STUDY OF THE BIOHEAT EQUATION WITH A SPHERICAL HEAT SOURCE FOR LOCAL MAGNETIC HYPERTHERMIA
|
|
- Eustace Jefferson
- 5 years ago
- Views:
Transcription
1 XVI Cngess n Nueial Mehds and hei Aliains Códba, Agenina Obe -7, 7 STUDY OF THE BIOHEAT EQUATION WITH A SPHERICAL HEAT SOURCE FOR LOCAL MAGNETIC HYPERTHERMIA Gusav Guieez Mehanial Engineeing Deaen Univesiy f Pue Ri Mayaguez, PR e-ail: gguie@euedu Absa Hyeheia is a ye f ane eaen in whih ane ells ae exsed high eeaues (u C) Reseah has shwn ha high eeaues an daage and kill ane ells, by a lalized and nenaed heaing sue By killing ane ells and daaging eins and suues wihin ells, hyeheia ay shink us, wih inial injuy nal issues In addiin in vi and in viv sudies, ue siulain an be used undesand ans henena inside a u In his sudy a sheial egin naining a agnei aile ebedded in a issue is deled using he bihea equain wih he Penne s del f he heal ineain beween he issue and he efused bld Analyial ehniques ae used slve he bihea equain wih a in hea sue f nsan densiy we laed as he ene f a sheial dain The in hea sue del he hea geneaed by agnei ailes unde he effe f an alenaing agnei field, used in sudies f lal agnei hyeeia Paaei sudies f he eeaue files ae aied u sudy he effe f diffeen aaees like he hea geneain ae, efusin ae and diaee f he in sue n he axiu eeaue and n he eeaue file Se disussin abu ian aaees eseah issues in ane hyeeia ae als addessed Key wds: Hyeheia; lalized hea sue; he bihea equain NOMENCLATURA ρ, C, k, α : densiy, seifi hea, heal nduiviy and heal diffusiviy f he issue ρ, C b b : densiy and seifi hea f he bld q : eabli hea geneain q : efusin hea sue
2 ω : efusin ae ( /s f vluei bld flw e f issue) T aeial eeaue T, T : lal issue eeaue and diensinless lal issue eeaue Q( ) : in sue hea geneain, : adial dinae and diensinless adial dinae, R : adius f he inenal hea sue, axiu adius f he dain, : ie and diensinless ie I/, K / : dified Bessel funins f de ½ INTRODUCTION Bihea ansfe esses in living issues ae fen influened by he influene f bld efusin hugh he vasula newk n he lal eeaue disibuin When hee is a signifian diffeene beween he eeaue f he bld and he issue hugh whih i flws, nveive hea ans will u, aleing he eeaues f bh he bld and he issue Pefusin based hea ansfe ineain is iial a nube f hysilgial esses suh as heegulain and inflaain The bld/issue heal ineain is a funin f seveal aaees inluding he ae f efusin and he vasula anay, whih vay widely ang he diffeen issues, gans f he bdy, and ahlgy The lieaue nains an exensive ilain f efusin ae daa f any issues and gans The ae f efusin f bld hugh diffeen issues and gans vaies deending n fas suh as hysial aiviy, hysilgial siulus and envinenal ndiins Fuhe, any disease esses ae haaeized by aleains in bld efusin, and se heaeui inevenins esul in eihe an inease deease in bld flw in a age issue A gd efeene f he sudy f bihea ansfe an be fund in he CRC Handbk f Theal Engineeing, hae 44(Ed Fank Keih, ) Bagaia, and Jhnsn (Bagaia, and Jhnsn,, 5) sudied he he bihea equain nueially and analyially f hyeheia aliains f ane eaens The del sudies he e disibuin f agnei ailes hughu he u uld iniize he daage he suunding healhy issue while sill ainaining a heaeui eeaue in he u Hweve, his disibuin is defined aheaially bu is n feasible nl in aial aliains And he analyial sluin is liae and bsue Rsensweig, (Rsensweig, ) esen a del f heaing agnei fluid wih alenaing agnei field In his ae an analyial sudy is uied u slve he bihea equain wih a hea sue f nsan densiy we laed as he ene f a sheial dain The in hea sue del he hea geneaed by agnei ailes unde he effe f an alenaing agnei field, used in sudies f lal agnei hyeeia Paaei sudies f he eeaue files ae aied u sudy he effe f diffeen aaees like he hea geneain ae, efusin ae and diaee f he in sue n he axiu eeaue and n he eeaue file Se disussin abu ian aaees eseah issues in ane hyeeia ae addessed
3 - MATHEMATICAL FORMULATION Pennes del (Pennes, 948) desibes he effes f eablis and bld efusin n he enegy balane wihin issue Basially, hese w effes ae inaed in he sandad heal diffusin equain and he equain is alled he bihea equain Hee, he dain f sudy will be a sheial dain wih a hea sue f adius a he ene f he sheial dain f adius R as is shwn sheaially in Figue f a healhy issue Figue Sheai f he sheial dain wih an inenal hea sue The bihea equain in sheial dinaes wih an inenal hea geneain a he ene f he shee an be wien as: q q ρc T T Q = k k k () Whee ρ, C, k ae he densiy, seifi hea and heal nduiviy f he issue, ρ, C ae densiy and seifi hea f he bld, q is he eabli hea geneain Pennes s del f ωρbc b he efusin hea sue is q = ( T T ) k, whee ω : is he efusin ae ( /s f vluei bld flw e f issue), T is he aeial eeaue and T is he lal issue eeaue Then, by inaing he Pennes s del in he diffusin equain () yields: ρc T T ωρbc b q Q = + ( T T ) + + () k k k k α T T Defining he fllwing diensinless aaees: =, = and T = Wiing R R T equain () in es f hese diensinless aaees, a diensinless equain is bained: b b T T RωρbC b Q R q R T = k kt kt ()
4 kt k By defining he fllwing nsans, Q = and C = ha diensinalize R R Q, q and ωρ C b b as: wien as: Q q Q = +, Q Q ωρ C =, he bihea equain in diensinless f an be C b b T T T Q = (4) Wih he fllwing iniial ndiin, eeaue us eain finie a he ene T (, = ) = and he fllwing bunday ndiins: he T (, ) = finie and he eeaue a he exenal sheial sufae is ainained a T, s he diensinless eeaue ( =, ) = T ANALYTICAL SOLUTION T bain an analyial sluin, le sli he diensinless hea geneain e nsan hea geneain due eablis ene q ( ) Q( ) = q + q Q in a q and a nsan hea sue f adius a he Then T T T q = q (5) Nw, le T T T = (, ) + and f nveniene le d he suesi T T T = q( ) T = T q (6) (7) Subje he fllwing bunday ndiins: T (, T (, (8) T T ( ) (9)
5 And he fllwing iniial ndiin: T (,) = T sine T T T (,) = (,) + = () Nw, le (, ) T (, ) = e U and subsiue in equain (6) U U = = (, ) q e g () Whee he sue e is nw a funin f and, g(, ) = q e Then, he bunday ndiins in es f U yields: U ( =, ) = and U ( =, ) = finie () And he iniial ndiin bees: U (, = ) = T () Then, equain (7) has be slved subje bunday ndiins (9) and equain () subje bunday ndiins () and iniial ndiin () Wih he fllwing hange f vaiables f H T =, equain (7) bees a dified Bessel equain in es f H and he sluin is bained in es f dified Bessel funins (see Aendix A) ( ) q I/ T = I/ The sluin equain () f U is bained using Geen funins wih an iniial ndiin given by I/ ( ) q U (,) = T = (5) I/ ( ) A sheial hea sue f adius laed a he ene f he sheial dain f inegain g(, ) = g e ( ) 4π δ (4) = β U (, ) = e sin ( β) 'sin ( β ')( T ( ')) d ' + + π sin ( ) sin ( ) τ = = β β τ τ e β β e g e dτ (6)
6 The inegal geneain τ = g ( β + ) τ e g dτ an be inegaed analyially f a nsan inensiy hea τ = ( β + ) τ ( ) ( ) e g β + β + τ e e g dτ = = g β + β + Ging bak T = Ue wih β = π, T (, ) akes he f ( ) ( ) g β + β + e T (, ) = e sin ( β) 'sin ( β ')( T( ') ) d ' + sin ( β) sin ( β ) π β + = = (7) The inegal ( β )( ) is T =T (,)+T () 'sin ' T ( ') d ' an be evaluaed nueially The final sluin f T q I/ I/ β+ q T (, ) = e sin ( β ) 'sin ( β ' ) d ' + + I / I/ = g e π β β + β + β sin ( β ) sin ( β ) = β (8) Whee β = π, =,,, And f he definiin f he diensinless eeaue, bained as T = T T + T T T T =, he eeaue T is T 5 - RESULTS AND DISCUSSION Hee, se yial values ae assued f he issue heal eies, he eabli hea geneain, he efusin ae and a adius f a sheial dain unde sudy k = 5 W ; ρb = kg ; C 6 J ; 7 ; 7 W, 5 ; = T = C q = w = R = C kg C s kt The adius f he inenal hea sue is = Wih hese values, Q = and R C = k R ae alulaed diensinalize qɺ and = wρbc b
7 W 5 7 C kt C W q 7 W / wρbc b Q ɺ = = 85 ; q 78 ; 6 = = = = = = R ( ) Q 85 W / C k R α The aaee diensinalize he ie R W 5 α k C = = = 9 R ρc kg J R 6 ( s ) kg C T evaluae equain (8), an analysis f de f agniude is efed fis The fis e f equain (8) ges ze when ie ges infiniy Thus, T eesens he seady sae eeaue file due a nsan eabli hea geneain Assuing nly eabli hea geneain, he axiu eeaue will u a he ene f he sheial dain a he seady sae The eeaue ise due yial values f eabli hea geneain is negligible aed wih he eeaue ise due he hea sue ha have be geneaed by he agnei ailes, in hyeheia aliains Then, negleing he fis w es in equain (8), he eeaue file geneaed by he hea sue f adius a he ene f he sheial dain f adius R will be disussed nw Figue shws he eeaue files geneaed by an inenal hea sue a he ene f he shee f g = W / The axiu eeaue us a he ene and is axiaely 55ºC The seady sae eeaue disibuin is shwn and i an be seen he eeaue gadiens a he ene ae vey see be able diffuse he hea geneaed Sine he nduiviy f he issue is lw and he ss seinal aea in he egin lse he hea sue is als sall, f Fuie law f nduin he eeaue gadiens have be high As he adius is ineasing, he hea fluxes ae eduing and hea an be diffusive wih lwe gadiens This ilies ha in he egin nex he hea sue, a vey see eeaue file an be ainained f a lng ie geneaing highe eeaue in a vey sall egin and lwe eeaues a a elaively sh disane f he hea sue, wihu affeing healhy ells This is vey ian in hyeheia eaens, sine is desiable iniize senday effes F aaei sudies, he seady sae file is eahed in a vey sh ie (uh less han ne send) A a disan f he eeaue is less han 9 C As an be seen, he highe eeaues ae nenaed a sh disane f he hea sue Figue shws he eeaue file f a adius f he inenal hea sue f = F he sae vluei hea geneain g = W / he hea we is uh highe sine he vlue inease as he ubi f he adius bu he eeaues geneaed ae lwe beause hea an diffuse easie in his ase Figue 4 shws he eeaue files f a adius f he inenal hea sue f = as in Figue bu a vluei hea geneain f g = 7 W / I an be seen ha he eeaue eneaes fuhe in he dain
8 Teeaue ( C) g = W / = 4 - P = π g = 49 W Radial dinae () Figue Seady sae eeaue file f = 9 Teeaue ( C) g = W / = 4-9 P = π g = 49 W Radial dinae () Figue Seady sae eeaue file f =
9 5 Teeaue ( C) g = 7 W / = 4-8 P = π g = 9 W Radial dinae () Figue 4 Seady sae eeaue file f = and g =7 W/ Finally, f he analyial sluin (8), he effe f he efusin ae is quanified by he e β F yial values f in he de f 6, /π is sall and he effe f efusin an be negleed f hyeheia aliains 6 - CONCLUSIONS An analyial sudy f he bihea equain has been aied u An analyial sluin was bained f he ase f eabli hea geneain in a sheial dain and a nenaed hea sue a he ene f he shee F aaei sudies, eabli hea geneain an be negleed beause he eeaue aise ha will geneae is sall aed wih he yial eeaue inease geneaed in hyeheia aliains f ane eaens Als, he effe f he efusin ae is n signifian F vey nenaed hea sues, he eeaues gadiens ae vey high and highe eeaues ae geneaed in a sall egin lse he hea sue A sh disane f he sue, eeaues an be ainained aially a a issue eeaue wihu affeing healhy ells If he size f he hea sue ineases, he hea diffuses easie and he eeaue file eneae fahe in he healhy ells
10 7 - ACKNOWLEDGMENT D Gusav Guieez aeiaes he su f he NSF-NIRT ga and he Univesiy f Pue Ri-Mayaguez f he finanial su his wk 8 - REFERENCES Keih F, Tiehaus K, Li N, Shaw H, Shah RK, Bell K J, The CRC Handbk f Theal Engineeing Ed Fank Keih, Ba Ran: CRC Pess LLC, H G Bagaia and D T Jhnsn, "Tansien sluin he bihea equain and iizain f agnei fluid hyeheia," Inenainal Junal f Hyeheia, vl, 57-75, 5 Bagaia, H and Jhnsn, DT, Analyial and Nueial Sluin a Cneni Shee Mdel and Oiizain f Magnei Fluid Hyeheia Teaen Inenainal Junal f Hyeheia (5) Bagaia, H and Jhnsn, DT Nueial Sluin he Magnei Fluid Hyeheia Heaing f Pailes Absbed n a Cell Wall Peedings f he AIChE Cnfeene, San Fanis, CA Nainal Cane Insiue Hyeheia in Cane Teaen: Quesins and Answes wwwninihgv Rsensweig, R E "Heaing agnei fluid wih alenaing agnei field," Junal f Magneis and Magnei Maeials, vl 5, 7-74, Pennes, H H "Analysis f issue and aeial bld eeaues in he esing huan fea," Junal f Alied Physilgy, vl, 9-, 948 APENDIX A T slve equain (A), given belw T = T q (A) The fllwing hange f vaiable dt = H ' H d / / T H( ) = is ade Then, equain (A) ansfs
11 ' d = d / H H / / H q Mulilying by and ding q = we bained he esnding hgeneus equain ' = d / / H H / H d By exanding / / / / / H ' + H '' H H ' H = 4 Mulilying by / H '' + H ' H = This is he dified Bessel equain f de ½ The sluin is bained in es f he dified Bessel funins I/, K / H = BI / + BK/ T saisfy he ndiin ha H has be finie B = Then I ( ) / = B + Paiula sluin T If q is nsan, hen he aiula sluin is T Then q = I ( ) q / = B + T B is fund f he ndiin T ( ) =, whih ily ha B = = I and he sluin f T is / ( ) q I/ T = I/ q
Maximum Cross Section Reduction Ratio of Billet in a Single Wire Forming Pass Based on Unified Strength Theory. Xiaowei Li1,2, a
Inenainal Fum n Enegy, Envinmen and Susainable evelpmen (IFEES 06 Maximum Css Sein Reduin Rai f Bille in a Single Wie Fming Pass Based n Unified Sengh They Xiawei Li,, a Shl f Civil Engineeing, Panzhihua
More information( t) Steady Shear Flow Material Functions. Material function definitions. How do we predict material functions?
Rle f aeial Funins in Rhelgial Analysis Rle f aeial Funins in Rhelgial Analysis QUALIY CONROL QUALIAIVE ANALYSIS QUALIY CONROL QUALIAIVE ANALYSIS mpae wih he in-huse daa n qualiaive basis unknwn maeial
More informationExample
hapte Exaple.6-3. ---------------------------------------------------------------------------------- 5 A single hllw fibe is placed within a vey lage glass tube. he hllw fibe is 0 c in length and has a
More informationMEAN GRAVITY ALONG PLUMBLINE. University of New Brunswick, Department of Geodesy and Geomatics Engineering, Fredericton, N.B.
MEA GRAVITY ALG PLUMBLIE Beh-Anne Main 1, Chis MacPhee, Rbe Tenze 1, Pe Vaníek 1 and Macel Sans 1 1. Inducin 1 Univesiy f ew Bunswick, Depamen f Gedesy and Gemaics Engineeing, Fedeicn,.B., E3B 5A3, Canada
More informationDiffusivity Equation
Perleum Enineerin 34 Reservir Perfrmane Diffusiviy Equain 13 February 008 Thmas A. lasiname, Ph.D., P.E. Dilhan Il Dearmen f Perleum Enineerin Dearmen f Perleum Enineerin Texas A&M Universiy Texas A&M
More information11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work
MÜHENDİSLİK MEKNİĞİ. HFT İş-Eneji Pwe f a fce: Pwe in he abiliy f a fce d wk F: The fce applied n paicle Q P = F v = Fv cs( θ ) F Q v θ Pah f Q v: The velciy f Q ÖRNEK: İŞ-ENERJİ ω µ k v Calculae he pwe
More information2. The units in which the rate of a chemical reaction in solution is measured are (could be); 4rate. sec L.sec
Kineic Pblem Fm Ramnd F. X. Williams. Accding he equain, NO(g + B (g NOB(g In a ceain eacin miue he ae f fmain f NOB(g was fund be 4.50 0-4 ml L - s -. Wha is he ae f cnsumpin f B (g, als in ml L - s -?
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationDetermining Well Test Pore Compressibility from Tidal Analysis
Deemining Well Tes Poe omessibiliy om Tidal Analysis Bob Foulse Deision Managemen Ld 9 Abbey See ene Abbas Dohese Dose DT2 7JQ Unied Kingdom Tel: E Mail: +44 (0) 1300 341311 boulse@deisionman.o.uk 1 1
More informationSuperluminal Near-field Dipole Electromagnetic Fields. 1 Introduction. 2 Analysis of electric dipole. 2.1 General solution
Supeluinal Nea-field Diple Eleanei Fields Willia D. Wale KTH-Visby Caéaan SE-6 7 Visby, Sweden Eail: bill@visby.h.se Pesened a: Inenainal Wshp Lenz Gup, CPT and Neuins Zaaeas, Mexi, June -6, 999 Induin
More informationPhysics 140. Assignment 4 (Mechanics & Heat)
Physis 14 Assignen 4 (Mehanis & Hea) This assignen us be handed in by 1 nn n Thursday 11h May. Yu an hand i in a he beginning f he leure n ha day r yu ay hand i yur labrary densrar befrehand if yu ish.
More informationLecture 9. Transport Properties in Mesoscopic Systems. Over the last 1-2 decades, various techniques have been developed to synthesize
eue 9. anspo Popeies in Mesosopi Sysems Ove he las - deades, vaious ehniques have been developed o synhesize nanosuued maeials and o fabiae nanosale devies ha exhibi popeies midway beween he puely quanum
More information`Derivation of Weinberg s Relation in a Inflationary Universe
1 `Derivain f Weinberg s Relain in a Inflainary Universe Iannis Iraklis aranas Yrk Universiy Deparen f Physis and Asrny 1A Perie Building Nrh Yrk, Onari MJ-1P CANADA e ail: iannis@yrku.a Absra We prpse
More informationSubject: Turbojet engines (continued); Design parameters; Effect of mass flow on thrust.
16.50 Leure 19 Subje: Turbje engines (ninued; Design parameers; Effe f mass flw n hrus. In his haper we examine he quesin f hw hse he key parameers f he engine bain sme speified perfrmane a he design ndiins,
More informationEngineering Accreditation. Heat Transfer Basics. Assessment Results II. Assessment Results. Review Definitions. Outline
Hea ansfe asis Febua 7, 7 Hea ansfe asis a Caeo Mehanial Engineeing 375 Hea ansfe Febua 7, 7 Engineeing ediaion CSUN has aedied pogams in Civil, Eleial, Manufauing and Mehanial Engineeing Naional aediing
More informationFitness-For-Service API 579-1/ASME FFS-1, JUNE 5, 2007 (API 579 SECOND EDITION) ERRATA February 2009
Finess-F-Sevie PI 579-/SME FFS-, JUNE 5, 007 (PI 579 SECOND EDITION) ERRT Febuay 009 Suay f Eaa and Ediial Changes f PI-579--SME_FFS-_Finess f Sevie Sunday, Febuay, 009 Sein Paagaph/Figue/Table Desipin
More information5.1 Angles and Their Measure
5. Angles and Their Measure Secin 5. Nes Page This secin will cver hw angles are drawn and als arc lengh and rains. We will use (hea) represen an angle s measuremen. In he figure belw i describes hw yu
More informationLecture 3: Resistive forces, and Energy
Lecure 3: Resisive frces, and Energy Las ie we fund he velciy f a prjecile ving wih air resisance: g g vx ( ) = vx, e vy ( ) = + v + e One re inegrain gives us he psiin as a funcin f ie: dx dy g g = vx,
More informationMaxwell Equations. Dr. Ray Kwok sjsu
Maxwell quains. Ray Kwk sjsu eeence: lecmagneic Fields and Waves, Lain & Csn (Feeman) Inducin lecdynamics,.. Giihs (Penice Hall) Fundamenals ngineeing lecmagneics,.k. Cheng (Addisn Wesley) Maxwell quains.
More information4/3/2017. PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103
PHY 7 Eleodnais 9-9:50 AM MWF Olin 0 Plan fo Leue 0: Coninue eading Chap Snhoon adiaion adiaion fo eleon snhoon deies adiaion fo asonoial objes in iula obis 0/05/07 PHY 7 Sping 07 -- Leue 0 0/05/07 PHY
More informationUIUC Physics 436 EM Fields & Sources II Fall Semester, 2015 Lect. Notes 14 Prof. Steven Errede LECTURE NOTES 14
UIUC Physis 46 EM Fields & Sues II Fall Semese, 05 Le. Nes 4 Pf. Seven Eede LECTURE NOTES 4 EM RADIATION FROM AN ARBITRARY SOURCE: We nw apply he fmalism/mehdlgy ha we have develped in he pevius leues
More informationSharif University of Technology - CEDRA By: Professor Ali Meghdari
Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationPhysics 442. Electro-Magneto-Dynamics. M. Berrondo. Physics BYU
Physis 44 Eleo-Magneo-Dynamis M. Beondo Physis BYU Paaveos Φ= V + Α Φ= V Α = = + J = + ρ J J ρ = J S = u + em S S = u em S Physis BYU Poenials Genealize E = V o he ime dependen E & B ase Podu of paaveos:
More informationJournal home page :
Jounal hoe page : hp://www.sienedie.o/siene/ounal/00460x Sabiliy analysis of oaing beas ubbing on an elasi iula suue Jounal of Sound and Vibaion, Volue 99, Issues 4-5, 6 Febuay 007, Pages 005-03 N. Lesaffe,
More informationTwo-Pion Exchange Currents in Photodisintegration of the Deuteron
Two-Pion Exchange Cuens in Phoodisinegaion of he Deueon Dagaa Rozędzik and Jacek Goak Jagieonian Univesiy Kaków MENU00 3 May 00 Wiiasbug Conen Chia Effecive Fied Theoy ChEFT Eecoagneic cuen oeaos wihin
More informationPiezoelectric anisotropy of a KNbO3 single crystal
Piezelei anispy f a KNbO3 single ysal Linyun Liang, Y. L. Li, S. Y. Hu, Lng-Qing Chen, and Guang-Hng Lu Ciain: J. Appl. Phys. 18, 94111 (21); di: 1.163/1.3511336 View nline: hp://dx.di.g/1.163/1.3511336
More informationβ A Constant-G m Biasing
p 2002 EE 532 Anal IC Des II Pae 73 Cnsan-G Bas ecall ha us a PTAT cuen efeence (see p f p. 66 he nes) bas a bpla anss pes cnsan anscnucance e epeaue (an als epenen f supply lae an pcess). Hw h we achee
More informationThe Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components
Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due
More informationFig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial
a b c Fig. S. The anenna consucion: (a) ain geoeical paaees, (b) he wie suppo pilla and (c) he console link beween wie and coaial pobe. Fig. S. The anenna coss-secion in he y-z plane. Accoding o [], he
More informationUIUC Physics 436 EM Fields & Sources II Fall Semester, 2015 Lect. Notes 13 Prof. Steven Errede LECTURE NOTES 13
UIUC Physis 436 EM Fields & Sues II Fall Semese, 015 Le. Nes 13 Pf. Seven Eede LECTURE NOTES 13 ELECTROMAGNETIC RADIATION In P436 Le. Nes 4-10.5 (Giffihs h. 9-10}, we disussed he ppagain f maspi EM waves,
More informationBrace-Gatarek-Musiela model
Chaper 34 Brace-Gaarek-Musiela mdel 34. Review f HJM under risk-neural IP where f ( T Frward rae a ime fr brrwing a ime T df ( T ( T ( T d + ( T dw ( ( T The ineres rae is r( f (. The bnd prices saisfy
More informationSTUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION
Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE
More informationMotor development 7/1 Mechanical motor design
oo developen 7/ ehanial oo design 7. ehanial oo design ehanial oo design is as vial as he eleoagnei oo design o build good oos. This opises quesions onening he - oo balaning, - oo beaing syses, - ooling
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationLecture 3. Electrostatics
Lecue lecsics In his lecue yu will len: Thee wys slve pblems in elecsics: ) Applicin f he Supepsiin Pinciple (SP) b) Applicin f Guss Lw in Inegl Fm (GLIF) c) Applicin f Guss Lw in Diffeenil Fm (GLDF) C
More informationLinear Quadratic Regulator (LQR) - State Feedback Design
Linear Quadrai Regulaor (LQR) - Sae Feedbak Design A sysem is expressed in sae variable form as x = Ax + Bu n m wih x( ) R, u( ) R and he iniial ondiion x() = x A he sabilizaion problem using sae variable
More informationFBD of SDOF Base Excitation. 2.4 Base Excitation. Particular Solution (sine term) SDOF Base Excitation (cont) F=-(-)-(-)= 2ζω ωf
.4 Base Exiaio Ipoa lass of vibaio aalysis Peveig exiaios fo passig fo a vibaig base hough is ou io a suue Vibaio isolaio Vibaios i you a Saellie opeaio Dis dives, e. FBD of SDOF Base Exiaio x() y() Syse
More informationNeutron Slowing Down Distances and Times in Hydrogenous Materials. Erin Boyd May 10, 2005
Neu Slwig Dw Disaces ad Times i Hydgeus Maeials i Byd May 0 005 Oulie Backgud / Lecue Maeial Neu Slwig Dw quai Flux behavi i hydgeus medium Femi eame f calculaig slwig dw disaces ad imes. Bief deivai f
More informationAlgebra 2A. Algebra 2A- Unit 5
Algeba 2A Algeba 2A- Ui 5 ALGEBRA 2A Less: 5.1 Name: Dae: Plymial fis O b j e i! I a evalae plymial fis! I a ideify geeal shapes f gaphs f plymial fis Plymial Fi: ly e vaiable (x) V a b l a y a :, ze a
More informationDepartment of Chemical Engineering University of Tennessee Prof. David Keffer. Course Lecture Notes SIXTEEN
D. Keffe - ChE 40: Hea Tansfe and Fluid Flow Deamen of Chemical Enee Uniesi of Tennessee Pof. Daid Keffe Couse Lecue Noes SIXTEEN SECTION.6 DIFFERENTIL EQUTIONS OF CONTINUITY SECTION.7 DIFFERENTIL EQUTIONS
More informationNSEP EXAMINATION
NSE 00-0 EXAMINATION CAEE OINT INDIAN ASSOCIATION OF HYSICS TEACHES NATIONAL STANDAD EXAMINATION IN HYSICS 00-0 Tal ie : 0 inues (A-, A- & B) AT - A (Tal Maks : 80) SUB-AT A- Q. Displaceen f an scillaing
More informationThe shortest path between two truths in the real domain passes through the complex domain. J. Hadamard
Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal
More informationStress Analysis of Infinite Plate with Elliptical Hole
Sess Analysis of Infinie Plae ih Ellipical Hole Mohansing R Padeshi*, D. P. K. Shaa* * ( P.G.Suden, Depaen of Mechanical Engg, NRI s Insiue of Infoaion Science & Technology, Bhopal, India) * ( Head of,
More information7 Wave Equation in Higher Dimensions
7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,
More informationELECTRONIC JOURNAL OF POLISH AGRICULTURAL UNIVERSITIES
Elerni Jurnal f Plish Agriulural Universiies is he very firs Plish sienifi jurnal published elusively n he Inerne funded n January 998 by he fllwing agriulural universiies and higher shls f agriulure:
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Finie Diffeence Mehod fo Odinay Diffeenial Eqaions Afe eading his chape, yo shold be able o. Undesand wha he finie diffeence mehod is and how o se i o solve poblems. Wha is he finie diffeence
More informationHeat transfer between shell and rigid body through the thin heat-conducting layer taking into account mechanical contact
Advanced Cmpuainal Meds in Hea Tansfe X 8 Hea ansfe beween sell and igid bdy ug e in ea-cnducing laye aking in accun mecanical cnac V. V. Zzulya Cen de Invesigación Cienífica de Yucaán, Méida, Yucaán,
More informationr r r r r EE334 Electromagnetic Theory I Todd Kaiser
334 lecoagneic Theoy I Todd Kaise Maxwell s quaions: Maxwell s equaions wee developed on expeienal evidence and have been found o goven all classical elecoagneic phenoena. They can be wien in diffeenial
More informationEstimation Method of Natural Water Bodies in the Fracture Cavity Carbonate Reservoir of the Sea
Advanes in Peoleu Exloaion and eveloen Vol 3, o, 7, 5-3 OI:3968/9599 ISS 95-54X [Pin] ISS 95-5438 [Online] sanadane sanadaog Esiaion Mehod o aual Wae Bodies in he Faue Caviy Cabonae Resevoi o he Sea ZHAG
More informationSMKA NAIM LILBANAT KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI. Kertas soalan ini mengandungi 7 halaman bercetak.
Name : Frm :. SMKA NAIM LILBANAT 55 KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI PEPERIKSAAN PERCUBAAN SPM / ADDITIONAL MATHEMATICS Keras ½ Jam ½ Jam Unuk Kegunaan Pemeriksa Arahan:. This quesin paper
More informationIrrItrol Products 2016 catalog
l Ps Valves 205, 200 an 2500 eies Valves M Pa Nmbe -205F 1" n-line E Valve w/ FC - se 2500 eies 3* -200 1" E n-line Valve w/ FC F x F 3-200F 1" n-line Valve w/ FC F x F -2500 1" E Valve w/ FC F x F -2500F
More informationSPE μ μ μ ...(1) r r. t p
PE 80534 Pemane Pediin a Well Unde Mulihase Fl Cndiins T Mahaendajana, T Aiadji, and AK Pemadi; nsiu Tenli andun Cyih 003, iey Peleum Eninees n This ae as eaed esenain a he PE Asia Paii Oil and Gas Cneene
More informationA) (0.46 î ) N B) (0.17 î ) N
Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.
More informationKINGS UNIT- I LAPLACE TRANSFORMS
MA5-MATHEMATICS-II KINGS COLLEGE OF ENGINEERING Punalkulam DEPARTMENT OF MATHEMATICS ACADEMIC YEAR - ( Even Semese ) QUESTION BANK SUBJECT CODE: MA5 SUBJECT NAME: MATHEMATICS - II YEAR / SEM: I / II UNIT-
More informationFinal Exam. Tuesday, December hours, 30 minutes
an Faniso ae Univesi Mihael Ba ECON 30 Fall 04 Final Exam Tuesda, Deembe 6 hous, 30 minues Name: Insuions. This is losed book, losed noes exam.. No alulaos of an kind ae allowed. 3. how all he alulaions.
More informationdp p v= = ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945).
ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945). It is shown that at lage distanes fom the body, moving with a. veloity exeeding that of
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationTransient Radial Flow Toward a Well Aquifer Equation, based on assumptions becomes a 1D PDE for h(r,t) : Transient Radial Flow Toward a Well
ansien Radial Flw wad a Well Aqife Eqain, based n assmpins becmes a D PDE f h(,) : -ansien flw in a hmgenes, ispic aqife -flly peneaing pmping well & infinie, hiznal, cnfined aqife f nifm hickness, hs
More informationLecture 22 Electromagnetic Waves
Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should
More informationVisco-elastic Layers
Visc-elasic Layers Visc-elasic Sluins Sluins are bained by elasic viscelasic crrespndence principle by applying laplace ransfrm remve he ime variable Tw mehds f characerising viscelasic maerials: Mechanical
More informationPseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)
Pseudoseady-Sae Flow Relaions fo a Radial Sysem fom Deamen of Peoleum Engineeing Couse Noes (1997) (Deivaion of he Pseudoseady-Sae Flow Relaions fo a Radial Sysem) (Deivaion of he Pseudoseady-Sae Flow
More informationAP Physics 1 MC Practice Kinematics 1D
AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec
More informationPhysics Courseware Physics I Constant Acceleration
Physics Curseware Physics I Cnsan Accelerain Equains fr cnsan accelerain in dimensin x + a + a + ax + x Prblem.- In he 00-m race an ahlee acceleraes unifrmly frm res his p speed f 0m/s in he firs x5m as
More informationA) N B) 0.0 N C) N D) N E) N
Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce
More informationExtra Examples for Chapter 1
Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is
More information, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t
Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission
More informationNon-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:
hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of
More informationFundamental Vehicle Loads & Their Estimation
Fundaenal Vehicle Loads & Thei Esiaion The silified loads can only be alied in he eliinay design sage when he absence of es o siulaion daa They should always be qualified and udaed as oe infoaion becoes
More informationCHAPTER 5. Exercises. the coefficient of t so we have ω = 200π
HPTER 5 Exerises E5. (a) We are given v ( ) 5 s(π 3 ). The angular frequeny is he effiien f s we have ω π radian/s. Then f ω / π Hz T / f ms m / 5 / 6. Furhermre, v() aains a psiive peak when he argumen
More informationOn Control Problem Described by Infinite System of First-Order Differential Equations
Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical
More information5. Differential Amplifiers
5. iffeential plifies eain: Sea & Sith: Chapte 8 MOS ptins an Chapte.. ECE, Winte, F. Najabai iffeential an Cn-Me Sinals Cnsie a linea iuit with TWO inputs By supepsitin: efine: iffeene iffeential Me Cn
More information1121 T Question 1
1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed
More informationPHYS PRACTICE EXAM 2
PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,
More informationCHAPTER 24 GAUSS LAW
CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and
More informationAnswers to Coursebook questions Chapter 2.11
Answes to Couseook questions Chapte 11 1 he net foe on the satellite is F = G Mm and this plays the ole of the entipetal foe on the satellite, ie mv mv Equating the two gives π Fo iula motion we have that
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationSchool of Chemical & Biological Engineering, Konkuk University
Schl f Cheical & Bilgical Engineeing, Knkuk Univesity Lectue 7 Ch. 2 The Fist Law Thecheisty Pf. Y-Sep Min Physical Cheisty I, Sping 2008 Ch. 2-2 The study f the enegy tansfeed as heat duing the cuse f
More informationDiffusivity Equations (Governing Flow Relations)
Diffusiviy Equains (Gvernin Fl Relains) Thmas A. lasiname, Ph.D., P.E. Dearmen f Perleum Enineerin Texas A&M Universiy Cllee Sain, TX 77843-3116 (USA) +1.979.845.9 -blasiname@amu.edu Orienain Diffusiviy
More informationEN221 - Fall HW # 7 Solutions
EN221 - Fall2008 - HW # 7 Soluions Pof. Vivek Shenoy 1.) Show ha he fomulae φ v ( φ + φ L)v (1) u v ( u + u L)v (2) can be pu ino he alenaive foms φ φ v v + φv na (3) u u v v + u(v n)a (4) (a) Using v
More informationNotes on Inductance and Circuit Transients Joe Wolfe, Physics UNSW. Circuits with R and C. τ = RC = time constant
Nes n Inducance and cu Tansens Je Wlfe, Physcs UNSW cus wh and - Wha happens when yu clse he swch? (clse swch a 0) - uen flws ff capac, s d Acss capac: Acss ess: c d s d d ln + cns. 0, ln cns. ln ln ln
More informationPart I. Labor- Leisure Decision (15 pts)
Eon 509 Sping 204 Final Exam S. Paene Pa I. Labo- Leisue Deision (5 ps. Conside he following sai eonom given b he following equaions. Uili ln( H ln( l whee H sands fo he househ f f Poduion: Ah whee f sands
More informationControl Volume Derivation
School of eospace Engineeing Conol Volume -1 Copyigh 1 by Jey M. Seizman. ll ighs esee. Conol Volume Deiaion How o cone ou elaionships fo a close sysem (conol mass) o an open sysem (conol olume) Fo mass
More informationLaplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff
Laplace ransfom: -ranslaion rule 8.03, Haynes Miller and Jeremy Orloff Inroducory example Consider he sysem ẋ + 3x = f(, where f is he inpu and x he response. We know is uni impulse response is 0 for
More information3 ) = 10(1-3t)e -3t A
haper 6, Sluin. d i ( e 6 e ) 0( - )e - A p i 0(-)e - e - 0( - )e -6 W haper 6, Sluin. w w (40)(80 (40)(0) ) ( ) w w w 0 0 80 60 kw haper 6, Sluin. i d 80 60 40x0 480 ma haper 6, Sluin 4. i (0) 6sin 4-0.7
More informationProblem Set 9 Due December, 7
EE226: Random Proesses in Sysems Leurer: Jean C. Walrand Problem Se 9 Due Deember, 7 Fall 6 GSI: Assane Gueye his problem se essenially reviews Convergene and Renewal proesses. No all exerises are o be
More informationCHE CHAPTER 11 Spring 2005 GENERAL 2ND ORDER REACTION IN TURBULENT TUBULAR REACTORS
CHE 52 - CHPTE Sping 2005 GENEL 2ND ODE ECTION IN TUULENT TUUL ECTOS Vassilats & T, IChEJ. (4), 666 (965) Cnside the fllwing stichiety: a + b = P The ass cnsevatin law f species i yields Ci + vci =. Di
More informationThe 37th International Physics Olympiad Singapore. Experimental Competition. Wednesday, 12 July, Sample Solution
The 37h Inernainal Physics Olypiad Singapre Experienal Cpeiin Wednesday, July, 006 Saple Sluin Par a A skech f he experienal seup (n required) Receiver Raing able Gnieer Fixed ar Bea splier Gnieer Mvable
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationUSING PHASED ARRAY TECHNOLOGY AND EMBEDDED ULTRASONIC STRUCTURAL RADAR FOR ACTIVE STRUCTURAL HEALTH MONITORING AND NONDESTRUCTIVE EVALUATION
Poeedings of IMECE 25: 25 ASME Inenaional Mehanial Engineeing Congess Novebe 5-3, Olando, Floida IMECE25-8227 USING PHASED ARRAY TECHNOLOGY AND EMBEDDED ULTRASONIC STRUCTURAL RADAR FOR ACTIVE STRUCTURAL
More informationPRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271.
PRINCE SULTAN UNIVERSITY Deparmen f Mahemaical Sciences Final Examinain Secnd Semeser 007 008 (07) STAT 7 Suden Name Suden Number Secin Number Teacher Name Aendance Number Time allwed is ½ hurs. Wrie dwn
More information6. Frequency Response
6. Frequency esnse eading: Sedra & Sith: hater.6, hater 3.6 and hater 9 (MOS rtins, EE 0, Winter 0, F. Najabadi Tyical Frequency resnse an liier U t nw we have ignred the caacitrs. T include the caacitrs,
More informationModule 4: Time Response of discrete time systems Lecture Note 2
Module 4: Time Response of discree ime sysems Lecure Noe 2 1 Prooype second order sysem The sudy of a second order sysem is imporan because many higher order sysem can be approimaed by a second order model
More informationdm dt = 1 V The number of moles in any volume is M = CV, where C = concentration in M/L V = liters. dcv v
Mg: Pcess Aalyss: Reac ae s defed as whee eac ae elcy lue M les ( ccea) e. dm he ube f les ay lue s M, whee ccea M/L les. he he eac ae beces f a hgeeus eac, ( ) d Usually s csa aqueus eeal pcesses eac,
More informationHeat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating
ISSN(Online): 319-8753 ISSN (Pin): 347-671 Inenaional Jounal of Innovaive Reseac in Science, Engineeing and Tecnology (An ISO 397: 7 Ceified Oganiaion) Vol 4, Issue 1, Decembe 15 Hea Concion Poblem in
More informationthe Crustal Magnetic Field for and Any Drilling Time Xiong Li and Benny Poedjono in Paris on March 8, 2013
An Accurae Deerinain f he rusal Magneic Field fr Any eference Mdel and Any Drilling Tie ing Li and enny Pedjn in Paris n March 8, 03 4 Slides fr he Presenain in San Anni Is he vecr crusal agneic field
More informationModeling Micromixing Effects in a CSTR
delig irixig Effes i a STR STR, f all well behaved rears, has he wides RTD i.e. This eas ha large differees i perfrae a exis bewee segregaed flw ad perais a axiu ixedess diis. The easies hig rea is he
More informationTwo-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch
Two-dimensional Effecs on he CS Ineacion Foces fo an Enegy-Chiped Bunch ui Li, J. Bisognano,. Legg, and. Bosch Ouline 1. Inoducion 2. Pevious 1D and 2D esuls fo Effecive CS Foce 3. Bunch Disibuion Vaiaion
More information