The Heat and Mass Transfer Modeling with Time Delay

Size: px
Start display at page:

Download "The Heat and Mass Transfer Modeling with Time Delay"

Transcription

1 465 A pliio of HEMIAL ENGINEERING TRANSATIONS OL Gs Ediors: Sro Piri Jiří Jromír Klmš Lr Pi Srfim Bklis opyrigh 07 AIDI Srii Srl ISBN ; ISSN Th Ili Assoiio of hmil Egirig Oli wwwidii/ DOI: 03303/ET75745 Th H d Mss Trsfr Modlig wih Tim Dly solod G Soroki Adry ymi* Alky I Zhro d yhsl Rik Adry D Polyi d Bm Mosow S Thil Uirsiy ory Bmsky l 5/ Mosow Rssi Dprm of hmil Egirig Mosow Polyhi Uirsiy Sry Bsmy /4 Mosow Rssi Siifi Rsrh Isi of Rr Idsry poslok NIIRP Srgi Posd Rssi d Ishliskii Isi for Prolms i Mhis RAS pr rdskogo Mosow Rssi 958@lisr Nolir hyproli rio-diffsio qios wih dly i im r isigd All qios osidrd hr oi o rirry fio E solios r lso prsd for mor ompl olir qios i whih dly rirrily dpds o im E solios wih grlid sprio of rils r fod or spil ss w solios i h form of rlig ws r oid som of whih rprsd i rms of lmry fios All of hs solios oi fr rirry prmrs so h o s hm o sol modlig prolms of h d mss rsfr wih rlio phom Irodio Proli qio of h- d mss-rsfr hs physilly prdoil propry i ifii disr propgio r whih is o osrd i r Solig o-sdy-s h- d mssrsfr prolms i is ssry o k io o rlio phom ssoid wih h fiiss of h r of h d mss rsfr s for mpl Dmirl 007 Th hrml d diffsio rlio ims ry i rmly wid limis from millisods or lss o srl s of sods d shold k io o i solig my h d mss rsfr prolms Polyi d ymi 03 Th sod impor fr of oliory prosss ildig h- d mss-rsfr prosss wih hmil orsios is h i h grl s h r of riios i h dsird qiis i hmil iologil physiohmil hmil girig d ohr sysms dpds o oly o h s h gi im poi lso o h ir prios olio of h pross Jo l 00; Poks l 05 Ths sysms r lld hrdiry sysms I h prilr s whr h s of h sysm is oly drmid y prilr im poi i h ps rhr h h ir olio of h sysm h sysm is rfrrd o s dlyd fdk sysm Sysms wih dlyd fdk r frqly modld y rio diffsio qios i whih h kii fio h r of hmil rios dpds o oh h sogh orio fio = d h sm fio wih h dlyd rgm w = τ Th spil s of w = fw hs simpl physil irprio i h- d mss-rsfr prosss i mdi wih lol o-qilirim h iril propris i h sysm dos o r o io isosly h gi im poi s i h lssil lol qilirim s i rs y h dly im τ lr Solig o-sdy-s mss rsfr prolms i hmil girig i is ssry o k io o rlio phom ssoid oh wih h fiiss of h im of rsfr prosss τ d wih h fiiss of h ims τ of hmil orsios d/or h mirokii irio w diffr phss h form sigl rspor mromdim solios o h followig o-lir hyproli rio diffsio qios r drid d lyd i his sdy s lso Polyi l 05: w w Pls i his ril s: Soroki G ymi A Zhro AI Rik Polyi AD 07 Th h d mss rsfr modlig wih im dly hmil Egirig Trsios DOI: 03303/ET75745

2 466 whr - diffsio offii - oordi I shold od h s prilr s τ = 0 osidrig qio ilds proli qios wih dly Mor ompl olir rio diffsio qios wih ril dly of h grl form τ = τ will lso osidrd I h dgr s τ = 0 i for h proli qio ri solios o Eq wr oid for mpls for rllig w y W d Zo 00;sig ompl grop lssifiio y Mlshko d Moyo 008; sig mhod of grlid d fiol sprio y Polyi d Zhro 04 or kii fio of wo grl forms w solios of qio will fod llow W mphsi h for h firs im solios r oid for h qio wih wo hrrisi dly ims whih h diffr physil mig d whih ppr i diffr rms of qio Ths rsls grli prios solios oid y ohr hors Mhods for fidig solios Th mril solig of rios olir pril diffril qios d sysms of qios wih dly d diffilis h ris i his s r dsrid y Jkiwi d Zik-Kowl 006 I y s h grl disdgs of mril mhods ild: s irsl ppliio wh hgig h gomri shp of h oj h yp of flid flow rio kiis d ippliiliy i h prs of siglr pois E solios o olir diffril qios promo h r drsdig of h qlii frs of h prosss dr dsripio oiqss spil loliio lowp rgims I shold mphsid h dly ssilly omplis h lysis of qios d is for h ld o h isiliy of h sysms ig modld Jord l 008 Th rm solios wih rsp o h olir dly of pril diffril qios r sd i h ss whr solio is prssd s follows: - Th solio prssd i rms of lmry fios or rprsd i h losd form h solio is prssd i rms of idfii or dfii igrls - Th solio prssd i rms of solios o ordiry diffril qios or dly ordiry diffril qios or sysms of hs qios - Th solio prssd i rms of solios o lir pril diffril qios - Th omiios of solios r lso llowl Solio mhods d rios ppliios of lir d olir ordiry diffril qios wih dly whih r ssilly simplr h olir pril diffril qios wih dly r dsrid for mpls y Bllm d ook 963; Kg 993 A mr of solios o ri olir pril diffril qios wih dly s wll s sysms of qios wih dly whih r diffr from rio diffsio qios r gi i ppr Thh 0 I his sdy o sk solios o olir hyproli rio diffsio qio sh s Eq w sd rios modifiios of h mhods of grlid d fiol sprio of rils s for iformio hdooks y Polyi d Mhiro 007; Glkioo d Sirshhskii 007; Polyi d Zis 0 d h fiol osris mhod for proli dly qios Polyi d Zhro 04; for proli qios wih ryig rsfr offiis Polyi d Zhro 04 rom his poi o irmdi llios r grlly omid for h sk of riy Eqio dos o modl y prilr hologil pross I grlis h diffsio qio; oid o h sis of h ik's lw i h qilirim for oqilirim prosss whih ks io o hir ow rs of prrio propgios i h mdim d is hmil rsformios Th oid rsls do o rqir y rifiio si hy r mhmilly r 3 E solios o Eq wih kii fio h dpds o h rio w/ L s osidr Eq i h followig form: w w whr is rirry fio 3 Eqio wih ril dly Eq yilds solio priodi wih rsp o os si 3

3 whr d λ r rirry oss d h fio ψ is dsrid y h followig ordiry diffril qio wih dly: Eq lso yilds solio of h form p p 4 whr h fio ψ is dsrid y h followig ordiry fiol-diffril qio: 3 Eqio wih os dly Now w osidr Eq wh τ = os I his s Eq yilds h sprl solio s h prod of h fios of diffr rgms s Eq 3 Th fio ψ i Eq 3 is dsrid y h followig ordiry diffril qio wih dly: 5 Eq 5 yilds h prilr solio ψ = A β whr A is rirry os d β is drmid from h lgri or rsdl qio 0 Eq lso yilds solio of h form Eq 4 whr h fio ψ is dsrid y h followig dly diffril qio: 6 Eq 6 yilds h prilr solio ψ = A β whr β is drmid from h lgri rsdl qio 0 3 Eq lso yilds h solio p 7 whr h fio θ is dsrid y h followig dly ordiry diffril qio: 0 / ' This qio yilds h prilr solio θ = A whr is drmid from h lgri rsdl qio 0 Solio i h form of Eq 7 is h olir sprposiio of wo diffr rlig ws 4 L h fio 8 y τ-priodi solio o h followig lir hyproli qio: 9 from his poi o for h sk of riy h dpd of Eqs 8 d 3 o h prmrs τ d whih ppr i Eqs 9 d 4 is o idid pliily I h s Eq yilds h grlid sprl solio 467

4 0 whr is rirry os I show h h grl solio o Eq 9 sj o h formiod odiio of τ-priodiiy wih rsp o im hs h followig form: si os p si os p 0 D B A whr A B d D r rirry oss whih sris i Eq r org h org srd g if w s A = B = = D = 0 > N whr N is y posii igr Th followig prilr ss disigishd: τ-priodi wih rsp o h im solios Eq 9 h dy r gi y Eqs d A 0 = B 0 = 0 = D = 0 d = ; τ-priodi wih rsp o h im solios odd r gi y Eqs d = D = 0 d = ; siory solio is gi y Eqs d A = B = = D = 0 d = 5 L h fio 3 τ-priodi solio o h followig lir hyproli qio: 4 I h s Eq yilds h grlid sprl solio 5 Th grl solio o Eq 4 hs h followig form: si os p si os p D B A 6 7 Solios τ-priodi o h im h dy r gi y Eqs 6 d 7 = D = 0 d = Eqs d 6 7 r ry similr Howr i h firs s h firs sm gis from = 0 d i h sod solio i gis from = ; h ls of β r lso diffr 4 E solios o Eq wih kii fio h dpds o h diffr w L s osidr Eq i h followig form: 468

5 w w 8 whr is rirry fio 4 Eqio wih ril dly Eq 8 yilds solio of h form 9 whr 0 p p 0; si os 0 d h fio ψ is dsrid y h followig dly diffril qio: 4 Eqio wih os dly Now w osidr Eq 8 wh τ = os I his s Eq 8 yilds h sprl solio s h sm of h fios of diffr rgms of h form of Eqs 9-0 d h fio ψ is dsrid y h followig dly diffril qio: A = 0 Eq 8 yilds h sprl solio h is qdri wih rsp o : whr h fio ψ is dsrid y h followig dly diffril qio: 3 Th solio o Eq 8 h grlis solio of h form Eq 9 hs h form whr φ is drmid y Eq 0 d θ is dsrid y h dly ordiry diffril qio: 0 ' A > 0 Eq dsris h olir irio w priodi sdig w d rlig w 4 A = 0 h solio of Eq 8 h grlis Eq hs h form whr h fio θ is dsrid y h followig dly ordiry diffril qio: 0 ' 5 Eq 8 yilds h dgr grlid sprl solio whr φ is drmid y Eqs 0 d ψ is dsrid y h lir ordiry diffril qio: Mor ompl solios o Eq 8 drid sig h followig propry L 0 solio o olir Eq 8 d = ; y τ-priodi solio o lir Eq9 I h s h sm

6 470 is h solio o Eq 8 Th form of h fio ; is drmid y Eqs or mpl h rlig w solio 0 = 0α + β sd i Eq 3 s h solio o olir Eq 8 5 olsios or hyproli diffsio-rio qios wih im dly solios r oid i poil form wih irm ompd from rsdl qio of spil yp hrogh dly ims Nw solios of his qio r fod i h form of olir sprposiio of wo diffr rlig ws Th form of solios sisfyig iiil-odry prolms is slishd ri solios r dsrid for mor ompl olir rio diffsio qios sh s hos wih ril dly of h grl form τ = τ Th drid solios oi fr prmrs i som ss hr y mr of hs prmrs d sd o sol ri modl prolms d s pproim lyil d mril mhods for solig similr or mor ompl olir dly pril diffril qios Akowldgms Th work is sppord y h Rssi odio for Bsi Rsrh proj No Rfr Bllm R ook KL 963 Diffril-Diffr Eqios Admi Prss Nw York/Lodo Egld Dmirl Y 007 Noqilirim Thrmodymis: Trspor d R Prosss i Physil hmil d Biologil Sysms Elsir Amsrdm Nhrlds Glkioo A Sirshhskii SR 007 E Solios d Iri Ssps of Nolir Pril Diffril Eqios i Mhis d Physis hpm & Hll/R Bo Ro USA Jkiwi Z Zik-Kowl B 006 Sprl olloio d wform rlio mhods for olir dly pril diffril qios Applid Nmril Mhmis Jord PM Di W Miks RE 008 A o o h dlyd h qio: isiliy wih rsp o iiil d Mhis Rsrh ommiios Jo D ss-q J Lo G 00 Edd Irrrsil Thrmodymis Sprigr Nw York USA Kg Y 993 Dly Diffril Eqios wih Appliios i Poplio Dymis Admi Prss Boso USA Mlshko S Moyo S 008 O h ompl grop lssifiio of h rio diffsio qio wih dly Jorl of Mhmil Alysis d Appliios Poks BG Krlo SP ymi A Nkrso DA 05 Diffsio phom i gls hmil Egirig Trsios Polyi AD Zis 0 Hdook of Nolir Pril Diffril Eqios hpm & Hll/R Bo Ro USA Polyi AD Zhro AI 04 Nw grlid d fiol sprl solios o o-lir dly rio diffsio qios Iriol Jorl of No-Lir Mhis 59 6 Polyi AD Zhro AI 04 iol osris mhod for osrig solios o dly rio diffsio qios d mor ompl olir qios ommiios i Nolir Si d Nmril Simlio Polyi AD Zhro AI 04 Th fiol osris mhod: ppliio o o-lir dly rio diffsio qios wih ryig rsfr offiis Iriol Jorl of No-Lir Mhis Polyi AD Mhiro A 007 Hdook of Mhmis for Egirs d Siiss hpm & Hll/R Bo Ro USA Polyi AD Soroki G ymi A 05 E solios d qlii frs of olir hyproli rio diffsio qios wih dly Thoril odios of hmil Egirig Polyi AD ymi A 03 Diffril-diffr h-odio d diffsio modls d qios wih fii rlio im Thoril odios of hmil Egirig Thh J 0 Symmry lysis of h ohomogos iisid Brgrs qio wih dly ommiios i Nolir Si d Nmril Simlio W J Zo X 00 Trllig w fros of rio diffsio sysms wih dly Jorl of Dymis d Diffril Eqios

1. Introduction and notations.

1. Introduction and notations. Alyi Ar om plii orml or q o ory mr Rol Gro Lyé olyl Roièr, r i lir ill, B 5 837 Tolo Fr Emil : rolgro@orgr W y hr q o ory mr, o ll h o ory polyomil o gi rm om orhogol or h mr Th mi rl i orml mig plii h

More information

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS Diol Bgyoko (0) I.INTRODUCTION LINEAR d ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS I. Dfiiio All suh diffril quios s i h sdrd or oil form: y + y + y Q( x) dy d y wih y d y d dx dx whr,, d

More information

Numerical Solution of a non-linear Volterra Integrodifferential Equation via Runge-Kutta-Verner Method

Numerical Solution of a non-linear Volterra Integrodifferential Equation via Runge-Kutta-Verner Method Iriol Jorl of Siifi Rsrh Pliios Volm 3 Iss 9 Spmr 3 ISSN -33 Nmril Solio of o-lir Volrr Igroiffril Eqio vi Rg-K-Vrr Mho Ali Filiz * * Dprm of Mhmis A Mrs Uivrsiy 9 AYDIN-TURKEY Asr- I his ppr highr-orr

More information

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is [STRAIGHT OBJECTIVE TYPE] l Q. Th vlu of h dfii igrl, cos d is + (si ) (si ) (si ) Q. Th vlu of h dfii igrl si d whr [, ] cos cos Q. Vlu of h dfii igrl ( si Q. L f () = d ( ) cos 7 ( ) )d d g b h ivrs

More information

EEE 303: Signals and Linear Systems

EEE 303: Signals and Linear Systems 33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =

More information

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012 AE7/AC/A7 SIGNALS AND SYSEMS DECEMBER Q. Drmi powr d rgy of h followig igl j i ii =A co iii = Solio: i E P I I l jw l I d jw d d Powr i fii, i i powr igl ii =A cow E P I co w d / co l I I l d wd d Powr

More information

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times.

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times. 2 Pupi / Css Rr W ssum wr hs b r wh i hs b ihr s r us rry s hr ims. Nm: D Bu: fr i bus brhr u firs hf hp hm s uh i iv iv my my mr muh m w ih w Tik r pp push pu sh shu sisr s sm h h hir hr hs im k w vry

More information

Right Angle Trigonometry

Right Angle Trigonometry Righ gl Trigoomry I. si Fs d Dfiiios. Righ gl gl msurig 90. Srigh gl gl msurig 80. u gl gl msurig w 0 d 90 4. omplmry gls wo gls whos sum is 90 5. Supplmry gls wo gls whos sum is 80 6. Righ rigl rigl wih

More information

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S.

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S. Rfrc: (i) (ii) (iii) Advcd Egirig Mhmic, K.A. Sroud, Dxr J. Booh Egirig Mhmic, H.K. D Highr Egirig Mhmic, Dr. B.S. Grwl Th mhod of m Thi coi of h followig xm wih h giv coribuio o h ol. () Mid-rm xm : 3%

More information

(1) (2) sin. nx Derivation of the Euler Formulas Preliminary Orthogonality of trigonometric system

(1) (2) sin. nx Derivation of the Euler Formulas Preliminary Orthogonality of trigonometric system orir Sri Priodi io A io i lld priodi io o priod p i p p > p: ir I boh d r io o priod p h b i lo io o priod p orir Sri Priod io o priod b rprd i rm o rioomri ri o b i I h ri ovr i i lld orir ri o hr b r

More information

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 4, Issue 1, July 2014

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 4, Issue 1, July 2014 7 hrl Srsss o Si Iii Rcglr B wih Irl H Sorc Schi Chhl; A. A. Nlr; S.H. Bg N. W. Khorg r o hics J ciol Cs R Ngr irsi Ngr Ii. Asrc- his r is cocr wih irs rsi hrolsic rol i which w o ri h rr isriio islc cio

More information

DIFFERENCE EQUATIONS

DIFFERENCE EQUATIONS DIFFERECE EQUATIOS Lier Cos-Coeffiie Differee Eqios Differee Eqios I disree-ime ssems, esseil feres of ip d op sigls pper ol speifi iss of ime, d he m o e defied ewee disree ime seps or he m e os. These

More information

Dark Solitons in Gravitational Wave and Pulsar Plasma Interaction

Dark Solitons in Gravitational Wave and Pulsar Plasma Interaction J Pl Fuio R SRIS ol 8 9 Dr Solio i Griiol W d Pulr Pl Irio U MOFIZ Dr of Mi d Nurl Si RC Uiri 66 Moli D- ld Rid: 4 uu 8 / d: 6 Jur 9 olir roio of riiol w rdiulr o urro i fild ird i lro-oiro ulr l i oidrd

More information

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series I Jorl of Mh Alysis, Vol 4, 2, o 2, 4-47 Approximio of Fcios Blogig o Lipschiz Clss by Triglr Mrix Mhod of Forir Sris Shym Ll Dprm of Mhmics Brs Hid Uivrsiy, Brs, Idi shym _ll@rdiffmilcom Biod Prsd Dhl

More information

x, x, e are not periodic. Properties of periodic function: 1. For any integer n,

x, x, e are not periodic. Properties of periodic function: 1. For any integer n, Chpr Fourir Sri, Igrl, d Tror. Fourir Sri A uio i lld priodi i hr i o poiiv ur p uh h p, p i lld priod o R i,, r priodi uio.,, r o priodi. Propri o priodi uio:. For y igr, p. I d g hv priod p, h h g lo

More information

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering Lcur No Lcur-6-9 Ar rdig his lsso, you will lr ou Fourir sris xpsio rigoomric d xpoil Propris o Fourir Sris Rspos o lir sysm Normlizd powr i Fourir xpsio Powr spcrl dsiy Ec o rsr ucio o PSD. FOURIER SERIES

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

82A Engineering Mathematics

82A Engineering Mathematics Class Nos 5: Sod Ordr Diffrial Eqaio No Homoos 8A Eiri Mahmais Sod Ordr Liar Diffrial Eqaios Homoos & No Homoos v q Homoos No-homoos q ar iv oios fios o h o irval I Sod Ordr Liar Diffrial Eqaios Homoos

More information

Quantum Properties of Idealized GW Detector

Quantum Properties of Idealized GW Detector Qm Prors of Idlzd GW Dor Sg Pyo Km Ks N l Uvrsy Osk Uvrsy J 3 Th 4 h Kor-J Worksho o KAGRA Ol Idlzd Dor for Grvol Wvs Qm Thory for Dsso Wgr Fo of Tm-Dd Osllor Dmd Osllor Drv by Erl Fors Colso Idlzd Dor

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

On the Existence and uniqueness for solution of system Fractional Differential Equations

On the Existence and uniqueness for solution of system Fractional Differential Equations OSR Jourl o Mhms OSR-JM SSN: 78-578. Volum 4 ssu 3 Nov. - D. PP -5 www.osrjourls.org O h Es d uquss or soluo o ssm rol Drl Equos Mh Ad Al-Wh Dprm o Appld S Uvrs o holog Bghdd- rq Asr: hs ppr w d horm o

More information

Special Curves of 4D Galilean Space

Special Curves of 4D Galilean Space Irol Jourl of Mhml Egrg d S ISSN : 77-698 Volum Issu Mrh hp://www.jms.om/ hps://ss.googl.om/s/jmsjourl/ Spl Curvs of D ll Sp Mhm Bkş Mhmu Ergü Alpr Osm Öğrmş Fır Uvrsy Fuly of S Dprm of Mhms 9 Elzığ Türky

More information

Boyce/DiPrima/Meade 11 th ed, Ch 7.1: Introduction to Systems of First Order Linear Equations

Boyce/DiPrima/Meade 11 th ed, Ch 7.1: Introduction to Systems of First Order Linear Equations Boy/DiPrim/Md h d Ch 7.: Iroduio o Sysms of Firs Ordr Lir Equios Elmry Diffril Equios d Boudry Vlu Problms h diio by Willim E. Boy Rihrd C. DiPrim d Doug Md 7 by Joh Wily & Sos I. A sysm of simulous firs

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

EE Control Systems LECTURE 11

EE Control Systems LECTURE 11 Up: Moy, Ocor 5, 7 EE 434 - Corol Sy LECTUE Copyrigh FL Lwi 999 All righ rrv POLE PLACEMET A STEA-STATE EO Uig fc, o c ov h clo-loop pol o h h y prforc iprov O c lo lc uil copor o oi goo y- rcig y uyig

More information

1a.- Solution: 1a.- (5 points) Plot ONLY three full periods of the square wave MUST include the principal region.

1a.- Solution: 1a.- (5 points) Plot ONLY three full periods of the square wave MUST include the principal region. INEL495 SIGNALS AND SYSEMS FINAL EXAM: Ma 9, 8 Pro. Doigo Rodrígz SOLUIONS Probl O: Copl Epoial Forir Sri A priodi ri ar wav l ad a daal priod al o o od. i providd wi a a 5% d a.- 5 poi: Plo r ll priod

More information

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction F Dtto Roto Lr Alr F Roto C Y I Ursty O solto: tto o l trs s s ys os ot. Dlt to t to ltpl ws. F Roto Aotr ppro: ort y rry s tor o so E.. 56 56 > pot 6556- stol sp A st o s t ps to ollto o pots ts sp. F

More information

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory Bo/DiPima/Mad h d Ch.: High Od Lia ODEs: Gal Tho Elma Diffial Eqaios ad Boda Val Poblms h diio b William E. Bo Rihad C. DiPima ad Dog Mad 7 b Joh Wil & Sos I. A h od ODE has h gal fom d d P P P d d W assm

More information

Chapter 5 Transient Analysis

Chapter 5 Transient Analysis hpr 5 rs Alyss Jsug Jg ompl rspos rs rspos y-s rspos m os rs orr co orr Dffrl Equo. rs Alyss h ffrc of lyss of crcus wh rgy sorg lms (ucors or cpcors) & m-ryg sgls wh rss crcus s h h quos rsulg from r

More information

A Study of the Solutions of the Lotka Volterra. Prey Predator System Using Perturbation. Technique

A Study of the Solutions of the Lotka Volterra. Prey Predator System Using Perturbation. Technique Inrnionl hmil orum no. 667-67 Sud of h Soluions of h o Volrr r rdor Ssm Using rurion Thniqu D.Vnu ol Ro * D. of lid hmis IT Collg of Sin IT Univrsi Vishnm.. Indi Y... Thorni D. of lid hmis IT Collg of

More information

Approximately Inner Two-parameter C0

Approximately Inner Two-parameter C0 urli Jourl of ic d pplid Scic, 5(9: 0-6, 0 ISSN 99-878 pproximly Ir Two-prmr C0 -group of Tor Produc of C -lgr R. zri,. Nikm, M. Hi Dprm of Mmic, Md rc, Ilmic zd Uivriy, P.O.ox 4-975, Md, Ir. rc: I i ppr,

More information

Mathcad Lecture #4 In-class Worksheet Vectors and Matrices 1 (Basics)

Mathcad Lecture #4 In-class Worksheet Vectors and Matrices 1 (Basics) Mh Lr # In-l Workh Vor n Mri (Bi) h n o hi lr, o hol l o: r mri n or in Mh i mri prorm i mri mh oprion ol m o linr qion ing mri mh. Cring Mri Thr r rl o r mri. Th "Inr Mri" Wino (M) B K Poin Rr o

More information

Ch. 22: Classical Theory of Harmonic Crystal

Ch. 22: Classical Theory of Harmonic Crystal C. : Clssl Toy o mo Cysl gl o ml moo o o os l s ld o ls o pl ollowg:. Eqlbm Pops p o ls d Islos Eqlbm sy d Cos Egs Tml Epso d lg. Tspo Pops T pd o lo Tm Fl o Wdm-Fz Lw pody Tml Cody o Islos Tsmsso o od.

More information

DETERMINATION OF THERMAL STRESSES OF A THREE DIMENSIONAL TRANSIENT THERMOELASTIC PROBLEM OF A SQUARE PLATE

DETERMINATION OF THERMAL STRESSES OF A THREE DIMENSIONAL TRANSIENT THERMOELASTIC PROBLEM OF A SQUARE PLATE DRMINAION OF HRMAL SRSSS OF A HR DIMNSIONAL RANSIN HRMOLASIC PROBLM OF A SQUAR PLA Wrs K. D Dpr o Mics Sr Sivji Co Rjr Mrsr Idi *Aor or Corrspodc ABSRAC prs ppr ds wi driio o prr disribio ow prr poi o

More information

NEW FLOODWAY (CLOMR) TE TE PIN: GREENS OF ROCK HILL, LLC DB: 12209, PG: ' S67 46'18"E APPROX. FLOODWAY NEW BASE FLOOD (CLOMR)

NEW FLOODWAY (CLOMR) TE TE PIN: GREENS OF ROCK HILL, LLC DB: 12209, PG: ' S67 46'18E APPROX. FLOODWAY NEW BASE FLOOD (CLOMR) W LOOWY (LOMR) RVRWLK PKWY ROK HLL, S PPROX. LOOWY W BS LOO (LOMR) lient nformation 4 SS- RM:4 V : PV Pipe V OU: PV Pipe JB SS- RM: V OU: PV Pipe RU R " PV Pipe @. LO SPS OL SSBL GRL ORMO: S OS: M BS LOO

More information

( A) ( B) ( C) ( D) ( E)

( A) ( B) ( C) ( D) ( E) d Smsr Fial Exam Worksh x 5x.( NC)If f ( ) d + 7, h 4 f ( ) d is 9x + x 5 6 ( B) ( C) 0 7 ( E) divrg +. (NC) Th ifii sris ak has h parial sum S ( ) for. k Wha is h sum of h sris a? ( B) 0 ( C) ( E) divrgs

More information

Global Solutions of the SKT Model in Population Dynamics

Global Solutions of the SKT Model in Population Dynamics Volm 7 No 7 499-5 ISSN: 3-88 rin rion; ISSN: 34-3395 on-lin rion rl: h://ijm ijm Glol Solion of h SK Mol in Polion Dnmi Rizg Hor n Mo Soilh USH El li Ezzor lgir lgri rizg@gmilom USH El li Ezzor lgir lgri

More information

Dec. 3rd Fall 2012 Dec. 31st Dec. 16th UVC International Jan 6th 2013 Dec. 22nd-Jan 6th VDP Cancun News

Dec. 3rd Fall 2012 Dec. 31st Dec. 16th UVC International Jan 6th 2013 Dec. 22nd-Jan 6th VDP Cancun News Fll 2012 C N P D V Lk Exii Aii Or Bifl Rr! Pri Dk W ri k fr r f rr. Ti iq fr ill fr r ri ir. Ii rlxi ill fl f ir rr r - i i ri r l ll! Or k i l rf fr r r i r x, ri ir i ir l. T i r r Cri r i l ill rr i

More information

Engine Thrust. From momentum conservation

Engine Thrust. From momentum conservation Airbrhing Propulsion -1 Airbrhing School o Arospc Enginring Propulsion Ovrviw w will b xmining numbr o irbrhing propulsion sysms rmjs, urbojs, urbons, urboprops Prormnc prmrs o compr hm, usul o din som

More information

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia Par B: rasform Mhods Profssor E. Ambikairaah UNSW, Ausralia Chapr : Fourir Rprsaio of Sigal. Fourir Sris. Fourir rasform.3 Ivrs Fourir rasform.4 Propris.4. Frqucy Shif.4. im Shif.4.3 Scalig.4.4 Diffriaio

More information

LED lighting + 2.3% + 2.2% Controlling energy costs, a major competitiveness driver. Our main projects

LED lighting + 2.3% + 2.2% Controlling energy costs, a major competitiveness driver. Our main projects Clli y ss, j piivss div Sdily isi y qis Dspi pss i y ffiiy, h wldwid liiy spi is wi by ii f 2.3% p y ss ll ss. d is ps hlp y lii h ip f y ss y bsiss Hih d isi pis Th pi f liiy is sdily isi i OECD (Oisi

More information

Fourier Series: main points

Fourier Series: main points BIOEN 3 Lcur 6 Fourir rasforms Novmbr 9, Fourir Sris: mai pois Ifii sum of sis, cosis, or boh + a a cos( + b si( All frqucis ar igr mulipls of a fudamal frqucy, o F.S. ca rprs ay priodic fucio ha w ca

More information

Jonathan Turner Exam 2-10/28/03

Jonathan Turner Exam 2-10/28/03 CS Algorihm n Progrm Prolm Exm Soluion S Soluion Jonhn Turnr Exm //. ( poin) In h Fioni hp ruur, u wn vrx u n i prn v u ing u v i v h lry lo hil in i l m hil o om ohr vrx. Suppo w hng hi, o h ing u i prorm

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

Single Correct Type. cos z + k, then the value of k equals. dx = 2 dz. (a) 1 (b) 0 (c)1 (d) 2 (code-v2t3paq10) l (c) ( l ) x.

Single Correct Type. cos z + k, then the value of k equals. dx = 2 dz. (a) 1 (b) 0 (c)1 (d) 2 (code-v2t3paq10) l (c) ( l ) x. IIT JEE/AIEEE MATHS y SUHAAG SIR Bhopl, Ph. (755)3 www.kolsss.om Qusion. & Soluion. In. Cl. Pg: of 6 TOPIC = INTEGRAL CALCULUS Singl Corr Typ 3 3 3 Qu.. L f () = sin + sin + + sin + hn h primiiv of f()

More information

DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR

DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR Bllei UASVM, Horilre 65(/008 pissn 1843-554; eissn 1843-5394 DERIVING THE DEMAND CURVE ASSUMING THAT THE MARGINAL UTILITY FUNCTIONS ARE LINEAR Crii C. MERCE Uiveriy of Agrilrl iee d Veeriry Mediie Clj-Npo,

More information

The Procedure Abstraction Part II: Symbol Tables and Activation Records

The Procedure Abstraction Part II: Symbol Tables and Activation Records Th Produr Absrion Pr II: Symbol Tbls nd Aivion Rords Th Produr s Nm Sp Why inrodu lxil soping? Provids ompil-im mhnism for binding vribls Ls h progrmmr inrodu lol nms How n h ompilr kp rk of ll hos nms?

More information

Signals & Systems - Chapter 3

Signals & Systems - Chapter 3 .EgrCS.cm, i Sigls d Sysms pg 9 Sigls & Sysms - Chpr S. Ciuus-im pridic sigl is rl vlud d hs fudml prid 8. h zr Furir sris cfficis r -, - *. Eprss i h m. cs A φ Slui: 8cs cs 8 8si cs si cs Eulrs Apply

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

Chapter 7 INTEGRAL EQUATIONS

Chapter 7 INTEGRAL EQUATIONS hpr 7 INTERAL EQUATIONS hpr 7 INTERAL EQUATIONS hpr 7 Igrl Eqios 7. Normd Vcor Spcs. Eclidi vcor spc. Vcor spc o coios cios ( ) 3. Vcor Spc L ( ) 4. chy-byowsi iqliy 5. iowsi iqliy 7. Lir Oprors - coios

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

MARTIN COUNTY, FLORIDA

MARTIN COUNTY, FLORIDA RA 5 OA. RFFY A A RA RVOAL R F 8+8 O 5+ 5+ 5+ ORI 55 OA. RFFY A A RA RVOAL R 8 F 5+ O 8+8 ROFIL ORIZ: = VR: = 5 ROFIL 5 5 5 5 5+ 5+ 5+ 5+ + 5+ 8+ + + + 8+ 8+ 8+ 8+ + 5+ 8+ 5+ - --A 8-K @.5 -K @.5 -K @.5

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s ν . Po Dfo ν Ps s - Do o - M os - o oos : o o w Uows o: - ss - - Ds W ows s o qos o so s os. w ows o fo s o oos s os of o os. W w o s s ss: - ss - - Ds - Ross o ows s s q s-s os s-sss os .. Do o ..

More information

EXERCISE - 01 CHECK YOUR GRASP

EXERCISE - 01 CHECK YOUR GRASP DEFNTE NTEGRATON EXERCSE - CHECK YOUR GRASP. ( ) d [ ] d [ ] d d ƒ( ) ƒ '( ) [ ] [ ] 8 5. ( cos )( c)d 8 ( cos )( c)d + 8 ( cos )( c) d 8 ( cos )( c) d sic + cos 8 is lwys posiiv f() d ( > ) ms f() is

More information

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 3: Ideal Nozzle Fluid Mechanics

16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 3: Ideal Nozzle Fluid Mechanics 6.5, Rok ropulsion rof. nul rinz-snhz Lur 3: Idl Nozzl luid hnis Idl Nozzl low wih No Sprion (-D) - Qusi -D (slndr) pproximion - Idl gs ssumd ( ) mu + Opimum xpnsion: - or lss, >, ould driv mor forwrd

More information

Erlkönig. t t.! t t. t t t tj "tt. tj t tj ttt!t t. e t Jt e t t t e t Jt

Erlkönig. t t.! t t. t t t tj tt. tj t tj ttt!t t. e t Jt e t t t e t Jt Gsng Po 1 Agio " " lkö (Compl by Rhol Bckr, s Moifi by Mrk S. Zimmr)!! J "! J # " c c " Luwig vn Bhovn WoO 131 (177) I Wr Who!! " J J! 5 ri ris hro' h spä h, I urch J J Nch rk un W Es n wil A J J is f

More information

More on FT. Lecture 10 4CT.5 3CT.3-5,7,8. BME 333 Biomedical Signals and Systems - J.Schesser

More on FT. Lecture 10 4CT.5 3CT.3-5,7,8. BME 333 Biomedical Signals and Systems - J.Schesser Mr n FT Lcur 4CT.5 3CT.3-5,7,8 BME 333 Bimdicl Signls nd Sysms - J.Schssr 43 Highr Ordr Diffrniin d y d x, m b Y b X N n M m N M n n n m m n m n d m d n m Y n d f n [ n ] F d M m bm m X N n n n n n m p

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

P a g e 3 6 of R e p o r t P B 4 / 0 9

P a g e 3 6 of R e p o r t P B 4 / 0 9 P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J

More information

Trigonometric Formula

Trigonometric Formula MhScop g of 9 FORMULAE SHEET If h lik blow r o-fucioig ihr Sv hi fil o your hrd driv (o h rm lf of h br bov hi pg for viwig off li or ju coll dow h pg. [] Trigoomry formul. [] Tbl of uful rigoomric vlu.

More information

Lecture 4: Laplace Transforms

Lecture 4: Laplace Transforms Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions

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

FOURIER ANALYSIS Signals and System Analysis

FOURIER ANALYSIS Signals and System Analysis FOURIER ANALYSIS Isc Nwo Whi ligh cosiss of sv compos J Bpis Josph Fourir Bor: Mrch 768 i Auxrr, Bourgog, Frc Did: 6 My 83 i Pris, Frc Fourir Sris A priodic sigl of priod T sisfis ft f for ll f f for ll

More information

Thermal Stresses of Semi-Infinite Annular Beam: Direct Problem

Thermal Stresses of Semi-Infinite Annular Beam: Direct Problem iol ol o L choloy i Eii M & Alid Scic LEMAS Vol V Fy 8 SSN 78-54 hl S o Si-ii Al B: Dic Pol Viv Fl M. S. Wh d N. W. hod 3 D o Mhic Godw Uiviy Gdchioli M.S di D o Mhic Svody Mhvidyly Sidwhi M.S di 3 D o

More information

I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o

I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o u l d a l w a y s b e t a k e n, i n c l u d f o l

More information

Chapter 3 Fourier Series Representation of Periodic Signals

Chapter 3 Fourier Series Representation of Periodic Signals Chptr Fourir Sris Rprsttio of Priodic Sigls If ritrry sigl x(t or x[] is xprssd s lir comitio of som sic sigls th rspos of LI systm coms th sum of th idividul rsposs of thos sic sigls Such sic sigl must:

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

Chapter 3 Linear Equations of Higher Order (Page # 144)

Chapter 3 Linear Equations of Higher Order (Page # 144) Ma Modr Dirial Equaios Lcur wk 4 Jul 4-8 Dr Firozzama Darm o Mahmaics ad Saisics Arizoa Sa Uivrsi This wk s lcur will covr har ad har 4 Scios 4 har Liar Equaios o Highr Ordr Pag # 44 Scio Iroducio: Scod

More information

CHAPEL HILL HIGH SCHOOL - CONCEPT PLAN

CHAPEL HILL HIGH SCHOOL - CONCEPT PLAN L R R '' ''.. '' '' '' R RI RI BBRII: F B FIIH R R L. RIM LI 'Y MBLY B/ B F RB B/L B LI B/ BM F IR B/ BM F L B H BI BR IFRI BRI RI RB R I RB IL /L RLI L L M R MM M RR M I L R I RR LI Y BI YR B B I R IL

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

a dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:

a dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system: Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.

More information

Chapter 8: Waveguides, Resonant Cavities, and doptical lfibers

Chapter 8: Waveguides, Resonant Cavities, and doptical lfibers 清大物理系 電動力學 ( 二 任課老師 : 張存續 lrodmis (II (PYS 53 Sprig Smsr, Dprm of Phsis, Niol Tsig u Uivrsi, Tiw Tl. 4978, -mil: hshg@phs.hu.du.w Offi hour: 3:3-4:3 pm @Rm. 47 助教 : 趙賢文 : 9335865, s9887@m98.hu.du.w 張家銓

More information

Inverse Fourier Transform. Properties of Continuous time Fourier Transform. Review. Linearity. Reading Assignment Oppenheim Sec pp.289.

Inverse Fourier Transform. Properties of Continuous time Fourier Transform. Review. Linearity. Reading Assignment Oppenheim Sec pp.289. Convrgnc of ourir Trnsform Rding Assignmn Oppnhim Sc 42 pp289 Propris of Coninuous im ourir Trnsform Rviw Rviw or coninuous-im priodic signl x, j x j d Invrs ourir Trnsform 2 j j x d ourir Trnsform Linriy

More information

3.4 Repeated Roots; Reduction of Order

3.4 Repeated Roots; Reduction of Order 3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &

More information

Response of LTI Systems to Complex Exponentials

Response of LTI Systems to Complex Exponentials 3 Fourir sris coiuous-im Rspos of LI Sysms o Complx Expoials Ouli Cosidr a LI sysm wih h ui impuls rspos Suppos h ipu sigal is a complx xpoial s x s is a complx umbr, xz zis a complx umbr h or h h w will

More information

TABLE 3 - HOUSING MATERIAL TABLE 5 - MICRON CODE TABLE 1 - PRESSURE TABLE 2 - PORT SIZE, TYPE TABLE 4 - ELEMENT CODE TABLE 8 - ACCESSORIES

TABLE 3 - HOUSING MATERIAL TABLE 5 - MICRON CODE TABLE 1 - PRESSURE TABLE 2 - PORT SIZE, TYPE TABLE 4 - ELEMENT CODE TABLE 8 - ACCESSORIES SSMLY: XMPL: S RPLM LM: XMPL: 20 20 6 SL KI: KI - -- - XMPL: KI - -- - R R RWI RV. H SIZ 0 PM/ 00 SM SIZ L 2a - WL SPIIIO L - HOUSI MRIL L - MIRO O L - PRSSUR L 2 - POR SIZ, YP POR SIZ, PIP SOK/U LUMIUM

More information

Cambridgeshire Minerals and Waste Development Scheme. August 2017

Cambridgeshire Minerals and Waste Development Scheme. August 2017 Cmbidshi is d Ws Dm hm s 2017 Cmbidshi C Ci hi H Cs Hi Cmbid CB3 0P www.mbidshi..k 1.0 ITRDUCTI 1.1 This is d Ws Dm hm is f Cmbidshi. 1.2 Th C Ci is ssib f h i f i i id f mi d ws mm ss. I s is d sss i

More information

counting statistics in thermal transport in nanojunctions

counting statistics in thermal transport in nanojunctions rs bhvor d fll cog sscs hrml rspor ojcos J-Shg Wg Dp PhysNUS Ol of h lk rodco Mhod of oqlbrm r s fcos Applcos hrml crrs D ch d obs rs problm Fll cog sscs MS workshop Forr s lw for h codco J [ ] f f d Forr

More information

The Licking County Health Department 675 Price Rd., Newark, OH (740)

The Licking County Health Department 675 Price Rd., Newark, OH (740) T Liki y Drm 675 Pri R. Nrk O 43055 (740) 349-6535.Liki.r @iki.r A R r # W Ar Pbi Amim i Liki y : U P Sri m LD ff i ri fr fbk iify ri f Br i y fr r mmi P. Imrvm R. J b R.S. M.S. M.B.A. Liki y r mmii m

More information

Chapter4 Time Domain Analysis of Control System

Chapter4 Time Domain Analysis of Control System Chpr4 im Domi Alyi of Corol Sym Rouh biliy cririo Sdy rror ri rpo of h fir-ordr ym ri rpo of h cod-ordr ym im domi prformc pcificio h rliohip bw h prformc pcificio d ym prmr ri rpo of highr-ordr ym Dfiiio

More information

Energy, entropy and work function in a molecule with degeneracy

Energy, entropy and work function in a molecule with degeneracy Avill oli t www.worldsitifiws.om WS 97 (08) 50-57 EISS 39-9 SHOR COMMICAIO Ergy, tropy d work futio i molul with dgry Mul Mlvr Dprtmt of si Sis, Mritim ivrsity of th Cri, Cti l Mr, ul E-mil ddrss: mmf.um@gmil.om

More information

Introduction to Finite Element Method

Introduction to Finite Element Method p. o C d Eo E. Iodo o E Mod s H L p. o C d Eo E o o s Ass L. o. H L p://s.s.. p. o C d Eo E. Cos. Iodo. Appoo o os & o Cs. Eqos O so. Mdso os-es 5. szo 6. wo so Es os 7. os ps o Es 8. Io 9. Co C Isop E.

More information

EE415/515 Fundamentals of Semiconductor Devices Fall 2012

EE415/515 Fundamentals of Semiconductor Devices Fall 2012 3 EE4555 Fudmls of Smicoducor vics Fll cur 8: PN ucio iod hr 8 Forwrd & rvrs bis Moriy crrir diffusio Brrir lowrd blcd by iffusio rducd iffusio icrsd mioriy crrir drif rif hcd 3 EE 4555. E. Morris 3 3

More information

5'-33 8 " 28' " 2'-2" CARPET 95'-7 8' " B04B 1'-0" STAIR B04 UP 19R F B F QT-1/ C-1 B WD/ P-2 W DW/P-1 C DW/P-1 8' " B05 B04A

5'-33 8  28'  2'-2 CARPET 95'-7 8'  B04B 1'-0 STAIR B04 UP 19R F B F QT-1/ C-1 B WD/ P-2 W DW/P-1 C DW/P-1 8'  B05 B04A 4" UI RI (SI PIP) YIH '- " '- '- " S 4" UI RI (SI PIP) YIH 2'- " 7'- 4 " '-" 2'- " '- 9'-7 2 9'- '-07 " " '-07 " '- " 0'- '- " 4'-0 " '-9 '- 4 " '- " '- 4 " '-" 2'- 04 29'- 7'- '-4" '-4" 2'-" 4'- 4'- 7

More information

Mathematical Statistics. Chapter VIII Sampling Distributions and the Central Limit Theorem

Mathematical Statistics. Chapter VIII Sampling Distributions and the Central Limit Theorem Mahmacal ascs 8 Chapr VIII amplg Dsrbos ad h Cral Lm Thorm Fcos of radom arabls ar sall of rs sascal applcao Cosdr a s of obsrabl radom arabls L For ampl sppos h arabls ar a radom sampl of s from a poplao

More information

BENEFITS OF COMPLETING COLLEGE Lesson Plan #3

BENEFITS OF COMPLETING COLLEGE Lesson Plan #3 BENEFITS OF COMPLETING COLLEGE L Pl #3 Til: Bi Cli Cll: Ci, Srr S Sl Pr: ( y l, r i i i r/rril) S ill lr rl vl bi y ill i r bii ry i. Lri O(): ( ill b bl /k by l) S ill r bii ry i bi ir rl l liyl. Ti ill

More information

Poisson Arrival Process

Poisson Arrival Process 1 Poisso Arrival Procss Arrivals occur i) i a mmorylss mar ii) [ o arrival durig Δ ] = λδ + ( Δ ) P o [ o arrival durig Δ ] = 1 λδ + ( Δ ) P o P j arrivals durig Δ = o Δ for j = 2,3, ( ) o Δ whr lim =

More information

Study on Non-linear Responses of Eccentric Structure

Study on Non-linear Responses of Eccentric Structure Th 4 h World ofr o Erh Egrg or -7 8 Bg h Sd o No-lr Rpo of Er Srr Hdz WATANABE oh USUNI Ar TASAI 3 Grd Sd Dpr of Arhr ooh Nol Uvr ooh Jp Ao Profor Dpr of Arhr ooh Nol Uvr ooh Jp ABSTRAT : 3 Profor Dpr

More information

Handout on. Crystal Symmetries and Energy Bands

Handout on. Crystal Symmetries and Energy Bands dou o Csl s d g Bds I hs lu ou wll l: Th loshp bw ss d g bds h bs of sp-ob ouplg Th loshp bw ss d g bds h ps of sp-ob ouplg C 7 pg 9 Fh Coll Uvs d g Bds gll hs oh Th sl pol ss ddo o h l slo s: Fo pl h

More information

How delay equations arise in Engineering? Gábor Stépán Department of Applied Mechanics Budapest University of Technology and Economics

How delay equations arise in Engineering? Gábor Stépán Department of Applied Mechanics Budapest University of Technology and Economics How y quos rs Egrg? Gábor Sépá Dprm of App Ms Bups Ursy of Toogy Eooms Cos Aswr: Dy quos rs Egrg by o of bos by formo sysm of oro - Lr sby bfuros summry - M oo bros - Smmyg ws of rus moorys - Bg um robo

More information

SHINGLETON FOREST AREA Stand Level Information Compartment: 44 Entry Year: 2009

SHINGLETON FOREST AREA Stand Level Information Compartment: 44 Entry Year: 2009 iz y U oy- kg g vg. To. i Ix Mg * "Compm Pk Gloy of Tm" oum lik o wb i fo fuh ipio o fiiio. Coiio ilv. Cii M? Mho Cu Tm. Pio v Pioiy Culul N 1 5 3 13 60 7 50 42 blk pu-wmp ol gowh N 20-29 y (poil o ul)

More information

ADAPTIVE MULTISCALE HOMOGENIZATION OF THE LATTICE DISCRETE PARTICLE MODEL FOR THE ANALYSIS OF DAMAGE AND FRACTURE IN CONCRETE

ADAPTIVE MULTISCALE HOMOGENIZATION OF THE LATTICE DISCRETE PARTICLE MODEL FOR THE ANALYSIS OF DAMAGE AND FRACTURE IN CONCRETE Ssl gg Gologl f ls (SG Dpm l ml gg om Shool gg ppld S s llo 6 US DT ULTSL HOOGZTO O TH LTT DSRT RTL ODL OR TH LYSS O DG D RTUR ORT Roozh Rzh w Zho Gl s SG TRL RORT o 7-/57 Smd l ol Solds Ss 7 dp ll Homogz

More information

Inventory Model with Quadratic Demand under the Two Warehouse Management System

Inventory Model with Quadratic Demand under the Two Warehouse Management System Prin : - nlin : - A K Mlik l. / nrnionl Jornl of Enginring nd hnology JE nnory Modl wih Qdri Dmnd ndr h wo Wrhos Mngmn ysm A K Mlik Dipk Chkrory Kpil Kmr Bnsl nd * ish Kmr Assoi Profssor Dprmn of Mhmis

More information

ENJOY ALL OF YOUR SWEET MOMENTS NATURALLY

ENJOY ALL OF YOUR SWEET MOMENTS NATURALLY ENJOY ALL OF YOUR SWEET MOMENTS NATURALLY I T R Fily S U Wi Av I T R Mkr f Sr I T R L L All-Nrl Sr N Yrk, NY (Mr 202) Crl Pki Cr., kr f Sr I T R Svi I T R v x ll-rl I T R fily f r il Av I T R, 00% ri v

More information

Let's revisit conditional probability, where the event M is expressed in terms of the random variable. P Ax x x = =

Let's revisit conditional probability, where the event M is expressed in terms of the random variable. P Ax x x = = L's rvs codol rol whr h v M s rssd rs o h rdo vrl. L { M } rrr v such h { M } Assu. { } { A M} { A { } } M < { } { } A u { } { } { A} { A} ( A) ( A) { A} A A { A } hs llows us o cosdr h cs wh M { } [ (

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

Designing A Concrete Arch Bridge

Designing A Concrete Arch Bridge This is th mous Shwnh ri in Switzrln, sin y Rort Millrt in 1933. It spns 37.4 mtrs (122 t) n ws sin usin th sm rphil mths tht will monstrt in this lsson. To pro with this lsson, lik on th Nxt utton hr

More information

L RO N LEVLND GENERAL NOTES: /' ROA S PROPOSED LAND AREAS OPEN SPA CE- E AC. EARTH DITCH TOTAL PHASE V OPEN SPACE =

L RO N LEVLND GENERAL NOTES: /' ROA S PROPOSED LAND AREAS OPEN SPA CE- E AC. EARTH DITCH TOTAL PHASE V OPEN SPACE = S R S 7 S Sh b Sh b Sh R & P R RKS P ) < M H SG S GRG & P S & S P SP & R P 7 SRMR MGM P ) ) GR S R PP GR MP G PR R R R MR R S G HR ) R P R H G PRKG H RS PRPS S S G SPS SH B G G p PRP M H S R BG SS PRS

More information

EXACT SOLUTIONS FOR THE FLOW OF A GENERALIZED OLDROYD-B FLUID INDUCED BY A SUDDENLY MOVED PLATE BETWEEN TWO SIDE WALLS PERPENDICULAR TO THE PLATE

EXACT SOLUTIONS FOR THE FLOW OF A GENERALIZED OLDROYD-B FLUID INDUCED BY A SUDDENLY MOVED PLATE BETWEEN TWO SIDE WALLS PERPENDICULAR TO THE PLATE THE PUBISHIG HOUSE PROCEEDIGS OF THE ROMAIA ACADEMY Si A OF THE ROMAIA ACADEMY Vol /. 3 EXACT SOUTIOS FOR THE FOW OF A GEERAIZED ODROYD-B FUID IDUCED BY A SUDDEY MOVED PATE BETWEE TWO SIDE WAS PERPEDICUAR

More information