THE HOMOGENIZED VISCOELASTIC AND RATE DEPENDENT PLASTIC MODEL FOR PLAIN WEAVE FABRIC REINFORCED POLYMER COMPOSITES

Size: px
Start display at page:

Download "THE HOMOGENIZED VISCOELASTIC AND RATE DEPENDENT PLASTIC MODEL FOR PLAIN WEAVE FABRIC REINFORCED POLYMER COMPOSITES"

Transcription

1 18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS THE HOMOENIZED ISCOELASTIC AND RATE DEPENDENT PLASTIC MODEL FOR PLAIN WEAE FABRIC REINFORCED POLYMER COMPOSITES 1 Introducton S. L 1, C. Cho 1 *, N. Wang 1, K. K. Cho 2 1 Dpartmnt of Mchancal Engnrng, Inha Unvrsty, Inchon, Kora, 2 Dpt. of Elctrcal and Computr Engnrng, Illnos Insttut of Tchnology, IL, U.S. * Corrspondng author(cdcho@nha.ac.kr) Kywords: Plan wav fabrc, Stran rat dpndnt bhavor, scolastcty, Prony srs, Composts rnforcd by wovn fabrc ar of ncrasng ntrst n many dvrs and unqu applcatons such as arospac, automotv, marn, and mltary. Th wovn fabrc composts hav bn found mor ffctv than th undrctonal composts du to ts rnforcmnt n all drctons wthn a sngl layr. In addton, thy also hav othr advantags ncludng bttr mpact rsstanc, bttr toughnss, and good conformablty to complx shap. Ths proprts mak th wovn fabrc composts attractv n many structural applcatons. Hnc, th analyss of wovn fabrc composts to charactrz thr bhavor s an ara of actv ntrst to rsarchrs. In gnral, th bhavor of composts strongly dpnds on th gomtrc and mchancal proprts of ts consttunts,.., rnforcng fbrs and matrx, and th fabrc archtctur. Many rsarchrs hav nvstgatd ths homognzaton tchnqu for analyzng bhavors of whol compost. Ishkawa and Chou [1] dvlopd thr analytcal ondmnsonal modls, known as mosac, crmp, and brdgng modls. Ths modls consdr only th undulaton of th yarns n th loadng drcton by usng classcal lamnat thory. Nak and Shmbkar [2] and Nak and ansh [3] xtndd th abov modl to two dmnsonal lastc modls. Thy usd paralll-srs assumptons for thr mcromchancal modls basd on classcal lamnat thory. Nak [4] dvlopd thr-dmnsonal lastc modls of wovn and bradd fabrc rnforcd composts. Ths modls wr ncorporatd n computr cod for falur analyss of fabrc composts. Th yarns ar dvdd n many slcs and ths slcs ar homognzd assumng snusodal undulaton of yarns. Th homognzaton of th matral proprts s basd on so-stran assumpton. Karayaka and Kurath [5] proposd mcro-mchancal modl basd on mxd boundary condtons, whch ar so-stran and so-strss homognzaton tchnqu. Tab and Jang [6] dvlopd a mcro-mchancal modl wth nonlnar consttunt. In ths modl, th rprsntatv volum cll (RC) was dvdd nto many sub-clls and th quvalnt proprts wr obtand by an avragng tchnqu. Charactrzaton of stran rat dpndnt bhavor of composts s ssntal to prdct th dynamc bhavor such as mpact or crp phnomna assocatd wth thm. Hgh stran rat xprmnts hav bn prformd on poxy n undrctonal comprsson only to dtrmn a rhologcal modl for th poxy [7]. A sprng n paralll wth two Maxwll lmnts s usd to gt th tm-dpndnt consttutv for th vsco-lastc matral. Wang [8] showd that two Maxwll lmnts ar nough to gt th hgh stran rat rspons of poxy, though th poxy was dfnd as nonlnar modl. Karm [9] usd a two-trm lnar sprng dashpot systm to gt th hgh stran rat of th poxy. In gnral, th constants of rat dpndnt bhavor ar dtrmnd from xprmntal rsults nvolvng strss and stran curv, stran rat, and th tm of load applcaton. A common form for ths consttunt mploys a Prony srs. In ths papr, rat dpndnt mchancal bhavor of plan wovn carbon fabrc rnforcd plastc compost s nvstgatd. Th polymr matrx s assumd sotropc and vsco-lastc n lastc rgon. Th vsco-lastc bhavor s dfnd as tm doman Prony srs. Rat-dpndnt bhavor n plastc rgon s nvstgatd by Splt-Hopknson Prssur Bar (SHPB) tst. Th coffcnts of Prony srs ar obtand nductvly from th SHPB tst rsult.

2 2 Rat-dpndnt consttunt 2.1 Homognzaton Rao, Mahajan and Mttal [1] proposd a homognzaton tchnqu basd on th prncpls of avrag strss-avrag stran as follows. 1 ( xydv, ) (1) () 1 X whr m () ( xydv, ) C Cmn yn H C ( ) () s unform stran, (2) s unform strss, X m s a prodc functon rprsntng charactrstc mods of th unt cll and C H s th quvalnt homognzd stffnss coffcnts. In th prsnt study, w usd ths tchnqu to nvstgat th unt modl of plan wovn consstng 3 layrs and of ths 2 hav.25 mm thcknss, fabrc layrs and a sngl rsn layr. 2.2 Quas-statc comprsson tst Fg. 2 Instron kN Unvrsal tstng machn Th spcmns wr manufacturd as 48 pls and by vacuum bag moldng mthod. Th stackng squnc was [45/-45//9] 6s. Thy wr curd at 35 F and 41 ps for 4 hours. Th spcmns wr plan wav carbon fabrc/poxy lamnats of sz mm. For th quas-statc tst, an unvrsal matral tst machn, Instron 6567, of capacty 5kN s usd, as shown n fg. Th comprsson tst s dsplacmnt control. And th stran rat s approxmatly.2 /s. Fg. 1 Rprsntatv Unt cll and two fabrc layrs To valdat ths modl, a xampl analyss s prformd. Th compost s mad of Hrculs AS4 grapht fbrs mprgnatd wth Hrculs poxy matrx. Th fbr damtr s.7 mm and fbr volum fracton s 5%. Th dal yarn fbr packng dnsty of.78 s usd n ths analyss. Tabl 1. Yarn and rsn proprts Matral E 11 E (Pa) (Pa) (Pa) ν 12 ν 23 Yarn Rsn Rsn vsco-lastcty Polymrs ar gnrally vsco-lastc but som xhbt vsco-plastcty,.. thy undrgo prmannt dformaton upon loadng. Most xprmntal rsults on fbr-rnforcd polymrs ndcat that rgardlss to th mod of loadng, th modulus ncrass wth ncrasng stran rat, and th strngth and fractur stran may ncras dpndng on th rang of stran rat. Snc th sam rat-dpndnt bhavor had bn obsrvd for unrnforcd polymrc matrals, t s assumd that th ratdpndnt charactrstcs of th compost can b dscrbd usng tm-dpndnt or vscolastc proprty of th polymr. Th rat-dpndnt consttutv quaton for carbon/poxy compost matral s xptrssd n trms of a tm-dpndnt rlaxaton modulus. Th tm-dpndnt rlaxaton modulus s found by consdrng how th matral rlaxs undr constant stran. Th consttutv quaton s thn xprssd by lnar hrdtary law. Snc all th hgh stran rat xprmntal rsults avalabl to us ar carrd out at constant stran rat, th hrdtary law basd on constant stran rat s

3 PAPER TITLE usd to fnd matral proprts approprat for a hgh stran rat consttutv law. Thus, th homognzd consttunt can b xprssd as: 1 t () ( x, ytdv, ) g ( ) ( ) R s tsds 1 ( x, ytdv, ) X t m () mn R y n (3) E E g ()( s ts) ds H E ( ) (4) W can assum that th vscolastc matral s dfnd by a Prony srs xpanson of th dmnsonlss rlaxaton modulus; N () t E (5) 1 P g t s/ whr, ( t s) ds 2.4 Rat-dpndnt plastc bhavor For hgh stran rat tstng, a modfd SHPB apparatus was usd. Th SHPB apparatus conssts of 16 mm damtr Inconl 718 strkr, ncdnt and transmttr bars whch ar 3, 16 and 16 mm n lngth, rspctvly. Tabl 2 Matral homognzaton comparson among 3 layr unt-cll modl, 1 layr modl and tst rsults Matral 1 layr (mmtxlam) E xx,e yy (Pa) xy (Pa) ν xy layr Tst Comparson btwn xprmntal and computatonal rsult for quas-statc comprsson tst Th comprsson tst was conductd on [45/- 45//9] 6S spcmn. Th lastc comprsson modulus of th fabrc s calculatd as Pa from 3-layr FEM analyss. Th proprts of rsn ar sam as n tabl 1. Fg. 4 shows th rsults of xprmnt and fnt lmnt analyss quas-statc comprsson of [45/-45//9] 6S CFRP spcmn. Th statc yld strss s obsrvd as 2 MPa at stran.8. In th xprmntal rsult, th strss valu ncrass aftr th drop at 2 MPa, whch ths can b rgardd as yld lmt and falur. Th strssstran bhavor shows vry good conformty btwn xprmntal and FEM rsults. Fg 3. SHPB apparatus 3 Rsults and Dscusson 3.1 aldaton of unt-cll modl Th lastc bhavor of 3 layr unt modl s compard wth valus obtand from mmtexlam and xprmnts [11]. Th rsults ar compard n tabl 2. Th 3-layr unt modl shows smlar rspons to tst rsult. Fg 4. Comparson btwn Quas-statc comprsson tst and FEM rsult 3.3 Rat dpndnt bhavor Th plastc bhavors undr stran rats of 4/s, 12/s, and 15/s ar plottd n Fg. 5, obtand from th SHPB tst. Th plastc proprts lk flow strss, ultmat strngth, and stran hardnng can b 3

4 obtand sparatly from ths graphs. In numrcal analyss, ach can b xprssd as a gnral mprcal plastc consttunt calld Johnson-Cook plastcty wthout tmpratur ffct. Th yld strss for Johnson-Cook stran-rat dpndnc s xprssd as blow. pl n pl A B 1 Cln (6) Th lft trm s for stran hardnng and th rght prsnts stran rat hardnng bhavor. A, B, n and C ar matral constants ar prsntd n Tabl 3. practcal complanc rang xpctd from SHPB tst ar shown n fg. 6. To fnd Prony constants, xpctd modulus of stran rats ar convrt to complancs and ach complanc s xprssd as ratos about statc complanc as shown n tabl 4. Tabl 4 Expctd lastc modulus at 8, 12, and 15 /s stran rats Stran rat (/s).2 (Qus-statc) Complanc (/pa) Complanc Rato (%) ~ ~ ~.1 2. ~ ~ ~ 18.5 Fg. 5 Strss-Stran curv rsult from SHPB tst Tabl 3 Th matral proprts of Johnson-Cook plastcty for th CFRP [45/-45//9] 6S composts. A B Matral n (MPa) (MPa) C CFRP [45/-45//9] 6S Though th xprmntal rsult shown n Fg.5 do not mply lastc bhavor, n composts th stmaton of xact flow strss s svrly dffcult bcaus of short plastc rang; and thrfor, th Johnson-Cook plastcty s usful to fnd rat dpndnt lastcty of compost matrals. 3.4 Prdcton of Prony coffcnts Th flow strss for ach stran rat calculatd from SHPB tst r can b usd to dfn th vsco-lastc coffcnts of Prony srs, P g and. Th Fg. 6 Expctd lastc modulus rang Th complanc rducton rato can b dtrmnd from th xpctd lastc modulus. And Prony constants can b xtractd by complanc rducton rato analyss lk tabl 5. Tabl 5 scolastc prony constants for th CFRP [45/- 45//9] 6S composts. Matral CFRP [45/-45//9] 6S P g K (s) Fg. 7 and Fg. 8 show th maxmum and th spcfc tm-normalzd complanc graphs calculatd by Prony constants lstd n tabl 5.

5 PAPER TITLE 3.5 Comparson wth homognzd numrcal modl Fg. 9 compars th computatonal rsults for strssstran bhavor of CFRP [45/-45//9] 6S. Ths modl s homognzd by 3 layr unt cll modl wth Johnson-Cook plastcty. Bcaus of short prod dynamc analyss, thr ar strss rtardatons n lastc rang. Fg. 7 Complanc ncrmnt along tm Fg.7 ndcats a vry short vscolastc bhavor prod wth th statc complanc convrgng to 5. Th computatonal analyss s prformd by ABAQUS/xplct. Boundary vlocty and analyss tm for stran rats, 8 /s, 12 /s and 15 /s ar rprsntd n tabl 6. Tabl 6 Paramtrs for complanc analyss Stran rat (/s) Boundary vlocty (mm/s) Analyss tm prod(s) E E E-5 Fg. 9 Th rat dpndnt mchancal bhavor of CFRP [45/-45//9] 6S compost. SHPB rsults for dffrnt stran rat showd vry small dvaton n thr strss-stran curvs. Thus, th rat dpndnt bhavor was not sgnfcant. Ths can also b obsrvd n Fg.1, whch s magnfd vw of computatonal curvs of Fg.9 n rd box. Fg. 8 Complanc ncrmnt along tm n short tm rang. In Fg.8, for stran rat of 8 /s, analyss tm s 2.5E-5 and th normalzd complanc s 2 at th momnt. And, th complanc rducton rato s 25%. Lkws, at stran rat 12 /s and 15 /s complanc rducton ratos ar 2% and 18%, rspctvly. Fg. 1 Th rat dpndnt plastcty of CFRP [45/- 45//9] 6S compost. Fg. 1 shows Johnson-Cook plastc hardnng wth stran rat. Bcaus th rat dpndnt hardnng of Johnson-Cook plastcty s logarthm functon, th 5

6 flow strss dffrnc btwn 8 /s, 12 /s, 15 /s s not larg compard wth that of 1 /s, 1 /s, and 1 /s. Nvrthlss th numrcal rsults ft wll to th xprmntal rsult as shown n Fg. 11. composts", AIAA Journal, 1983, ol. 21, No. 12, pp [2] Nak N. K., Shmbrkar, P. S., "Elastc bhavor of wovn fabrc composts: I-lamna analyss", Journal of Compost Matral, 1992, ol. 26, No. 15, pp [3] Nak N. K., ansh,. K., "Falur bhavor of plan wav fabrc lamnats undr on-axs unaxal tnsl loadng: II analytcal prdctons", Journal of Compost Matral, 1996, ol. 3, No. 16, pp [4] Nak R. A., "Falur analyss of wovn and bradd fabrc rnforcd composts", Journal of Compost Matral, 1995, ol. 29, pp Fg. 11 Th suprposd total mchancal bhavor wth vscolastcty and rat dpndnt plastcty. Th matral modl nclud homognzd vscolastc and rat-dpndnt plastcty appld smultanously. In gnral, t s vry dffcult to masur or vn obsrv plastc bhavor n composts, partcularly th rat dpndnt bhavor n short tm lk mpact loadng. Thrfor, from practcal pont of vw th computatonal analyss and tchnqus of ths study can of sgnfcant hlp to composts and mpact ngnrng flds. In addton, t can b xtndd to nclud long trm vscolastcty. 4 Concluson Unt cll modl of plan wovn polymr compost s valdatd aftr comparson aganst commrcal softwar, mmtexlam. Th stran rat dpndnt matral consttunt s nclusvly xprssd n th lastc and plastc rgons. Ths consttunt bhavor s analyzd for wovn fabrc polymr compost undr dynamc bhavor lk mpact or crp. Acknowldgmnt Ths work was supportd by Inha unvrsty. Rfrncs [1] Ishkawa, T., and Chou T. W., "On-dmnsonal mcromchancal analyss of wovn fabrc [5] Karayaka, M. and Kurath, P., "Dformaton and falur bhavor of wovn compost lamnats", Journal of Engnrng Matral Tchnology, 1994, ol. 116, pp [6] Tab A, Jang Y, "Wovn fabrc compost matral modl wth matral nonlnarty for nonlnar fnt lmnt smulaton", Intrnatonal Journal of Solds Structur, 1999, ol. 36, No. 18, pp [7] Wks, C. A. and Sun, C. T., Modlng non-lnar rat-dpndnt bhavor n fbr-rnforcd composts, Compost Scnc and tchnology, 58, 1998, [8] Wang, L., Strss wav propagaton for nonlnar vscolastc polymrc matrals at hgh stran rats, Th Chns Journal of Mchancs- Srs A, ol.19, No. 1 [9] Mohammd R. K., "Consttutv modlng and falur crtra of carbon-fbr rnforcd polymr unr hgh stran rats", PhD dssrtaton, Unvrsty of Akron, 25 [1] M.. Rao, P. Mahajan and R. K. Mttal, Effct of archtctur on mchancal proprts of carbon/carbon compostss, Compost structur, ol 83, pp , 28 [11] K. N. Shvakumar, P. Challa and D. R. Rddy, "Mcromchancs and Lamnat Analyss of Txtl Fabrc Compost Usrs Manual", NASA lnn Rsarch Cntr, 2.

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES

HORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WITH VARIABLE PROPERTIES 13 th World Confrnc on Earthquak Engnrng Vancouvr, B.C., Canada August 1-6, 4 Papr No. 485 ORIZONTAL IMPEDANCE FUNCTION OF SINGLE PILE IN SOIL LAYER WIT VARIABLE PROPERTIES Mngln Lou 1 and Wnan Wang Abstract:

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

Constitutive Modeling of Progressive Damage in Composite Laminates

Constitutive Modeling of Progressive Damage in Composite Laminates Consttutv Modlng of Progrssv amag n Compost Lamnats Chatanya A. nadayalu *, Adt Chattopadhyay and Xu Zhou Arzona Stat Unvrsty, Tmp, AZ 8587-606 A procdur has bn dvlopd for smulatng progrssv damag n compost

More information

EXTENDED MULTISCALE FINITE ELEMENT METHOD FOR GEOMETRICALLY NONLINEAR ANALYSIS OF THIN COMPOSITE PLATES ON BENDING PROBLEMS

EXTENDED MULTISCALE FINITE ELEMENT METHOD FOR GEOMETRICALLY NONLINEAR ANALYSIS OF THIN COMPOSITE PLATES ON BENDING PROBLEMS 21 st Intrnatonal Confrnc on Compost Matrals X an, 20-25 th August 2017 XTNDD MULTISCAL FINIT LMNT MTHOD FOR GOMTRICALLY NONLINAR ANALYSIS OF THIN COMPOSIT PLATS ON BNDING PROBLMS Mngfa Rn 1, J Cong 1

More information

From Structural Analysis to FEM. Dhiman Basu

From Structural Analysis to FEM. Dhiman Basu From Structural Analyss to FEM Dhman Basu Acknowldgmnt Followng txt books wr consultd whl prparng ths lctur nots: Znkwcz, OC O.C. andtaylor Taylor, R.L. (000). Th FntElmnt Mthod, Vol. : Th Bass, Ffth dton,

More information

Spectral stochastic finite element analysis of structures with random field parameters under bounded-but-uncertain forces

Spectral stochastic finite element analysis of structures with random field parameters under bounded-but-uncertain forces Southrn Cross Unvrsty Publcatons@SCU 23rd Australasan Confrnc on th Mchancs of Structurs and Matrals 24 Spctral stochastc fnt lmnt analyss of structurs wth random fld paramtrs undr boundd-but-uncrtan forcs

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP

COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP ISAHP 00, Bal, Indonsa, August -9, 00 COMPLEX NUMBER PAIRWISE COMPARISON AND COMPLEX NUMBER AHP Chkako MIYAKE, Kkch OHSAWA, Masahro KITO, and Masaak SHINOHARA Dpartmnt of Mathmatcal Informaton Engnrng

More information

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM

Three-Node Euler-Bernoulli Beam Element Based on Positional FEM Avalabl onln at www.scncdrct.com Procda Engnrng 9 () 373 377 Intrnatonal Workshop on Informaton and Elctroncs Engnrng (IWIEE) Thr-Nod Eulr-Brnoull Bam Elmnt Basd on Postonal FEM Lu Jan a *,b, Zhou Shnj

More information

Analyzing Frequencies

Analyzing Frequencies Frquncy (# ndvduals) Frquncy (# ndvduals) /3/16 H o : No dffrnc n obsrvd sz frquncs and that prdctd by growth modl How would you analyz ths data? 15 Obsrvd Numbr 15 Expctd Numbr from growth modl 1 1 5

More information

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions

Stress-Based Finite Element Methods for Dynamics Analysis of Euler-Bernoulli Beams with Various Boundary Conditions 9 Strss-Basd Fnt Elmnt Mthods for Dynamcs Analyss of Eulr-Brnoull Bams wth Varous Boundary Condtons Abstract In ths rsarch, two strss-basd fnt lmnt mthods ncludng th curvatur-basd fnt lmnt mthod (CFE)

More information

Journal of Chemical and Pharmaceutical Research, 2014, 6(7): Research Article

Journal of Chemical and Pharmaceutical Research, 2014, 6(7): Research Article Avalabl onln www.ocpr.com Journal of Chmcal and Pharmacutcal Rsarch, 214, 6(7):1394-14 Rsarch Artcl ISSN : 975-7384 COEN(USA) : JCPRC5 Rsarch on fatgu damag of suckr rod basd on damag mchancs Ru-fn Zhou,

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Linear Algebra Provides a Basis for Elasticity without Stress or Strain

Linear Algebra Provides a Basis for Elasticity without Stress or Strain Soft, 05, 4, 5-4 Publshd Onln Sptmbr 05 n ScRs. http://www.scrp.org/ournal/soft http://dx.do.org/0.46/soft.05.400 Lnar Algbra Provds a Bass for Elastcty wthout Strss or Stran H. H. Hardy Math/Physcs Dpartmnt,

More information

Optimal Topology Design for Replaceable of Reticulated Shell Based on Sensitivity Analysis

Optimal Topology Design for Replaceable of Reticulated Shell Based on Sensitivity Analysis Optmal Topology Dsgn for Rplacabl of Rtculatd Shll Basd on Snstvty Analyss Yang Yang Dpartmnt of Naval Archtctur, Dalan Unvrsty of Tchnology, Laonng, CN Ma Hu Collg of Rsourc and Cvl Engnrng, Northastrn

More information

Influence of Fiber Orientation on the Natural Frequencies of Laminated Composite Beams

Influence of Fiber Orientation on the Natural Frequencies of Laminated Composite Beams Intrnatonal Journal of Engnrng Rsarch And Advancd Tchnology (IJERAT) DOI: http://d.do.org/.74/ijerat.7.5 E-ISS : 454-65 Vol. (9) Sp -7 Influnc of Fbr Orntaton on th atural Fruncs of Lamnatd Compost Bams

More information

OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS

OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS Th Svnth East Asa-Pacfc Confrnc on Structural Engnrng & Constructon August 27-29, 1999, Koch, Japan OPTIMAL TOPOLOGY SELECTION OF CONTINUUM STRUCTURES WITH STRESS AND DISPLACEMENT CONSTRAINTS Qng Quan

More information

CHAPTER 33: PARTICLE PHYSICS

CHAPTER 33: PARTICLE PHYSICS Collg Physcs Studnt s Manual Chaptr 33 CHAPTER 33: PARTICLE PHYSICS 33. THE FOUR BASIC FORCES 4. (a) Fnd th rato of th strngths of th wak and lctromagntc forcs undr ordnary crcumstancs. (b) What dos that

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS

Lecture 23 APPLICATIONS OF FINITE ELEMENT METHOD TO SCALAR TRANSPORT PROBLEMS COMPUTTION FUID DYNMICS: FVM: pplcatons to Scalar Transport Prolms ctur 3 PPICTIONS OF FINITE EEMENT METHOD TO SCR TRNSPORT PROBEMS 3. PPICTION OF FEM TO -D DIFFUSION PROBEM Consdr th stady stat dffuson

More information

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS

ACOUSTIC WAVE EQUATION. Contents INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS ACOUSTIC WAE EQUATION Contnts INTRODUCTION BULK MODULUS AND LAMÉ S PARAMETERS INTRODUCTION As w try to vsualz th arth ssmcally w mak crtan physcal smplfcatons that mak t asr to mak and xplan our obsrvatons.

More information

Naresuan University Journal: Science and Technology 2018; (26)1

Naresuan University Journal: Science and Technology 2018; (26)1 Narsuan Unvrsty Journal: Scnc and Tchnology 018; (6)1 Th Dvlopmnt o a Corrcton Mthod or Ensurng a Contnuty Valu o Th Ch-squar Tst wth a Small Expctd Cll Frquncy Kajta Matchma 1 *, Jumlong Vongprasrt and

More information

INTERFACE CORNERS IN ANISOTROPIC/PIEZOELECTRIC/ VISCOELASTIC MATERIALS

INTERFACE CORNERS IN ANISOTROPIC/PIEZOELECTRIC/ VISCOELASTIC MATERIALS INERFAE ORNERS IN ANISOROPI/PIEZOELERI/ VISOELASI MAERIALS hyanbn Hwu a-lang uo Insttut of Aronautcs and Astronautcs Natonal hng ung Unvrsty anan AIWAN R.O.. Ansotropc matrals bhav dffrntly n dffrnt drctons.

More information

Mullins Effect and Thixotropy

Mullins Effect and Thixotropy Mullns Effct and Thxotropy Engnrng Strss (MPa) 006 NNF Summr Radng Srs August 9, 006 Artcls λ (= L/L o ) Shawna M. Lff Insttut for Soldr Nanotchnologs Dpartmnt of Mchancal Engnrng MIT, Cambrdg, MA 039

More information

EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12

EEC 686/785 Modeling & Performance Evaluation of Computer Systems. Lecture 12 EEC 686/785 Modlng & Prformanc Evaluaton of Computr Systms Lctur Dpartmnt of Elctrcal and Computr Engnrng Clvland Stat Unvrsty wnbng@.org (basd on Dr. Ra Jan s lctur nots) Outln Rvw of lctur k r Factoral

More information

Physics 256: Lecture 2. Physics

Physics 256: Lecture 2. Physics Physcs 56: Lctur Intro to Quantum Physcs Agnda for Today Complx Numbrs Intrfrnc of lght Intrfrnc Two slt ntrfrnc Dffracton Sngl slt dffracton Physcs 01: Lctur 1, Pg 1 Constructv Intrfrnc Ths wll occur

More information

Dynamic Modeling and Vibration Control for Spacecraft s Solar Array Jian-Ping JIANG 1,a, *, Rui XU 2,b

Dynamic Modeling and Vibration Control for Spacecraft s Solar Array Jian-Ping JIANG 1,a, *, Rui XU 2,b Intrnatonal Confrnc on Mchancs and Cvl Engnrng (ICMCE 2014) Dynamc Modlng and Vbraton Control for Spaccraft s Solar Array Jan-Png JIANG 1,a, *, Ru XU 2,b 1,2 Collg of Arospac Scnc and Engnrng, Natonal

More information

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous

ST 524 NCSU - Fall 2008 One way Analysis of variance Variances not homogeneous ST 54 NCSU - Fall 008 On way Analyss of varanc Varancs not homognous On way Analyss of varanc Exampl (Yandll, 997) A plant scntst masurd th concntraton of a partcular vrus n plant sap usng ELISA (nzym-lnkd

More information

Review - Probabilistic Classification

Review - Probabilistic Classification Mmoral Unvrsty of wfoundland Pattrn Rcognton Lctur 8 May 5, 6 http://www.ngr.mun.ca/~charlsr Offc Hours: Tusdays Thursdays 8:3-9:3 PM E- (untl furthr notc) Gvn lablld sampls { ɛc,,,..., } {. Estmat Rvw

More information

PREDICTION OF STRESS CONCENTRATION FACTORS IN UNLAPPED SQUARE HOLLOW "K" JOINTS BY THE FINITE ELEMENT METHOD

PREDICTION OF STRESS CONCENTRATION FACTORS IN UNLAPPED SQUARE HOLLOW K JOINTS BY THE FINITE ELEMENT METHOD Ngran Journal of chnology, Vol. 5, No., March 006 Jk 5 PREDICION OF SRESS CONCENRAION FACORS IN UNLAPPED SQUARE HOLLOW "K" JOINS BY HE FINIE ELEMEN MEHOD DR.P.N.JIKI Dpartmnt of Cvl Engnrng, Unvrsty of

More information

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Univ.-Prof. Dr. Jan Franke-Viebach Unv.Prof. r. J. FrankVbach WS 067: Intrnatonal Economcs ( st xam prod) Unvrstät Sgn Fakultät III Unv.Prof. r. Jan FrankVbach Exam Intrnatonal Economcs Wntr Smstr 067 ( st Exam Prod) Avalabl tm: 60 mnuts

More information

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D Comp 35 Introducton to Machn Larnng and Data Mnng Fall 204 rofssor: Ron Khardon Mxtur Modls Motvatd by soft k-mans w dvlopd a gnratv modl for clustrng. Assum thr ar k clustrs Clustrs ar not rqurd to hav

More information

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces

Electrochemical Equilibrium Electromotive Force. Relation between chemical and electric driving forces C465/865, 26-3, Lctur 7, 2 th Sp., 26 lctrochmcal qulbrum lctromotv Forc Rlaton btwn chmcal and lctrc drvng forcs lctrochmcal systm at constant T and p: consdr G Consdr lctrochmcal racton (nvolvng transfr

More information

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges

Physics of Very High Frequency (VHF) Capacitively Coupled Plasma Discharges Physcs of Vry Hgh Frquncy (VHF) Capactvly Coupld Plasma Dschargs Shahd Rauf, Kallol Bra, Stv Shannon, and Kn Collns Appld Matrals, Inc., Sunnyval, CA AVS 54 th Intrnatonal Symposum Sattl, WA Octobr 15-19,

More information

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University

External Equivalent. EE 521 Analysis of Power Systems. Chen-Ching Liu, Boeing Distinguished Professor Washington State University xtrnal quvalnt 5 Analyss of Powr Systms Chn-Chng Lu, ong Dstngushd Profssor Washngton Stat Unvrsty XTRNAL UALNT ach powr systm (ara) s part of an ntrconnctd systm. Montorng dvcs ar nstalld and data ar

More information

Heating of a solid cylinder immersed in an insulated bath. Thermal diffusivity and heat capacity experimental evaluation.

Heating of a solid cylinder immersed in an insulated bath. Thermal diffusivity and heat capacity experimental evaluation. Hatng of a sold cylndr mmrsd n an nsulatd bath. Thrmal dffusvty and hat capacty xprmntal valuaton. Žtný R., CTU FE Dpartmnt of Procss Engnrng, arch. Introducton Th problm as ntatd by th follong E-mal from

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

Lecture 3: Phasor notation, Transfer Functions. Context

Lecture 3: Phasor notation, Transfer Functions. Context EECS 5 Fall 4, ctur 3 ctur 3: Phasor notaton, Transfr Functons EECS 5 Fall 3, ctur 3 Contxt In th last lctur, w dscussd: how to convrt a lnar crcut nto a st of dffrntal quatons, How to convrt th st of

More information

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint

Optimal Ordering Policy in a Two-Level Supply Chain with Budget Constraint Optmal Ordrng Polcy n a Two-Lvl Supply Chan wth Budgt Constrant Rasoul aj Alrza aj Babak aj ABSTRACT Ths papr consdrs a two- lvl supply chan whch consst of a vndor and svral rtalrs. Unsatsfd dmands n rtalrs

More information

A Study on Nonlinear Forced Vibration of an Axial Moving Viscoelasticity Beam using the Multi-Scale Approach

A Study on Nonlinear Forced Vibration of an Axial Moving Viscoelasticity Beam using the Multi-Scale Approach BAO-FU KOU t al: A STUDY ON NONLINEAR FORCED VIBRATION OF AN AXIAL MOVING A Study on Nonlnar Forcd Vbraton of an Axal Movng Vscolastcty Bam usng th Mult-Scal Approach Bao-Fu Kou *, Xao-L Hu Collg of Mchancal

More information

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization

Economics 600: August, 2007 Dynamic Part: Problem Set 5. Problems on Differential Equations and Continuous Time Optimization THE UNIVERSITY OF MARYLAND COLLEGE PARK, MARYLAND Economcs 600: August, 007 Dynamc Part: Problm St 5 Problms on Dffrntal Equatons and Contnuous Tm Optmzaton Quston Solv th followng two dffrntal quatons.

More information

Modelling of new generation plasma optical devices

Modelling of new generation plasma optical devices NUKLEONIKA 216;61(2):27212 do: 1.1515/nuka-216-35 ORIGINAL PAPER Modllng of nw gnraton plasma optcal dvcs Irna V. Ltovko, Aly A. Goncharov, Andrw N. Dobrovolsky, Lly V. Nako, Irna V. Nako Abstract. Th

More information

GPC From PeakSimple Data Acquisition

GPC From PeakSimple Data Acquisition GPC From PakSmpl Data Acquston Introducton Th follong s an outln of ho PakSmpl data acquston softar/hardar can b usd to acqur and analyz (n conjuncton th an approprat spradsht) gl prmaton chromatography

More information

Transient Multiexponential Data Analysis Using A Combination of ARMA and ECD Methods

Transient Multiexponential Data Analysis Using A Combination of ARMA and ECD Methods 4 th Intrnatonal Confrnc on Computr Engnrng and Tchnology (ICCET IPCIT vol.4 ( ( IACIT Prss, ngapor Transnt ultxponntal Data Analyss Usng A Combnaton of ARA and ECD thods Abdussamad U. Jba, omoh-jmoh E.

More information

Polytropic Process. A polytropic process is a quasiequilibrium process described by

Polytropic Process. A polytropic process is a quasiequilibrium process described by Polytropc Procss A polytropc procss s a quasqulbrum procss dscrbd by pv n = constant (Eq. 3.5 Th xponnt, n, may tak on any valu from to dpndng on th partcular procss. For any gas (or lqud, whn n = 0, th

More information

FINITE ELEMENT METHOD II Autumn 2015

FINITE ELEMENT METHOD II Autumn 2015 FEM II - Lctur Pag of 4 FINITE ELEMENT METHOD II Autumn 05 Lcturs (5h):. Accuracy, rror stmaton and adaptv rmshng. Hat flow and thrmal strsss n FEM 3. Introducton to structural dynamcs, fr vbratons 4.

More information

A Simple FEM Formulation Applied to Nonlinear Problems of Impact with Thermomechanical Coupling

A Simple FEM Formulation Applied to Nonlinear Problems of Impact with Thermomechanical Coupling 2439 A Smpl FEM Formulaton Appld to Nonlnar Problms of Impact wth Thrmomchancal Couplng Abstract Th thrmal ffcts of problms nvolvng dformabl structurs ar ssntal to dscrb th bhavor of matrals n fasbl trms.

More information

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs.

Two-Temperature Plasma Modeling of Argon Gas Tungsten Arcs. Ttl Autor(s) Two-Tmpratur Plasma Modlng of Argon Gas Tungstn Arcs Tasro, Snc; Tanaa, Manabu Ctaton Transactons of JWRI. 37(1) P.7-P.11 Issu Dat 2008-07 Txt Vrson publsr URL ttp://dl.andl.nt/11094/8887

More information

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved.

Journal of Theoretical and Applied Information Technology 10 th January Vol. 47 No JATIT & LLS. All rights reserved. Journal o Thortcal and Appld Inormaton Tchnology th January 3. Vol. 47 No. 5-3 JATIT & LLS. All rghts rsrvd. ISSN: 99-8645 www.att.org E-ISSN: 87-395 RESEARCH ON PROPERTIES OF E-PARTIAL DERIVATIVE OF LOGIC

More information

Performance assessment of the window-wall interface. PhD-meeting Nathan Van Den Bossche - 04/06/2010 Department of Architecture Ghent University

Performance assessment of the window-wall interface. PhD-meeting Nathan Van Den Bossche - 04/06/2010 Department of Architecture Ghent University Prformanc assssmnt of th wndow-wall ntrfac Start: 04/2007 Stop: 01/2012 Nathan Van Dn Bossch Suprvsor: Arnold Janssns Hstory of Enrgy cods n Flandrs: 1992: Vntlaton and nsulaton dcr nsulaton lvl K65 1993:

More information

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 1, 2011

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 1, 2011 INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volum, No, Copyrght All rghts rsrvd Intgratd Publshng srvcs Rsarch artcl ISSN 9 99 An conomc comparson of Drct dsplacmnt basd Dsgn wth IS-9 Rspons

More information

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D

Soft k-means Clustering. Comp 135 Machine Learning Computer Science Tufts University. Mixture Models. Mixture of Normals in 1D Comp 35 Machn Larnng Computr Scnc Tufts Unvrsty Fall 207 Ron Khardon Th EM Algorthm Mxtur Modls Sm-Suprvsd Larnng Soft k-mans Clustrng ck k clustr cntrs : Assocat xampls wth cntrs p,j ~~ smlarty b/w cntr

More information

EFFECTS OF SECONDARY STRUCTURE ON ELASTIC BEHAVIOR OF PROTEIN-LIKE CHAINS *

EFFECTS OF SECONDARY STRUCTURE ON ELASTIC BEHAVIOR OF PROTEIN-LIKE CHAINS * Chns Journal of Polymr Scnc Vol. 27, No. 2, (2009), 253 265 Chns Journal of Polymr Scnc 2009 World Scntfc EFFECTS OF SECONDARY STRUCTURE ON ELASTIC BEHAVIOR OF PROTEIN-LIKE CHAINS * Tng-tng Sun a**, Ha-zhu

More information

Discrete Shells Simulation

Discrete Shells Simulation Dscrt Shlls Smulaton Xaofng M hs proct s an mplmntaton of Grnspun s dscrt shlls, th modl of whch s govrnd by nonlnar mmbran and flxural nrgs. hs nrgs masur dffrncs btwns th undformd confguraton and th

More information

CHAPTER 4. The First Law of Thermodynamics for Control Volumes

CHAPTER 4. The First Law of Thermodynamics for Control Volumes CHAPTER 4 T Frst Law of Trodynacs for Control olus CONSERATION OF MASS Consrvaton of ass: Mass, lk nrgy, s a consrvd proprty, and t cannot b cratd or dstroyd durng a procss. Closd systs: T ass of t syst

More information

EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In the absence of or in between ELMs)

EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In the absence of or in between ELMs) I. EDGE PEDESTAL STRUCTURE AND TRANSPORT INTERPRETATION (In th absnc of or n btwn ELMs) Abstract W. M. Stacy (Gorga Tch) and R. J. Grobnr (Gnral Atomcs) A constrant on th on prssur gradnt s mposd by momntum

More information

A Novel Finite Volume Scheme with Geometric Average Method for Radiative Heat Transfer Problems *

A Novel Finite Volume Scheme with Geometric Average Method for Radiative Heat Transfer Problems * Appld Physcs Frontr Novmbr 013 Volum 1 Issu 4 PP.3-44 A Novl Fnt Volum Schm wth Gomtrc Avrag Mthod for Radatv Hat Transfr Problms * Cunyun N 1 Hayuan Yu 1. Dpartmnt of Mathmatcs and Physcs Hunan Insttuton

More information

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS

ON THE COMPLEXITY OF K-STEP AND K-HOP DOMINATING SETS IN GRAPHS MATEMATICA MONTISNIRI Vol XL (2017) MATEMATICS ON TE COMPLEXITY OF K-STEP AN K-OP OMINATIN SETS IN RAPS M FARAI JALALVAN AN N JAFARI RA partmnt of Mathmatcs Shahrood Unrsty of Tchnology Shahrood Iran Emals:

More information

SCITECH Volume 5, Issue 1 RESEARCH ORGANISATION November 17, 2015

SCITECH Volume 5, Issue 1 RESEARCH ORGANISATION November 17, 2015 Journal of Informaton Scncs and Computng Tchnologs(JISCT) ISSN: 394-966 SCITECH Volum 5, Issu RESEARCH ORGANISATION Novmbr 7, 5 Journal of Informaton Scncs and Computng Tchnologs www.sctcrsarch.com/journals

More information

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS

FREE VIBRATION ANALYSIS OF FUNCTIONALLY GRADED BEAMS Journal of Appl Mathatcs an Coputatonal Mchancs, (), 9- FREE VIBRATION ANAYSIS OF FNCTIONAY GRADED BEAMS Stansław Kukla, Jowta Rychlwska Insttut of Mathatcs, Czstochowa nvrsty of Tchnology Czstochowa,

More information

Chapter 6 Student Lecture Notes 6-1

Chapter 6 Student Lecture Notes 6-1 Chaptr 6 Studnt Lctur Nots 6-1 Chaptr Goals QM353: Busnss Statstcs Chaptr 6 Goodnss-of-Ft Tsts and Contngncy Analyss Aftr compltng ths chaptr, you should b abl to: Us th ch-squar goodnss-of-ft tst to dtrmn

More information

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering

Phys 774: Nonlinear Spectroscopy: SHG and Raman Scattering Last Lcturs: Polaraton of Elctromagntc Wavs Phys 774: Nonlnar Spctroscopy: SHG and Scattrng Gnral consdraton of polaraton Jons Formalsm How Polarrs work Mullr matrcs Stoks paramtrs Poncar sphr Fall 7 Polaraton

More information

Shape sensing of aerospace structures by coupling of isogeometric analysis and inverse finite element method

Shape sensing of aerospace structures by coupling of isogeometric analysis and inverse finite element method Shap snsng of arospac structurs by couplng of sogomtrc analyss and nvrs fnt lmnt mthod dnan Kfal and Erkan Otrkus Unvrsty of Strathclyd, 00 Montros Strt, Glasgow G4 0LZ, UK Ths papr prsnts a novl sogomtrc

More information

ANALYTICITY THEOREM FOR FRACTIONAL LAPLACE TRANSFORM

ANALYTICITY THEOREM FOR FRACTIONAL LAPLACE TRANSFORM Sc. Rs. hm. ommn.: (3, 0, 77-8 ISSN 77-669 ANALYTIITY THEOREM FOR FRATIONAL LAPLAE TRANSFORM P. R. DESHMUH * and A. S. GUDADHE a Prof. Ram Mgh Insttt of Tchnology & Rsarch, Badnra, AMRAVATI (M.S. INDIA

More information

Electrostatic Surface Waves on Semi-Bounded Quantum Electron-Hole Semiconductor Plasmas

Electrostatic Surface Waves on Semi-Bounded Quantum Electron-Hole Semiconductor Plasmas Commun. Thor. Phys. 67 07 37 3 Vol. 67 No. 3 March 07 Elctrostatc Surfac Wavs on Sm-Boundd Quantum Elctron-Hol Smconductor Plasmas Afshn Morad Dpartmnt of Engnrng Physcs Krmanshah Unvrsty of Tchnology

More information

Stretching and bending deformations due to normal and shear tractions of doubly curved shells using third-order shear and normal deformable theory

Stretching and bending deformations due to normal and shear tractions of doubly curved shells using third-order shear and normal deformable theory MECHANICS OF ADVANCED MATERIALS AND STRUCTURES 2016,VOL.0,NO.0,1 20 http://dx.do.org/10.1080/15376494.2016.1194505 ORIGINAL ARTICLE Strtchng and bndng dformatons du to normal and shar tractons of doubly

More information

Transient Response of Strain Rate Dependent Polymer Matrix Composite Laminates

Transient Response of Strain Rate Dependent Polymer Matrix Composite Laminates ransnt Rspons o tran Rat Dpndnt Polmr Matr Compost Lamnats Lna Zu * and Adt Cattopada Dpartmnt o Mcancal and Arospac Engnrng Arona tat Unvrst mp AZ 887- and Robrt K. Goldbrg atonal Aronautcs and pac Admnstraton

More information

Group Codes Define Over Dihedral Groups of Small Order

Group Codes Define Over Dihedral Groups of Small Order Malaysan Journal of Mathmatcal Scncs 7(S): 0- (0) Spcal Issu: Th rd Intrnatonal Confrnc on Cryptology & Computr Scurty 0 (CRYPTOLOGY0) MALAYSIA JOURAL OF MATHEMATICAL SCIECES Journal hompag: http://nspm.upm.du.my/ournal

More information

Plasma Simulation Algorithm for the Two-Fluid Plasma Model

Plasma Simulation Algorithm for the Two-Fluid Plasma Model ELIGIBLE Plasma Smulaton Algorthm for th Two-Flud Plasma Modl U. Shumlak, C. Abrl, A. Hakm, and J. Lovrch Arospac & Enrgtcs Rsarch Program Unvrsty of Washngton, Sattl, USA Confrnc on Computatonal Physcs

More information

Numerical simulation of ultra precision machining based on molecular dynamics and finite element simulation

Numerical simulation of ultra precision machining based on molecular dynamics and finite element simulation Rvsta d la Facultad d Ingnría U.C.V., Vol. 3, N 14, pp. 315-30, 017 Numrcal smulaton of ultra prcson machnng basd on molcular dynamcs and fnt lmnt smulaton Wgang Guo 1,, Julong Yuan 1, Zhn Xang 1, Png

More information

Constitutive behaviour of masonry

Constitutive behaviour of masonry Hstorcal Constructons, P.B. Lournço, P. Roca (Eds.), Gumarãs, 21 585 Consttutv bhavour of masonry G. Frunzo, M. Monaco S. U. N. Scond Unvrsty of Napls, Faculty of Archtctur, Abbaza d S. Lornzo, 8131 Avrsa

More information

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION

CHAPTER 7d. DIFFERENTIATION AND INTEGRATION CHAPTER 7d. DIFFERENTIATION AND INTEGRATION A. J. Clark School o Engnrng Dpartmnt o Cvl and Envronmntal Engnrng by Dr. Ibrahm A. Assakka Sprng ENCE - Computaton Mthods n Cvl Engnrng II Dpartmnt o Cvl and

More information

Numerical Study of Two-fluid Flowing Equilibria of Helicity-driven Spherical Torus Plasmas

Numerical Study of Two-fluid Flowing Equilibria of Helicity-driven Spherical Torus Plasmas Numrcal Study of Two-flud Flowng Equlbra of Hlcty-drvn Sphrcal Torus Plasmas T. Kank M. Nagata and T. Uyama Japan Coast Guard Acadmy 5-1 Wakaba Kur Hroshma 737-851 Japan Dpartmnt of Elctrcal Engnrng and

More information

VIBRATION ANALYSIS AND DAMPING CHARACTERISTICS OF Hybrid COMPOSITE PLATE USING FINITE ELEMENT ANALYSIS

VIBRATION ANALYSIS AND DAMPING CHARACTERISTICS OF Hybrid COMPOSITE PLATE USING FINITE ELEMENT ANALYSIS VIBRION NLYSIS ND DMPING CHRCERISICS OF Hybrd COMPOSIE PLE USING FINIE ELEMEN NLYSIS hss submttd n partal fulfllmnt of th Rqurmnts for th dgr of Mastr of chnology In Mchancal Engnrng Spcalzaton: Machn

More information

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS

APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF 3D DIFFUSION IN SOLIDS Cênca/Scnc APPLICATION OF GALERKIN FINITE ELEMENT METHOD IN THE SOLUTION OF D DIFFUSION IN SOLIDS E C Romão a, M D d Campos c, J A Martns b, and L F M d Moura a Unvrsdad Estadual d Campnas Faculdad d Engnhara

More information

te Finance (4th Edition), July 2017.

te Finance (4th Edition), July 2017. Appndx Chaptr. Tchncal Background Gnral Mathmatcal and Statstcal Background Fndng a bas: 3 2 = 9 3 = 9 1 /2 x a = b x = b 1/a A powr of 1 / 2 s also quvalnt to th squar root opraton. Fndng an xponnt: 3

More information

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn.

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn. Modul 10 Addtonal Topcs 10.1 Lctur 1 Prambl: Dtrmnng whthr a gvn ntgr s prm or compost s known as prmalty tstng. Thr ar prmalty tsts whch mrly tll us whthr a gvn ntgr s prm or not, wthout gvng us th factors

More information

Mathematical Model of Arterial Hemodynamics, Description, Computer Implementation, Results Comparison

Mathematical Model of Arterial Hemodynamics, Description, Computer Implementation, Results Comparison Appld Physcs Rsarch; Vol. 5, No. 3; 3 ISSN 96-9639 E-ISSN 96-9647 Publshd by Canadan Cntr of Scnc and Educaton Mathmatcal Modl of Artral Hmodynamcs, Dscrpton, Computr Implmntaton, Rsults Comparson Elshn

More information

Los Alamos. Numerical Simulation of Industrial Superplastic Formin; Final Report LA-13222

Los Alamos. Numerical Simulation of Industrial Superplastic Formin; Final Report LA-13222 LA-13222 Numrcal Smulaton of Industral Suprplastc Formn; Fnal Rport Los Alamos N A T I O N A L LABORATORY Los Alumos Natonal Luborutoy s opruld b.v th Unvrs& of CulJornufor th Unld Stats Dpurfmnt of Enrgv

More information

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time.

??? Dynamic Causal Modelling for M/EEG. Electroencephalography (EEG) Dynamic Causal Modelling. M/EEG analysis at sensor level. time. Elctroncphalography EEG Dynamc Causal Modllng for M/EEG ampltud μv tm ms tral typ 1 tm channls channls tral typ 2 C. Phllps, Cntr d Rchrchs du Cyclotron, ULg, Blgum Basd on slds from: S. Kbl M/EEG analyss

More information

NON-SYMMETRY POWER IN THREE-PHASE SYSTEMS

NON-SYMMETRY POWER IN THREE-PHASE SYSTEMS O-YMMETRY OWER THREE-HAE YTEM Llana Marlna MATCA nvrsty of Orada, nvrstat str., no., 487, Orada; lmatca@uorada.ro Abstract. For thr-phas lctrcal systms, n non-symmtrcal stuaton, an analyz mthod costs on

More information

Simplified damage models applied in the numerical analysis of reinforced concrete structures

Simplified damage models applied in the numerical analysis of reinforced concrete structures Volum 5, Numbr 1 (Fbruary, 1 p. 637 ISSN 19834195 Smplfd damag modls appld n th numrcal analyss of rnforcd concrt structurs Sobr o mprgo d modlos smplfcados d dano na análs d struturas m concrto armado

More information

CLASSICAL STATISTICS OF PARAMAGNETISM

CLASSICAL STATISTICS OF PARAMAGNETISM Prof. Dr. I. assr Phys 530 8-Dc_0 CLASSICAL STATISTICS OF PARAMAGETISM Th most famous typs of Magntc matrals ar: () Paramagntc: A proprty xhbt by substancs whch, whn placd n a magntc fld, ar magntd paralll

More information

RESEARCH ARTICLE. An incremental-secant mean-field homogenisation method with second statistical moments for elasto-plastic composite materials

RESEARCH ARTICLE. An incremental-secant mean-field homogenisation method with second statistical moments for elasto-plastic composite materials May 8, 5 Phlosophcal Magazn manuscrpt-pm Phlosophcal Magazn Vol., No., Month, 6 RESEARCH ARTICLE An ncrmntal-scant man-fld homognsaton mthod wth scond statstcal momnts for lasto-plastc compost matrals

More information

A NON-LINEAR MODEL FOR STUDYING THE MOTION OF A HUMAN BODY. Piteşti, , Romania 2 Department of Automotive, University of Piteşti

A NON-LINEAR MODEL FOR STUDYING THE MOTION OF A HUMAN BODY. Piteşti, , Romania 2 Department of Automotive, University of Piteşti ICSV Carns ustrala 9- July 7 NON-LINER MOEL FOR STUYING THE MOTION OF HUMN OY Ncola-oru Stănscu Marna Pandra nl Popa Sorn Il Ştfan-Lucan Tabacu partnt of ppld Mchancs Unvrsty of Ptşt Ptşt 7 Roana partnt

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

From Structural Analysis to Finite Element Method

From Structural Analysis to Finite Element Method From Structural Analyss to Fnt Elmnt Mthod Dhman Basu II Gandhnagar -------------------------------------------------------------------------------------------------------------------- Acknowldgmnt Followng

More information

TEARING OF STYRENE BUTADIENE RUBBER USING FINITE ELEMENT ANALYSIS. A Thesis. Presented to. The Graduate Faculty of The University of Akron

TEARING OF STYRENE BUTADIENE RUBBER USING FINITE ELEMENT ANALYSIS. A Thesis. Presented to. The Graduate Faculty of The University of Akron EARING O SYRENE BUADIENE RUBBER USING INIE ELEMEN ANALYSIS A hss Prsntd to h Graduat aculty of h Unrsty of Akron In Partal ulfllmnt of th Rqurmnts for th Dgr Mastr of Scnc Vnkata Rama Lakshm Prth Bahadursha

More information

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation Lctur Rlc nutrnos mpratur at nutrno dcoupln and today Effctv dnracy factor Nutrno mass lmts Saha quaton Physcal Cosmoloy Lnt 005 Rlc Nutrnos Nutrnos ar wakly ntractn partcls (lptons),,,,,,, typcal ractons

More information

MECH321 Dynamics of Engineering System Week 4 (Chapter 6)

MECH321 Dynamics of Engineering System Week 4 (Chapter 6) MH3 Dynamc of ngnrng Sytm Wk 4 (haptr 6). Bac lctrc crcut thor. Mathmatcal Modlng of Pav rcut 3. ompl mpdanc Approach 4. Mchancal lctrcal analogy 5. Modllng of Actv rcut: Opratonal Amplfr rcut Bac lctrc

More information

APPLICABILITY OF LINEARIZED DUSTY GAS MODEL FOR MULTICOMPONENT DIFFUSION OF GAS MIXTURES IN POROUS SOLIDS. Jelena Markovi and Radovan Omorjan

APPLICABILITY OF LINEARIZED DUSTY GAS MODEL FOR MULTICOMPONENT DIFFUSION OF GAS MIXTURES IN POROUS SOLIDS. Jelena Markovi and Radovan Omorjan APTEFF, 38, 1-19 (7) UC: 66.71.6:66.11 OI:1.98/APT73875M BIBLI: 145-7188 (7) 38, 75-84 Orgnal scntfc papr APPLICABILITY OF LINEARIZE USTY GAS MOEL FOR MULTICOMPONENT IFFUSION OF GAS MIXTURES IN POROUS

More information

Strain gradient plasticity: theory versus experiment. Microbending tests

Strain gradient plasticity: theory versus experiment. Microbending tests MOTIATION FOR STRAIN GRADIENT ASTICITY: Th Sz Effct n Wr Torson (Flck, Mullr, Ashby & Hutch, 994) Stran gradnt lastcty: thory vrsus xrmnt Norman A Flck Cambrdg Unvrsty Engnrng Dt. Polycrystalln Cor wrs

More information

Variational Approach in FEM Part II

Variational Approach in FEM Part II COIUUM & FIIE ELEME MEHOD aratonal Approach n FEM Part II Prof. Song Jn Par Mchancal Engnrng, POSECH Fnt Elmnt Mthod vs. Ralgh-Rtz Mthod On wants to obtan an appromat solton to mnmz a fnctonal. On of th

More information

An Overview of Markov Random Field and Application to Texture Segmentation

An Overview of Markov Random Field and Application to Texture Segmentation An Ovrvw o Markov Random Fld and Applcaton to Txtur Sgmntaton Song-Wook Joo Octobr 003. What s MRF? MRF s an xtnson o Markov Procss MP (D squnc o r.v. s unlatral (causal: p(x t x,

More information

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics Thermodynamics & Statistical Mechanics JEST-2012

fiziks Institute for NET/JRF, GATE, IIT JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics Thermodynamics & Statistical Mechanics JEST-2012 Q. monatomc dal gas at hrmodynamcs & Statstcal Mchancs JS- volum. h tmpratur aftr comprsson s ns. : (d) Soluton:. C (b) P costant, P R 7 C s adabatcally comprssd to /8 of ts orgnal 7 C (c).5 C (d) costant

More information

Damage Indices using Energy Criterion for Seismic Evaluation of Steel Frame Buildings

Damage Indices using Energy Criterion for Seismic Evaluation of Steel Frame Buildings amag Indcs usng Enrgy Crtron for Ssmc Evaluaton of Stl Fram Buldngs Prasad Prahlad Assstant Profssor, partmnt of Cvl Engnrng, N.I.T. Jamshdpur, Jharkhand, Inda Shrkhand Mansh & Agarwal Pankaj Assocat Profssor

More information

Fakultät III Wirtschaftswissenschaften Univ.-Prof. Dr. Jan Franke-Viebach

Fakultät III Wirtschaftswissenschaften Univ.-Prof. Dr. Jan Franke-Viebach Unvrstät Sgn Fakultät III Wrtschaftswssnschaftn Unv.-rof. Dr. Jan Frank-Vbach Exam Intrnatonal Fnancal Markts Summr Smstr 206 (2 nd Exam rod) Avalabl tm: 45 mnuts Soluton For your attnton:. las do not

More information

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added

Relate p and T at equilibrium between two phases. An open system where a new phase may form or a new component can be added 4.3, 4.4 Phas Equlbrum Dtrmn th slops of th f lns Rlat p and at qulbrum btwn two phass ts consdr th Gbbs functon dg η + V Appls to a homognous systm An opn systm whr a nw phas may form or a nw componnt

More information

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University

Static/Dynamic Deformation with Finite Element Method. Graphics & Media Lab Seoul National University Statc/Dynamc Dormaton wth Fnt Elmnt Mthod Graphcs & Mda Lab Sol Natonal Unvrsty Statc/Dynamc Dormaton Statc dormaton Dynamc dormaton ndormd shap ntrnal + = nrta = trnal dormd shap statc qlbrm dynamc qlbrm

More information

Outlier-tolerant parameter estimation

Outlier-tolerant parameter estimation Outlr-tolrant paramtr stmaton Baysan thods n physcs statstcs machn larnng and sgnal procssng (SS 003 Frdrch Fraundorfr fraunfr@cg.tu-graz.ac.at Computr Graphcs and Vson Graz Unvrsty of Tchnology Outln

More information