Velocity of Blood flow through uniform rigid artery of human body
|
|
- Susan Young
- 6 years ago
- Views:
Transcription
1 IOS Joual of athmatics (IOS-J) -ISSN: ISSN: X. Volum 3 Issu 3 V. IV (ay - Ju 7) PP Vlocity of loo flow though uifom igi aty of huma boy D.Amajyoti Goswami* Safa Ahm* D.Kisha Goal Sigha# *Kaiaga ivaity Assam Iia #Kaaga Gils H.S.S. Assam Iia. Abstact: A attmt is ma i this aalysis to stuy th flow of bloo though a uifom igi aty with a axial vlocity sli coitio at vssl wall has b cosi by assumig bloo a ow flui. It has b obsv that th ffct of th Hatma umb a th yols umb o th vlocity fil as wll as o th wall sha stss is vy omit a wh th Hatma umb a yols umb icass th flui vlocity cass. It also iclus Poisuill flui mols of bloo fo both sli a o-sli at a wall a olay ow flui mol a o sli at tub wall as its scial cass. Th ol of sli i iflucig th flow vaiabls a hysiological imlicatios of this thotical molig a iscuss i bif. Kywos: Pow flui mol stos vssls agtic ffct yols umb Hatma umb loo flow. I. Itouctio Huma bloo is a sussio of clls i a cotiuous a aquous substac call lasma (oy [5]).Plasma bhavs as Nwtoia flui whas whol bloo shows o-nwtoia chaactistic (Fug [9]) cdoal [3] has oit out that i a cas of bloo vssls with iamt abov 5 micomts bloo may b cosi as a Nwtoia flui.stosis is fom by substac ositig o vssl walls. Stosis is fom by substac ositig o vssl walls. A stosis may la to atial o total vssl blockag i som istacs a thfo oss a sious mical oblm. I a huma boy hysiological fluis st i huma systms iclu igstiv juics swatig bloo saliva ui tc. Amog th boy fluis th most imotat is obviously bloo which is ga as a sussio of ifft clls i a cotiuous aquous solutio call lasma (oy [5]). Plasma bhavs as Nwtoia flui whas whol bloo shows o- Nwtoia chaactistics (Fug [9]) cdoal [3] has oit out. ut at low sha ats bloo xhibits o- Nwtoia bhavio.it is wll kow that o-nwtoia atu of bloo sigificatly iflucs th flows aticulaly i th cass wh bloo vssls a cuv bachig o aow tc a xlai by.ustafa.ahma Kha[4].ustafa T.HayatI.Po a A. Ai also stui ustay bouay lay flow of a casso flui u to a imulsiv stat movig flat lat[]. Futh bloo has a fiit yil stss a asso s quatio ca tak ca of this oty which has b ot by may ivstigatos (oklt t al. [8] il t al. [5] huya. a Haaika []). Owig to th itmittt umig of hat muscls it oucs a ssu gait a as a cosquc bloo flows though th ciculatoy systms (Su V.K [7] atho V.P [8]). Atial systm is also subjct to cotiuous sha stss chags. O of th ciculatoy isass is athosclosis which has u to lii o lim osits (athoma) o th i coat of th atis. About 75% of all aths i th iustiali wol a caus u to ciculatoy isas. Th accumulatio of lii fat a oth aticls alog th isi aty wall la to aowig of th vssl. I som cass it is obsv that a so-call stosis of th vssl with ag that mas lastic fibs i vssl wall a lac by mo igi collag fibs a this ocss is accomai by th wiig of th atial lum (alik []). Also th isas aas of bloo vssls a chaacti by ahsivss haig loss of lasticity a cotactio i th coss-sctio fou omiatly i th viciity of bas bifucatios a oth lacs. As a cosquc th may ais sious comlicatios a isos i bloo suly u to aowig i th bo of th vssls o wiig of th i wall. To sto omal bloo suly i isas vssls it sms is a itouctio of vlocity sli at tub wall will b maigful (Nuba [6] u [7] iswas a Nath [6]). I o to stuy th hology of bloo alog with its ol i th fuamtal ustaig of may caiovascula isass lik myocaial ifactio stok thombosis sickl cll isass tc. I thi mols flow has b cosi stay o ulsatil flui as a Nwtoia o a th bouay coitio o o-sli at wall tc. As bloo shows som viatios fom Nwtoia bhavio it sms cosiatio of bloo i bhavig lik a o-nwtoia flui alog with sli at vssl wall tc as is o h will b aoiat a sigificat fom th hysiological oit of viw. Th alicatio of magto hyoyamics icils i mici giig is of gowig itst.e.ali[]. ay ivstigatios hav b ma o bloo flow u th ffct of magtic fil. aothy [] has show that by th alicatio of a xtal magtic fil th biological systms a gatly affct. Vaaya [9] show DOI:.979/ Pag
2 Vlocity of loo flow though uifom igi aty of huma boy DOI:.979/ Pag that th alicatio of magtic fil ucs th flow of bloo. huya a Haaika [] hav ivstigat th oblm of bloo flow with ffcts of sli i atial stosis u to sc of tasvs magtic fil a thy hav also obsv that th ali magtic fil ucs th vlocity of bloo though atis. athmatical Fomulatio Of Th Poblm A two-flui mol fo bloo flow i a uifom tub has b vlo i th st oblm. Th mol basically cosists of a co of a cll sussio i th mil lay a th ihal lasma i th out lay. Th stay lamia flow of a icomssibl flui assumig it to bhav as a ow flui (Fug [9] huya. Haaika [][3][4]) though a igi cicula tub is cosi. Th axial cooiat a vlocity a ẑ a v sctivly. is th ali magtic fil i ictio. Flow is gov by th cotiuity a Navi-Stoks quatios a i aitio ow costitutiv quatio th magtic fil ali i a ictio th quatios i th axial a aial ictios i imsiolss fom. Fom th ot of Youg [] a Su [7] cosiig th axisymmtic lamia stay flow of bloo th gal costitutiv quatio i th cas of mil stosis subjct to th aitio may thfo b witt as: () u () Fom which w obsv that ssu os ot vay i th aial ( cicumftial ( ) a axial ictio a that ssu mai costat acoss ay coss-sctio of th tub a Is a fuctio of th oly that is a so ssu gait tm i th last quatio abov bcoms Th () v (3) No-imsioal fom V P P v (4) SOLVING THE EQATION (4): k v v Wh K Solutio: Lt D 4 V (5) Also sha stss comot at ay istac fom th tub axis is giv by
3 Vlocity of loo flow though uifom igi aty of huma boy v v (6) Exss fo wall sha stss ca b obtai fom th fomula ( ) (7) w w sig Equatio (6) a c y I btw Y a ( c ) y xss fo will la to th fom w th may ais two cass wall sha stss is gat a that yil stss. I cas Y w that is if th th will occu o flow accoigly vlocity fuctio will bcom w w w Agai ow flui th costitutiv quatio may b ouc i th followig fom k y K is a costat a is th scala stai at fo th flow th stai at ca b xss as = wh is th axial vlocity v k Itgat with sct to w w( ) c w wc ( ) c c Th volum flux Q of th flow though th i is giv by Q w II. sults A Discussio Th objctiv of this aalysis is to stuy th flow chaactistics of a ow flui mol fo bloo flow with vlocity sli i sc of magtic ffct. Th oblm is solv umically usig Shootig mtho. Numical calculatios hav b o fo vaious cosiatios of aamts i.. th Hatma Numb a th yols umb...numical sults a show gahically. It has b obsv that th ffct of th Hatma umb a th yols umb o th vlocity fil as wll as o th wall sha stss is vy omit. If sha stss is gat tha yil stss y th a flow of bloo is ossibl othwis th will b o bloo flow. Fig () shows that th atu of vlocity ofil is sam if th is o sli. Fig () Illustat that th vlocity ofils with a ffct of a magtic fil fo vaious valus of yols umb. It is s that th vlocity ofil cass as th yols umb icass with sli. Fig (3).Illustat that th vlocity ofil v i atu is ot chag if o sli. Th aalysis vlo h is bas o ctai assumtios which may la to som hysiological imlicatios vi. (a) Flow is assum stay which is i tu fo vy thi atis i VS wh th ulsatility ffcts a small. (b) Th assumtio that DOI:.979/ Pag
4 Vlocity of loo flow though uifom igi aty of huma boy vlocity vaiatio i a axial ictio is gligibl as coma to its vaiatio i aial ictio may la to th imlicatio that th lgth of th aty is too lag as coma to th aius. Fig-4 Illustat that th vlocity ofil v cass with icass of Hatma umb i sc of sli. It is also obsv that Hatma Numb icass th ffct of magtic fil is cass DOI:.979/ Pag
5 Vlocity of loo flow though uifom igi aty of huma boy fcs []. aothy.f. (.) iological ffcts of agtic fil Vol-I & II Plum Pss (969). []. huya. a Haaika G. io-scic sach ullti Vol.7() PP.5-(). [3]. huya. a Haaika. G. oc. Natioal cofc o ali athmatics -7(). [4]. huya.. a Haaika G.. loo flow i chals of vayig coss sctio with mabl bouais i sc of tasvs of magtic fil io scic sach ullti Vol. 8 (No. ) () [5]. oy W. Txt ook of Pathology: Stuctu a Fuctios i Disass La a Fbiga Philalhia (963). [6]. iswas D a Nath J. Oscillatig loo flow though a uifom Aty with wall sli Joual of Assam ivsity 4(). 4-54(999). [7]. u P. Th Vlocity Sli of Pola Fluis hol. Acta (975). [8]. ocklt G.. Th hology of huma bloo iomchaics. Y.. Fug. 63. (97). [9]. Fug Y.. iomchaics: chaical Potis of Livig Tissus Sig-Vlag Nw Yok Ic. (98). []..E. Ali N. Sa attao-histov mol fo aioactiv hat tasf of magto hyoyamics asso-fo flui: A umical stuy s.hy. 7(7) -3. []..ustafa T.Hayat I.Po A.Ai stay bouay lay flow of a asso flui u to a imulsivly stat movig flat lat Hat Tasf. Asia s4() []..Y. alik. Nas S. Nam Abul hma Th bouay lay flow of assomooflui ov a vtical xotial sttchig cyli Al. Naosci.4(4). [3]. acdoal D.A. O Stay Flow Though oll Vascula Stoss J. iomchaics. 3- (979) [4].. ustafa J. Ahma Kha ol fo flow of cassoaoflui ast a o-lialysttchig sht cosiig magtic fil ffcts AIP Av. 5 (5). [5]. ill F.W. hology of Huma loo a Som Sculatios o its ol i Vascula Homostatics iomchaical chaisms i Vascula Homostatics a Itavascula Thombosis. P.N. Sawy Alto tuy ofts Nw Yok (965). [6]. Nuba Y. loo Flow Sli a Viscomty iohys. J (97). [7]. Su V.K. a Skho G.S. Phy.. iol. Vol (989). [8]. atho V.P. Gayati Ali Scic ioical vol.() PP 5-58(). [9]. Vaaya V.A. iohysics Vol. 8 (3) (973) []. YougD.F J.Egg I.Tas.Am.Soc.ch.Egs.Vol (968) DOI:.979/ Pag
The Hydrogen Atom. Chapter 7
Th Hyog Ato Chapt 7 Hyog ato Th vy fist pobl that Schöig hislf tackl with his w wav quatio Poucig th oh s gy lvls a o! lctic pottial gy still plays a ol i a subatoic lvl btw poto a lcto V 4 Schöig q. fo
More informationDielectric Waveguide 1
Dilctic Wavgui Total Ital Rflctio i c si c t si si t i i i c i Total Ital Rflctio i c i cos si Wh i t i si c si cos t j o cos t t o si i si bcoms pul imagia pul imagia i, al Total Ital Rflctio 3 i c i
More informationSAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.
he 47 Lctu Fall 5 SFE OPERION OF UBULR (PFR DIBI REORS I a xthmic acti th tmatu will ctiu t is as mvs alg a lug flw act util all f th limitig actat is xhaust. Schmatically th aiabatic tmatu is as a fucti
More informationENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles
ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh
More informationOn Jackson's Theorem
It. J. Cotm. Math. Scics, Vol. 7, 0, o. 4, 49 54 O Jackso's Thom Ema Sami Bhaya Datmt o Mathmatics, Collg o Educatio Babylo Uivsity, Babil, Iaq mabhaya@yahoo.com Abstact W ov that o a uctio W [, ], 0
More informationELEC9721: Digital Signal Processing Theory and Applications
ELEC97: Digital Sigal Pocssig Thoy ad Applicatios Tutoial ad solutios Not: som of th solutios may hav som typos. Q a Show that oth digital filts giv low hav th sam magitud spos: i [] [ ] m m i i i x c
More information1985 AP Calculus BC: Section I
985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b
More informationThe tight-binding method
Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i
More informationToday s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom
Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What
More informationHomework 1: Solutions
Howo : Solutos No-a Fals supposto tst but passs scal tst lthouh -f th ta as slowss [S /V] vs t th appaac of laty alty th path alo whch slowss s to b tat to obta tavl ts ps o th ol paat S o V as a cosquc
More informationCh. 6 Free Electron Fermi Gas
Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio
More informationON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS
Joual of Pue ad Alied Mathematics: Advaces ad Alicatios Volume 0 Numbe 03 Pages 5-58 ON EUCLID S AND EULER S PROOF THAT THE NUMBER OF PRIMES IS INFINITE AND SOME APPLICATIONS ALI H HAKAMI Deatmet of Mathematics
More informationGalaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes
Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds
More informationAnouncements. Conjugate Gradients. Steepest Descent. Outline. Steepest Descent. Steepest Descent
oucms Couga Gas Mchal Kazha (6.657) Ifomao abou h Sma (6.757) hav b pos ol: hp://www.cs.hu.u/~msha Tch Spcs: o M o Tusay afoo. o Two paps scuss ach w. o Vos fo w s caa paps u by Thusay vg. Oul Rvw of Sps
More informationANALYSIS OF RING BEAMS FOR DISCRETELY SUPPORTED CYLINDRICAL SILOS
ANALYSIS OF RING BEAS FOR DISCRETELY SUPPORTED CYLINDRICAL SILOS Öz Zybk Rsach Assistat Dpatmt of Ciil Eii, il East Tchical Uisity, Akaa, Tuky E-mail: ozybk@mtu.u.t Cm Topkaya Pofsso Dpatmt of Ciil Eii,
More informationand integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform
NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists
More informationRelation between wavefunctions and vectors: In the previous lecture we noted that:
Rlatio tw wavuctios a vctos: I th pvious lctu w ot that: * Ψm ( x) Ψ ( x) x Ψ m Ψ m which claly mas that th commo ovlap itgal o th lt must a i pouct o two vctos. I what ss is ca w thi o th itgal as th
More informationInstrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential
Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii
More informationECE534, Spring 2018: Final Exam
ECE534, Srig 2018: Fial Exam Problem 1 Let X N (0, 1) ad Y N (0, 1) be ideedet radom variables. variables V = X + Y ad W = X 2Y. Defie the radom (a) Are V, W joitly Gaussia? Justify your aswer. (b) Comute
More informationChapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series
Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris
More informationExponential Atomic Decomposition in Generalized Weighted Lebesgue Spaces
Joual of Mathatics Rsach; Vol 6 No 4; 4 ISSN 96-9795 E-ISSN 96-989 Publish by Caaia Ct of Scic a Eucatio Exotial Atoic Dcoosio i Galiz Wight Lbsgu Sacs Nasibova NP Istut of Mathatics a Mchaics of NAS of
More informationPeriodic Structures. Filter Design by the Image Parameter Method
Prioic Structurs a Filtr sig y th mag Paramtr Mtho ECE53: Microwav Circuit sig Pozar Chaptr 8, Sctios 8. & 8. Josh Ottos /4/ Microwav Filtrs (Chaptr Eight) microwav filtr is a two-port twork us to cotrol
More information2011 HSC Mathematics Extension 1 Solutions
0 HSC Mathmatics Etsio Solutios Qustio, (a) A B 9, (b) : 9, P 5 0, 5 5 7, si cos si d d by th quotit ul si (c) 0 si cos si si cos si 0 0 () I u du d u cos d u.du cos (f) f l Now 0 fo all l l fo all Rag
More informationBINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a
BINOMIAL THEOREM hapte 8 8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4 5y, etc., ae all biomial epessios. 8.. Biomial theoem If
More informationBINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a
8. Oveview: 8.. A epessio cosistig of two tems, coected by + o sig is called a biomial epessio. Fo eample, + a, y,,7 4, etc., ae all biomial 5y epessios. 8.. Biomial theoem BINOMIAL THEOREM If a ad b ae
More informationCollisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center
Collisionlss Hall-MHD Modling Na a Magntic Null D. J. Stoi J. J. Ramos MIT Plasma Scinc and Fusion Cnt Collisionlss Magntic Rconnction Magntic connction fs to changs in th stuctu of magntic filds, bought
More informationStudy of the Balance for the DHS Distribution
Itatioal Mathmatical Foum, Vol. 7, 01, o. 3, 1553-1565 Study of th Balac fo th Distibutio S. A. El-Shhawy Datmt of Mathmatics, Faculty of scic Moufiya Uivsity, Shbi El-Kom, Egyt Cut addss: Datmt of Mathmatics,
More informationNoise in electronic components.
No lto opot5098, JDS No lto opot Th PN juto Th ut thouh a PN juto ha fou opot t: two ffuo ut (hol fo th paa to th aa a lto th oppot to) a thal at oty ha a (hol fo th aa to th paa a lto th oppot to, laka
More informationLecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t
Cla ot fo EE6318/Phy 6383 Spg 001 Th doumt fo tutoal u oly ad may ot b opd o dtbutd outd of EE6318/Phy 6383 tu 7 Dffuo Ou flud quato that w dvlopd bfo a: f ( )+ v v m + v v M m v f P+ q E+ v B 13 1 4 34
More information(Reference: sections in Silberberg 5 th ed.)
ALE. Atomic Structur Nam HEM K. Marr Tam No. Sctio What is a atom? What is th structur of a atom? Th Modl th structur of a atom (Rfrc: sctios.4 -. i Silbrbrg 5 th d.) Th subatomic articls that chmists
More informationInternational Journal of Mathematics Trends and Technology (IJMTT) Volume 47 Number 1 July 2017
Iteatioal Joual of Matheatics Teds ad Techology (IJMTT) Volue 47 Nube July 07 Coe Metic Saces, Coe Rectagula Metic Saces ad Coo Fixed Poit Theoes M. Sivastava; S.C. Ghosh Deatet of Matheatics, D.A.V. College
More information( ) ( ) ( ) 2011 HSC Mathematics Solutions ( 6) ( ) ( ) ( ) π π. αβ = = 2. α β αβ. Question 1. (iii) 1 1 β + (a) (4 sig. fig.
HS Mathmatics Solutios Qustio.778.78 ( sig. fig.) (b) (c) ( )( + ) + + + + d d (d) l ( ) () 8 6 (f) + + + + ( ) ( ) (iii) β + + α α β αβ 6 (b) si π si π π π +,π π π, (c) y + dy + d 8+ At : y + (,) dy 8(
More informationConditional Convergence of Infinite Products
Coditioal Covegece of Ifiite Poducts William F. Tech Ameica Mathematical Mothly 106 1999), 646-651 I this aticle we evisit the classical subject of ifiite poducts. Fo stadad defiitios ad theoems o this
More informationPLS-CADD DRAWING N IC TR EC EL L RA IVE ) R U AT H R ER 0. IDT FO P 9-1 W T OO -1 0 D EN C 0 E M ER C 3 FIN SE W SE DE EA PO /4 O 1 AY D E ) (N W AN N
A IV ) H 0. IT FO P 9-1 W O -1 0 C 0 M C FI S W S A PO /4 O 1 AY ) ( W A 7 F 4 H T A GH 1 27 IGO OU (B. G TI IS 1/4 X V -S TO G S /2 Y O O 1 A A T H W T 2 09 UT IV O M C S S TH T ) A PATO C A AY S S T
More informationThe angle between L and the z-axis is found from
Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt
More informationADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction
ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS Ghiocl Goza*, S. M. Ali Khan** Abstact Th additiv intgal functions with th cofficints in a comlt non-achimdan algbaically closd fild of chaactistic 0 a studid.
More informationMapping Radius of Regular Function and Center of Convex Region. Duan Wenxi
d Iteatioal Cofeece o Electical Compute Egieeig ad Electoics (ICECEE 5 Mappig adius of egula Fuctio ad Cete of Covex egio Dua Wexi School of Applied Mathematics Beijig Nomal Uivesity Zhuhai Chia 363463@qqcom
More informationWeek 03 Discussion. 30% are serious, and 50% are stable. Of the critical ones, 30% die; of the serious, 10% die; and of the stable, 2% die.
STAT 400 Wee 03 Discussio Fall 07. ~.5- ~.6- At the begiig of a cetai study of a gou of esos, 5% wee classified as heavy smoes, 30% as light smoes, ad 55% as osmoes. I the five-yea study, it was detemied
More informationChapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is
Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )
More informationLoad Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.
oa Euatons Thoughout all of chapt 4, ou focus s on th machn tslf, thfo w wll only pfom a y smpl tatmnt of th ntwok n o to s a complt mol. W o that h, but alz that w wll tun to ths ssu n Chapt 9. So lt
More informationMATH /19: problems for supervision in week 08 SOLUTIONS
MATH10101 2018/19: poblems fo supevisio i week 08 Q1. Let A be a set. SOLUTIONS (i Pove that the fuctio c: P(A P(A, defied by c(x A \ X, is bijective. (ii Let ow A be fiite, A. Use (i to show that fo each
More informationHow many neutrino species?
ow may utrio scis? Two mthods for dtrmii it lium abudac i uivrs At a collidr umbr of utrio scis Exasio of th uivrs is ovrd by th Fridma quatio R R 8G tot Kc R Whr: :ubblcostat G :Gravitatioal costat 6.
More informationCHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method
CHAPTER 5 : SERIES 5.1 Seies 5. The Sum of a Seies 5..1 Sum of Powe of Positive Iteges 5.. Sum of Seies of Patial Factio 5..3 Diffeece Method 5.3 Test of covegece 5.3.1 Divegece Test 5.3. Itegal Test 5.3.3
More informationFinite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler
Fiite -idetities elated to well-ow theoems of Eule ad Gauss Joha Cigle Faultät fü Mathemati Uivesität Wie A-9 Wie, Nodbegstaße 5 email: oha.cigle@uivie.ac.at Abstact We give geealizatios of a fiite vesio
More informationSums of Involving the Harmonic Numbers and the Binomial Coefficients
Ameica Joual of Computatioal Mathematics 5 5 96-5 Published Olie Jue 5 i SciRes. http://www.scip.og/oual/acm http://dx.doi.og/.46/acm.5.58 Sums of Ivolvig the amoic Numbes ad the Biomial Coefficiets Wuyugaowa
More informationBy Joonghoe Dho. The irradiance at P is given by
CH. 9 c CH. 9 c By Joogo Do 9 Gal Coao 9. Gal Coao L co wo po ouc, S & S, mg moocomac wav o am qucy. L paao a b muc ga a. Loca am qucy. L paao a b muc ga a. Loca po obvao P a oug away om ouc o a a P wavo
More informationRecurrence Relations
Recurrece Relatios Aalysis of recursive algorithms, such as: it factorial (it ) { if (==0) retur ; else retur ( * factorial(-)); } Let t be the umber of multiplicatios eeded to calculate factorial(). The
More informationz 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z
Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist
More informationDiscussion 02 Solutions
STAT 400 Discussio 0 Solutios Spig 08. ~.5 ~.6 At the begiig of a cetai study of a goup of pesos, 5% wee classified as heavy smoes, 30% as light smoes, ad 55% as osmoes. I the fiveyea study, it was detemied
More informationPURE MATHEMATICS A-LEVEL PAPER 1
-AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio
More informationLøsningsførslag i 4M
Norges tekisk aturviteskapelige uiversitet Istitutt for matematiske fag Side 1 av 6 Løsigsførslag i 4M Oppgave 1 a) A sketch of the graph of the give f o the iterval [ 3, 3) is as follows: The Fourier
More informationFall 2013 MTH431/531 Real analysis Section Notes
Fall 013 MTH431/531 Real aalysis Sectio 8.1-8. Notes Yi Su 013.11.1 1. Defiitio of uiform covergece. We look at a sequece of fuctios f (x) ad study the coverget property. Notice we have two parameters
More informationStatics. Consider the free body diagram of link i, which is connected to link i-1 and link i+1 by joint i and joint i-1, respectively. = r r r.
Statcs Th cotact btw a mapulato ad ts vomt sults tactv ocs ad momts at th mapulato/vomt tac. Statcs ams at aalyzg th latoshp btw th actuato dv tous ad th sultat oc ad momt appld at th mapulato dpot wh
More informationMinimal order perfect functional observers for singular linear systems
Miimal ode efect fuctioal obseves fo sigula liea systems Tadeusz aczoek Istitute of Cotol Idustial lectoics Wasaw Uivesity of Techology, -66 Waszawa, oszykowa 75, POLAND Abstact. A ew method fo desigig
More informationContinuous Functions
Cotiuous Fuctios Q What does it mea for a fuctio to be cotiuous at a poit? Aswer- I mathematics, we have a defiitio that cosists of three cocepts that are liked i a special way Cosider the followig defiitio
More informationInverse Matrix. A meaning that matrix B is an inverse of matrix A.
Iverse Matrix Two square matrices A ad B of dimesios are called iverses to oe aother if the followig holds, AB BA I (11) The otio is dual but we ofte write 1 B A meaig that matrix B is a iverse of matrix
More informationStatistical Analysis on Uncertainty for Autocorrelated Measurements and its Applications to Key Comparisons
Statistical Aalysis o Ucertaity for Autocorrelated Measuremets ad its Applicatios to Key Comparisos Nie Fa Zhag Natioal Istitute of Stadards ad Techology Gaithersburg, MD 0899, USA Outlies. Itroductio.
More informationNew bounds on Poisson approximation to the distribution of a sum of negative binomial random variables
Sogklaaka J. Sc. Tchol. 4 () 4-48 Ma. -. 8 Ogal tcl Nw bouds o Posso aomato to th dstbuto of a sum of gatv bomal adom vaabls * Kat Taabola Datmt of Mathmatcs Faculty of Scc Buaha Uvsty Muag Chobu 3 Thalad
More informationKEB INVERTER L1 L2 L3 FLC - RELAY 1 COMMON I1 - APPROACH CLOSE 0V - DIGITAL COMMON FLA - RELAY 1 N.O. AN1+ - ANALOG 1 (+) CRF - +10V OUTPUT
XT SSMLY MOL 00 (O FS) 00 (I- PT) 00 (SIGL SLI) WG O 0 0-0 0-0-0 0.0. 0 0-0 0-0-0 0 0-0 0-0-0 VOLTG F.L...0..0..0.0..0 IIG POW FOM US SUPPLI ISOT (S TL) US OP OUTOS T T 0 O HIGH H IUIT POTTIO OT: H IUIT
More informationPhysics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas
Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain
More informationValley Forge Middle School Fencing Project Facilities Committee Meeting February 2016
Valley Forge iddle chool Fencing roject Facilities ommittee eeting February 2016 ummer of 2014 Installation of Fencing at all five istrict lementary chools October 2014 Facilities ommittee and
More informationChapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures
Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.
More informationEuropean and American options with a single payment of dividends. (About formula Roll, Geske & Whaley) Mark Ioffe. Abstract
866 Uni Naions Plaza i 566 Nw Yo NY 7 Phon: + 3 355 Fa: + 4 668 info@gach.com www.gach.com Eoan an Amican oions wih a singl amn of ivins Abo fomla Roll Gs & Whal Ma Ioff Absac Th aicl ovis a ivaion of
More informationMon. Tues. 6.2 Field of a Magnetized Object 6.3, 6.4 Auxiliary Field & Linear Media HW9
Fi. on. Tus. 6. Fild of a agntid Ojct 6.3, 6.4 uxiliay Fild & Lina dia HW9 Dipol t fo a loop Osvation location x y agntic Dipol ont Ia... ) ( 4 o I I... ) ( 4 I o... sin 4 I o Sa diction as cunt B 3 3
More information5.61 Fall 2007 Lecture #2 page 1. The DEMISE of CLASSICAL PHYSICS
5.61 Fall 2007 Lctu #2 pag 1 Th DEMISE of CLASSICAL PHYSICS (a) Discovy of th Elcton In 1897 J.J. Thomson discovs th lcton and masus ( m ) (and inadvtntly invnts th cathod ay (TV) tub) Faaday (1860 s 1870
More informationTechnical Report: Bessel Filter Analysis
Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we
More informationNew Advanced Higher Mathematics: Formulae
Advcd High Mthmtics Nw Advcd High Mthmtics: Fomul G (G): Fomul you must mmois i od to pss Advcd High mths s thy ot o th fomul sht. Am (A): Ths fomul giv o th fomul sht. ut it will still usful fo you to
More informationOn a Problem of Littlewood
Ž. JOURAL OF MATHEMATICAL AALYSIS AD APPLICATIOS 199, 403 408 1996 ARTICLE O. 0149 O a Poblem of Littlewood Host Alze Mosbache Stasse 10, 51545 Waldbol, Gemay Submitted by J. L. Bee Received May 19, 1995
More informationKEY. Math 334 Midterm II Fall 2007 section 004 Instructor: Scott Glasgow
KEY Math 334 Midtem II Fall 7 sectio 4 Istucto: Scott Glasgow Please do NOT wite o this exam. No cedit will be give fo such wok. Rathe wite i a blue book, o o you ow pape, pefeably egieeig pape. Wite you
More informationLESSON 15: COMPOUND INTEREST
High School: Expoeial Fuctios LESSON 15: COMPOUND INTEREST 1. You have see this fomula fo compoud ieest. Paamete P is the picipal amou (the moey you stat with). Paamete is the ieest ate pe yea expessed
More informationAppendix: The Laplace Transform
Appedix: The Laplace Trasform The Laplace trasform is a powerful method that ca be used to solve differetial equatio, ad other mathematical problems. Its stregth lies i the fact that it allows the trasformatio
More informationLecture #4: Integration Algorithms for Rate-independent Plasticity (1D)
5-0735: Damic behavior of materials a structures Lecture #4: Itegratio Algorithms for Rate-ieeet Plasticit (D) b Dirk Mohr TH Zurich, Deartmet of Mechaical a Process gieerig, Chair of Comutatioal Moelig
More informationEffects of Some Structural Parameters on the Vibration of a Simply Supported Non-prismatic Double-beam System
Poceeigs of the Wol Cogess o Egieeig 017 Vol WCE 017, July 5-7, 017, Loo, U.K. Effects of Some Stuctual Paametes o the Vibatio of a Simply Suppote No-pismatic Double-beam System Olasumbo O. Agboola, Membe,
More informationNuclear Physics Worksheet
Nuclear Physics Worksheet The ucleus [lural: uclei] is the core of the atom ad is comosed of articles called ucleos, of which there are two tyes: rotos (ositively charged); the umber of rotos i a ucleus
More informationSession : Plasmas in Equilibrium
Sssio : Plasmas i Equilibrium Ioizatio ad Coductio i a High-prssur Plasma A ormal gas at T < 3000 K is a good lctrical isulator, bcaus thr ar almost o fr lctros i it. For prssurs > 0.1 atm, collisio amog
More informationOn ARMA(1,q) models with bounded and periodically correlated solutions
Reseach Repot HSC/03/3 O ARMA(,q) models with bouded ad peiodically coelated solutios Aleksade Weo,2 ad Agieszka Wy oma ska,2 Hugo Steihaus Cete, Woc aw Uivesity of Techology 2 Istitute of Mathematics,
More informationMid Year Examination F.4 Mathematics Module 1 (Calculus & Statistics) Suggested Solutions
Mid Ya Eamination 3 F. Matmatics Modul (Calculus & Statistics) Suggstd Solutions Ma pp-: 3 maks - Ma pp- fo ac qustion: mak. - Sam typ of pp- would not b countd twic fom wol pap. - In any cas, no pp maks
More informationHOMEWORK #10 SOLUTIONS
Math 33 - Aalysis I Sprig 29 HOMEWORK # SOLUTIONS () Prove that the fuctio f(x) = x 3 is (Riema) itegrable o [, ] ad show that x 3 dx = 4. (Without usig formulae for itegratio that you leart i previous
More information( ) 1 Comparison Functions. α is strictly increasing since ( r) ( r ) α = for any positive real number c. = 0. It is said to belong to
Compaiso Fuctios I this lesso, we study stability popeties of the oautoomous system = f t, x The difficulty is that ay solutio of this system statig at x( t ) depeds o both t ad t = x Thee ae thee special
More information( ) L = D e. e e. Example:
xapl: A Si p juctio diod av acoss sctioal aa of, a accpto coctatio of 5 0 8 c -3 o t p-sid ad a doo coctatio of 0 6 c -3 o t -sid. T lif ti of ols i -gio is 47 s ad t lif ti of lctos i t p-gio is 5 s.
More informationTHE ANALYTIC LARGE SIEVE
THE ANALYTIC LAGE SIEVE 1. The aalytic lage sieve I the last lectue we saw how to apply the aalytic lage sieve to deive a aithmetic fomulatio of the lage sieve, which we applied to the poblem of boudig
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationStability of Stratified Rotating Viscoelastic Rivlin Ericksen Fluid in The Presence of Variable Magnetic Field
vailabl oli at.plaiasacliba.co vacs i ppli Scic Rsac,, (5):5-58 ISSN: 976-86 COEN (US): SRFC Stabilit of Statifi Rotati iscolastic Rivli Eics Flui i T Psc of aiabl Matic Fil Rajs Kua Gupta a Mai Si patt
More informationSolid state physics. Lecture 3: chemical bonding. Prof. Dr. U. Pietsch
Solid stat physics Lctu 3: chmical bonding Pof. D. U. Pitsch Elcton chag dnsity distibution fom -ay diffaction data F kp ik dk h k l i Fi H p H; H hkl V a h k l Elctonic chag dnsity of silicon Valnc chag
More information3D Viewing. Vanishing Points. Two ways Intersection of transformed lines Transformation of points at infinity. Y VP z. VP x
Vaishig Poits Two ways Itsctio of tasfomd lis Tasfomatio of oits at ifiity Y Y VP z X VP x X Z Pla Gomtic Pojctios Paalll Pscti Othogahic Axoomtic Obliq Sigl Poit Timtic Dimtic Isomtic Caali Cabit Two
More informationA sequence of numbers is a function whose domain is the positive integers. We can see that the sequence
Sequeces A sequece of umbers is a fuctio whose domai is the positive itegers. We ca see that the sequece,, 2, 2, 3, 3,... is a fuctio from the positive itegers whe we write the first sequece elemet as
More information) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition:
Assigm Thomas Aam, Spha Brumm, Haik Lor May 6 h, 3 8 h smsr, 357, 7544, 757 oblm For R b X a raom variabl havig ormal isribuio wih ma µ a variac σ (his is wri as ~ (,) X. by: R a. Is X ) a urhrmor all
More informationAnalytic Number Theory Solutions
Aalytic Number Theory Solutios Sea Li Corell Uiversity sl6@corell.eu Ja. 03 Itrouctio This ocumet is a work-i-progress solutio maual for Tom Apostol s Itrouctio to Aalytic Number Theory. The solutios were
More informationExtinction Ratio and Power Penalty
Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application
More informationLyapunov Stability Analysis for Feedback Control Design
Copyright F.L. Lewis 008 All rights reserved Updated: uesday, November, 008 Lyapuov Stability Aalysis for Feedbac Cotrol Desig Lyapuov heorems Lyapuov Aalysis allows oe to aalyze the stability of cotiuous-time
More information9.3 Power Series: Taylor & Maclaurin Series
9.3 Power Series: Taylor & Maclauri Series If is a variable, the a ifiite series of the form 0 is called a power series (cetered at 0 ). a a a a a 0 1 0 is a power series cetered at a c a a c a c a c 0
More informationEffect of Material Gradient on Stresses of Thick FGM Spherical Pressure Vessels with Exponentially-Varying Properties
M. Zamai Nejad et al, Joual of Advaced Mateials ad Pocessig, Vol.2, No. 3, 204, 39-46 39 Effect of Mateial Gadiet o Stesses of Thick FGM Spheical Pessue Vessels with Expoetially-Vayig Popeties M. Zamai
More informationStructure and Features
Thust l Roll ans Thust Roll ans Stutu an atus Thust ans onsst of a psly ma a an olls. Thy hav hh ty an hh loa apats an an b us n small spas. Thust l Roll ans nopoat nl olls, whl Thust Roll ans nopoat ylnal
More informationOn the approximation of the constant of Napier
Stud. Uiv. Babş-Bolyai Math. 560, No., 609 64 O th approximatio of th costat of Napir Adri Vrscu Abstract. Startig from som oldr idas of [] ad [6], w show w facts cocrig th approximatio of th costat of
More informationMa 530 Introduction to Power Series
Ma 530 Itroductio to Power Series Please ote that there is material o power series at Visual Calculus. Some of this material was used as part of the presetatio of the topics that follow. What is a Power
More informationPrevious knowlegde required. Spherical harmonics and some of their properties. Angular momentum. References. Angular momentum operators
// vious owg ui phica haoics a so o thi poptis Goup thoy Quatu chaics pctoscopy H. Haga 8 phica haoics Rcs Bia. iv «Iucib Tso thos A Itouctio o chists» Acaic ss D.A. c Quai.D. io «hii hysiu Appoch oécuai»
More informationChapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1
Chatr Fiv Mor Dimsios 51 Th Sac R W ar ow rard to mov o to sacs of dimsio gratr tha thr Ths sacs ar a straightforward gralizatio of our Euclida sac of thr dimsios Lt b a ositiv itgr Th -dimsioal Euclida
More informationClassical Theory of Fourier Series : Demystified and Generalised VIVEK V. RANE. The Institute of Science, 15, Madam Cama Road, Mumbai
Clssil Thoy o Foi Sis : Dmystii Glis VIVEK V RANE Th Istitt o Si 5 Mm Cm Ro Mmbi-4 3 -mil ss : v_v_@yhoooi Abstt : Fo Rim itgbl tio o itvl o poit thi w i Foi Sis t th poit o th itvl big ot how wh th tio
More informationPropagation of Light About Rapidly Rotating Neutron Stars. Sheldon Campbell University of Alberta
Ppagatin f Light Abut Rapily Rtating Nutn Stas Shln Campbll Univsity f Albta Mtivatin Tlscps a nw pcis nugh t tct thmal spcta fm cmpact stas. What flux is masu by an bsv lking at a apily tating lativistic
More informationDFT: Discrete Fourier Transform
: Discrt Fourir Trasform Cogruc (Itgr modulo m) I this sctio, all lttrs stad for itgrs. gcd m, = th gratst commo divisor of ad m Lt d = gcd(,m) All th liar combiatios r s m of ad m ar multils of d. a b
More information