Composite model 131: Ply types 1 and 7 calibration

Size: px
Start display at page:

Download "Composite model 131: Ply types 1 and 7 calibration"

Transcription

1 Composte model 3: Ply types and 7 calbraton Model calbraton Composte Global Ply model 3 for elastc, damage and falre PAM-CRASH materal model 3 s for mlt-layered composte shell elements. Wthn ths model dfferent ply types can be sed for dfferent fbre renforcements and damage laws. Ths docment covers the ESI composte Global Ply damage law for:. Ply type for n-drectonal compostes (shell elements only).. Ply type 7 for woven type compostes (shell elements only). The Global Ply law s not avalable for sold elements. Problem descrpton Otlne Analyss type(s): Applcaton of the Global Ply composte damage model to a sngle element nder varos loadngs Explct Element type(s): Applcable to shell elements (materal model 3) Materals law(s): PAM-CRASH materal model 3 (composte ply types and 7). Fbre and matrx are calbrated for: ) Orthotropc elastcty ) Orthotropc fbre and matrx damage wth falre Model optons: Key reslts: Prepared by: Date: Bondary condtons, Imposed velocty loads, Composte materals Otpts for compostes (fbre stresses and strans, matrx damage, fbre orentatons ) Anthony Pckett, ESI GmbH/Insttte for Arcra Desgn, Stttgart September

2 Composte model 3: Ply types and 7 calbraton Backgrond nformaton Pre-processor, Solver and Post-processor sed: Vsal-Crash PAM: To assgn materal, loadng, constrant and control data. Analyss (PAM-CRASH Explct): To perform the explct Fnte Element analyss. Vsal-Vewer: To evalate reslts for contor plots, stresses and strans, etc. Pror knowledge for the exercse It s assmed the ser has some knowledge of Vsal-Crash PAM and PAM-CRASH. Problem data and descrpton Unts: kn, mm, kg, ms Descrpton: Sngle shell element mm * mm and mm thck Loadng: Imposed constant velocty at mm/msec (draton of stdy msec) total dsplacement mm and stran. (= %) Loadng cases: 4 3 y x Case : Axal fbre Case : Transverse matrx Case 3: Shear loadng Materal: The materal to be analysed s a hgh performance balanced woven fabrc composte. The data s presented from mechancal testng n the exercse. Sppled datasets All completed datasets are sppled. The man am s to demonstrate the strategy for model calbraton whch s done here sng the shell element (materal model 3, ply type ). Calbraton for orthotropc elastc propertes: Fbre drecton n tenson Fbre drecton n compresson Shear loadng Calbraton for damage, plastcty and falre: Fbre drecton n tenson (fbre falre) Fbre drecton n compresson (fbre falre) Shear loadng (elasto-plastc shear) Shear loadng (elasto-plastc shear) Shear loadng (elasto-plastc shear) Cyclc loadng (elasto-plastc shear) Ply_TensonX_Elastc.pc Ply_CompressonX_Elastc.pc Ply_ShearXY_Elastc.pc Ply_TensonX_ElastcFbreFalre.pc Ply_CompressonX_ElastcFbreFalre.pc Ply_ShearXY_ElastcDamageFalre_Opton_Plastc.pc Ply_ShearXY_ElastcDamageFalre_Opton_Plastc.pc Ply_ShearXY_ElastcDamageFalre_Opton3_Plastc.pc Ply_ShearXY_ElastcDamageFalre_Opton3_Plastc_Cyclc.pc

3 Composte model 3: Ply types and 7 calbraton Comments concernng ply types and 7 Two ply types are avalable that se the Global ply damage law for UD and woven type compostes: Ply type s ntended for UD compostes, bt can also be sed to approxmate a woven fabrc by stackng two UD layers wth approprate fbre angles and dstrbton of mechancal propertes. Indeed, t can be advantageos for non-orthogonal renforcement (e.g. ±3 ) and cases where large ntra-ply shear strans occr. Ply type 7 s for woven fabrcs and mostly sted to orthogonal renforcement and applcatons where shear strans are small. The followng table smmarses these three cases. Opton / Ply type Representaton Comments (Ply type ) t Standard representaton for UD composte ples The woven composte s dealsed as two (Two layers of Ply type ) t E WOVEN t/ t/ E -UD E -UD stacked pled of ply type In plane and shear propertes mst be careflly dstrbted between ples Usefl for non-orthogonal renforcement and large shear loadng 3 (Ply type 7) t E WOVEN Standard representaton for woven composte ples: Ideally for orthogonal renforcement Intra-ply shear strans shold not be large Ths docment demonstrates the calbraton strategy for opton n the above table appled to a balanced woven fabrc composte. Actal tests reslts are sed n ths calbraton. The methods sed are dentcal f standard ply types or 7 are sed. Basc theory A fll descrpton of the Global ply model s gven n the orgnal reference and also n the ESI PAM- CRASH TM ser s manal. Essentally the fbre phase ses a stran based falre crtera for tenson and compresson; non-lnear (elastc) behavor s possble n compresson and s oen necessary to accont for mcro-bcklng effects n compresson. The shear behavor ses a copled damage and plastcty model that acconts for modls redcton and permanent plastc deformatons. The fbre and matrx laws are decopled, bt parameters are avalable that allow coplng of transverse and shear matrx damage. Ladevèze P, Le Dantec E, Damage Modellng of the elementary ply for lamnated compostes, Compostes Scence and Technology, Vol. 43, Isse 3, 99, pp PAM-CRASH Users manals, Engneerng Systems Internatonal, Re Saarnen, Slc 7, Rngs- Cedex, France. 3

4 Composte model 3: Ply types and 7 calbraton Part : Some basc explanaton of the npt data Typcal model loadngs and spports (e.g. for dataset Ply_TensonX_Elastc.pc) Load the dataset nto the Vsal-Crash Program (VCP) and stdy the spports and the loadng:. In Loads > Dsplacement Bondary Condton the followng defntons are fond: Node s flly constraned. Node s flly fxed, except free n the x-drecton. Node 4 s flly fxed, except free n the y-drecton.. In Loads > 3D BC nodes and 3 are loaded at constant velocty n the postve x-drecton (for tenson fbre loadng). 4 y x 3 Remark: Ths smple setp ensres the element s properly spported and has pre tenson loadng n the x-drecton wth free contracton n the y-drecton. Ply, Materal and Part data cards Note from the dataset:. The parts data contan nformaton on geometrc data sch as the reference fber orentaton. A lnk to assocated materal data (varable IMAT) s also made.. The materals cards (IMAT) contan nformaton on densty, the nmber of ples n the lamnate and the stackng seqence. Wthn ths stackng seqence nformaton on each ply, ncldng the reference ply set (parameter IDPLY), the ply thckness and a fbre orentaton angle are defned. 3. The ply cards (IDPLY) contan all ply mechancal data for stffness, damage and falre. Consderng the seqence n whch the data refers to each other ( 3) t s best to defne thngs n reverse order;.e. the ples frst, then materals and fnally parts; all three are needed. 4

5 Composte model 3: Ply types and 7 calbraton Ply cards (e.g. Ply propertes for dataset Ply_TensonX_Elastc.pc). In the ply cards yo wll fnd the mechancal, damage and falre data assgned to the ply. o IDPLY s the ply dentfcaton nmber and ITYP s the ply type ( or 7). o The mechancal data (densty, modls, shear and Poson s rato) are gven on the frst cards. Ths s then followed by falre, compresson, plastcty and stran rate data. o Note: Contrary to the PAM-CRASH B-phase model all mechancal data represents homogensed propertes. Materal cards (e.g. Materal propertes for dataset Ply_TensonX_Elastc.pc).. The nmber of ples n the lamnate are defned (NOPLY) and for each ply the assocated ply nmber (IDPLY), the ply thckness (THKPL) and fbre angle (ANGPL) are defned. Note the fbre angle s wth respect to a reference vector defned n the Parts cards (see below) and that two stacked ples are defned.. Specal otpt reslts to the.thp and.dsy fles (or.enf fle f sed) are possble sch as fber, transverse and shear stresses/strans. For ths the ply nmber n the lamnate lay-p and an axlary reference nmber for the varable to be otpt are gven. Examples of axlary reference nmbers are Ax s -3 for fbre stran, stran and shear stran, and Ax s 6-8 for correspondng fber stresses. Axlary reference nmbers are also avalable for reslts sch as fbre and matrx damage. Part cards (e.g. Part propertes for dataset Ply_TensonX_Elastc.pc).. The connecton to the assocated materal s made va the IDMAT nmber (n ths case = ).. A vector for the reference fbre drecton s defned. Here the global vector opton wth a reference vector,, (.e. the global x-drecton) s sed. For shell elements the transverse drecton s normal to the fber drecton n the element plane. 5

6 Composte model 3: Ply types and 7 calbraton Part : Determnaton of orthotropc elastc and falre propertes from test measrements In ths exercse test reslts are frst presented from whch the necessary materal propertes for stffness and falre are extracted. The model and npt data are then valdated sng a sngle element test case. For the woven fabrc composte the tests needed to extract data are:. Tenson test on specmens elastc and falre propertes. Compresson test on specmens elastc and falre propertes 3a. Shear elastc propertes (Tenson test on a ±45 specmen) 3b. Shear damage propertes (Cyclc tenson test on a ±45 specmen) 3c. Shear plastcty propertes (Cyclc tenson test on a ±45 specmen). Tenson test on specmens: Elastc and falre propertes For test copons loaded n the drecton (=9 drecton for a balanced woven fabrc composte) are shown. For a smple copon: L = and L L = T by defnton = E E t L t L = L (Mpa) sample 9 sample3 8 sample5 7 sample ,,4,6,8,,,4 There s some scatter n the test data; bt reasonable averages for stffness and falre data are smmarsed n the table below. Property Vale t E Tensle elastc modls (fbre drecton) 67.5 GPa Tensle falre stress (fbre drecton) 88 MPa Tensle falre stran (fbre drecton) - ntaton.3 Tensle falre stran (fbre drecton) - ltmate.3 d Assmed ltmate damage (fbre drecton). 6

7 Composte model 3: Ply types and 7 calbraton. Compresson test on specmens: Elastc and falre propertes C E In ths case s gven by the ntal slope of the compresson stress-stran crve (dashed lne); e.g. C E 4 /.575 GPa = 69. GPa. (Mpa) smlaton All other falre data s estmated and gven n the table below. Property Vale t E Compresson elastc modls (fbre drecton) 69. GPa Compresson falre stress (fbre drecton) 65 MPa Compresson falre stran (fbre drecton) - ntaton.4 Compresson falre stran (fbre drecton) - ltmate.5 d Ultmate compresson damage (fbre drecton). A frther sefl parameter n compresson s the correctve parameter (γ) to help approxmate the nonlnear compresson crve (de to fbre crmp and mcro-bcklng). Ths s gven by,. Performng ths comptaton abot an arbtrary pont ( e.g. stran =.8) gves γ =.7 3a. Shear elastc propertes (Tenson test on a ±45 specmen) For the elastc shear data the ntal (ndamaged) porton of the tensle loaded cyclc shear test s sed; an example for the woven fabrc s gven below. The stress-stran relatons n the fbre frame are defned as follow: = and L / = L T G o s gven by the ntal slope of the shear stress ( ) verss the engneerng shear stran ( ). 7

8 Composte model 3: Ply types and 7 calbraton (GPa) (GPa) G,,4,6,8.75. The ntal shear modls s defned as the ntal slope of the test crve (rememberng that engneerng shear stran mst be sed (γ = ), G o = / = 6 / (*.75) = 4. GPa. 3b. Shear damage propertes (cyclc tenson test on a ±45 specmen) The prevos cyclc shear test for tensle loadng of a ±45 copon s sed to extract damage evolton, plastcty and fnal shear falre data. Shear damage s gven by the change n slope of the cyclc modls G and plastcty by the growth n p and each loadng cycle. G O G Fve loadng cycles have been performed on the copon as shown n the next crve. Note that ths fgre shows test reslts wth, and wthot, takng accont of changes n cross sectonal area n the comptaton of. If these changes can be measred drng testng and nclded then the model calbraton wll be more accrate. The crve wth secton varaton s sed here. 8

9 Composte model 3: Ply types and 7 calbraton 6 4 sample3 sample3 wth cross secton varaton (GPa) 8 6 4,,4,6,8,,,4,6 At each cycle the stffness loss s charactersed by the shear modls redcton. The degree of shear damage d s gven by the relatonshp: d G = G Shear modls and damage vales for every cycle are smmarsed n the table below; agan sng engneerng shear stran (γ = ) to calclate the G vales, cycle Shear modls G d Ths model ses the term Y to defne how damage s progressng (t s the change of stored elastc energy wth damage). The stored energy for a ply s, E D e = : ν = E E + + E ( d + G ( d Consderng only stored energy for shear () the conjgate qantty Y s + ) E ) Y δ E = δ d D = G ( d ) From e = Y G o = G ( ) ( d ) A smlar expresson to Y cold be developed for UD ples where damage wll occr n the nrenforced transverse drecton; however ths s not needed here for the woven fabrc. The conjgate force qantty at each cycle () s therefore gven by, 9

10 Composte model 3: Ply types and 7 calbraton Y e = G ( ). From the cyclc test crve and the above expresson, e cycle Y.E E E E E E-.873 It s now possble to plot the evolton of Y wth damage d. cycle Y d The damage s ntally lnear (for small strans and then ncreases rapdly close to falre), as shown n the adjacent plot. Several optons are avalable n PAM-CRASH to characterse damage evolton; for example, an exponental fncton, a crve fncton and the followng (orgnal) lnear damage fncton, Y = YC d + Y, where Yo s the ntal constant and Yc s the slope of the lnear fncton. A frther parameter YR s sed to specfy falre (Yo, Yc and YR are data npt vales for PAM-CRASH shear damage evolton and falre). Two examples to try and the lnear fncton to the test crve are shown n the graph wth data n the table below; clearly ths s not accrate. For ths dctle matrx the exponental or crve fncton methods wold be better. Y (Gpa^.5) Y verss d 6 ponts approx 4 ponts approx y =.464x +.4 y =.4x d Y O Y C Y R Ln. Fncton Ln. Fncton Crve fncton Usng the data ponts n the table above.88

11 Composte model 3: Ply types and 7 calbraton 3c. Shear plastcty propertes (Cyclc tenson test on a ±45 specmen) The nelastc deformaton s descrbed by a plastcty law whch coples transverse () and shear () strans only. The plastc stran p j s the measre of effectve plastc stran and the term R s sed to determne how the vale of d affects the yeld stress n each cycle. In ths model the terms effectve stress and effectve stran are ntrodced as measres of actal materal stress and stran carred by the damaged materal. The damage (mcro-crackng) redces the effectve area of the load carryng materal casng effectve materal stress to be rased and effectve materal stran to be lowered. Note ths termnology s not the same as Von Mses effectve stress and stran whch s commonly sed n plastcty n the lteratre. The term p j and R are calclated n the followng eqatons: p R = P j p p = p ( d ) = j = p = d R R, j nmber of cyclc loads = β ( P ) j m (Eq.) where P s the plastc stran at each cycle, as shown on fgre below. The followng table gves the plastc stran measred from the cyclc shear test crve and the damage term whch are sed to calclate p. Accordng to Eqatons a plot of -d verss P allows the (p ) vales to be fond by ntegraton for each cycle. The vales for (P j ) are then compted from smmaton of these vales. The followng crve and table smmarse reslts of ths ntegraton and the smmaton. (GPa) sample3 sample3 wth cross secton varaton,,4,6,8,,,4,6 cycle p - d 7.4E E E E E-.5838

12 Composte model 3: Ply types and 7 calbraton, p,8 -d,6,4 p 3 p 4 p 5,,5,,5, plast Cycle p P j R (MPa) Fnally, a crve tng exercse s performed to the PAM-CRASH exponental plastcty fncton (wth parameters β and m) to the R verss P crve. Ths has prodced the followng reslts wth the ntal plastcty yeld stress Ro = MPa.,3,5, R (MPa),5,,5 R =.566 ( P j ).7986Pj expermental gor power law,,4,6,8,, P j P

13 Composte model 3: Ply types and 7 calbraton Part 3: Smmary of the Global Ply dataset for elastc, damage, plastcty and falre For the prpose of ths calbraton a total ply thckness of.mm s assmed meanng that each ply n the stacked approxmaton s.5mm (Make sre the tre vale s sed n any real composte). In order to compensate for the halved ply thckness n ths dealsed model: Doble the modls for tenson and compresson modls. Use nchanged shear modls (and shear damage/plastcty) for each ply. Use a low modls (say GPa) for the transverse drecton (to mnmse nteracton effects). Note: Any modfcatons to ply modl wll correspondngly modfy the stress levels; however, damage and falre s always controlled by stran and therefore the approach (to treat a woven compostes as two stacked UD ples) s vald. The followng table smmarses the data so far for each ply (thckness =.5mm) n the dealsed woven compostes. Inplane Tenson Inplane Compresson t E c = (*67.5)=35 GPa E = t E =. GPa = fc ν =.33 = fc =.3 = (*69,)=38 GPa γ fc =.3 = d =. d. Table : Inplane stffness/falre data For the shear the followng data/optons were determned (to be sed for each ply): Stffness G O = 4. GPa Damage Yo Yc YR Ln. Fncton Ln. Fncton Crve fncton Usng the Y-d data ponts.89 Plastcty R =.566 ( P j ).7986Pj R = MPa, β =.7986, m =.566 Table : Shear stffness, damage and plastcty data 3

14 Composte model 3: Ply types and 7 calbraton Part 4: Checkng the npt wth smlaton reslts Smlaton reslts Fbre tenson (elastc wthot and wth falre) Usng dataset: Ply_TensonX_ElastcFbre.pc (for no falre) Ply_TensonX_ElastcFbreFalre.pc (for fbre falre) Postve x-velocty s appled to nodes,3 (.mm/sec) (= Case, Pg ).. Fbre tenson (for the falre case) The shell element tme hstory plot Comp. Ax4 (fbre stress) aganst Ax (fbre stran) s plotted for the fbre drecton ply. For a stran of. the correspondng fbre drecton stress s.35gpa; note:. Ths stress s ( correctly) doble that of the test vale (7N/mm at. stran) snce the eqvalent ply thckness s half of the tre woven ply. The dfference s de to the small contrbton from the transverse drecton n the second ply; calbraton cold be done to correct ths.. The falre data =.3, =.3 and d = 4 3 y x. s mposed. In ths case tensle fbre falre s ntated at the reqred.3% stran and fll damage occrs (d=.). 3. If a resdal damage s reqred se d<.. E.g. for d=.3 only 3% of damage occrs (Edamage =.7 * Eo) and the stress wll reman constant aer ths damage state s reached. Reslts: fbre compresson Usng dataset: Ply_CompressonX_ElastcFbre.pc (for no falre) Ply_CompressonX_ElastcFbreFalre.pc (for fbre falre) Negatve x-velocty (=-.mm/sec) s appled to nodes,3.. Fbre compresson (for the falre case) The nonlnear form of the compresson fbre stress (Ax 4) verss fbre stran (Ax ) s evdent de to the factor γ =.7. Stress n the fbre ply (x-drecton) s approxmately twce the test vale de to the prevosly mentoned reason; for example, at fbre stran.9, the smlaton stress s.kn compared to test.54kn. fc fc The falre data =., =. fc and d =. s mposed. Falre s ntated and completed, as expected, wth total damage de to d=.. 4

15 Composte model 3: Ply types and 7 calbraton Transverse drecton (= Case, Pg ) Snce ths composte has a balanced fabrc the second ply transverse drecton wll have the same propertes as the fbre drecton calbrated above. Ths s assred n the dataset sng layers for the model wth dentcal propertes for layer (n the ) and layer (n the 9 ). Shear (for the elastc case sng dataset - Ply_ShearXY_Elastc.pc) The sngle element test case s loaded n the postve x and negatve y drectons to mpose pre shear loadng (= Case 3, Pg ). The fbre drectons are set to ±45 wth respect to the x-drecton. A tme hstory plot of shear stress (Ax6) aganst shear stran (Ax3) s shown. At.75 shear stran the shear stress s 6MPa; whch corresponds to the vale of the ntal slope of the expermental shear stress verss shear stran crve. Shear (for the damage wth falre pls plastcty) Shear damage can be treated sng the lnear damage fncton, an exponental fncton or the crve fncton; ltmate shear falre s specfed by the vale of YR. The prevos table for shear damage evolton and falre s repeated below wth the three optons (,, 3) evalated here to compte shear damage. In each case the prevosly determned plastcty data s sed. Shear damage data Plastcty data Opton Damage fncton Yo Yc YR Ro β m Ln. Fncton MPa Ln. Fncton Crve fncton sng the data ponts n the Y-D table The three sppled datasets for the above cases are:. Ply_ShearXY_ElastcDamageFalre_Opton_Plastc.pc. Ply_ShearXY_ElastcDamageFalre_Opton_Plastc.pc 3. Ply_ShearXY_ElastcDamageFalre_Opton3_Plastc.pc Usng the lnear shear fncton (optons and ): For some sem-brttle materals the lnear may be satsfactory; bt n ths case the s poor, especally to descrbe the rapd damage growth at large shear strans. The followng crves llstrate the poor of the lnear fncton to the test (damage) crve and the correspondngly poor correlaton of the sngle element analyss to the test shear stressstran crve. 5

16 Composte model 3: Ply types and 7 calbraton Y (Gpa^.5) Y verss d 6 ponts approx 4 ponts approx y =.464x +.4 y =.4x d (GPa),4,,,8,6,4 expermental 4 ponts lnear law, 6 ponts lnear law,,4,6,8,,,4,6 Usng the crve shear fncton (opton 3) In PAM-CRASH (verson V8+) exponental and crve descrptons for shear and transverse damage evolton are avalable. In the Opton 3 dataset the Lnear parameters for Yo, Yo are removed and the varable ISH s set to. A crve descrpton of Y aganst d s sed wth the prevosly determned data (note the, start pont) n an axlary crve; set ths crve nmber to the parameter ICURV n the ply data. The ltmate shear stran parameter YR s set to.89. From the reslts a plot of shear stress (Ax 6) aganst shear stran (Ax 3) shows a good agreement wth the test crve for both shape and falre; althogh some mprovements sng more data ponts cold help to smooth the shape, especally at shear stran.4. Cyclc shear loadng Usng shear damage (opton 3) and the dataset Ply_ShearXY_ElastcDamageFalre_Opton3 _Plastc_Cyclc.pc The adjacent plot shows cyclc (velocty) loadng of the sngle element test case. The change n slope of the nloadng crve represents damaged shear modls. Also, the nelastc (permanent) plastc strans are evdent. 6

17 Composte model 3: Ply types and 7 calbraton Part 5: Alternatve optons for damage and falre Damage crve fnctons Dfferent methods can be sed to defne the form of the damage fnctons; namely, Lnear, Exponental or Crve. For most compostes an exponental or Crve fncton wll be needed to reasonably descrbe the damage fncton evolton. Spermposed falre crtera For fbre and matrx damage the Global ply model has so far been sed. However, t s also possble to spermpose a classcal falre crtera sch as Tsa-W, Max. stress, etc. Set IFAIL_INP= and choose the falre crtera wth flag FAILTYP. Dependng on the selected falre crtera addtonal falre nformaton s reqred. If the state of stress or stran reaches the falre crtera the element wll be elmnated (for FAILDAM = ). In the materals cards the IFAIL opton mst also be set. Part 6: Specfc nformaton for woven renforcement (Mat 3 ply type 7) The data shown s typcal nformaton for ply type 7. Some ponts to note are:. The strctre and general nformaton reqred s smlar to ply type.. The two man fbre drectons are assmed to be orthogonal. 3. Tenson and compresson nformaton s provded for the man fbre drecton (E, Ec) and the second fbre drecton (E, Ec). 4. For tenson fbre falre drvng force vales YIIC, Y and YR are sed, for compresson YIIcC, Yc and YcR are sed. Note that crrently ths nformaton s appled to both renforcement drectons, so strctly the fabrc shold be balanced (.e. E = E and Ec = Ec). 5. Stran rate can be appled. 7

MEMBRANE ELEMENT WITH NORMAL ROTATIONS

MEMBRANE ELEMENT WITH NORMAL ROTATIONS 9. MEMBRANE ELEMENT WITH NORMAL ROTATIONS Rotatons Mst Be Compatble Between Beam, Membrane and Shell Elements 9. INTRODUCTION { XE "Membrane Element" }The comple natre of most bldngs and other cvl engneerng

More information

AE/ME 339. K. M. Isaac. 8/31/2004 topic4: Implicit method, Stability, ADI method. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept.

AE/ME 339. K. M. Isaac. 8/31/2004 topic4: Implicit method, Stability, ADI method. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept. AE/ME 339 Comptatonal Fld Dynamcs (CFD) Comptatonal Fld Dynamcs (AE/ME 339) Implct form of dfference eqaton In the prevos explct method, the solton at tme level n,,n, depended only on the known vales of,

More information

OFF-AXIS MECHANICAL PROPERTIES OF FRP COMPOSITES

OFF-AXIS MECHANICAL PROPERTIES OF FRP COMPOSITES ICAMS 204 5 th Internatonal Conference on Advanced Materals and Systems OFF-AXIS MECHANICAL PROPERTIES OF FRP COMPOSITES VLAD LUPĂŞTEANU, NICOLAE ŢĂRANU, RALUCA HOHAN, PAUL CIOBANU Gh. Asach Techncal Unversty

More information

Composite models 30 and 131: Ply types 0 and 8 calibration

Composite models 30 and 131: Ply types 0 and 8 calibration Model calibration Composite Bi-Phase models 30 and 3 for elastic, damage and failure PAM-CRASH material model 30 is for solid and 3 for multi-layered shell elements. Within these models different ply types

More information

Research Note NONLINEAR ANALYSIS OF SEMI-RIGID FRAMES WITH RIGID END SECTIONS * S. SEREN AKAVCI **

Research Note NONLINEAR ANALYSIS OF SEMI-RIGID FRAMES WITH RIGID END SECTIONS * S. SEREN AKAVCI ** Iranan Jornal of Scence & Technology, Transacton, Engneerng, Vol., No., pp 7-7 rnted n The Islamc Repblc of Iran, 7 Shraz Unversty Research Note NONLINER NLYSIS OF SEMI-RIGID FRMES WIT RIGID END SECTIONS

More information

BAR & TRUSS FINITE ELEMENT. Direct Stiffness Method

BAR & TRUSS FINITE ELEMENT. Direct Stiffness Method BAR & TRUSS FINITE ELEMENT Drect Stness Method FINITE ELEMENT ANALYSIS AND APPLICATIONS INTRODUCTION TO FINITE ELEMENT METHOD What s the nte element method (FEM)? A technqe or obtanng approxmate soltons

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,

More information

STRATEGIES FOR BUILDING AN AC-DC TRANSFER SCALE

STRATEGIES FOR BUILDING AN AC-DC TRANSFER SCALE Smposo de Metrología al 7 de Octbre de 00 STRATEGIES FOR BUILDING AN AC-DC TRANSFER SCALE Héctor Laz, Fernando Kornblt, Lcas D Lllo Insttto Naconal de Tecnología Indstral (INTI) Avda. Gral Paz, 0 San Martín,

More information

CHAPTER 9 CONCLUSIONS

CHAPTER 9 CONCLUSIONS 78 CHAPTER 9 CONCLUSIONS uctlty and structural ntegrty are essentally requred for structures subjected to suddenly appled dynamc loads such as shock loads. Renforced Concrete (RC), the most wdely used

More information

SE Story Shear Frame. Final Project. 2 Story Bending Beam. m 2. u 2. m 1. u 1. m 3. u 3 L 3. Given: L 1 L 2. EI ω 1 ω 2 Solve for m 2.

SE Story Shear Frame. Final Project. 2 Story Bending Beam. m 2. u 2. m 1. u 1. m 3. u 3 L 3. Given: L 1 L 2. EI ω 1 ω 2 Solve for m 2. SE 8 Fnal Project Story Sear Frame Gven: EI ω ω Solve for Story Bendng Beam Gven: EI ω ω 3 Story Sear Frame Gven: L 3 EI ω ω ω 3 3 m 3 L 3 Solve for Solve for m 3 3 4 3 Story Bendng Beam Part : Determnng

More information

A Modified Neuber Method Avoiding Artefacts Under Random Loads

A Modified Neuber Method Avoiding Artefacts Under Random Loads A Modfed Neuber Method Avodng Artefacts Under Random Loads T. Herbland a,b, G. Calletaud a, J. L. Chaboche c, S. Qulc a, F. Gallerneau c a Mnes Pars Pars Tech, CNRS UMR 7633, P 87, 91003 vry cedex, France

More information

Numerical Modeling of Woven Carbon Composite Failure

Numerical Modeling of Woven Carbon Composite Failure 8 th Internatonal LS-DYNA Users Conference Smulaton Technology (3) Numercal Modelng of Woven Carbon Composte Falure Paul F. Deslaurers, Duane S. Cronn Unversty of Waterloo Alex Duquette Multmatc Techncal

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

COMBINED HIGH AND LOW CYCLE FATIGUE MODEL FOR PREDICTION OF STEEL BRIDGE LIVES

COMBINED HIGH AND LOW CYCLE FATIGUE MODEL FOR PREDICTION OF STEEL BRIDGE LIVES 505 COMBINED HIGH AND LOW CYCLE FATIGUE MODEL FOR PREDICTION OF STEEL BRIDGE LIVES M. OHGA *, K. KARUNANANDA, P.B.R. DISSANAYAKE 2 and S.A.S.C. SIRIWARDANE 3 Department of Cvl and Envronmental Engneerng,

More information

Indeterminate pin-jointed frames (trusses)

Indeterminate pin-jointed frames (trusses) Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all

More information

Lifetime prediction of EP and NBR rubber seal by thermos-viscoelastic model

Lifetime prediction of EP and NBR rubber seal by thermos-viscoelastic model ECCMR, Prague, Czech Republc; September 3 th, 2015 Lfetme predcton of EP and NBR rubber seal by thermos-vscoelastc model Kotaro KOBAYASHI, Takahro ISOZAKI, Akhro MATSUDA Unversty of Tsukuba, Japan Yoshnobu

More information

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST Appled Computer Scence, vol. 13, no. 4, pp. 56 64 do: 10.23743/acs-2017-29 Submtted: 2017-10-30 Revsed: 2017-11-15 Accepted: 2017-12-06 Abaqus Fnte Elements, Plane Stress, Orthotropc Materal Bartosz KAWECKI

More information

Introduction to elastic wave equation. Salam Alnabulsi University of Calgary Department of Mathematics and Statistics October 15,2012

Introduction to elastic wave equation. Salam Alnabulsi University of Calgary Department of Mathematics and Statistics October 15,2012 Introdcton to elastc wave eqaton Salam Alnabls Unversty of Calgary Department of Mathematcs and Statstcs October 15,01 Otlne Motvaton Elastc wave eqaton Eqaton of moton, Defntons and The lnear Stress-

More information

Chapter 13: Multiple Regression

Chapter 13: Multiple Regression Chapter 13: Multple Regresson 13.1 Developng the multple-regresson Model The general model can be descrbed as: It smplfes for two ndependent varables: The sample ft parameter b 0, b 1, and b are used to

More information

Finite Element Modelling of truss/cable structures

Finite Element Modelling of truss/cable structures Pet Schreurs Endhoven Unversty of echnology Department of Mechancal Engneerng Materals echnology November 3, 214 Fnte Element Modellng of truss/cable structures 1 Fnte Element Analyss of prestressed structures

More information

EMISSION MEASUREMENTS IN DUAL FUELED INTERNAL COMBUSTION ENGINE TESTS

EMISSION MEASUREMENTS IN DUAL FUELED INTERNAL COMBUSTION ENGINE TESTS XVIII IEKO WORLD NGRESS etrology for a Sstanable Development September, 17, 006, Ro de Janero, Brazl EISSION EASUREENTS IN DUAL FUELED INTERNAL BUSTION ENGINE TESTS A.F.Orlando 1, E.Santos, L.G.do Val

More information

Structure and Drive Paul A. Jensen Copyright July 20, 2003

Structure and Drive Paul A. Jensen Copyright July 20, 2003 Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.

More information

In this section is given an overview of the common elasticity models.

In this section is given an overview of the common elasticity models. Secton 4.1 4.1 Elastc Solds In ths secton s gven an overvew of the common elastcty models. 4.1.1 The Lnear Elastc Sold The classcal Lnear Elastc model, or Hooean model, has the followng lnear relatonshp

More information

DUE: WEDS FEB 21ST 2018

DUE: WEDS FEB 21ST 2018 HOMEWORK # 1: FINITE DIFFERENCES IN ONE DIMENSION DUE: WEDS FEB 21ST 2018 1. Theory Beam bendng s a classcal engneerng analyss. The tradtonal soluton technque makes smplfyng assumptons such as a constant

More information

Traceability and uncertainty for phase measurements

Traceability and uncertainty for phase measurements Traceablty and ncertanty for phase measrements Karel Dražl Czech Metrology Insttte Abstract In recent tme the problems connected wth evalatng and expressng ncertanty n complex S-parameter measrements have

More information

EVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES

EVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES EVALUATION OF THE VISCO-ELASTIC PROPERTIES IN ASPHALT RUBBER AND CONVENTIONAL MIXES Manuel J. C. Mnhoto Polytechnc Insttute of Bragança, Bragança, Portugal E-mal: mnhoto@pb.pt Paulo A. A. Perera and Jorge

More information

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE Prof. J. N. Mandal Department of cvl engneerng, IIT Bombay, Powa, Mumba 400076, Inda. Tel.022-25767328 emal: cejnm@cvl.tb.ac.n Module - 9 LECTURE - 48

More information

χ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body

χ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body Secton.. Moton.. The Materal Body and Moton hyscal materals n the real world are modeled usng an abstract mathematcal entty called a body. Ths body conssts of an nfnte number of materal partcles. Shown

More information

Second Order Analysis

Second Order Analysis Second Order Analyss In the prevous classes we looked at a method that determnes the load correspondng to a state of bfurcaton equlbrum of a perfect frame by egenvalye analyss The system was assumed to

More information

ESS 265 Spring Quarter 2005 Time Series Analysis: Error Analysis

ESS 265 Spring Quarter 2005 Time Series Analysis: Error Analysis ESS 65 Sprng Qarter 005 Tme Seres Analyss: Error Analyss Lectre 9 May 3, 005 Some omenclatre Systematc errors Reprodcbly errors that reslt from calbraton errors or bas on the part of the obserer. Sometmes

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Fourth Edton CHTER MECHNICS OF MTERIS Ferdnand. Beer E. Russell Johnston, Jr. John T. DeWolf ecture Notes: J. Walt Oler Texas Tech Unversty Stress and Stran xal oadng Contents Stress & Stran: xal oadng

More information

C PLANE ELASTICITY PROBLEM FORMULATIONS

C PLANE ELASTICITY PROBLEM FORMULATIONS C M.. Tamn, CSMLab, UTM Corse Content: A ITRODUCTIO AD OVERVIEW mercal method and Compter-Aded Engneerng; Phscal problems; Mathematcal models; Fnte element method. B REVIEW OF -D FORMULATIOS Elements and

More information

Physics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding.

Physics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding. Physcs 53 Rotatonal Moton 3 Sr, I have found you an argument, but I am not oblged to fnd you an understandng. Samuel Johnson Angular momentum Wth respect to rotatonal moton of a body, moment of nerta plays

More information

APPENDIX F A DISPLACEMENT-BASED BEAM ELEMENT WITH SHEAR DEFORMATIONS. Never use a Cubic Function Approximation for a Non-Prismatic Beam

APPENDIX F A DISPLACEMENT-BASED BEAM ELEMENT WITH SHEAR DEFORMATIONS. Never use a Cubic Function Approximation for a Non-Prismatic Beam APPENDIX F A DISPACEMENT-BASED BEAM EEMENT WITH SHEAR DEFORMATIONS Never use a Cubc Functon Approxmaton for a Non-Prsmatc Beam F. INTRODUCTION { XE "Shearng Deformatons" }In ths appendx a unque development

More information

Lecture 8 Modal Analysis

Lecture 8 Modal Analysis Lecture 8 Modal Analyss 16.0 Release Introducton to ANSYS Mechancal 1 2015 ANSYS, Inc. February 27, 2015 Chapter Overvew In ths chapter free vbraton as well as pre-stressed vbraton analyses n Mechancal

More information

Here is the rationale: If X and y have a strong positive relationship to one another, then ( x x) will tend to be positive when ( y y)

Here is the rationale: If X and y have a strong positive relationship to one another, then ( x x) will tend to be positive when ( y y) Secton 1.5 Correlaton In the prevous sectons, we looked at regresson and the value r was a measurement of how much of the varaton n y can be attrbuted to the lnear relatonshp between y and x. In ths secton,

More information

Chapter 11: Simple Linear Regression and Correlation

Chapter 11: Simple Linear Regression and Correlation Chapter 11: Smple Lnear Regresson and Correlaton 11-1 Emprcal Models 11-2 Smple Lnear Regresson 11-3 Propertes of the Least Squares Estmators 11-4 Hypothess Test n Smple Lnear Regresson 11-4.1 Use of t-tests

More information

Constitutive Modelling of Superplastic AA-5083

Constitutive Modelling of Superplastic AA-5083 TECHNISCHE MECHANIK, 3, -5, (01, 1-6 submtted: September 19, 011 Consttutve Modellng of Superplastc AA-5083 G. Gulano In ths study a fast procedure for determnng the constants of superplastc 5083 Al alloy

More information

Connection and Tension Member Design

Connection and Tension Member Design ACH 631 Note Set 17.1 F2015abn Connecton and Tenson Member Desgn Notaton: A = area (net = wth holes, bearng = n contact, etc...) A e = effectve net area fond from the prodct of the net area A n by the

More information

DESIGN OPTIMIZATION OF CFRP RECTANGULAR BOX SUBJECTED TO ARBITRARY LOADINGS

DESIGN OPTIMIZATION OF CFRP RECTANGULAR BOX SUBJECTED TO ARBITRARY LOADINGS Munch, Germany, 26-30 th June 2016 1 DESIGN OPTIMIZATION OF CFRP RECTANGULAR BOX SUBJECTED TO ARBITRARY LOADINGS Q.T. Guo 1*, Z.Y. L 1, T. Ohor 1 and J. Takahash 1 1 Department of Systems Innovaton, School

More information

Problem Set 1 Issued: Wednesday, February 11, 2015 Due: Monday, February 23, 2015

Problem Set 1 Issued: Wednesday, February 11, 2015 Due: Monday, February 23, 2015 MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING CAMBRIDGE MASSACHUSETTS 09.9 NUMERICAL FLUID MECHANICS SPRING 05 Problem Set Issed: Wednesday Febrary 05 De: Monday Febrary 05

More information

PHYS 705: Classical Mechanics. Calculus of Variations II

PHYS 705: Classical Mechanics. Calculus of Variations II 1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary

More information

Modeling Mood Variation and Covariation among Adolescent Smokers: Application of a Bivariate Location-Scale Mixed-Effects Model

Modeling Mood Variation and Covariation among Adolescent Smokers: Application of a Bivariate Location-Scale Mixed-Effects Model Modelng Mood Varaton and Covaraton among Adolescent Smokers: Applcaton of a Bvarate Locaton-Scale Mxed-Effects Model Oksana Pgach, PhD, Donald Hedeker, PhD, Robn Mermelsten, PhD Insttte for Health Research

More information

Solutions to selected problems from homework 1.

Solutions to selected problems from homework 1. Jan Hagemejer 1 Soltons to selected problems from homeork 1. Qeston 1 Let be a tlty fncton hch generates demand fncton xp, ) and ndrect tlty fncton vp, ). Let F : R R be a strctly ncreasng fncton. If the

More information

SEISMIC DRIFT PERFORMANCE-BASED DESIGN OPTIMIZATION OF REINFORCED CONCRETE BUILDINGS

SEISMIC DRIFT PERFORMANCE-BASED DESIGN OPTIMIZATION OF REINFORCED CONCRETE BUILDINGS 3 th World Conference on Earthqake Engneerng Vancover, B.C., Canada Agst -6, 2004 Paper No. 223 SEISMIC DRIFT PERFORMANCE-BASED DESIGN OPTIMIZATION OF REINFORCED CONCRETE BILDINGS Xao-Kang ZO and Chn-Man

More information

A comprehensive study: Boundary conditions for representative volume elements (RVE) of composites

A comprehensive study: Boundary conditions for representative volume elements (RVE) of composites Insttute of Structural Mechancs A comprehensve study: Boundary condtons for representatve volume elements (RVE) of compostes Srhar Kurukur A techncal report on homogenzaton technques A comprehensve study:

More information

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential

Open Systems: Chemical Potential and Partial Molar Quantities Chemical Potential Open Systems: Chemcal Potental and Partal Molar Quanttes Chemcal Potental For closed systems, we have derved the followng relatonshps: du = TdS pdv dh = TdS + Vdp da = SdT pdv dg = VdP SdT For open systems,

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

Fracture analysis of FRP composites using a meshless finite point collocation method

Fracture analysis of FRP composites using a meshless finite point collocation method Forth Internatonal Conference on FRP Compostes n Cvl Engneerng (CICE008) -4Jly 008, Zrch, Swtzerland Fractre analyss of FRP compostes sng a meshless fnte pont collocaton method M. Shahverd & S. Mohammad

More information

Chapter 9: Statistical Inference and the Relationship between Two Variables

Chapter 9: Statistical Inference and the Relationship between Two Variables Chapter 9: Statstcal Inference and the Relatonshp between Two Varables Key Words The Regresson Model The Sample Regresson Equaton The Pearson Correlaton Coeffcent Learnng Outcomes After studyng ths chapter,

More information

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp.

ORIGIN 1. PTC_CE_BSD_3.2_us_mp.mcdx. Mathcad Enabled Content 2011 Knovel Corp. Clck to Vew Mathcad Document 2011 Knovel Corp. Buldng Structural Desgn. homas P. Magner, P.E. 2011 Parametrc echnology Corp. Chapter 3: Renforced Concrete Slabs and Beams 3.2 Renforced Concrete Beams -

More information

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS

NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS IJRRAS 8 (3 September 011 www.arpapress.com/volumes/vol8issue3/ijrras_8_3_08.pdf NON-CENTRAL 7-POINT FORMULA IN THE METHOD OF LINES FOR PARABOLIC AND BURGERS' EQUATIONS H.O. Bakodah Dept. of Mathematc

More information

LAB 4: Modulus of elasticity

LAB 4: Modulus of elasticity LAB 4: Modulus of elastcty 1. Preparaton: modulus of elastcty (chapter15, p.79) Hook s law graphcal determnaton of modulus of elastcty (p.8) determnaton of modulus of elastcty n tenson and flexural stress

More information

Some modelling aspects for the Matlab implementation of MMA

Some modelling aspects for the Matlab implementation of MMA Some modellng aspects for the Matlab mplementaton of MMA Krster Svanberg krlle@math.kth.se Optmzaton and Systems Theory Department of Mathematcs KTH, SE 10044 Stockholm September 2004 1. Consdered optmzaton

More information

Statistics MINITAB - Lab 2

Statistics MINITAB - Lab 2 Statstcs 20080 MINITAB - Lab 2 1. Smple Lnear Regresson In smple lnear regresson we attempt to model a lnear relatonshp between two varables wth a straght lne and make statstcal nferences concernng that

More information

Fastener Modeling for Joining Composite Parts

Fastener Modeling for Joining Composite Parts AM-VPD09-006 Fastener Modelng for Jonng Composte Parts Alexander Rutman, Assocate Techncal Fellow, Sprt AeroSystems Chrs Boshers, Stress ngneer, Sprt AeroSystems John Parady, Prncpal Applcaton ngneer,

More information

Negative Binomial Regression

Negative Binomial Regression STATGRAPHICS Rev. 9/16/2013 Negatve Bnomal Regresson Summary... 1 Data Input... 3 Statstcal Model... 3 Analyss Summary... 4 Analyss Optons... 7 Plot of Ftted Model... 8 Observed Versus Predcted... 10 Predctons...

More information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1 P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal

More information

Torsion Stiffness of Thin-walled Steel Beams with Web Holes

Torsion Stiffness of Thin-walled Steel Beams with Web Holes Torson Stffness of Thn-walled Steel Beams wth Web Holes MARTN HORÁČEK, JNDŘCH MELCHER Department of Metal and Tmber Structures Brno Unversty of Technology, Faculty of Cvl Engneerng Veveří 331/95, 62 Brno

More information

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project

November 5, 2002 SE 180: Earthquake Engineering SE 180. Final Project SE 8 Fnal Project Story Shear Frame u m Gven: u m L L m L L EI ω ω Solve for m Story Bendng Beam u u m L m L Gven: m L L EI ω ω Solve for m 3 3 Story Shear Frame u 3 m 3 Gven: L 3 m m L L L 3 EI ω ω ω

More information

FUZZY FINITE ELEMENT METHOD

FUZZY FINITE ELEMENT METHOD FUZZY FINITE ELEMENT METHOD RELIABILITY TRUCTURE ANALYI UING PROBABILITY 3.. Maxmum Normal tress Internal force s the shear force, V has a magntude equal to the load P and bendng moment, M. Bendng moments

More information

The Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites

The Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites 7 Asa-Pacfc Engneerng Technology Conference (APETC 7) ISBN: 978--6595-443- The Two-scale Fnte Element Errors Analyss for One Class of Thermoelastc Problem n Perodc Compostes Xaoun Deng Mngxang Deng ABSTRACT

More information

Lecture Note 3. Eshelby s Inclusion II

Lecture Note 3. Eshelby s Inclusion II ME340B Elastcty of Mcroscopc Structures Stanford Unversty Wnter 004 Lecture Note 3. Eshelby s Incluson II Chrs Wenberger and We Ca c All rghts reserved January 6, 004 Contents 1 Incluson energy n an nfnte

More information

Correlation and Regression. Correlation 9.1. Correlation. Chapter 9

Correlation and Regression. Correlation 9.1. Correlation. Chapter 9 Chapter 9 Correlaton and Regresson 9. Correlaton Correlaton A correlaton s a relatonshp between two varables. The data can be represented b the ordered pars (, ) where s the ndependent (or eplanator) varable,

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

Chapter 5 Multilevel Models

Chapter 5 Multilevel Models Chapter 5 Multlevel Models 5.1 Cross-sectonal multlevel models 5.1.1 Two-level models 5.1.2 Multple level models 5.1.3 Multple level modelng n other felds 5.2 Longtudnal multlevel models 5.2.1 Two-level

More information

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4)

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4) I. Classcal Assumptons Econ7 Appled Econometrcs Topc 3: Classcal Model (Studenmund, Chapter 4) We have defned OLS and studed some algebrac propertes of OLS. In ths topc we wll study statstcal propertes

More information

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng

More information

Week 9 Chapter 10 Section 1-5

Week 9 Chapter 10 Section 1-5 Week 9 Chapter 10 Secton 1-5 Rotaton Rgd Object A rgd object s one that s nondeformable The relatve locatons of all partcles makng up the object reman constant All real objects are deformable to some extent,

More information

Code_Aster. Identification of the model of Weibull

Code_Aster. Identification of the model of Weibull Verson Ttre : Identfcaton du modèle de Webull Date : 2/09/2009 Page : /8 Responsable : PARROT Aurore Clé : R70209 Révson : Identfcaton of the model of Webull Summary One tackles here the problem of the

More information

Composite Hypotheses testing

Composite Hypotheses testing Composte ypotheses testng In many hypothess testng problems there are many possble dstrbutons that can occur under each of the hypotheses. The output of the source s a set of parameters (ponts n a parameter

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

SIMPLIFIED APPROACH TO THE NON-LINEAR BEHAVIOR OF RC MEMBERS

SIMPLIFIED APPROACH TO THE NON-LINEAR BEHAVIOR OF RC MEMBERS SIMPLIFIED APPROACH TO THE NON-LINEAR BEHAVIOR OF RC MEMBERS Shahd NASIR 1, Supratc GUPTA 2 And Hdetaka UMEHARA 3 SUMMARY In ths paper, a smplfed one-dmensonal analytcal tool based on fnte dfference technque

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

THE IDENTIFICATION OF MATERIAL PARAMETERS IN NONLINEAR DEFORMATION MODELS OF METALLIC-PLASTIC CYLINDRICAL SHELLS UNDER PULSED LOADING

THE IDENTIFICATION OF MATERIAL PARAMETERS IN NONLINEAR DEFORMATION MODELS OF METALLIC-PLASTIC CYLINDRICAL SHELLS UNDER PULSED LOADING Materals Physcs and Mechancs (2015) 66-70 Receved: March 27, 2015 THE IDENTIFICATION OF MATERIAL PARAMETERS IN NONLINEAR DEFORMATION MODELS OF METALLIC-PLASTIC CYLINDRICAL SHELLS UNDER PULSED LOADING N.А.

More information

The Folded Normal Stochastic Frontier. Gholamreza Hajargasht Department of Economics University of Melbourne, Australia

The Folded Normal Stochastic Frontier. Gholamreza Hajargasht Department of Economics University of Melbourne, Australia The Folded Normal Stochastc Fronter Gholamreza Hajargasht Department of Economcs Unversty of Melborne, Astrala Abstract We ntrodce a stochastc fronter model wth a folded normal neffcency dstrbton. Ths

More information

Linear Regression Analysis: Terminology and Notation

Linear Regression Analysis: Terminology and Notation ECON 35* -- Secton : Basc Concepts of Regresson Analyss (Page ) Lnear Regresson Analyss: Termnology and Notaton Consder the generc verson of the smple (two-varable) lnear regresson model. It s represented

More information

Professor Terje Haukaas University of British Columbia, Vancouver The Q4 Element

Professor Terje Haukaas University of British Columbia, Vancouver  The Q4 Element Professor Terje Haukaas Unversty of Brtsh Columba, ancouver www.nrsk.ubc.ca The Q Element Ths document consders fnte elements that carry load only n ther plane. These elements are sometmes referred to

More information

A method of two-scale analysis with micro-macro decoupling scheme: application to hyperelastic composite materials

A method of two-scale analysis with micro-macro decoupling scheme: application to hyperelastic composite materials Comput Mech (213) 52:1199 1219 DOI 1.17/s466-13-872-5 ORIGINAL PAPER A method of two-scale analyss wth mcro-macro decouplng scheme: applcaton to hyperelastc composte materals K. Terada J. Kato N. Hrayama

More information

Code_Aster. Identification of the Summarized

Code_Aster. Identification of the Summarized Verson Ttre : Identfcaton du modèle de Webull Date : 2/09/2009 Page : /8 Responsable : Aurore PARROT Clé : R70209 Révson : 609 Identfcaton of the Summarzed Webull model One tackles here the problem of

More information

Lecture 14: Forces and Stresses

Lecture 14: Forces and Stresses The Nuts and Bolts of Frst-Prncples Smulaton Lecture 14: Forces and Stresses Durham, 6th-13th December 2001 CASTEP Developers Group wth support from the ESF ψ k Network Overvew of Lecture Why bother? Theoretcal

More information

1 Matrix representations of canonical matrices

1 Matrix representations of canonical matrices 1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:

More information

One Dimensional Axial Deformations

One Dimensional Axial Deformations One Dmensonal al Deformatons In ths secton, a specfc smple geometr s consdered, that of a long and thn straght component loaded n such a wa that t deforms n the aal drecton onl. The -as s taken as the

More information

SPANC -- SPlitpole ANalysis Code User Manual

SPANC -- SPlitpole ANalysis Code User Manual Functonal Descrpton of Code SPANC -- SPltpole ANalyss Code User Manual Author: Dale Vsser Date: 14 January 00 Spanc s a code created by Dale Vsser for easer calbratons of poston spectra from magnetc spectrometer

More information

C PLANE ELASTICITY PROBLEM FORMULATIONS

C PLANE ELASTICITY PROBLEM FORMULATIONS C M.. Tamn, CSMLab, UTM Corse Content: A ITRODUCTIO AD OVERVIEW mercal method and Compter-Aded Engneerng; Phscal problems; Mathematcal models; Fnte element method. B REVIEW OF -D FORMULATIOS Elements and

More information

NON LINEAR ANALYSIS OF STRUCTURES ACCORDING TO NEW EUROPEAN DESIGN CODE

NON LINEAR ANALYSIS OF STRUCTURES ACCORDING TO NEW EUROPEAN DESIGN CODE October 1-17, 008, Bejng, Chna NON LINEAR ANALYSIS OF SRUCURES ACCORDING O NEW EUROPEAN DESIGN CODE D. Mestrovc 1, D. Czmar and M. Pende 3 1 Professor, Dept. of Structural Engneerng, Faculty of Cvl Engneerng,

More information

Inductance Calculation for Conductors of Arbitrary Shape

Inductance Calculation for Conductors of Arbitrary Shape CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors

More information

Visco-Rubber Elastic Model for Pressure Sensitive Adhesive

Visco-Rubber Elastic Model for Pressure Sensitive Adhesive Vsco-Rubber Elastc Model for Pressure Senstve Adhesve Kazuhsa Maeda, Shgenobu Okazawa, Koj Nshgch and Takash Iwamoto Abstract A materal model to descrbe large deformaton of pressure senstve adhesve (PSA

More information

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009 College of Computer & Informaton Scence Fall 2009 Northeastern Unversty 20 October 2009 CS7880: Algorthmc Power Tools Scrbe: Jan Wen and Laura Poplawsk Lecture Outlne: Prmal-dual schema Network Desgn:

More information

Numerical Nonlinear Analysis with the Boundary Element Method

Numerical Nonlinear Analysis with the Boundary Element Method Blucher Mechancal Engneerng Proceedngs May 2014, vol. 1, num. 1 www.proceedngs.blucher.com.br/evento/10wccm Numercal Nonlnear Analyss wth the Boundary Element Method E. Pneda 1, I. Vllaseñor 1 and J. Zapata

More information

STATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION

STATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION STATIC ANALYSIS OF TWO-LERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION Ákos József Lengyel István Ecsed Assstant Lecturer Emertus Professor Insttute of Appled Mechancs Unversty of Mskolc Mskolc-Egyetemváros

More information

The Analysis and the Performance Simulation of the Capacity of Bit-interleaved Coded Modulation System

The Analysis and the Performance Simulation of the Capacity of Bit-interleaved Coded Modulation System Sensors & Transdcers, Vol. 79, Isse 9, September 4, pp. 5-57 Sensors & Transdcers 4 by IFSA Pblshng, S. L. http://www.sensorsportal.com The Analyss and the Performance Smlaton of the Capacty of Bt-nterleaved

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

STUDY ON SEISMIC BEHAVIOR OF RC COMPOSITE CORE WALLS WITH CONCEALED STEEL TRUSS SUBJECTED TO COMBINED ACTION

STUDY ON SEISMIC BEHAVIOR OF RC COMPOSITE CORE WALLS WITH CONCEALED STEEL TRUSS SUBJECTED TO COMBINED ACTION STUDY ON SEISMIC BEHAVIOR OF RC COMPOSITE CORE WALLS WITH CONCEALED STEEL TRUSS SUBJECTED TO COMBINED ACTION CAO Wanln 1, CHANG Wehua 2, ZHANG Janwe 1 1 College of archtecture and Cvl Engneerng, Bejng

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

A how to guide to second quantization method.

A how to guide to second quantization method. Phys. 67 (Graduate Quantum Mechancs Sprng 2009 Prof. Pu K. Lam. Verson 3 (4/3/2009 A how to gude to second quantzaton method. -> Second quantzaton s a mathematcal notaton desgned to handle dentcal partcle

More information

MMA and GCMMA two methods for nonlinear optimization

MMA and GCMMA two methods for nonlinear optimization MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons

More information

Effect of anisotropy on laminated composite plates containing circular holes

Effect of anisotropy on laminated composite plates containing circular holes Indan Journal of ngneerng & Materals Scences Vol. 1, June 005, pp. 07-13 ffect of ansotropy on lamnated composte plates contanng crcular holes H Murat Arslan Cukurova Unversty, Cvl ngneerng Department,

More information