An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics
|
|
- Easter Higgins
- 5 years ago
- Views:
Transcription
1 Adv Theo Appl Mech Vol no An Analyical Sdy of Song Non Plane Shock Waves in Magneogasdynaics L P Singh Depaen of Applied Maheaics Insie of Technology Banaas Hind Univesiy Vaanasi-5 India Akal Hsain Depaen of Applied Maheaics Insie of Technology and DST-CIMS Banaas Hind Univesiy Vaanasi-5 India ahsainsap@ibhacin M Singh Depaen of Applied Maheaics Insie of Technology Banaas Hind Univesiy Vaanasi-5 India Absac An analyical appoach is sed o deive a new exac solion of a poble of onediensional nseady adiabaic flow of a plane and cylindical song shock wave popagaing in a plasa whose densiy ahead of he shock fon is assed o vay as a powe of he disance fo he soce of explosion The plasa is assed o be an ideal gas wih infinie elecical condciviy peeaed by a ansvese agneic field A coplee invesigaion is ade fo he cases of plane and cylindical flows in he pesence of agneic field An analyical solion of he poble is obained in es of flow vaiables velociy densiy and he pesse in he pesence of he agneic field which exhibis space ie dependence Also he analyical expession fo he oal enegy nde he inflence of ansvese agneic field is deeined
2 9 L P Singh A Hsain and M Singh Maheaics Sbjec Classificaion: 76L5 76W5 Keywods: Shock waves Magneogasdynaics Rankine-Hgonio condiion Analyical solion Inodcion The occence of shock waves in a gaseos edi has dawn he aenion of seveal invesigaos ding pas decades The popagaion of shock waves nde he inflence of song agneic field consies a poble of gea inees o eseaches in a vaiey of fields sch as asophysics nclea science geophysics and plasa physics Koobeinikov [] Geifinge and Cole [] and Hne [] sdied he poble of blas wave popagaion in a hoogeneos and inhoogeneos edi The pioneeing sdies of his phenoenon wee caied o by Taylo and Sedov [4] and hei neical solion based on self-siilaiy consideaion wee fond in good ageeen wih expeienal esls A nbe of analyical solions fo he blas wave popagaion have been obained by Roges [5] Bach and Lee [6] Labach and Pobsein [7] Sachdev [8] Poslavskii [9] Chisnell [] and Maa [] Labach and Pobsein [7] and Sachdev [8] sed an appoach based on he shock popagaion heoy of Binkley and Kikwood [] which peis a siple analyical solion o be obained diecly fo he govening eqaions Chisnell [] povided an analyical solion of he poble of conveging shock waves by he sdy of singla poins of he diffeenial eqaions A fhe conibion owads he deeinaion of exac solion of gasdynaic eqaions involving disconiniies via Lie gop ansfoaion has been caied o by any ahos eg Olivei and Speciale [-4] Radha and Shaa [5] Pandey e al [6] Singh e al [7] Olivei and Speciale [-4] sed sbsiion pinciple o obain an exac solion fo nseady eqaion of pefec gas and ideal agneogasdynaic eqaion Roges [5] and Maa [] obained he closed fo solion fo spheical blas wave poble when he densiy of he gas ahead of he shock fon vaies as a powe of he disance fo he oigin Singh e al [7] sed he ehod of Lie gop ansfoaion o obain an appoxiae analyical solion o he syse of fis ode qasi-linea paial diffeenial eqaions ha govens a one diensional nseady plane cylindically syeic and spheically syeic oion in a non-ideal gas involving song shock waves In he pesen pape we have consideed he poble of popagaion of a onediensional nseady non-plane flow of an inviscid ideal gas peeaed by a ansvese agneic field wih infinie elecical condciviy I is assed ha ass densiy disibion in he edi follows a powe law of he adial disance fo he poin of explosion An analyical solion of he poble is obained in es of flow vaiables velociy densiy and he pesse in he pesence of he agneic field Also he analyical expession fo he oal enegy nde he
3 Analyical sdy of song non plane shock wave 9 inflence of ansvese agneic field is deeined To o knowledge sch an analyic solion inflenced by he ansvese agneic field which exhibis space ie dependence has no been discssed in he pas Folaion of he Poble Assing he elecical condciviy o be infinie and he diecion of he agneic field ohogonal o he ajecoies of he gas paicles he govening eqaions fo a one-diensional nseady non-plane oion can be wien as [8] ρ ρ ρ ) ρ / ) ρ p h ) ) p p a ρ ρ ) ) h h h h ) / 4) whee is he gas velociy; ρ is he densiy; p is he pesse; is he consan specific hea aio; is he ie; is he single spaial co-odinae being eihe axial in flows wih plane geoey o adial in cylindically syeic flows; a p / ρ is he eqilibi speed of sond ; h is he agneic pesse defined by h μh / wih μ as agneic peeabiliy and H is he ansvese agneic field; and coespond especively o plane and cylindical syey A coa followed by a sbscip o denoes paial diffeeniaion nless saed ohewise The syse of eqaion )-4) is sppleened wih an eqaion of sae p ρrt whee R is he gas consan and T is he epeae I is well known ha a shock wave ay be iniiaed in he flow egion and once i is foed i will popagae by sepaaing he poions of coninos egion A shock he coec genealized solion saisfies he Rankine- Hgonio jp condiions Le χ) be he song shock wih he shock speed W dχ d popagaing ino he edi chaaceized by ρ ρ ) p p ) h h ) 5) Theefoe he bonday condiions a he shock fon can be wien as [] a ρ ρ 6) W W a W p ρ W - a ) - C ρ W W ) a W 7) 8)
4 94 L P Singh A Hsain and M Singh ) a h Cρ W 9) ) W whee a is he sond speed of he ndisbed edi C o h / ρw is he shock Cowling nbe and he sffix denoe evalaion of he flow paaees js ahead of he shock especively Since he iniial enegy inp E of explosion is vey lage he shocks speed W >> a so ha a W in he song shock lii Theefoe he Rankine-Hgonio jp condiions in he case of song shock waves can be wien as ρ ρ W ) ) ) p ρw CρW h C ρw ) ) ) I is assed ha a ie an explosion akes place ove a plane o along a line accopanied by elease of a finie aon of enegy E A plane o cylindical song shock is insananeosly foed which begins o popagae owad ino a pefecly condcing gas a es The densiy ρ is assed o vay as he invese powe of he adial disance fo he soce of explosion δ ρ ρ c χ ) whee δ and ρ c ae consans The oal enegy E inside a blas wave is eqal o he enegy spplied by he explosive and hs consan The oal enegy is given by he expession W p ) E 4π ρ h) d ) which epesens he s of he kineic and inenal enegies of he gas Analyical Solion wih Shocks Wih he help of eqaion ) eqaion ) can be wien as C ) ) p ρ ρ h Cρ 8 ) 8 ) 4) Afe sing eqaion 4) he govening eqaions ) ) and 4) can be ansfoed o ρ ) ρ 5) ) ) 6)
5 Analyical sdy of song non plane shock wave 95 ) 7) Using eqaions 5) and 6) and hen inegaing wih espec o we ge ) ) ρ 8) whee ) is an abiay fncion of inegaion Using he solion 8) eqaion ) edces of he fo ) d d 9) On solving eqaions 6) and 9) we have d d η whee ) ) ) ) η ) Plgging in eqaion ) in eqaion 9) and hen inegaing we obained whee ) ) ) ) ) ) ) and is abiay consan Wih he help of bonday condiion ) we can obain he analyical expession of he disance χ as χ whee ) ) ) ) Using he Rankine-Hgonio jp condiion ) and powe law of he densiy ) gives a vale of he consan δ as ) ) ) ) δ ) Conseqenly wih he help of eqaion ) he analyical solions of he flow vaiables and oal enegy in he pesence of he agneic field is given by ) ) ) ) ) 8 8 ) ) ρ C h C p 4) In view of above solion 4) he analyical expession fo he oal enegy is given by ) ) ) 8 π C E 5) I ay be noed hee ha in he absence of he agneic field he analyical solions 4) and 5) obained in his anne which exhibis space ie
6 96 L P Singh A Hsain and M Singh dependence is a well known solion o he blas wave poble nde he consideaion ha he enegy eleased in he blas wave is conseved is caied o by vaios appoaches {[][]} 4 Conclding Reaks In he pesen invesigaion a siple analyic ehod is sed o obain he solion of he poble of he popagaion of a one-diensional nseady adiabaic non-plane shock wave hogh a pefecly condcing inviscid gas peeaed by a ansvese agneic field The densiy ahead of he shock fon is assed o vay accoding o powe of he disance fo he soce of explosion Hee i is assed ha he aospheic pesse and agneic pesse saisfy he elaed Rankine-Hgonio condiions aoaically Then he govening eqaions ae inegaed o povide he shock fon as a fncion of ie An exac solion of he poble in fo of powe in he disance and ie is obained I ay be eaked ha in he absence of he agneic field sch an analyical solions ae in close ageeen wih ealie esls obained {[] []} Acknowledgeens Ahos acknowledge he financial sppo fo DST- CIMS Banaas Hind Univesiy Vaanasi India Refeences [] V P Koobeinikov Pobles in he Theoy of Poin Explosions in Gases Povidence RI: Aeican Maheaical Sociey 976 [] C Geifinge and J D Cole Siilaiy solions fo cylindical agneohydodynaic blas waves Phys Flids 5 96) [] C Hne Siilaiy solions fo he flow ino a caviy J Flid Mech 5 96) 89-5 [4] L I Sedov Siilaiy and Diensional Mehods in Mechanics Acadeic Pess New Yok 959 [5] M H Roges Analyical solion fo he blas wave poble wih an aosphee of vaying densiy Asophysical J 5 957) [6] GG Bach and J H S Lee An analyical solion fo blas waves AIAA 8 97) 7-75 [7] DD Labach and R F Pobeisein A poin explosion in a cold aosphee Pa II Radiaing flow J Flid Mech 4 969) [8] P L Sachdev Popagaion of a blas wave in nifo o non-nifo edia: a nifoly valid analyic solion J Flid Mech 5 97) [9] S A Poslavskii A new class of exac solions wih shock waves in gas dynaics PMM )
7 Analyical sdy of song non plane shock wave 97 [] R F Chisnell An analyic descipion of conveging shock waves J Flid Mech ) [] S Maa New exac solion of he blas waves poble in gas dynaics Chos Solions & Facals 8 6) 7- \ [] S R Binkley and J G Kikwood Theoy of he popagaion of he shock wave Phys Rev Le 7 947) 66-6 [] F Olivei and M P Speciale Exac solions o he nseady eqaions of pefec gases hogh Lie gop analysis and sbsiion pinciples In J Non-linea Mech 7 ) [4] F Olivei and M P Speciale Exac solions o he ideal agneogasdynaic eqaions of pefec gases hogh Lie gop analysis and sbsiion pinciples J Phys A 8 5) [5] V D Shaa and R Radha Exac solions of Ele eqaions of ideal gasdynaics via Lie gop analysis ZAMP 59 8) 9-8 [6] M Pandey V D Shaa and R Radha Syey analysis and exac solion of agneogasdynaic eqaions Q J Mech Appl Mah 6 8) 9- [7] L P Singh Akal Hsain and M Singh An appoxiae analyical solion of iploding song shocks in a non-ideal gas hogh Lie gop analysis Chinese Phys Le 7 ) 47-)-47-4) [8] G B Whiha Linea and Non-linea Waves John Wiley & Sons New Yok 974 Received: Ocobe 9
The sudden release of a large amount of energy E into a background fluid of density
10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy
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 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 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 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 informationA FINITE-MEMORY DISCRETE-TIME CONVOLUTION APPROACH FOR THE NON-LINEAR DYNAMIC MODELLING OF S/H-ADC DEVICES
FINITE-MEMORY DISCRETE-TIME CONVOLUTION PPROCH FOR THE NON-LINER DYNMIC MODELLING OF S/H-DC DEVICES D. Mii, G. Pasini, P.. Taveso 2, F. Filicoi 2, G. Iclano 3 Depaen of Elecical Engineeing, Univesiy of
More informationSolvability of nonlinear Klein-Gordon equation by Laplace Decomposition Method
Vol. 84 pp. 37-4 Jly 5 DOI:.5897/JMCSR4.57 icle Nbe: 63F95459 ISSN 6-973 Copyigh 5 hos ein he copyigh of his icle hp://www.cdeicjonls.og/jmcsr ficn Jonl of Mheics nd Cope Science Resech Fll Lengh Resech
More informationInteraction of Lamb Waves with Geometric Discontinuities: An Analytical Approach Compared with FEM
Ineacion of Lamb Waves ih Geomeic Disconiniies: An Analyical Appoach Compaed ih FEM Banibaa Podda a) and Vico Gigii a) a) Depamen of Mechanical Engineeing, Univesiy of Soh Caolina, USA Absac. The non-descive
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 informationEffects of Heat Absorption and Porosity of the Medium on MHD Flow past a Vertical Plate
ailable online.ejae.o Eopean Jonal of danes in Engineeing and ehnology 7 4 4: 87-94 Reseah ile ISSN: 394-658X Effes of Hea bsopion and Poosiy of he Medi on MHD Flo pas a Veial Plae US Rajp and aa a Depaen
More informationPropagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface
Applied Mahemaical Sciences Vol. 7 no. 9 49 437 Popagaion of Tosional Sface Waves in Heeogeneos Half-Space wih Iegla Fee Sface M. M. Selim Depamen of Mahemaics Facly of Еdcaion Se Canal Univesiy Se Egyp
More informationEVENT HORIZONS IN COSMOLOGY
Mahemaics Today Vol7(Dec-)54-6 ISSN 976-38 EVENT HORIZONS IN COSMOLOGY K Punachanda Rao Depamen of Mahemaics Chiala Engineeing College Chiala 53 57 Andha Padesh, INDIA E-mail: dkpaocecc@yahoocoin ABSTRACT
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 informationGeneral Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security
1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid
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 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 informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More informationME 3560 Fluid Mechanics
ME3560 Flid Mechanics Fall 08 ME 3560 Flid Mechanics Analsis of Flid Flo Analsis of Flid Flo ME3560 Flid Mechanics Fall 08 6. Flid Elemen Kinemaics In geneal a flid paicle can ndego anslaion, linea defomaion
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 informationPhysics 207 Lecture 13
Physics 07 Lecue 3 Physics 07, Lecue 3, Oc. 8 Agenda: Chape 9, finish, Chape 0 Sa Chape 9: Moenu and Collision Ipulse Cene of ass Chape 0: oaional Kineaics oaional Enegy Moens of Ineia Paallel axis heoe
More informationMonochromatic Wave over One and Two Bars
Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,
More informationSome algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER
. Soe lgoi o solving syse o line vole inegl eqion o second ind by sing MATLAB 7 ALAN JALAL ABD ALKADER College o Edcion / Al- Msnsiiy Univesiy Depen o Meics تقديم البحث :-//7 قبول النشر:- //. Absc ( /
More informationScalar Conservation Laws
MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )
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 informationCritical statics and dynamics of QCD CEP
Ciical saics and dynamics of QCD CEP Eiji Nakano Dep. Physics, Kochi Univesiy, and ExeMe Mae Insie @ GSI,Gemany w/ B. Fiman, V. Skokov, K. Redlich, and B-J. Schaefe Conen: 1. Moivaion. Basics on ciical
More informationInternational Journal of Mathematical Archive-5(6), 2014, Available online through ISSN
Inenaional Jonal o Mahemaical Achive-6, 0, 09-8 Availale online hogh www.ijma.ino ISSN 9 06 EXISENCE OF NONOSCILLAORY SOLUIONS OF A CLASS OF NONLINEAR NEURAL DELAY DIFFERENIAL EQUAIONS OF HIRD ORDER K
More informationScholars Journal of Physics, Mathematics and Statistics
DOI:.76/sjps holas Jonal of Physis aheais and aisis h. J. Phys. ah. a. 7; :5- holas adei and ienifi Pblishes Pblishes n Inenaional Pblishe fo adei and ienifi Resoes IN 9-856 Pin IN 9-86 Online Effes of
More informationA Mathematical study of Two Species Amensalism Model With a Cover for the first Species by Homotopy Analysis Method
Available online a www.pelagiaeseachlibay.co Advances in Applied Science Reseach,, 3 (3):8-86 A Maheaical sudy of Two Species Aensalis Model Wih a Cove fo he fis Species by Hooopy Analysis Mehod B. Sia
More informationOutline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem
adial diffsio eqaio Febay 4 9 Diffsio Eqaios i ylidical oodiaes ay aeo Mechaical Egieeig 5B Seia i Egieeig Aalysis Febay 4, 9 Olie eview las class Gadie ad covecio boday codiio Diffsio eqaio i adial coodiaes
More informationInternational Journal of Pure and Applied Sciences and Technology
In. J. Pue Appl. Sci. Technol., 4 (211, pp. 23-29 Inenaional Jounal of Pue and Applied Sciences and Technology ISS 2229-617 Available online a www.ijopaasa.in eseach Pape Opizaion of he Uiliy of a Sucual
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 informationElastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density
Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially
More informationLecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light
Lecue 5 Chape 3 lecomagneic Theo, Phoons, and Ligh Gauss s Gauss s Faada s Ampèe- Mawell s + Loen foce: S C ds ds S C F dl dl q Mawell equaions d d qv A q A J ds ds In mae fields ae defined hough ineacion
More informationExact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method
Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
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 informationMEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING
MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens
More informationBMOA estimates and radial growth of B φ functions
c Jounal of echnical Univesiy a Plovdiv Fundamenal Sciences and Applicaions, Vol., 995 Seies A-Pue and Applied Mahemaics Bulgaia, ISSN 3-827 axiv:87.53v [mah.cv] 3 Jul 28 BMOA esimaes and adial gowh of
More informationr P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,
Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:
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 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 informationEuropean Option Pricing for a Stochastic Volatility Lévy Model with Stochastic Interest Rates
Jonal of Mahemaical Finance 98-8 doi:.436/mf..33 Pblished Online Noembe (hp://www.scirp.og/onal/mf) Eopean Opion Picing fo a Sochasic Volailiy Léy Model wih Sochasic Inees Raes Saisa Pinkham Paioe Saayaham
More informationD DAVID PUBLISHING. Simultaneous Exact Controllability of Wave Sound Propagations in Multilayer Media. 1. Introduction. v t q t.
Jornal of Maheaics and Syse Science 6 (6-9 doi:.765/59-59/6.8. D DAVID PUBLISHING Silaneos Exac Conrollabiliy of Wave Sond Propagaions in Mlilayer Media Alexis Rodrigez Carranza, Lis. J. Cacha, Obidio
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 informationEarthquake, Volcano and Tsunami
A. Merapi Volcano Erpion Earhqake, Volcano and Tsnami Qesion Answer Marks A. Using Black s Principle he eqilibrim emperare can be obained Ths,.5 A. For ideal gas, pv e e RTe, hs.3 A.3 The relaive velociy
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 informationNumerical Simulation of Reaction-Diffusion Systems of Turing Pattern Formation
Inernaional Jornal of Modern Nonlinear Theory and Applicaion 15 4 15-5 Pblished Online Deceber 15 in SciRes. hp://www.scirp.org/ornal/ina hp://dx.doi.org/1.436/ina.15.416 Nerical Silaion of Reacion-Diffsion
More informationNumerical Inversion of the Abel Integral Equation using Homotopy Perturbation Method
Numeical Invesion of the Abel Integal Equation using Homotopy Petubation Method Sunil Kuma and Om P Singh Depatment of Applied Mathematics Institute of Technology Banaas Hindu Univesity Vaanasi -15 India
More informationAn Exact Solution of Navier Stokes Equation
An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in
More information@FMI c Kyung Moon Sa Co.
Annals of Fuzzy Mahemaics Infomaics Volume, No. 2, (Apil 20), pp. 9-3 ISSN 2093 930 hp://www.afmi.o.k @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com On lacunay saisical convegence in inuiionisic fuzzy
More informationThe Method of Images in Velocity-Dependent Systems
>1< The Mehod of Images in Velociy-Dependen Sysems Dan Censo Ben Guion Univesiy of he Negev Depamen of Elecical and Compue Engineeing Bee Sheva, Isael 8415 censo@ee.bgu.ac.il Absac This sudy invesigaes
More informationPHYS GENERAL RELATIVITY AND COSMOLOGY PROBLEM SET 7 - SOLUTIONS
PHYS 54 - GENERAL RELATIVITY AND COSMOLOGY - 07 - PROBLEM SET 7 - SOLUTIONS TA: Jeome Quinin Mach, 07 Noe ha houghou hee oluion, we wok in uni whee c, and we chooe he meic ignaue (,,, ) a ou convenion..
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 informationWORK POWER AND ENERGY Consevaive foce a) A foce is said o be consevaive if he wok done by i is independen of pah followed by he body b) Wok done by a consevaive foce fo a closed pah is zeo c) Wok done
More informationPressure Vessels Thin and Thick-Walled Stress Analysis
Pessue Vessels Thin and Thick-Walled Sess Analysis y James Doane, PhD, PE Conens 1.0 Couse Oveview... 3.0 Thin-Walled Pessue Vessels... 3.1 Inoducion... 3. Sesses in Cylindical Conaines... 4..1 Hoop Sess...
More informationA Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method
Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen
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 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 informationOn the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources
Jounal of Applied Mahemaics and Physics 25 3 478-487 Published Online May 25 in SciRes. hp://www.scip.og/jounal/jamp hp://dx.doi.og/.4236/jamp.25.356 On he Semi-Discee Davey-Sewason Sysem wih Self-Consisen
More informationON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS
Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol. 8 9-33, Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy
More informationMethod for simulation of the fractional order chaotic systems
Aca Monanisica Slovaca Ročník (26), číslo 4, 273-277 Mehod fo siulaion of he facional ode chaoic syses Ivo Peáš Absac This pape deals wih he ehod of siulaion of facional ode chaoic syses. We pesen a bief
More informationDispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems.
Dispersive Sysems 1) Schrödinger eqaion ) Cbic Schrödinger 3) KdV 4) Discreerised hyperbolic eqaion 5) Discree sysems KdV + + ε =, = ( ) ( ) d d + = d d =, =. ( ) = ( ) DISCONTINUITY, prescribed cri Collision
More informationDYNAMIC ION BEHAVIOR IN PLASMA SOURCE ION IMPLANTATION BİLGE BOZKURT
B. BOZKURT METU 6 DYNAMIC ION BEHAVIOR IN PLASMA SOURCE ION IMPLANTATION BİLGE BOZKURT JANUARY 6 DYNAMIC ION BEHAVIOR IN PLASMA SOURCE ION IMPLANTATION A THESIS SUBMITTED TO THE GRADUATE SCHOOL OF NATURAL
More informationLecture 23: Central Force Motion
Lectue 3: Cental Foce Motion Many of the foces we encounte in natue act between two paticles along the line connecting the Gavity, electicity, and the stong nuclea foce ae exaples These types of foces
More informationAn Automatic Door Sensor Using Image Processing
An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion
More informationExtremal problems for t-partite and t-colorable hypergraphs
Exemal poblems fo -paie and -coloable hypegaphs Dhuv Mubayi John Talbo June, 007 Absac Fix ineges and an -unifom hypegaph F. We pove ha he maximum numbe of edges in a -paie -unifom hypegaph on n veices
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More information4. Fundamental of A.C. Circuit
4. Fundaenal of A.. icui 4. Equaion fo geneaion of alenaing induce EMF An A geneao uses he pinciple of Faaday s elecoagneic inducion law. saes ha when cuen caying conduco cu he agneic field hen ef induced
More informationAdsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity
The Open-Access Jounal fo the Basic Pinciples of Diffusion Theoy, Expeient and Application Adsoption and Desoption Kinetics fo Diffusion Contolled Systes with a Stongly Concentation Dependent Diffusivity
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 informationIntegration of the constitutive equation
Inegaion of he consiive eqaion REMAINDER ON NUMERICAL INTEGRATION Analyical inegaion f ( x( ), x ( )) x x x f () Exac/close-fom solion (no always possible) Nmeical inegaion. i. N T i N [, T ] [ i, i ]
More informationA GENERAL METHOD TO STUDY THE MOTION IN A NON-INERTIAL REFERENCE FRAME
The Inenaional onfeence on opuaional Mechanics an Viual Engineeing OME 9 9 OTOBER 9, Basov, Roania A GENERAL METHOD TO STUDY THE MOTION IN A NON-INERTIAL REFERENE FRAME Daniel onuache, Vlaii Mainusi Technical
More informationThe Global Trade and Environment Model: GTEM
The Global Tade and Envionmen Model: A pojecion of non-seady sae daa using Ineempoal GTEM Hom Pan, Vivek Tulpulé and Bian S. Fishe Ausalian Bueau of Agiculual and Resouce Economics OBJECTIVES Deive an
More informationENERGY CONTENT OF GRAVITATION AS A WAY TO QUANTIFY BOTH ENTROPY AND INFORMATION GENERATION IN THE EARLY UNIVERSE
ENERGY CONTENT OF GRAVITATION AS A WAY TO QUANTIFY BOTH ENTROPY AND INFORMATION GENERATION IN THE EARLY UNIVERSE ANDREW WALCOTT BECKWITH beckwih@iibep,og,abeckwih@uh.edu Chongquing Univesiy depaen o physics;
More informationInfluence of Velocity Slip on the Peristaltic Pumping of a Jeffrey Fluid in a Non Uniform Annulus
ISSN(Online): 39-8753 ISSN (Pin): 37-670 Inenaional Jonal of Innovaive Reseach in Science, Engineeing and Technoy (An ISO 397: 007 Ceified Oganiaion) ol. 5, Isse, Janay 06 Inflence of elociy Sli on he
More informationAbsorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere
Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in
More informationChapter 7. Interference
Chape 7 Inefeence Pa I Geneal Consideaions Pinciple of Supeposiion Pinciple of Supeposiion When wo o moe opical waves mee in he same locaion, hey follow supeposiion pinciple Mos opical sensos deec opical
More informationAN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS
AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe
More informationNotes on Optimal Control
F.L. Lewis Moncief-O Donnell Endowed Chai Head Conols & Sensos Gop Aomaion & Roboics Reseach Insie ARRI he Univesiy of eas a Alingon Noes on Opimal Conol Sppoed by : NSF - PAUL WERBOS ARO RANDY ZACHERY
More informationElectromagnetic Theory 1
/ lectomagnetic Theoy uestion : lectostatic Potential negy A sphee of adius caies a positive chage density ρ constant Obviously the spheical coodinates system is appopiate hee Take - C m - and cm τ a)
More informationA Stochastic EOQ Policy of Cold-Drink-For a Retailer
Vietnam Jounal of Mathematics 33:4 005) 437 44 9LHWQDP -RXUQDO RI 0$7+0$7,&6 9$67 A Stochastic EOQ Policy of Cold-Dink-Fo a Retaile Shib Sanka Sana 1 Kipasindhu Chaudhui 1 Depatment of Math., Bhanga Mahavidyalaya
More informationAn Open cycle and Closed cycle Gas Turbine Engines. Methods to improve the performance of simple gas turbine plants
An Open cycle and losed cycle Gas ubine Engines Mehods o impove he pefomance of simple gas ubine plans I egeneaive Gas ubine ycle: he empeaue of he exhaus gases in a simple gas ubine is highe han he empeaue
More informationCircular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.
1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule
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 informationEN40: Dynamics and Vibrations. Midterm Examination Tuesday March
EN4: Dynaics and Vibations Midte Exaination Tuesday Mach 8 16 School of Engineeing Bown Univesity NME: Geneal Instuctions No collaboation of any kind is peitted on this exaination. You ay bing double sided
More informationPerturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion
Commun. Theo. Phys. Beijing, China) 43 25) pp. 577 581 c Intenational Academic Publishes Vol. 43, No. 4, Apil 15, 25 Petubation to Symmeties and Adiabatic Invaiants of Nonholonomic Dynamical System of
More informationVariance and Covariance Processes
Vaiance and Covaiance Pocesses Pakash Balachandan Depamen of Mahemaics Duke Univesiy May 26, 2008 These noes ae based on Due s Sochasic Calculus, Revuz and Yo s Coninuous Maingales and Bownian Moion, Kaazas
More informationIntroduction to Arrays
Intoduction to Aays Page 1 Intoduction to Aays The antennas we have studied so fa have vey low diectivity / gain. While this is good fo boadcast applications (whee we want unifom coveage), thee ae cases
More informationATMO 551a Fall 08. Diffusion
Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path
More informationDual Hierarchies of a Multi-Component Camassa Holm System
Commun. heo. Phys. 64 05 37 378 Vol. 64, No. 4, Ocobe, 05 Dual Hieachies of a Muli-Componen Camassa Holm Sysem LI Hong-Min, LI Yu-Qi, and CHEN Yong Shanghai Key Laboaoy of uswohy Compuing, Eas China Nomal
More informationON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt
a 1/α s)ds < Indian J. pre appl. Mah., 396): 491-507, December 2008 c Prined in India. ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS SAID R. GRACE 1, RAVI P. AGARWAL 2 AND MUSTAFA
More informationMillennium Theory Equations Original Copyright 2002 Joseph A. Rybczyk Updated Copyright 2003 Joseph A. Rybczyk Updated March 16, 2006
Millennim heoy Eqaions Oiginal Copyigh 00 Joseph A. Rybzyk Updaed Copyigh 003 Joseph A. Rybzyk Updaed Mah 6, 006 Following is a omplee lis o he Millennim heoy o Relaiviy eqaions: Fo easy eeene, all eqaions
More informationAsymptotic Solution of the Anti-Plane Problem for a Two-Dimensional Lattice
Asympoic Solion of he Ani-Plane Problem for a Two-Dimensional Laice N.I. Aleksandrova N.A. Chinakal Insie of Mining, Siberian Branch, Rssian Academy of Sciences, Krasnyi pr. 91, Novosibirsk, 6391 Rssia,
More informationThermal Radiation and the Second Law of Thermodynamics
IOS Jounal of Applied Physics (IOS-JAP) e-issn: 2278-4861.olue 9, Issue 4 e. III (Jul. Aug. 2017), PP 82-89 www.iosjounals.og heal adiation and the Second Law of heodynaics * D. akhanlall echanical Engineeing,
More informationLINEAR MOMENTUM Physical quantities that we have been using to characterize the motion of a particle
LINEAR MOMENTUM Physical quantities that we have been using to chaacteize the otion of a paticle v Mass Velocity v Kinetic enegy v F Mechanical enegy + U Linea oentu of a paticle (1) is a vecto! Siple
More informationChapter 5. Canopy Spectral Invariants
Chape 5 Canopy Specal Invaians. Inoducion.... Physical Pinciples of Specal Invaians... 3. RT Theoy of Specal Invaians... 5 4. Scaling Popeies of Specal Invaians... 6 Poble Ses... 39 Refeences... 4. Inoducion
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 informationConvective Heat Transfer (6) Forced Convection (8) Martin Andersson
Convecive Hea Tansfe (6) Foced Convecion (8) Main Andesson Agenda Convecive hea ansfe Conini eq. Convecive dc flow (inodcion o ch. 8) Convecive hea ansfe Convecive hea ansfe Convecive hea ansfe f flid
More informationK. G. Malyutin, T. I. Malyutina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE
Математичнi Студiї. Т.4, 2 Maemaychni Sudii. V.4, No.2 УДК 57.5 K. G. Malyuin, T. I. Malyuina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE
More information