Energy Research and Studies / Tripoli-Libya

University of Tripoli / Tripoli - Libya. ** Centre for Solar Energy Research and Studies / Tripoli-Libya Analyss and Smulatn f ntrlavd Bst Cnvrtr fr Autmtv Applcatns Farag. S. Alargt **, Ahmd. S. Ashur * * Dpartmnt f Elctrcal and Elctrnc Engnrng Unvrsty f Trpl / Trpl - bya. ** Cntr fr Slar Enrgy Rsarch and

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

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

Finite Element Models for Steady Flows of Viscous Incompressible Fluids

Finite Element Models for Steady Flows of Viscous Incompressible Fluids Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod

More information

Inter-Ing INTERDISCIPLINARITY IN ENGINEERING SCIENTIFIC INTERNATIONAL CONFERENCE, TG. MUREŞ ROMÂNIA, November 2007.

Inter-Ing INTERDISCIPLINARITY IN ENGINEERING SCIENTIFIC INTERNATIONAL CONFERENCE, TG. MUREŞ ROMÂNIA, November 2007. Intr-Ing 2007 INERDISCIPLINARIY IN ENGINEERING SCIENIFIC INERNAIONAL CONFERENCE, G. MUREŞ ROMÂNIA, 15-16 Nvmbr 2007. EXERGEIC ANALYSIS HE OPIMIZAION WAY OF HE POWER SEAM GENERAORS OPERAING WIH COAL PULVERIZAION

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

SCRIBE: JAKE LEVINSON

SCRIBE: JAKE LEVINSON GL n REPRESENTATION THEORY NOTES FOR 12-03 SCRIBE: JAKE LEVINSON As th th last lctur, ths on s basd on John Stmbrdg s papr: A local charactrzaton of smpl-lacd crstals, Trans. Amr. Math. Soc. 355 (2003),

More information

OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS

OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS Th Svnth East Asa-Pacfc Confrnc on Structural Engnrng & Constructon August 27-29, 1999, Koch, Japan OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS Qng Quan

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

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

10.5 Linear Viscoelasticity and the Laplace Transform

10.5 Linear Viscoelasticity and the Laplace Transform Scn.5.5 Lnar Vclacy and h Lalac ranfrm h Lalac ranfrm vry uful n cnrucng and analyng lnar vclac mdl..5. h Lalac ranfrm h frmula fr h Lalac ranfrm f h drvav f a funcn : L f f L f f f f f c..5. whr h ranfrm

More information

Group Codes Define Over Dihedral Groups of Small Order

Group Codes Define Over Dihedral Groups of Small Order Malaysan Journal of Mathmatcal Scncs 7(S): 0- (0) Spcal Issu: Th rd Intrnatonal Confrnc on Cryptology & Computr Scurty 0 (CRYPTOLOGY0) MALAYSIA JOURAL OF MATHEMATICAL SCIECES Journal hompag: http://nspm.upm.du.my/ournal

More information

ISSN (ONLINE): , ISSN (PRINT):

ISSN (ONLINE): , ISSN (PRINT): lm-7 Iss-4 Jl-Ags 7 Inrnanal Jrnal f Engnrng and Managmn Rsarch Pag Nmbr: 7-43 havr f assn Fld Sl Fl Pas a rcall Inclnd Pla Flld n Prs Mdm Sbmd n Magnc Fld: Ha Absrn and hmcal Racn Effcs P. Srsh M.. Ramana

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

Numerical Simulation of the Buckley-Leverett Problem

Numerical Simulation of the Buckley-Leverett Problem Prc. Schl. Eng. Ta Ta Unv., Unv., Sr. ESr. E 38 (13) - (13) 9-14 by bdullah Z *1 and Shg HONM * (cvd n Mar. 3, 13 and acctd n May 16, 13) bstract Th dslacnt f l by atr n a trlu rsrvr s analyzd va th faus

More information

Introduction to logistic regression

Introduction to logistic regression Itroducto to logstc rgrsso Gv: datast D { 2 2... } whr s a k-dmsoal vctor of ral-valud faturs or attrbuts ad s a bar class labl or targt. hus w ca sa that R k ad {0 }. For ampl f k 4 a datast of 3 data

More information

Conduction Heat Transfer

Conduction Heat Transfer Cnductn Heat Transfer Practce prblems A steel ppe f cnductvty 5 W/m-K has nsde and utsde surface temperature f C and 6 C respectvely Fnd the heat flw rate per unt ppe length and flux per unt nsde and per

More information

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles

In this lecture... Subsonic and supersonic nozzles Working of these nozzles Performance parameters for nozzles Lct-30 Lct-30 In this lctur... Subsonic and suprsonic nozzls Working of ths nozzls rformanc paramtrs for nozzls rof. Bhaskar Roy, rof. A M radp, Dpartmnt of Arospac, II Bombay Lct-30 Variation of fluid

More information

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune

Chapter 7. Systems 7.1 INTRODUCTION 7.2 MATHEMATICAL MODELING OF LIQUID LEVEL SYSTEMS. Steady State Flow. A. Bazoune Chapter 7 Flud Systems and Thermal Systems 7.1 INTODUCTION A. Bazune A flud system uses ne r mre fluds t acheve ts purpse. Dampers and shck absrbers are eamples f flud systems because they depend n the

More information

Microwave Noise and LNA Design

Microwave Noise and LNA Design Mcrwav and LA Dgn Mcrwav Crcut,6, JJEOG Outln Bac cncpt : thrmal n Equvalnt n tmpratur, n fgur maurmnt f pav ntwrk Rcvr dgn f trantr hry Maurmnt LA dgn bac LA dgn xampl Mcrwav Crcut,6, JJEOG Bac 3 Mcrwav

More information

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved.

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved. Journal o Thortcal and Appld Inormaton Tchnology th January 3. Vol. 47 No. 5-3 JATIT & LLS. All rghts rsrvd. ISSN: 99-8645 www.att.org E-ISSN: 87-395 RESEARCH ON PROPERTIES OF E-PARTIAL DERIVATIVE OF LOGIC

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

element k Using FEM to Solve Truss Problems

element k Using FEM to Solve Truss Problems sng EM t Slve Truss Prblems A truss s an engneerng structure cmpsed straght members, a certan materal, that are tpcall pn-ned at ther ends. Such members are als called tw-rce members snce the can nl transmt

More information

Reducing the Impact of Uplift Pressures on the Base of a Concrete. Dam by Configuration of Drainage Holes (Hypothetical Case Study)

Reducing the Impact of Uplift Pressures on the Base of a Concrete. Dam by Configuration of Drainage Holes (Hypothetical Case Study) Cvl and Envronmntal Rsarc ISS 4-5790 (Papr) ISS 5-054 (Onln) Vol.6, o., 04 www.st.org Rducng t Impact of Uplft Prssurs on t Bas of a Concrt Dam b Confguraton of Dranag ols (pottcal Cas Stud) Imad. Obad

More information

N J of oscillators in the three lowest quantum

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

More information

Lecture 27: The 180º Hybrid.

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

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

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

Mullins Effect and Thixotropy

Mullins Effect and Thixotropy Mullns Effct and Thxotropy Engnrng Strss (MPa) 006 NNF Summr Radng Srs August 9, 006 Artcls λ (= L/L o ) Shawna M. Lff Insttut for Soldr Nanotchnologs Dpartmnt of Mchancal Engnrng MIT, Cambrdg, MA 039

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك

FEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D

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

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Snsrs and Actuatrs Intrductin t snsrs Sandr Stuijk (s.stuijk@tu.nl) Dpartmnt f Elctrical Enginring Elctrnic Systms APAITIVE IUITS (haptr., 7., 9., 0.6,.,.) apaciti snsr capacitanc dpnds n physical prprtis

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

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

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

More information

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom Mdrn Physics Unit 5: Schrödingr s Equatin and th Hydrgn Atm Lctur 5.6: Enrgy Eignvalus f Schrödingr s Equatin fr th Hydrgn Atm Rn Rifnbrgr Prfssr f Physics Purdu Univrsity 1 Th allwd nrgis E cm frm th

More information

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

A C 1 Beam Element Based on Overhauser Interpolation

A C 1 Beam Element Based on Overhauser Interpolation 9 A C Bam Elmnt Basd on Ovrhausr Intrpolaton Abstract A nw C lmnt s proposd to modl Eulr-Brnoull bams n on and two-dmnsonal problms. Th proposd formulaton assurs C contnuty rqurmnt wthout th us of rotatonal

More information

14. MODELING OF THIN-WALLED SHELLS AND PLATES. INTRODUCTION TO THE THEORY OF SHELL FINITE ELEMENT MODELS

14. MODELING OF THIN-WALLED SHELLS AND PLATES. INTRODUCTION TO THE THEORY OF SHELL FINITE ELEMENT MODELS 4. ODELING OF IN-WALLED SELLS AND PLAES. INRODUCION O E EORY OF SELL FINIE ELEEN ODELS Srő: Dr. András Skréns Dr. András Skréns BE odlng of thn-walld shlls and plats. Introducton to th thor of shll fnt

More information

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer.

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer. R A T T L E R S S L U G S NAME: ANSWER KEY DATE: PERIOD PREAP PHYSICS REIEW TWO KINEMATICS / GRAPHING FORM A DIRECTIONS: MULTIPLE CHOICE. Chs h r f h rr answr. Us h fgur bw answr qusns 1 and 2. 0 10 20

More information

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS Journal of Appl Mathatcs an Coputatonal Mchancs, (), 9- FREE VIBRATION ANAYSIS OF FNCTIONAY GRADED BEAMS Stansław Kukla, Jowta Rychlwska Insttut of Mathatcs, Czstochowa nvrsty of Tchnology Czstochowa,

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

Chapter 2 Linear Waveshaping: High-pass Circuits

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

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

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