Effects of Couple Stress and Porous Medium on Transient Magneto Peristaltic Flow under the Action of Heat Transfer

Size: px
Start display at page:

Download "Effects of Couple Stress and Porous Medium on Transient Magneto Peristaltic Flow under the Action of Heat Transfer"

Transcription

1 IOSR Jonl of Meics IOSR-JM e-iss: ISS: 9-765X. Vole Isse Ve. V Jl. - Ag.6 PP Effecs of Cole Sess nd Poos Medi on nsien Mgneo Peislic Flow nde e Acion of He nsfe Aed M. Abdldi Al Wleed Sle Deen of Meics College of Science Uniesiy of Bgdd Bgdd Iq. Absc: Anlyicl nd coionl sdies on nsien eislic e flow og finie leng oos cnnel e esened in is e. e exession fo eee field xil elociy ole flow e esse diffeence locl wll se sess se fncion e obined nde e ssion of long weleng nd low Reynolds nbe. Effecs of diffeen ysicl ees eflecing cole-sess ee eebiliy ee Hn nbe consn e diion fco nd sof nbe s well s lide ion on ing cceisics nd ficionl foce se lines en nd ing of eislic flow en sdied wi icl esis.e effec of e nsfe on wo ineen enoen of eislic flow is discssed neiclly. is e inesiges e inflence of MHD on eislic flow of ewonin flid wi cole sess og oos edi wee e no-sli ssion beween wll nd e flid is no longe lid. Keywods: nsien eislic flow He nsfe Pesse gdien Locl wll se sess Cole sess Mgneic field Poos Medi. I. Inodcion Peislsis is nl ecnis of ing is obseed in e cse of os ysiologicl flids. is beio is slly ssocied wi ogessie we of e concion o exnsion long e leng of e bondy of flid-filled disensible be. is ecnis es lce in ny cicl linces inclding olle nd finge s e-lng cines blood cines dilysis cines nd lso nso of noxios flids in e ncle nd ceicl wse indsies.owing o e ionce of eislic flow soe significn inesigion on is sbjec e been eoed. Hisoiclly eislic flid dynics sdies wee iniied by Sio e l.969 wo eoeiclly exined e eislic flow of iscos flid indced by sinsoidl wll ogion. He nsfe ecniqes cnge e inenl enegy of bo syses inoled nd follow e fis lw of eodynics. He is genelly nsfeed fo objecs of ying eees i condcion nd conecion. Seel ocesses ely on e nsfe nd e coesonding el coefficiens. Seel os. Hy M.U. Qesi K.S. Meeie Y. Abd elbod 8 e eefoe eoed e inflence of e nsfe on eislic flow of ewonin nd non-ewonin flids Reine Rilin flid Jeffey-six consn flid second gde flid id ode flid fo gde flid Hescel Blley flid nd Jonson Segln flid wi o wio e effec of gneic field og nifo/nonnifo/syeic cnnels/eicl nnls syses nd lso oos edi. Fe ineesing sdies inclde e ecen es byabd elbod nd Meeie wic consideed el nso in nsien flow in eicl consiced nnls. A oos edi wic conins nbe of sll oles disibed ogo e e lys ey ole in e sdy of nso ocess in bio- flid ecnics indsil ecnics nd engineeing fields. A good exle of eislic in oos edi is focsed in inesinl flid dynics by Y. Miyoo e l.98&b.jeffey e l.. Soe os A.R. Ro M. Mis. Hy. Ali S. Asg7 sdied eislic flow of ewonin nd non- ewonin flids sc s owe lw flid gneo flid nd Mxwell flid og e oos edi. Hy M.U. Qesi Q. Hssin8inesiged e eislic flow wi e nsfe in oos sce.d. ii O.A. Beg eoed e inflence of e nsfe on nsedy ysiologicl gneo flid flow. D. ii. fe sdied e effec of e nsfe on eislic flow en og finie leng cnnel nd discssed e ic of ysicl ees on flow beio Wile e exended e eislic flow odel in D. ii.fo finie oos cnnel nd coe esls wi e esls of D. ii.in iew of e boe discssion in is e effec of e nsfe fo non- ewonin flid wi cole sess in MHD field og oos edi wi no sli bondy condiion nde e ssions of long we leng nd low Reynolds nbe. is nsien cole sess eislic flow of ewonin flid og finie leng cnnel wll og oos edi..in-bols esse disibion locl wll se sess nd elociy ofiles coed fo e effecs of e ey ydodynic ees.e inflence of ios einen ees on e flow cceisics Wee sdy e discssed og gs. DOI:.979/ Pge

2 DOI:.979/ Pge II. Meicl Folions Conside nsien eislic flow of iscos ewonin flid wi cole sess og oos edi in nifo cnnel wi e nsfe. Since we e consideing nifo cnnel eefoe e wll is inined eee nd de o syey e cene of e cnnel e cnge of e eee is en o be zeo wi consn seed c long e cnnel wlls. Fig : eoey of e oble e geoey of wll sfce see Fig. is descibed s : c cos Wee nd c eesen e nsese ibion of e wll e xil coodine ie e lf wid of e cnnel e lide of e we e weleng nd e we elociy eseciely. III.Bsic eqion e bsic eqions goening e non-ewonin flid flow nde e effec of nsese gneic field e gien by : e coniniy eqion : e oen eqions e : g B B c 5

3 DOI:.979/ Pge Wee is e flid densiy xil elociy nsese elociy nsese coodine esse iscosiy consn ssocied wi cole sess elecicl condciiy B nsese gneic field nd eebiliy ee g cceleion de o giy coefficien of line el exnsion of flid eee c secific e consn esse nd consn e ddiion / bsoion. eseciely. In ode o silify e goening eqions of e oion We inodcing e following diensionless ee : K c c c c P B M c c c g Re Wee is e we nbe Re Reynolds nbe is e cole sess ee M is e Hnn nbe K is e el condciiy sof nbe P Pndle nbe eee disibion nd consn e diion.sbsiing 6 ino eqions - 5 we obin e following non-diensionl eqions nd bondy condiions : cos 7. 8 M Re 9 c c c c c Re Re P e boe oble will be sole sbjec o e following bondy condiions : 6

4 DOI:.979/ Pge no sli condiion e egliy condiion e nising of cole sesses η = η = finie leng condiions l 5 e eee condiions 6 III. Solion of e oble e genel solion of e goening eqions 8 - in e genel cse sees o be iossible ; eefoe we sll confine e nlysis nde e ssion of sll diensionless we nbe. I follows δ. In oe wods we consideed e long - weleng oxiion. Along o is ssion eqions 8 - becoe : Wee K M e solion of Eq. sbjec o e ssocied bondy condiions 6 is fond of e fo.. Sbsied in Eq.8 nd e solion of Eq. 8 sbjec o e ssocied bondy condiion is fond of e fo cos cos cos cos Wee

5 DOI:.979/ Pge e locl wll se sess defined s w fe by sing Eq. n n w Vole flow e n ion ee in cnnel flows is defined s d Q wic on ineging Eq. yields : Q n n e following exession define e exising elion beween e eged flow e nd flow e in e we fe nd in e lbooy fe : Q q Q 5 A sile nilion of Eq. followed by licion of Eq. 5 yields e esse gdien s follows : f Q 6 f n n 7 Wic on inegion beween nd ξ genees e following exession fo esse diffeence : ds f Q 8 e esse diffeence l coss e one weleng wic on ilizing Eq.6 sses e fo : d l 9 Se fncion cn be obined by ineging eqion wi esec o η nd sing Eq. 6

6 6 f Q sin sin cos cos IV. eicl Resls nd Discssion In is secion e neicl nd coionl esls e discssed fo e oble of cole-sess ewonin flid in be wi oos edi og e gicl illsions. e nsien gneo - eislic flow of cole-sess flids og e oos edi wi effec of e nsfe e discssed og Figes -7. MAHEMAICA og is sed o find o neicl esls nd illsions. A. Bsed on Eq. 5 Figs.-5 illses e effecs of e ees ie sof nbe consn e diion nd eebiliy ee on e xil elociy disibion eseciely. Figes sow e elion beween xil elociy nd nsese dislceen. I is obseed e xil elociy ofile egion inceses wi incesing gnides of nd Wile elociy decese wen e oe ees incese finlly noiced e elociy e e og loced nd will be iniized e cnnel cene. B. Figs. 6-9 sows e inflence of e nsfe on locl wll se sess wi xil disnce long e leng of e cnnel ios insn.e elion beween locl se sess nd xil disnce is nonline wee e ces exibi bolic se. C. Figs. - illse e elion beween esse diffeence coss one weleng nd eged ole flow e exibis line elion beween e. fo e effec of nd. ole flow e incese wi incesing e gnide of sof nbe consn e diion. D. Figs.-6 illse e esse disibion long e leng of cnnel ios insns fo e inflence of nd ios ies wees l =.I is ysiclly ineeed if e nsfe is effecie en less esse is eqied fo e eislic flow of iscos flid og e cnnel. E. Figs.789dwn fo seline ens. e ics of sof ee consn e ee cole- sess ee Hn ee eebiliy ee nd ie e discssed og ese figes. I is ion o obsee e size of ing bols edces wen e gnide of sid ees M nd inceses. Fig. e xil elociy s. nsese dislceen fo diffeen les DOI:.979/ Pge

7 of wi M.6 5. Fig. e xil elociy s. nsese dislceen fo diffeen les of wi M.6 5. Fig. e xil elociy s. nsese dislceen fo diffeen les of wi M.6 5. Fig 5. e xil elociy s. nsese dislceen fo diffeen les DOI:.979/ Pge

8 of wi M.6. Fig 6. Locl wll se sess s. xil disnce fo diffeen les of wi M l.9 5. Fig 7. Locl wll se sess s. xil disnce fo diffeen les of wi. M l.9 5. Fig 8. Locl wll se sess s. xil disnce fo diffeen les of wi. M l.9 5. DOI:.979/ Pge

9 Fig 9. Locl wll se sess s. xil disnce fo diffeen les of wi M l.9.. Fig. e esse diffeence s. eged flow e fo diffeen les of wi l. M.. Fig. e esse diffeence s. eged flow e fo diffeen les of wi l. M.. DOI:.979/ Pge

10 Fig. e esse diffeence s. eged flow e fo diffeen les of wi l. M. Fig. e esse diffeence s. eged flow e fo diffeen les of wi l M.. Fig. e esse disibion s. xil disnce fo diffeen les of wi. M Q DOI:.979/ Pge

11 Fig 5. e esse disibion s. xil disnce fo diffeen les of wi. M Q Fig 6. e esse disibion s. xil disnce fo diffeen les of. M Q Fig 7. Seline in e we fe Q. 95 &. 5 Wen. M b.6 M DOI:.979/ Pge

12 c.9 M Fig 8. Seline in e we fe Q. 95 &. 5 Wen. M b 6. M c 9. M Fig 9. Seline in e we fe Q. 95 &. 5 Wen. M b. M c 8. M DOI:.979/ Pge

13 V. Conclding es we e discssed e inflence of e nsfe on nsien gneo eislic flow wi cole-sess flid og oos edi on ewonin flid in finie leng cnnel nde nsese gneic field. e esls e discssed og gs. We e conclded e following obseions:. e xil elociies incese wi e incese in nd decese wi e incese in.. e locl wll se sess decese wi incesing in nd. e incesing of sof nbe ie edces locl wll se sess ll disnces long e cnnel xis wi decese on i.. e esse diffeence decese wi incesing in nd φ wee s i incese wi incesing in nd. 5. A line elionsi is coed beween xil esse diffeence nd ole flow e e esse disibion deceses wi e incesing in nd wees i dislced fe long e cnnel xis wi incesing in. 7. e decesing in leng of e finie cnnel s jo effec on e esse disibion nd in soe cses on gnides. 8. Finlly i is conclded e ing ennces wi incesing e effec of oosiy wees i edces wi incesing e effec of e nsfe Refeences []. A.H. Sio M.Y. Jffin S.L. Weinbeg 969.Peislic ing wi long welengs low Reynolds nbe Jonl of Flid Mecnics []. A.R. Ro M. Mis Peislic nso of owe-lw flid in oos be. Jonl of on-ewonin Flid Mecnics6-7. []. B. Jeffey H.S. Udy K.S. Sclze.Flow fields geneed by eislic eflex in isoled gine ig ile: ic of concion de nd soldes Aeicn Jonl of Pysiology-soinesinl nd Lie Pysiology []. D. iio. A. Beg. A sdy of nsedy ysiologicl gneo-flid flow nd e nsfe og finie leng cnnel by eislic ing Poceedings of e Insiion of Mecnicl Enginees P H: Jonl of Engineeing in Medicine [5]. D. ii. A eicl odel fo swllowing of food bols og e oesogs nde e inflence of e nsfe Inenionl Jonl of el Science 5 9. [6]. D. ii.sdy of nsien eislic flow og finie oos cnnel Meicl nd Coe Modelling [7].. Rdisncy C. Sinisl 7. Inflence of wll oeies on eislic nso wi e nsfe Coes Rends Mecniqe [8]. K.S. Meeie Y. Abd elbod 8.e inflence of e nsfe nd gneic field on eislic nso of ewonin flid in eicl nnls: Alicion of endoscoe Pysics Lees A [9]. K.S. Meeie online eislic nso og oos edi in n inclined ln cnnel.jonl of Poos Medi []. K. Vjel. Rdisncy V.Rdisny7. Peislic nso nd e nsfe in eicl oos nnls wi long we oxiion Inenionl Jonl of on-line Mecnics []. M. Kondni S. Sinis 8. On e inflence of wll oeies in e MHD eislic nso wi e nsfe nd oos edi Pysics Lees A []..S. Ab S. dee.silion of e nd ceicl ecions on Reine Rilin flid odel fo blood flow og eed ey wi senosis He nd Mss nsfe []. S. dee.s. Ab M. Heed.Peislic nso nd e nsfe of MHD ewonin flid wi ible iscosiy Inenionl Jonl fo eicl Meods in Flids []. S. dee.s. Ab. Silion of second gde flid odel fo blood flow og eed ey wi senosis Cinise Pysics Lees [5]. S. dee.s. Ab.Inflence of e nd ss nsfe on e eislic flow of Jonson Segln flid in eicl syeic cnnel wi indced MHD Jonl of e iwn Insie of Ceicl Enginees [6]. S. Sinis M. Kondni 9.e inflence of e nd ss nsfe on MHD eislic flow og oos sce wi colin wlls Alied Meics nd Coion [7]. S. Sinis R.yi9. Peislic nso of ewonin flid in eicl syeic cnnel wi e nsfe nd oos edi Alied Meics nd Coion [8].. Hy S. oeen.peislic nso of fo gde flid wi e nsfe nd indced gneic field Coes Rends Mécniqe [9].. Hy. Ali S. Asg Hll effecs on eislic flow of Mxwell flid in oos edi 7.Pysics Lees A [].. Hy M.U. Qesi Effec of e nsfe on e eislic flow of n eleciclly flid in oos sce8.alied Meicl Modelling []. Y. Abd elbod K.S. Meeie. Unsedy lsile flow og eicl consiced nnls wi e nsfe Zeiscif fü foscng []. Y.Miyoo M. Hnno. Ig 98 Concenion ofile in e ines inl c nd dg bsoion odel:wo-diensionl lin flow in cicl oos be Jonl of eoeicl Biology DOI:.979/ Pge.

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER

Some 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 information

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD)

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD) Eoen Jonl of Sisics n Poiliy Vol. No..9- Mc Plise y Eoen Cene fo Resec Tinin n Develoen UK www.e-onls.o ISSUES RELATED WITH ARMA PQ PROCESS Sl H. Ai AL-Msnsiy Univesiy - Collee Of Ecion Deen of Meics IRAQ

More information

Compressive modulus of adhesive bonded rubber block

Compressive modulus of adhesive bonded rubber block Songklnkin J. Sci. Tecnol. 0 (, -5, M. - Ap. 008 p://www.sjs.ps.c. Oiginl Aicle Compessive modls of desive bonded bbe block Coeny Decwykl nd Wiiy Tongng * Depmen of Mecnicl Engineeing, Fcly of Engineeing,

More information

ME 141. Engineering Mechanics

ME 141. Engineering Mechanics ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics

More information

Solvability of nonlinear Klein-Gordon equation by Laplace Decomposition Method

Solvability 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 information

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems Lecre 4: Liner Time Invrin LTI sysems 2. Liner sysems, Convolion 3 lecres: Implse response, inp signls s coninm of implses. Convolion, discree-ime nd coninos-ime. LTI sysems nd convolion Specific objecives

More information

EFFECT OF TEMPERATURE ON NON-LINEAR DYNAMICAL PROPERTY OF STUFFER BOX CRIMPING AND BUBBLE ELECTROSPINNING

EFFECT OF TEMPERATURE ON NON-LINEAR DYNAMICAL PROPERTY OF STUFFER BOX CRIMPING AND BUBBLE ELECTROSPINNING Hng, J.-X., e l.: Effec of empee on Nonline ynmicl Popey... HERM SCIENCE: Ye, Vol. 8, No. 3, pp. 9-53 9 Open fom EFFEC OF EMPERURE ON NON-INER YNMIC PROPERY OF SUFFER BOX CRIMPING N BUBBE EECROSPINNING

More information

Motion on a Curve and Curvature

Motion on a Curve and Curvature Moion on Cue nd Cuue his uni is bsed on Secions 9. & 9.3, Chpe 9. All ssigned edings nd execises e fom he exbook Objecies: Mke cein h you cn define, nd use in conex, he ems, conceps nd fomuls lised below:

More information

Classification of Equations Characteristics

Classification of Equations Characteristics Clssiiion o Eqions Cheisis Consie n elemen o li moing in wo imensionl spe enoe s poin P elow. The ph o P is inie he line. The posiion ile is s so h n inemenl isne long is s. Le he goening eqions e epesene

More information

Technical Vibration - text 2 - forced vibration, rotational vibration

Technical Vibration - text 2 - forced vibration, rotational vibration Technicl Viion - e - foced viion, oionl viion 4. oced viion, viion unde he consn eenl foce The viion unde he eenl foce. eenl The quesion is if he eenl foce e is consn o vying. If vying, wh is he foce funcion.

More information

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration

() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration Secion 1.4 Moion in Spce: Velociy nd Acceleion We e going o dive lile deepe ino somehing we ve ledy inoduced, nmely () nd (). Discuss wih you neighbo he elionships beween posiion, velociy nd cceleion you

More information

Ch.4 Motion in 2D. Ch.4 Motion in 2D

Ch.4 Motion in 2D. Ch.4 Motion in 2D Moion in plne, such s in he sceen, is clled 2-dimensionl (2D) moion. 1. Posiion, displcemen nd eloci ecos If he picle s posiion is ( 1, 1 ) 1, nd ( 2, 2 ) 2, he posiions ecos e 1 = 1 1 2 = 2 2 Aege eloci

More information

Chapter Finite Difference Method for Ordinary Differential Equations

Chapter 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 information

D zone schemes

D zone schemes Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic

More information

Convection in Superposed Fluid and Porous Layers in the Presence of a Vertical Magnetic Field

Convection in Superposed Fluid and Porous Layers in the Presence of a Vertical Magnetic Field WSEAS RANSACIONS on FLUI MECANICS ni M. Bnje Ab A. Ab Conecion in Seose Fi n oos Les in e esence o Veic Mgneic Fie ANAI M. BANJER n ABULLA A. ABULLA een o Meic Sciences U A- Uniesi. O. Bo 67 M SAUI ARABIA

More information

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm

1. Viscosities: μ = ρν. 2. Newton s viscosity law: 3. Infinitesimal surface force df. 4. Moment about the point o, dm 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess 3- Fluid Mecnics Clss Emple 3: Newton s Viscosit Lw nd Se Stess Motition Gien elocit field o ppoimted elocit field, we wnt to be ble to estimte

More information

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas 6. Gs dynmics Dr. Gergely Krisóf De. of Fluid echnics, BE Februry, 009. Seed of infiniesiml disurbnces in sill gs dv d, dv d, Coninuiy: ( dv)( ) dv omenum r r heorem: ( ( dv) ) d 3443 4 q m dv d dv llievi

More information

1. Kinematics of Particles

1. Kinematics of Particles 1. Kinemics o Picles 1.1 Inoducion o Dnmics Dnmics - Kinemics: he sud o he geome o moion; ele displcemen, eloci, cceleion, nd ime, wihou eeence o he cuse o he moion. - Kineics: he sud o he elion eising

More information

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.

LECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1. LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle

More information

176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s

176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps

More information

Influence of Velocity Slip on the Peristaltic Pumping of a Jeffrey Fluid in a Non Uniform Annulus

Influence 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 information

Beechwood Music Department Staff

Beechwood Music Department Staff Beechwood Music Department Staff MRS SARAH KERSHAW - HEAD OF MUSIC S a ra h K e rs h a w t r a i n e d a t t h e R oy a l We ls h C o l le g e of M u s i c a n d D ra m a w h e re s h e ob t a i n e d

More information

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

ÖRNEK 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 information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

Physics 232 Exam I Feb. 13, 2006

Physics 232 Exam I Feb. 13, 2006 Phsics I Fe. 6 oc. ec # Ne..5 g ss is ched o hoizol spig d is eecuig siple hoic oio. The oio hs peiod o.59 secods. iiil ie i is oud o e 8.66 c o he igh o he equiliiu posiio d oig o he le wih eloci o sec.

More information

Physics 201, Lecture 5

Physics 201, Lecture 5 Phsics 1 Lecue 5 Tod s Topics n Moion in D (Chp 4.1-4.3): n D Kinemicl Quniies (sec. 4.1) n D Kinemics wih Consn Acceleion (sec. 4.) n D Pojecile (Sec 4.3) n Epeced fom Peiew: n Displcemen eloci cceleion

More information

An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics

An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics Adv Theo Appl Mech Vol no 6 9-97 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

More information

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA

Adrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA Innionl Jonl of Phoonis n Oil Thnolo Vol. 3 Iss. : 36-4 Jn 7 Rliisi Dnis n lonis in Unifol l n in Unifol Roin s-th Gnl ssions fo h loni 4-Vo Ponil in Sfi Unisi of Clifoni 387 So Hll UC Bkl Clifoni US s@ll.n

More information

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T.

The sphere of radius a has the geographical form. r (,)=(acoscos,acossin,asin) T =(p(u)cos v, p(u)sin v,q(u) ) T. Che 5. Dieeil Geome o Sces 5. Sce i meic om I 3D sce c be eeseed b. Elici om z =. Imlici om z = 3. Veco om = o moe geel =z deedig o wo mees. Emle. he shee o dis hs he geoghicl om =coscoscossisi Emle. he

More information

An object moving with speed v around a point at distance r, has an angular velocity. m/s m

An object moving with speed v around a point at distance r, has an angular velocity. m/s m Roion The mosphere roes wih he erh n moions wihin he mosphere clerly follow cure phs (cyclones, nicyclones, hurricnes, ornoes ec.) We nee o epress roion quniiely. For soli objec or ny mss h oes no isor

More information

SQUEEZE FILM CHARACTERISTICS WITH EFFECT OF NON NEWTONIAN COUPLE STRESS FLUID AND PIEZOVISCOUS DEPENDENCY BETWEEN POROUS PARALLEL CIRCULAR PLATES

SQUEEZE FILM CHARACTERISTICS WITH EFFECT OF NON NEWTONIAN COUPLE STRESS FLUID AND PIEZOVISCOUS DEPENDENCY BETWEEN POROUS PARALLEL CIRCULAR PLATES Intenational Jonal of Ciil Engineeing and Tecnology (IJCIET) Volme 9 Isse 8 Agst 8. 78 789 Aticle ID: IJCIET_9_8_79 Aailable online at tt://www.iaeme.com/ijciet/isses.as?jtye=ijciet&vtye=9&itye=8 ISSN

More information

Fluid-Solid Coupling Analysis of Deep Foundation Pit s Seepage Under Non-Saturated Conditions

Fluid-Solid Coupling Analysis of Deep Foundation Pit s Seepage Under Non-Saturated Conditions Physicl nd Nmeicl Simlion of Geoechnicl Engineeing 1s Isse, Sep. 2010 Flid-Solid Copling Anlysis of Deep Fondion Pi s Seepge Unde Non-Sed Condiions CHENG Wei, HE Xing School of Civil Engineeing nd Achiece,

More information

Nonlocal Boundary Value Problem for Nonlinear Impulsive q k Symmetric Integrodifference Equation

Nonlocal Boundary Value Problem for Nonlinear Impulsive q k Symmetric Integrodifference Equation OSR ol o Mec OSR-M e-ssn: 78-578 -SSN: 9-765X Vole e Ve M - A 7 PP 95- wwwojolog Nolocl Bo Vle Poble o Nole lve - Sec egoeece Eo Log Ceg Ceg Ho * Yeg He ee o Mec Yb Uve Yj PR C Abc: A oe ole lve egoeece

More information

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings. T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson

More information

P 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 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 information

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes

Ans: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes omewok # P7-3 ecngul loop of widh w nd heigh h is siued ne ve long wie cing cuen i s in Fig 7- ssume i o e ecngul pulse s shown in Fig 7- Find he induced cuen i in he ecngul loop whose self-inducnce is

More information

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type J N Sce & Mh Res Vol 3 No (7) -7 Alble ole h://orlwlsogocd/deh/sr P-Coey Proery Msel-Orlcz Fco Sce o Boher ye Yl Rodsr Mhecs Edco Deree Fcly o Ss d echology Uerss sl Neger Wlsogo Cerl Jdoes Absrcs Corresodg

More information

v T Pressure Extra Molecular Stresses Constitutive equations for Stress v t Observation: the stress tensor is symmetric

v T Pressure Extra Molecular Stresses Constitutive equations for Stress v t Observation: the stress tensor is symmetric Momenum Blnce (coninued Momenum Blnce (coninued Now, wh o do wih Π? Pessue is p of i. bck o ou quesion, Now, wh o do wih? Π Pessue is p of i. Thee e ohe, nonisoopic sesses Pessue E Molecul Sesses definiion:

More information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

Two-Pion Exchange Currents in Photodisintegration of the Deuteron

Two-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 information

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9 OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at

More information

Hyperbolic Heat Equation as Mathematical Model for Steel Quenching of L-shape and T-shape Samples, Direct and Inverse Problems

Hyperbolic Heat Equation as Mathematical Model for Steel Quenching of L-shape and T-shape Samples, Direct and Inverse Problems SEAS RANSACIONS o HEA MASS RANSER Bos M Be As Bs Hpeo He Eo s Me Moe o See Qe o L-spe -spe Spes De Iese Poes ABIA BOBINSKA o Pss Mes es o L Ze See 8 L R LAIA e@o MARARIA BIKE ANDRIS BIKIS Ise o Mes Cope

More information

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253

Science Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis   2/3/2007 Physics 253 Science Adeisemen Inegoenmenl Pnel on Clime Chnge: The Phsicl Science Bsis hp://www.ipcc.ch/spmfeb7.pdf /3/7 Phsics 53 hp://www.fonews.com/pojecs/pdf/spmfeb7.pdf /3/7 Phsics 53 3 Sus: Uni, Chpe 3 Vecos

More information

Solution to Theoretical Question 2. A Piezoelectric Crystal Resonator under an Alternating Voltage Part A

Solution to Theoretical Question 2. A Piezoelectric Crystal Resonator under an Alternating Voltage Part A Solion o eoreical Qesion A Piezoelecric Crysal Resonaor ner an Alernaing olage Par A a Refer o Figre A e lef face of e ro oves a isance v wile e ressre wave ravels a isance wi / ρ e srain a e lef face

More information

Effects of Heat Absorption and Porosity of the Medium on MHD Flow past a Vertical Plate

Effects 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 information

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =

Physic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = = Mi i fd l Phsic 3 Lecure 4 Min poins of od s lecure: Emple: ddiion of elociies Trjecories of objecs in dimensions: dimensions: g 9.8m/s downwrds ( ) g o g g Emple: A foobll pler runs he pern gien in he

More information

An Optimization Model for Empty Container Reposition under Uncertainty

An Optimization Model for Empty Container Reposition under Uncertainty n Omzon Mode o Emy onne Reoson nde neny eodo be n Demen o Mnemen nd enooy QM nd ene de Reee s es nsos Moné nd Mssmo D Fneso Demen o Lnd Enneen nesy o Iy o Zdds Demen o Lnd Enneen nesy o Iy Inodon. onne

More information

Executive Committee and Officers ( )

Executive Committee and Officers ( ) Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r

More information

Overview. Overview Page 1 of 8

Overview. Overview Page 1 of 8 COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSITE BEAM DESIGN AISC-LRD93 Tecnical Noe Compac and Noncompac Requiemens Tis Tecnical Noe descibes o e pogam cecks e AISC-LRD93 specificaion

More information

Convective Heat Transfer (6) Forced Convection (8) Martin Andersson

Convective 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 information

PHYSICS 1210 Exam 1 University of Wyoming 14 February points

PHYSICS 1210 Exam 1 University of Wyoming 14 February points PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher

More information

Available online Journal of Scientific and Engineering Research, 2018, 5(10): Research Article

Available online   Journal of Scientific and Engineering Research, 2018, 5(10): Research Article vilble online www.jse.com Jounl of Scienific n Engineeing Resech, 8, 5():5-58 Resech icle ISSN: 94-6 CODEN(US): JSERBR Soluion of he Poblem of Sess-Sin Se of Physiclly Non-Line Heeiily Plsic Infinie Ple

More information

MODELLING OF ROTATIONAL FLUID WITH AN ACCELERATED VERTICAL PLATE EMBEDDED IN A DARCIAN POROUS REGIME

MODELLING OF ROTATIONAL FLUID WITH AN ACCELERATED VERTICAL PLATE EMBEDDED IN A DARCIAN POROUS REGIME MODELLING OF ROAIONAL FLUID WIH AN AELERAED VERIAL PLAE EMEDDED IN A DARIAN POROUS REGIME. Sahin AHMED. HEA RANSFER AND FLUID MEHANIS RESEARH DEPARMEN OF MAHEMAIS GOALPARA OLLEGE GOALPARA- 78 ASSAM INDIA

More information

Derivation of the differential equation of motion

Derivation of the differential equation of motion Divion of h iffnil quion of oion Fis h noions fin h will us fo h ivion of h iffnil quion of oion. Rollo is hough o -insionl isk. xnl ius of h ll isnc cn of ll (O) - IDU s cn of gviy (M) θ ngl of inclinion

More information

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.

Circuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt. 4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss

More information

Convective Heat Transfer (6) Forced Convection (8) Martin Andersson

Convective 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 information

ME 3560 Fluid Mechanics

ME 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 information

Fundamental Vehicle Loads & Their Estimation

Fundamental 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 information

Mucus Transport in the Larger Airway Due to Prolonged Mild Cough: Effect of Serous Fluid and Cilia Beating

Mucus Transport in the Larger Airway Due to Prolonged Mild Cough: Effect of Serous Fluid and Cilia Beating Cheicl nd oce Engineeing eech ISSN -767 (pe) ISSN 5- (Online) Vol., 5 www.iie.og Mc npo in he Lge Aiwy De o olonged Mild Cogh: Effec of Seo Flid nd Cili Being Ai Sxen * A.. ygi.depen of Mheic,FE, Mnv chn

More information

Scholars Journal of Physics, Mathematics and Statistics

Scholars 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 information

Chapter Direct Method of Interpolation

Chapter Direct Method of Interpolation Chper 5. Direc Mehod of Inerpolion Afer reding his chper, you should be ble o:. pply he direc mehod of inerpolion,. sole problems using he direc mehod of inerpolion, nd. use he direc mehod inerpolns o

More information

Chapter 4 Circular and Curvilinear Motions

Chapter 4 Circular and Curvilinear Motions Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion

More information

Numerical Simulation of Natural Gas Flow in Transmission Lines through CFD Method Considering Effective Parameters

Numerical Simulation of Natural Gas Flow in Transmission Lines through CFD Method Considering Effective Parameters J. Bsi. Appl. Si. Res. (8)773-787 0 0 TexRod bliion ISSN 090-30 Jonl of Bsi nd Applied Sienifi Reseh www.exod.om Nmeil Simlion of Nl Gs Flow in Tnsmission Lines hogh CFD Mehod Consideing Effeive mees Nikn

More information

SOLUTIONS TO CONCEPTS CHAPTER 11

SOLUTIONS TO CONCEPTS CHAPTER 11 SLUTINS T NEPTS HPTE. Gvittionl fce of ttction, F.7 0 0 0.7 0 7 N (0.). To clculte the gvittionl fce on t unline due to othe ouse. F D G 4 ( / ) 8G E F I F G ( / ) G ( / ) G 4G 4 D F F G ( / ) G esultnt

More information

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA

TWO INTERFACIAL COLLINEAR GRIFFITH CRACKS IN THERMO- ELASTIC COMPOSITE MEDIA WO INERFIL OLLINER GRIFFIH RS IN HERMO- ELSI OMOSIE MEDI h m MISHR S DS * Deme o Mheml See I Ie o eholog BHU V-5 I he oee o he le o he e e o eeg o o olle Gh e he ee o he wo ohoo mel e e e emee el. he olem

More information

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of

One of the common descriptions of curvilinear motion uses path variables, which are measurements made along the tangent t and normal n to the path of Oe of he commo descipios of cuilie moio uses ph ibles, which e mesuemes mde log he ge d oml o he ph of he picles. d e wo ohogol xes cosideed sepely fo eey is of moio. These coodies poide ul descipio fo

More information

Average & instantaneous velocity and acceleration Motion with constant acceleration

Average & instantaneous velocity and acceleration Motion with constant acceleration Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s . Ioo ssfo of ss Ms 분체역학 G Ms 역학 Ms 열역학 o Ms 유체역학 F Ms o Ms 고체역학 o Ms 구조해석 ss Dfo of Ms o B o w oo of os o of fos s s w o s s. Of fs o o of oo fos os o o o. s s o s of s os s o s o o of fos o. G fos

More information

ON THE EXTENSION OF WEAK ARMENDARIZ RINGS RELATIVE TO A MONOID

ON THE EXTENSION OF WEAK ARMENDARIZ RINGS RELATIVE TO A MONOID wwweo/voue/vo9iue/ijas_9 9f ON THE EXTENSION OF WEAK AENDAIZ INGS ELATIVE TO A ONOID Eye A & Ayou Eoy Dee of e Nowe No Uvey Lzou 77 C Dee of e Uvey of Kou Ou Su E-: eye76@o; you975@yooo ABSTACT Fo oo we

More information

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A 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 information

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under

More information

Karachi-75270, Pakistan. Karachi-75270, Pakistan.

Karachi-75270, Pakistan. Karachi-75270, Pakistan. Maeaical and Copaional Applicaions, Vol., No., pp. 8-89,. Associaion for Scienific Researc ANALYTICAL ASPECT OF FOURTH-ORDER PARABOLIC PARTIAL DIFFERENTIAL EQUATIONS WITH VARIABLE COEFFICIENTS Najeeb Ala

More information

SOME USEFUL MATHEMATICS

SOME USEFUL MATHEMATICS SOME USEFU MAHEMAICS SOME USEFU MAHEMAICS I is esy o mesure n preic he behvior of n elecricl circui h conins only c volges n currens. However, mos useful elecricl signls h crry informion vry wih ime. Since

More information

I N A C O M P L E X W O R L D

I N A C O M P L E X W O R L D IS L A M I C E C O N O M I C S I N A C O M P L E X W O R L D E x p l o r a t i o n s i n A g-b eanste d S i m u l a t i o n S a m i A l-s u w a i l e m 1 4 2 9 H 2 0 0 8 I s l a m i c D e v e l o p m e

More information

Fractional Order Thermoelastic Deflection in a Thin Circular Plate

Fractional Order Thermoelastic Deflection in a Thin Circular Plate Aville ://vuedu/ Al Al M ISSN: 93-9466 Vol Iue Decee 7 898-99 Alicion nd Alied Meic: An Inenionl Jounl AAM Fcionl Ode eoelic Deflecion in in Cicul Ple J J ii S D We C Deuk 3 nd J Ve 4 Deen of Meic D Aedk

More information

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1. Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)

More information

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf

Faraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf Objecie F s w Tnsfome Moionl To be ble o fin nsfome. moionl nsfome n moionl. 331 1 331 Mwell s quion: ic Fiel D: Guss lw :KV : Guss lw H: Ampee s w Poin Fom Inegl Fom D D Q sufce loop H sufce H I enclose

More information

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c L i f e t i m e M a n a g e m e n t o f F l a-b s ah s e d S S D s U s i n g R e c o v e r-a y w a r e D y n a m i c T h r o t t l i n g S u n g j i n L e, e T a e j i n K i m, K y u n g h o, Kainmd J

More information

Nine lectures for the Maths II course given to first year physics students in the Spring Term. Lecturer: Professor Peter Main

Nine lectures for the Maths II course given to first year physics students in the Spring Term. Lecturer: Professor Peter Main Nine leces o e Ms II cose gien o is e psics sens in e Sping Tem. Lece: Poesso Pee Min Ao e cose Tis cose sows o ow o ieenie n inege ncions o seel iles. I is pesene s n eension o e clcls o le now wic els

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s ν . Ioo ssfo of ss Ms 분체역학 G Ms 역학 Ms 열역학 o Ms 유체역학 F Ms o Ms 고체역학 o Ms 구조해석 ss Dfo of Ms o o w oo of os o of fos s s w o s s. Of fs o o of oo fos os o o o. s s o s of s os s o s o o of fos o. G fos

More information

An Integral Two Space-Variables Condition for Parabolic Equations

An Integral Two Space-Variables Condition for Parabolic Equations Jornl of Mhemics nd Sisics 8 (): 85-9, ISSN 549-3644 Science Pblicions An Inegrl Two Spce-Vribles Condiion for Prbolic Eqions Mrhone, A.L. nd F. Lkhl Deprmen of Mhemics, Lborory Eqions Differenielles,

More information

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1

Week 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1 Week : DTMC Alictions Rnking Web ges & Slotted ALOHA etwok efonce - Outline Aly the theoy of discete tie Mkov chins: Google s nking of web-ges Wht ge is the use ost likely seching fo? Foulte web-gh s Mkov

More information

X-Ray Notes, Part III

X-Ray Notes, Part III oll 6 X-y oe 3: Pe X-Ry oe, P III oe Deeo Coe oupu o x-y ye h look lke h: We efe ue of que lhly ffee efo h ue y ovk: Co: C ΔS S Sl o oe Ro: SR S Co o oe Ro: CR ΔS C SR Pevouly, we ee he SR fo ye hv pxel

More information

T h e C S E T I P r o j e c t

T 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 information

H STO RY OF TH E SA NT

H STO RY OF TH E SA NT O RY OF E N G L R R VER ritten for the entennial of th e Foundin g of t lair oun t y on ay 8 82 Y EEL N E JEN K RP O N! R ENJ F ] jun E 3 1 92! Ph in t ed b y h e t l a i r R ep u b l i c a n O 4 1922

More information

THIS PAGE DECLASSIFIED IAW EO 12958

THIS PAGE DECLASSIFIED IAW EO 12958 L " ^ \ : / 4 a " G E G + : C 4 w i V T / J ` { } ( : f c : < J ; G L ( Y e < + a : v! { : [ y v : ; a G : : : S 4 ; l J / \ l " ` : 5 L " 7 F } ` " x l } l i > G < Y / : 7 7 \ a? / c = l L i L l / c f

More information

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2

f(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2 Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe

More information

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10 Chper 0 Siple Hronic Moion nd Elsiciy Gols or Chper 0 o ollow periodic oion o sudy o siple hronic oion. o sole equions o siple hronic oion. o use he pendulu s prooypicl syse undergoing siple hronic oion.

More information

Evaluation of Finite Element Formulation for One-Dimensional Consolidation

Evaluation of Finite Element Formulation for One-Dimensional Consolidation Inernionl Jornl of Scienific & Engineering Reserch,Vole 3, Isse 5, y- ISSN 9-558 Elion of Finie Eleen Forlion for One-Diensionl Consolidion Wn NrFirds Wn ssn, ishohd Absrc Consolidion process is defined

More information

Effects of wall properties and heat transfer on the peristaltic transport of a jeffrey fluid through porous medium channel

Effects of wall properties and heat transfer on the peristaltic transport of a jeffrey fluid through porous medium channel Mhemicl heor nd Modeling ISSN -58 Per ISSN 5-5 Online Vol. No.9 www.iise.org Effecs of wll roeries nd he rnsfer on he erislic rnsor of jeffre flid hrogh oros medim chnnel Dhei G. Slih Al-Khfj College of

More information

Investigations of Electromagnetic Space-Charge Effects in Beam Physics

Investigations of Electromagnetic Space-Charge Effects in Beam Physics Invesigions of Elecogneic Spce-Chge Effecs in Be Physics Chong Shik Pk Depen of Physics Indin Univesiy Indin Univesiy Cycloon Fciliy @ effenson Lb Sep. 9 Ouline Moivions Exising Spce-Chge Modeling Spce-Chge

More information

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f Essential Skills Chapter f ( x + h) f ( x ). Simplifying the difference quotient Section. h f ( x + h) f ( x ) Example: For f ( x) = 4x 4 x, find and simplify completely. h Answer: 4 8x 4 h. Finding the

More information

Addition & Subtraction of Polynomials

Addition & Subtraction of Polynomials Addiion & Sucion of Polynomil Addiion of Polynomil: Adding wo o moe olynomil i imly me of dding like em. The following ocedue hould e ued o dd olynomil 1. Remove enhee if hee e enhee. Add imil em. Wie

More information

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f C H A P T E R I G E N E S I S A N D GROWTH OF G U IL D S C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f i n a v a r i e t y o f f o r m s - s o c i a l, r e l i g i

More information

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list:

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list: k Ax W ls i ms im s i sfly. f w is T x, ls lk g sci Bld Cicl Js lik wi sig kivs, w w sig x w v k d s cl. Wi xs; cl (bld cicl) is s lg f y m ls lg f x ll d s d bv s. T c b bcs, wigs, scs, c. isid y bld

More information

Contraction Mapping Principle Approach to Differential Equations

Contraction Mapping Principle Approach to Differential Equations epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of

More information

Computer Aided Geometric Design

Computer Aided Geometric Design Copue Aided Geoei Design Geshon Ele, Tehnion sed on ook Cohen, Riesenfeld, & Ele Geshon Ele, Tehnion Definiion 3. The Cile Given poin C in plne nd nue R 0, he ile ih ene C nd dius R is defined s he se

More information

Solutions to Homework #9

Solutions to Homework #9 9- Soltions to Homewok #9 9-5 he fo pocesses of an ai-standad cycle ae descibed. he cycle is to be shown on - and -s diagams, and e net wok pt and e emal efficiency ae to be detemed. Assmptions he ai-standad

More information

Propagation of Torsional Surface Waves. in Heterogeneous Half-Space. with Irregular Free Surface

Propagation 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 information

Example: Two Stochastic Process u~u[0,1]

Example: Two Stochastic Process u~u[0,1] Co o Slo o Coco S Sh EE I Gholo h@h. ll Sochc Slo Dc Slo l h PLL c Mo o coco w h o c o Ic o Co B P o Go E A o o Po o Th h h o q o ol o oc o lco q ccc lco l Bc El: Uo Dbo Ucol Sl Ab bo col l G col G col

More information