STRUCTURAL ANALYSIS OF MONO-SYMMETRIC PLATE GIRDERS IN COMPOSITE BRIDGES
|
|
- Gabriel Richard
- 5 years ago
- Views:
Transcription
1 ACTA TEHNICA CORVINIENSIS Bullin of Enginring Tom VIII [05] Fascicul [Januar March] ISSN: Mohamd A. A. El-SHAER,. Ghada M. El-MAHDY STRUCTURAL ANALYSIS OF MONO-SYMMETRIC PLATE GIRDERS IN COMPOSITE BRIDGES. Civil and Consrucion Enginring Dparmn, Highr Tchnological Insiu, 0 h of Ramadan Ci, EGYPT Sl Srucurs, Srucurs & Mallic Consrucion Rsarch Insiu, Housing &Building Naional Rsarch Cnr, Giza, EGYPT Asrac: Mono-smmric pla girdrs ar ofn usd in simpl suppord composi ridgs o limina local pla uckling in h comprssion flang during consrucion. This causs h nural axis of h pla girdr o shif downwards sujcing mor of h w o comprssiv srsss du o nding. In slndr ws his inass h possiili of local uckling in h comprssion par of h w during consrucion. Howvr, dpnding on h slndrnss (widh-o-hicknss raio of h w, h pos-uckling rsrv capaci ma accommoda his local uckling wihin h lasic limi of h w for during consrucion loads. Hnc, his would allow for h us of mor slndr ws in composi pla girdr consrucion wihou h nd for longiudinal w siffnrs or h rducion of h ovrall composi scion du o local pla uckling in h w. Rcommndd valus of srss lvl ar givn for mono-smmric pla girdrs in h non-composi sag asd on h rsuls of a non-linar fini lmn analsis. Kwords: composi ridgs, ffciv widh, FEA, local pla uckling, mono-smmric scions, pla girdrs, srss gradin, srss lvl INTRODUCTION Pla girdrs in conjuncion wih a rinforcd con sla ar ofn usd as composi pla girdr ridgs in posiiv nding. This has h advanag of rh possiili of local pla uckling in h pla girdr s w and comprssion flang as a rsul of composi acion undr srvic loads. In addiion o his, h during consrucion loads acing on h pla girdr scion alon, DL, ma dsignd o allow for local uckling in h w whil kping h srsss wihin h lasic limi of h pla girdr scion during consrucion > > -.0 Gross sl scion Effciv sl scion Srss disriuion (DL (a Un-shord non-composi scion wih inffciv con sla (DL onl > Composi scion Srss disriuion (DL +LL Final srss disriuion ( Un-shord composi scion afr hardning of con sla (DL +DL +LL (.0.7 > upwards wih h ons of composi acion, as shown in Figur (. Hnc, prvning rsidual srains du o h ilding of h scion during h consrucion non-composi sag and h afr consrucion composi sag. Th srss disriuion for oh h non-composi and composi sags for un-shord consrucion is shown in Figur. Ohr rsarchrs o sud composi I-girdrs ar Gupa [], Gupa al. [], Baskr al. [3], and Yakl and Azizinamini [4]. Rcn rsarch was also conducd on I-scion flxural ams Shokouhian and Shi [5] and L al. []. LOCAL PLATE BUCKLING Local pla uckling occurs in slndr pla lmns whn h comprssiv srss in h pla lmn xcds h iical pla uckling srss of h pla lmn, as shown in Figur. Afr h ons of pla uckling, a wav-lik propagaion of ou-of-plan dformaions raks ou inasing in ampliud wih h inas in loading. This causs h comprssiv srsss o rdisriu in h pla lmn, concnraing in h rgions suppord sal oundar condiions. Du o h loss of in-plan siffnss of h unsuppord rgions, comprssiv and nsil nding srsss Figur : Srss disriuion in composi consrucion For pla girdrs wih ws having a widh-o-hicknss raio in h vr slndr rang, h iical srss is wll low h ild srss, and wih h inas in loading afr h ons of local uckling up o h undr h ffc of consrucion loads onl, Figur (a, h posuckling sa of h slndr w ma caus a nonlinar srss ild srss,. Onc h dg srss has rachd h ild srss, h disriuion, u h srsss in h w ma sill in h lasic rang. This would allow for h us of mor slndr ws for rachd h ild srss. Whras, h unsuppord unsal inrnal composi pla girdrs kping in mind ha h nural axis will shif par of h pla lmn is assumd o inffciv. Hnc, h dvlop hrough h hicknss of h pla, flucuaing along h lngh of h pla. Th srss a h sal dgs graduall inass plasicizaion of h pla lmn propagas in h nar rgions ill h suppord pars of h pla lmn ar assumd o hav coprigh Facul of Enginring - Hundoara, Univrsi POLITEHNICA Timisoara
2 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] pla lmn dos hav a pos-uckling rsrv capaci which can Assuming ha h avrag uniform srss of h nonlinar posuckling srss disriuion is av as shown in Figur, h ffciv wihin h lasic limi of h lmn if h dg srss dos no rach h ild srss capaci. widh is assumd o h widh sujc o a srss qual o h dg srss,, of h nonlinar srss disriuion such ha i dvlops a srngh qual o h avrag srss acing on h whol widh. Hnc, = av (5 giving > Acual srss disriuion. Rgion assumd no o ransmi srss caus of uckling. Figur : Concp of ffciv widh Th lasic uckling srss,, of slndr plas as drivd von Kàrmàn al. [7] is kπ E = ( ν ( which is invrsl proporional o h squar of h widh-ohicknss raio, /, of h pla lmn. Th pla uckling facor, k, dpnds on h longiudinal oundar condiions of h pla lmn and h normal srss disriuion in h pla, shown in Figur. Exprssions for k for diffrn oundar condiions can found in h Eurocod EC3 EN 993--:003 [8] or h Egpian Cod of Pracic for Sl Consrucion and Bridgs ECOP-ASD [9]. Th modulus of lasici, E, can akn as 0,000 MPa and Poisson s raio, can akn as 0.3. From h xprssion for h uniform lasic iical srss, givn in Eq. (, acing on a pla wih a widh-o-hicknss raio of / w g = kπ E ( ν Assuming an ffciv widh of and a uniform srss acing on i of, which can hav a valu anwhr from h iical srss o h ild srss as shown in Figur, hn analog w g = kπ E ( ν Hnc, h raio of h ffciv widh, o h original widh, known as h ffciv widh paramr ρ, is = ρ = av av > (4 av = = Taking h non-dimnsional slndrnss paramr λ n as ( ν = = kπ E and susiuing his ino Eq. ( givs av = (8 To accoun for h ffc of rsidual srsss in h modral slndr and h non-compac slndrnss rangs, h Amrican Iron and Sl Insiu (AISI [0] suggss h following xprssion for h avrag srss. λ 0. n av = Boh Eqs. (8 and (9 ar plod in Figur 3. Figur 3: Normalizd pla uckling curvs EFFECT OF STRESS GRADIENT ON LOCAL PLATE BUCKLING To includ h ffc of srss gradin in h pla lmn du o comind comprssiv and flxural srsss in h mmr, as shown ( in Figur 4, h ffciv widh paramr, ρ, is assumd o ak h form av x ψ (0 whr x and can drmind from h limis of / for siffnd (3 slndr pla lmns in pur comprssion, ψ = +.0, and pur nding, ψ = -.0. This is h sam mhod usd El-Mahd and Au-Hamd [,, and 3] o driv h currn quaion for h ffciv widh of siffnd slndr pla lmns sujc o a srss gradin in h Egpian Cod of Pracic for h Dsign of Sl Consrucion and Bridgs [9]. ( (7 (9 48
3 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] = comprssion flang and h nsion flang. This causs a sligh das of h srss gradin in h w du o a minor chang in = +.0 h posiion of h modl s nural axis, u his das is = 0.5 = 0.5 ngligil. Boh flangs wr larall suppord as shown in Figur = +0.5 = +0.5 (a o prvn an ou-of-plan laral orsional-flxural uckling occurring in h comprssion flang. Elasic-plasic shll lmns = 0.0 = 0.0 wr usd o modl h flang and w pla lmns, howvr, h = 0.0 = = 0.0 nd pars of h op and oom flangs wr siffnd inasing hir hicknss and akn as lasic shll lmns o ovrcom local dformaions du o loads applid o hs flangs. Th marial of h modl was akn as lasic-prfcl plasic wih a modulus of = -0.5 = -0.5 lasici of 0 GPa and a ild srss of 350 MPa. = -0.5 = -.0 = - = -0.5 Figur 4: Schmaic rprsnaion of srss gradin, ψ, du o comind comprssiv and flxural srsss For xampl, using h limis for pur comprssion and pur nding givn in h Eurocod EC3 [], = 4ε for ψ = +.0 = 4ε for ψ = -.0 whr ε = 35/ ( and aking k = 4.0 for h cas of pur comprssion and k = 3.9 for h cas of pur nding and assuming = givs h valus 0.44 and for x and, rspcivl. Hnc, according o h limis of h EC3 [8]: av ψ ( Facorizing and approximaing his lads o h xprssion av 0. 05(3 ψ + (3 which is clos o h xprssion givn in h EC3 EN :00 [4] av (3 ψ + (4 Th normalizd avrag srss for h cass of ψ = +.0 and ψ = -.0, according o Eq. (, ar plod in Figur 3. FINITE ELEMENT ANALYSIS A fini lmn paramric analsis, using COSMOS. sofwar, was conducd on modls of pla girdrs having a w dph of 000 mm and varing h w hicknss, w, from 5 mm o mm giving a widh-o-hicknss raio for h w varing from 00 o 9. Th comprssion flang was kp consan in h non-compac rang having a siz of 00 x mm, whras, h siz of h nsion flang was inasd o achiv a srss gradin in h w of ψ = -.0, - 0.8, -0., and -0.4, as shown in Figur 5. A modl wih a simpl suppord span of lngh L = 0 m was usd. In h acual fini lmn modl h high of h w was modld having a dph of 000 mm plus half h hicknss of oh h 49 = -.0 = -0.8 = -0. = -0.4 Figur 5: Schmaic rprsnaion of paramric pla girdr ross-scions Figur : Tpical fini lmn modl and normal srss disriuion of linar analsis; a Fini lmn modl; Dformd shap and srss disriuion Th comprssion and nsion flangs of ach modl wr loadd o caus a momn qual o h ild capaci of h scion. This was achivd appling quivaln nd comprssion and nsion forcs a
4 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] in h op and oom flangs, rspcivl, according o h DISCUSSION OF RESULTS following formulas: Figur 8 illusras h in-plan mmran normal srss disriuion ( = Aw and h ou-of-plan local pla uckling of h w in flxural F Af F + comprssion for h modl wih a w slndrnss of 00 (i.., w = 5 Af 3 ψ (5 mm and a srss raio of ψ = -0.. ( Aw ψ F = ψ + ( Af F Af 3 ψ ( This givs a ild momn, M, of 3 A + ψ ( ( ( f Af Aw + ψ M = hwf + ψ 3 ψ (7 whr F and F ar h quivaln comprssion and nsion forcs assumd o concnrad a h cnroids of h flangs ha caus a momn qual o h ild momn capaci of h scion, a rspcivl; A f and A f ar h aras of h op and oom flang plas, rspcivl; and h w and A w ar h dph and ara of h modl s w pla, rspcivl. Th rsuls of h linar analsis conducd on h fini lmn modls vrif ha h gross siffnss of h modl, calculad from h midpoin dflcion,, compar accural wih h analic xprssion for a simpl suppord am sujc o a uniform momn, M, viz., I = ML /8E. Th posiion of h nural axis can also drmind from h normal srss disriuion in h dflcd modl. Excssiv srsss wr nod in h flangs nar h loadd dgs. Figur ( shows h normal srss disriuion in h dformd modl wih a w hicknss of 5 mm or a w slndrnss of 00 and a oom flang sizd o giv a srss gradin of ψ = -0.. A nonlinar analsis which follows h Nwon-Raphson inmnaliraiv procdur was usd o dc h propagaion of local pla uckling in h slndr w. An iniial mm ou-of-flanss a h cnr-poin of h w was usd in h modl o iniia local w uckling. Finall, a fini lmn analsis of h composi scion, shown in Figur 7, using a sla of 000 x 00 mm wih a con cu c srngh, f c, of 40 MPa and uniforml loadd aov h sla gav approxima valus of h rsidual capaci of h composi scion in h afr consrucion phas. Figur 7: Normal srss disriuion in composi scion d Figur 8: Dformd shap and normal mmran srss disriuion for modl wih w slndrnss 00 and ψ= -0.; a Srss lvl.7 Srss lvl c Srss disriuion along h w a diffrn srss lvls d Load-dflcion curvs A a srss lvl of.7, shown in Figur 8(a, i can sn ha a noal amoun of local uckling in h comprssion par of h w 50
5 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] occurrd wihou causing an disorional uckling in h noncompac adjacn comprssion flang, and wihou xcding h considral nonlinari in h srss disriuion occurs nar h uckling has iniiad a h iical srss lvl, howvr, lasic limi as shown h maximum comprssiv srss of 4 nd of h nonlinar analsis as h srss lvl approachs h ild MPa. Whras, for a srss lvl of = 350 MPa, shown in Figur srss. This is also dmonsrad h load-dflcion curvs shown 8(, h local uckling of h w in comprssion is gral magnifid in Figur 8(d. I can also nod ha h nural axis nds o shif causing disorional uckling in h adjacn comprssion flang. upwards wih h occurrnc of local pla uckling in h w and h nonlinar srss disriuion. a a c c Figur 9: Dformd shap and normal mmran srss disriuion for modl wih w slndrnss 5 and ψ = -0.; a Srss lvl.47 ; Srss lvl ; c Srss disriuion along h w a diffrn srss lvls; dload-dflcion curvs Figur 8(c shows h srss disriuion along h w for h sam modl a diffrn srss lvls. I can sn ha h srss disriuion along h w rmains rlaivl linar vn afr local 5 d Figur 0: Dformd shap and normal mmran srss disriuion for modl wih w slndrnss 00 and ψ = -0.; Srss lvl.09 ; csrss disriuion along h w a diffrn srss lvls; dloaddflcion curvs Figur 9 shows h dformd shap and normal mmran srss disriuion for h modl wih a w slndrnss of 5 (i.., w = 8 mm and a oom flang proporiond o giv a srss raio of ψ = -
6 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] 0.. A sligh amoun of local w uckling can dcd a a srss formulas givn in Eq. (8 ar also compard o h curvs oaind lvl of.47 whr h maximum comprssiv srss is 337 MPa for h nonlinar fini lmn analsis in Figur. Th maximum and hnc is sill low h ild srss, as shown in Figur 9(a. rror wn hs wo curvs is lss han % and is consrvaiv for Howvr, a a srss lvl of h local uckling in h w is all valus of /. magnifid causing disorional uckling in h comprssion flang, as.8x0 for ψ = -.0 = shown in Figur 9(. Figur 9(c shows h srss disriuion along ( hw w h w for his modl a diffrn srss lvls. I can sn ha.x0 for ψ = -0.8 =.30.0 (8 h srss disriuion along h w rmains rlaivl linar vn ( hw w afr local uckling has iniiad a h iical srss lvl, howvr, a.74x0 for ψ = -0. =.45.0 sligh nonlinari in h srss disriuion occurs nar h nd of h ( hw w nonlinar analsis as h srss lvl approachs h ild srss. Th 5.58x0 sligh nonlinari is again shown in h load-dflcion curv in for ψ = -0.4 =.5.0 ( hw w Figur 9(d. Finall, Figur 0 shows h dformd shap and normal srss disriuion for h modl wih a w slndrnss of 00 (i.., w = 0 mm and a lowr flang proporiond o giv a srss raio of ψ = -0.. A a srss lvl of h maximum srss is clos o and vr lil local w uckling has occurrd, as shown in Figur 0(a. In fac, a a srss lvl of.09 h local uckling is sill hard o dc alhough h scion has ildd, as shown in Figur 0(. Figur 0(c shows h srss disriuion along h w for his modl a diffrn srss lvls. I can sn ha h srss disriuion along Figur : Comparison of Eq. (8 wih h FEA rsuls h w rmains linar up o h nd of h nonlinar analsis as h From h fini lmn rsuls of h composi scions, i can srss lvl approachs h ild srss. This linari is also dpicd nod ha inasing h hicknss of h w rsuls in a minor in h load-dflcion curvs shown in Figur 0(d. inas in composi capaci. Whras using a grar valu of Th rcommndd valus of srss lvl wih rspc o h iical srss for ohr srss gradins as drmind h nonlinar fini lmn analsis ar lisd in Tal and ar plod in Figur. Tal : Rcommndd valus of srss lvl wih rspc o iical srss / h w / w ψ Figur : Rcommndd valus of srss lvl for mono-smmric girdrs A procss of curv fiing has ld o h drivaion of h formulas givn in Eq. (8 for h rcommndd valus of srss lvl as a funcion of h w slndrnss raio for ach valu of ψ. Th srss gradin (i.., ψ = -0.4 gral inass h composi capaci 3 ims, and an loss in h capaci of h non-composi scion du o h uckling of h slndr w can compnsad for using shoring during consrucion. CONCLUSION Th fini lmn paramric analsis shows ha mono-smmric non-composi pla girdrs wih slndr ws can srssd ond h iical srss, iniiaing h ons of local uckling of h w in flxural comprssion, wihou xcding h lasic limi. Howvr, du o h occurrnc of xcssiv local uckling dformaions in slndr ws causing disorional uckling in h comprssion flang h following srss limis ar rcommndd dpnding on h srss raio in h w;.7 for ws in h vr slndr rang dasing o.0 for ws in h lss slndr rang. Smols A f = ara of oom flang pla A f = ara of op flang pla A w = ara of w pla = pla widh = ffciv widh E = modulus of lasici f c = con cu srngh F = quivaln nsil forc in oom flang F = quivaln comprssiv forc in op flang h w = dph of w pla k = pla uckling facor 5
7 ACTA TEHNICA CORVINIENSIS Fascicul [Januar March] Bullin of Enginring Tom VIII [05] L = span of girdr M = nding momn M = ild momn of girdr = pla hicknss w = hicknss of w pla x, = varials = midpoin dflcion ε = 35 / λ n =non-dimnsional slndrnss paramr ν = Poisson s raio ρ = ffciv widh paramr = srss = largr dg comprssiv srss = smallr dg comprssiv srss or nsil srss av = avrag srss = iical uckling srss = dg srss = ild srss ψ = srss gradin Rfrncs [.] Gupa, V.K., Dvlopmn of scion classificaion irion and ulima flxural quaion for composi I-girdrs, Docoral Dissraion, Saiama Univrsi, Japan, 00. [.] Gupa, V.K., Yoshiaki, O., and Nagai, M., Dvlopmn of w slndrnss limis for composi I-girdrs accouning for iniial nding momn, Dooku Gakkai Ronunshuu A (JSCE Journal of Srucural and Earhquak Enginring, Vol., No. 4, pp , 00. [3.] Baskr, K., Shanmugan, N.E., and Thvndran, V., Fini-lmn analsis of sl-con composi pla girdr, J. Sruc. Eng., ASCE, Vol. 8, No. 9, pp. 58-8, 00. [4.] Yakl, A.J. and Azizinamini, A., Improvd momn srngh prdicion of composi sl pla girdrs in posiiv nding, J. Bridg Eng., ASCE, Vol. 0, No., pp. 8-38, 005. [5.] Shokouhian, M. and Shi, Y., Classificaion of I-scion flxural mmrs asd on mmr ducili, Journal of Consrucional Sl Rsarch, Vol. 95, April, pp. 98-0, 04. [.] L, C.H., Han, K.H., Uang, C.M., Kim, D.K., Park, C.H., and Kim, J.H., Flxural srngh and roaion capaci of I-shapd ams faricad from 800 MPa sl, J. Sruc. Eng., ASCE, Vol. 39, No., pp , 03. [7.] von Kármán, T., Schlr, E.E., and Donll, L.H., Srngh of hin plas in comprssion, Transacions of h Amrican Soci of Mchanical Enginrs, Vol. 54, No. APM-54-5, p. 53, 93. [8.] Eurocod 3, Dsign of sl srucurs Par. Gnral srucural ruls (EN 993--:003, Europan Commi for Sandardizaion (CEN, Brussls, Blgium, 005. [9.] ECOP-ASD, Egpian Cod of Pracic for Sl Consrucion and Bridgs Allowal Srss Dsign, Egp, 00. [0.] Amrican Iron and Sl Insiu, Spcificaion for h dsign of coldformd sl srucural mmrs, AISI, Washingon DC, 007. [.] Au-Hamd, M.H. and Elmahd, G.M., Th ffciv widh of slndr pla lmns in pla girdrs, Journal of Enginring and Applid Scinc, Facul of Enginring - Cairo Univrsi, 50(: 59-78, 003. [.] Elmahd, G. and Au-Hamd, M., Nw formula for h ffciv widh of slndr pla lmns, Procdings of h CSCE Annual Confrnc - h Srucural Spciali Confrnc, Quc Ci, Quc, Canada, 008. [3.] El-Mahd, G. and Au-Hamd, M., Local uckling of slndr pla girdrs in composi ridgs, Procdings of h SSRC Annual Saili Confrnc, Orlando, Florida, USA, 00. [4.] Eurocod 3, Dsign of sl srucurs Par.5 Plad srucural lmns (EN :00, Europan Commi for Sandardizaion (CEN, Brussls, Blgium, 00. coprigh Univrsi POLITEHNICA Timisoara, Facul of Enginring Hundoara, 5, Rvoluii, 338, Hundoara, ROMANIA hp://aca.fih.up.ro 53
4.3 Design of Sections for Flexure (Part II)
Prsrssd Concr Srucurs Dr. Amlan K Sngupa and Prof. Dvdas Mnon 4. Dsign of Scions for Flxur (Par II) This scion covrs h following opics Final Dsign for Typ Mmrs Th sps for Typ 1 mmrs ar xplaind in Scion
More informationLogistic equation of Human population growth (generalization to the case of reactive environment).
Logisic quaion of Human populaion growh gnralizaion o h cas of raciv nvironmn. Srg V. Ershkov Insiu for Tim aur Exploraions M.V. Lomonosov's Moscow Sa Univrsi Lninski gor - Moscow 999 ussia -mail: srgj-rshkov@andx.ru
More informationUNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS
Answr Ky Nam: Da: UNIT # EXPONENTIAL AND LOGARITHMIC FUNCTIONS Par I Qusions. Th prssion is quivaln o () () 6 6 6. Th ponnial funcion y 6 could rwrin as y () y y 6 () y y (). Th prssion a is quivaln o
More informationApplied Statistics and Probability for Engineers, 6 th edition October 17, 2016
Applid Saisics and robabiliy for Enginrs, 6 h diion Ocobr 7, 6 CHATER Scion - -. a d. 679.. b. d. 88 c d d d. 987 d. 98 f d.. Thn, = ln. =. g d.. Thn, = ln.9 =.. -7. a., by symmry. b.. d...6. 7.. c...
More informationMidterm Examination (100 pts)
Econ 509 Spring 2012 S.L. Parn Midrm Examinaion (100 ps) Par I. 30 poins 1. Dfin h Law of Diminishing Rurns (5 ps.) Incrasing on inpu, call i inpu x, holding all ohr inpus fixd, on vnuall runs ino h siuaion
More informationFailure Load of Plane Steel Frames Using the Yield Surface Method
ISBN 978-93-84422-22-6 Procdings of 2015Inrnaional Confrnc on Innovaions in Civil and Srucural Enginring (ICICSE'15) Isanbul (Turky), Jun 3-4, 2015. 206-212 Failur Load of Plan Sl Frams Using h Yild Surfac
More informationAR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )
AR() Procss Th firs-ordr auorgrssiv procss, AR() is whr is WN(0, σ ) Condiional Man and Varianc of AR() Condiional man: Condiional varianc: ) ( ) ( Ω Ω E E ) var( ) ) ( var( ) var( σ Ω Ω Ω Ω E Auocovarianc
More informationBoyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors
Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar
More informationCharging of capacitor through inductor and resistor
cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.
More informationExperimental and Computer Aided Study of Anisotropic Behavior of Material to Reduce the Metal Forming Defects
ISSN 2395-1621 Exprimnal and Compur Aidd Sudy of Anisoropic Bhavior of Marial o Rduc h Mal Forming Dfcs #1 Tausif N. Momin, #2 Vishal B.Bhagwa 1 ausifnmomin@gmail.com 2 bhagwavb@gmail.com #12 Mchanical
More informationNotes on the AISC Provisions for Slender Compression Elements in Compression Members
Nos on h AISC 36-16 Provisions for Slndr Comprssion lmns in Comprssion Mmrs LOUIS. GSCHWINDNR and MATTHW TROMNR ABSTRACT Comprssion mmr srngh is onrolld h limi sas of flxural ukling, orsional ukling, and
More informationUNSTEADY FLOW OF A FLUID PARTICLE SUSPENSION BETWEEN TWO PARALLEL PLATES SUDDENLY SET IN MOTION WITH SAME SPEED
006-0 Asian Rsarch Publishing work (ARP). All righs rsrvd. USTEADY FLOW OF A FLUID PARTICLE SUSPESIO BETWEE TWO PARALLEL PLATES SUDDELY SET I MOTIO WITH SAME SPEED M. suniha, B. Shankr and G. Shanha 3
More informationInstitute of Actuaries of India
Insiu of Acuaris of India ubjc CT3 Probabiliy and Mahmaical aisics Novmbr Examinaions INDICATIVE OLUTION Pag of IAI CT3 Novmbr ol. a sampl man = 35 sampl sandard dviaion = 36.6 b for = uppr bound = 35+*36.6
More information2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35
MATH 5 PS # Summr 00.. Diffrnial Equaions and Soluions PS.# Show ha ()C #, 4, 7, 0, 4, 5 ( / ) is a gnral soluion of h diffrnial quaion. Us a compur or calculaor o skch h soluions for h givn valus of h
More informationLecture 2: Current in RC circuit D.K.Pandey
Lcur 2: urrn in circui harging of apacior hrough Rsisr L us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R and a ky K in sris. Whn h ky K is swichd on, h charging
More information4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b
4. Th Uniform Disribuion Df n: A c.r.v. has a coninuous uniform disribuion on [a, b] whn is pdf is f x a x b b a Also, b + a b a µ E and V Ex4. Suppos, h lvl of unblivabiliy a any poin in a Transformrs
More informationLecture 1: Numerical Integration The Trapezoidal and Simpson s Rule
Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -
More informationPhysics 160 Lecture 3. R. Johnson April 6, 2015
Physics 6 Lcur 3 R. Johnson April 6, 5 RC Circui (Low-Pass Filr This is h sam RC circui w lookd a arlir h im doma, bu hr w ar rsd h frquncy rspons. So w pu a s wav sad of a sp funcion. whr R C RC Complx
More informationEXERCISE - 01 CHECK YOUR GRASP
DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationElementary Differential Equations and Boundary Value Problems
Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ
More informationPhys463.nb Conductivity. Another equivalent definition of the Fermi velocity is
39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h
More informationCSE 245: Computer Aided Circuit Simulation and Verification
CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy
More informationThe transition:transversion rate ratio vs. the T-ratio.
PhyloMah Lcur 8 by Dan Vandrpool March, 00 opics of Discussion ransiion:ransvrsion ra raio Kappa vs. ransiion:ransvrsion raio raio alculaing h xpcd numbr of subsiuions using marix algbra Why h nral im
More informationH is equal to the surface current J S
Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion
More informationWave Equation (2 Week)
Rfrnc Wav quaion ( Wk 6.5 Tim-armonic filds 7. Ovrviw 7. Plan Wavs in Losslss Mdia 7.3 Plan Wavs in Loss Mdia 7.5 Flow of lcromagnic Powr and h Poning Vcor 7.6 Normal Incidnc of Plan Wavs a Plan Boundaris
More informationLecture 1: Growth and decay of current in RL circuit. Growth of current in LR Circuit. D.K.Pandey
cur : Growh and dcay of currn in circui Growh of currn in Circui us considr an inducor of slf inducanc is conncd o a DC sourc of.m.f. E hrough a rsisr of rsisanc and a ky K in sris. Whn h ky K is swichd
More informationCPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees
CPSC 211 Daa Srucurs & Implmnaions (c) Txas A&M Univrsiy [ 259] B-Trs Th AVL r and rd-black r allowd som variaion in h lnghs of h diffrn roo-o-laf pahs. An alrnaiv ida is o mak sur ha all roo-o-laf pahs
More informationOn the Speed of Heat Wave. Mihály Makai
On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.
More informationChapter 12 Introduction To The Laplace Transform
Chapr Inroducion To Th aplac Tranorm Diniion o h aplac Tranorm - Th Sp & Impul uncion aplac Tranorm o pciic uncion 5 Opraional Tranorm Applying h aplac Tranorm 7 Invr Tranorm o Raional uncion 8 Pol and
More information4.2 Design of Sections for Flexure
4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt
More informationA MATHEMATICAL MODEL FOR NATURAL COOLING OF A CUP OF TEA
MTHEMTICL MODEL FOR NTURL COOLING OF CUP OF TE 1 Mrs.D.Kalpana, 2 Mr.S.Dhvarajan 1 Snior Lcurr, Dparmn of Chmisry, PSB Polychnic Collg, Chnnai, India. 2 ssisan Profssor, Dparmn of Mahmaics, Dr.M.G.R Educaional
More informationTransfer function and the Laplace transformation
Lab No PH-35 Porland Sa Univriy A. La Roa Tranfr funcion and h Laplac ranformaion. INTRODUTION. THE LAPLAE TRANSFORMATION L 3. TRANSFER FUNTIONS 4. ELETRIAL SYSTEMS Analyi of h hr baic paiv lmn R, and
More informationMicroscopic Flow Characteristics Time Headway - Distribution
CE57: Traffic Flow Thory Spring 20 Wk 2 Modling Hadway Disribuion Microscopic Flow Characrisics Tim Hadway - Disribuion Tim Hadway Dfiniion Tim Hadway vrsus Gap Ahmd Abdl-Rahim Civil Enginring Dparmn,
More information14.02 Principles of Macroeconomics Problem Set 5 Fall 2005
40 Principls of Macroconomics Problm S 5 Fall 005 Posd: Wdnsday, Novmbr 6, 005 Du: Wdnsday, Novmbr 3, 005 Plas wri your nam AND your TA s nam on your problm s Thanks! Exrcis I Tru/Fals? Explain Dpnding
More informationEquation For non-self Energizing Gasket
Jun 0 0:05: - ASMEScDiv_WNFlangDsign.sm Dsign of Wld Nck Flang as pr ASME Scion Division ar.6 Dsign ol oads STE : Dsign ondiion Dsign rssur 0. Ma Dsign Tmpraur T 80 d STE : ask Facors 'm' and Minimum Dsign
More informationAn Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT
[Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI
More informationLet s look again at the first order linear differential equation we are attempting to solve, in its standard form:
Th Ingraing Facor Mhod In h prvious xampls of simpl firs ordr ODEs, w found h soluions by algbraically spara h dpndn variabl- and h indpndn variabl- rms, and wri h wo sids of a givn quaion as drivaivs,
More informationA THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER
A THREE COPARTENT ATHEATICAL ODEL OF LIVER V. An N. Ch. Paabhi Ramacharyulu Faculy of ahmaics, R D collgs, Hanamonda, Warangal, India Dparmn of ahmaics, Naional Insiu of Tchnology, Warangal, India E-ail:
More informationSpring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review
Spring 6 Procss Dynamics, Opraions, and Conrol.45 Lsson : Mahmaics Rviw. conx and dircion Imagin a sysm ha varis in im; w migh plo is oupu vs. im. A plo migh imply an quaion, and h quaion is usually an
More information5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t
AP CALCULUS FINAL UNIT WORKSHEETS ACCELERATION, VELOCTIY AND POSITION In problms -, drmin h posiion funcion, (), from h givn informaion.. v (), () = 5. v ()5, () = b g. a (), v() =, () = -. a (), v() =
More information16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 3: Ideal Nozzle Fluid Mechanics
6.5, Rok ropulsion rof. nul rinz-snhz Lur 3: Idl Nozzl luid hnis Idl Nozzl low wih No Sprion (-D) - Qusi -D (slndr) pproximion - Idl gs ssumd ( ) mu + Opimum xpnsion: - or lss, >, ould driv mor forwrd
More informationControl System Engineering (EE301T) Assignment: 2
Conrol Sysm Enginring (EE0T) Assignmn: PART-A (Tim Domain Analysis: Transin Rspons Analysis). Oain h rspons of a uniy fdack sysm whos opn-loop ransfr funcion is (s) s ( s 4) for a uni sp inpu and also
More information3(8 ) (8 x x ) 3x x (8 )
Scion - CHATER -. a d.. b. d.86 c d 8 d d.9997 f g 6. d. d. Thn, = ln. =. =.. d Thn, = ln.9 =.7 8 -. a d.6 6 6 6 6 8 8 8 b 9 d 6 6 6 8 c d.8 6 6 6 6 8 8 7 7 d 6 d.6 6 6 6 6 6 6 8 u u u u du.9 6 6 6 6 6
More informationDEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018
DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Aoc. Prof. Dr. Burak Kllci Spring 08 OUTLINE Th Laplac Tranform Rgion of convrgnc for Laplac ranform Invr Laplac ranform Gomric valuaion
More information4.4 Design of Sections for Flexure (Part III)
4.4 Dsign of Sctions for Flxur (Part ) This sction covrs th following topics. Choic of Sctions Dtrmination of Limiting Zon Post-tnsioning in Stags 4.4.1 Choic of Sctions Th typ of sction is slctd asd on
More informationOn the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument
Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn
More information1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to:
Rfrncs Brnank, B. and I. Mihov (1998). Masuring monary policy, Quarrly Journal of Economics CXIII, 315-34. Blanchard, O. R. Proi (00). An mpirical characrizaion of h dynamic ffcs of changs in govrnmn spnding
More informationInstability Analysis of Laminated Composite Beams Subjected to Parametric Axial Load
Insabiliy Analysis of aminad Composi Bams Subjcd o Paramric Axial oad Alirza Fridooni, Kamran Bhdinan, Zouhir Fawaz Absrac h ingral form of quaions of moion of composi bams subjcd o varying im loads ar
More informationMEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control
MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ
More informationArturo R. Samana* in collaboration with Carlos Bertulani*, & FranjoKrmpotic(UNLP-Argentina) *Department of Physics Texas A&M University -Commerce 07/
Comparison of RPA-lik modls in Nurino-Nuclus Nuclus Procsss Aruro R. Samana* in collaboraion wih Carlos Brulani* & FranjoKrmpoicUNLP-Argnina *Dparmn of Physics Txas A&M Univrsiy -Commrc 07/ 0/008 Aomic
More informationReliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach.
Inrnaional Journal of Compuaional Sin and Mahmais. ISSN 97-3189 Volum 3, Numr 3 11, pp. 351-3 Inrnaional Rsarh Puliaion Hous hp://www.irphous.om Rliailiy Analysis of a Bridg and Paralll Sris Nworks wih
More informationEE 529 Remote Sensing Techniques. Review
59 Rmo Snsing Tchniqus Rviw Oulin Annna array Annna paramrs RCS Polariaion Signals CFT DFT Array Annna Shor Dipol l λ r, R[ r ω ] r H φ ηk Ilsin 4πr η µ - Prmiiviy ε - Prmabiliy
More informationNONLINEAR ANALYSIS OF PLATE BENDING
NONLINEAR ANALYSIS OF PLATE BENDING CONTENTS Govrning Equations of th First-Ordr Shar Dformation thor (FSDT) Finit lmnt modls of FSDT Shar and mmbran locking Computr implmntation Strss calculation Numrical
More informationDouble Slits in Space and Time
Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an
More informationC From Faraday's Law, the induced voltage is, C The effect of electromagnetic induction in the coil itself is called selfinduction.
Inducors and Inducanc C For inducors, v() is proporional o h ra of chang of i(). Inducanc (con d) C Th proporionaliy consan is h inducanc, L, wih unis of Hnris. 1 Hnry = 1 Wb / A or 1 V sc / A. C L dpnds
More informationBifurcation Theory. , a stationary point, depends on the value of α. At certain values
Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local
More informationVoltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!
Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr
More informationCHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano
Expcaions: Th Basic Prpard by: Frnando Quijano and Yvonn Quijano CHAPTER CHAPTER14 2006 Prnic Hall Businss Publishing Macroconomics, 4/ Olivir Blanchard 14-1 Today s Lcur Chapr 14:Expcaions: Th Basic Th
More informationELASTO-PLASTIC ANALYSIS OF STRUCTURES USING HEXAHEDRICAL ELEMENTS WITH EIGHT NODES AND ONE-POINT QUADRATURE
Mcánica Compuacional Vol XXV, pp. 86-878 Albro Cardona, Norbro Nigro, Vicorio Sonzogni, Mario Sori. (Eds.) Sana F, Argnina, Novimbr 26 ELASTO-PLASTIC ANALYSIS OF STRUCTURES USING HEXAHEDRICAL ELEMENTS
More informationModelling of three dimensional liquid steel flow in continuous casting process
AMME 2003 12h Modlling of hr dimnsional liquid sl flow in coninuous casing procss M. Jani, H. Dyja, G. Banasz, S. Brsi Insiu of Modlling and Auomaion of Plasic Woring Procsss, Faculy of Marial procssing
More informationModeling and Experimental Investigation on the Internal Leakage in a CO2 Rotary Vane Expander
urdu Univrsiy urdu -ubs Inrnaional Comprssor Enginring Confrnc School of chanical Enginring 2008 odling and Exprimnal Invsigaion on h Inrnal Lakag in a CO2 Roary Van Expandr Bingchun Yang Xi an Jiaoong
More informationEconomics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 3/28/2012. UW Madison
Economics 302 (Sc. 001) Inrmdia Macroconomic Thory and Policy (Spring 2011) 3/28/2012 Insrucor: Prof. Mnzi Chinn Insrucor: Prof. Mnzi Chinn UW Madison 16 1 Consumpion Th Vry Forsighd dconsumr A vry forsighd
More informationEE 434 Lecture 22. Bipolar Device Models
EE 434 Lcur 22 Bipolar Dvic Modls Quiz 14 Th collcor currn of a BJT was masurd o b 20mA and h bas currn masurd o b 0.1mA. Wha is h fficincy of injcion of lcrons coming from h mir o h collcor? 1 And h numbr
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More information7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS *
Andri Tokmakoff, MIT Dparmn of Chmisry, 5/19/5 7-11 7.4 QUANTUM MECANICAL TREATMENT OF FLUCTUATIONS * Inroducion and Prviw Now h origin of frquncy flucuaions is inracions of our molcul (or mor approprialy
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationA STUDY OF MINDLIN PLATE FINITE ELEMENTS
Th 4h Inrnaional Confrnc Copaional Mchanics and Viral Enginring COMEC - OCTOBER Brasov Roania A STUY OF MINLIN LATE FINITE ELEMENTS Ada osa Hadan Ahd Af Alqaain Univrsi TRANSILVANIA Brasov ROMANIA adadosa@ahooco
More informationa dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:
Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.
More informationGENERALIZATION OF NON-ITERATIVE NUMERICAL METHODS FOR DAMAGE-PLASTIC BEHAVIOUR MODELING
VIII Inrnaional Confrnc on Fracur Mchanics of Concr and Concr Srucurs FraMCoS-8 J.G.M. Van Mir, G. Ruiz, C. ndrad, R.C. Yu and X.X. Zhang (Eds) GENERLIZTIN F NN-ITERTIVE NUMERICL METHDS FR DMGE-PLSTIC
More information3.9 Carbon Contamination & Fractionation
3.9 arbon onaminaion & Fracionaion Bcaus h raio / in a sampl dcrass wih incrasing ag - du o h coninuous dcay of - a small addd impuriy of modrn naural carbon causs a disproporionaly larg shif in ag. (
More informationME311 Machine Design
ME311 Machin Dsign Lctur 4: Strss Concntrations; Static Failur W Dornfld 8Sp017 Fairfild Univrsit School of Enginring Strss Concntration W saw that in a curvd bam, th strss was distortd from th uniform
More informationChapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System
EE 422G No: Chapr 5 Inrucor: Chung Chapr 5 Th Laplac Tranform 5- Inroducion () Sym analyi inpu oupu Dynamic Sym Linar Dynamic ym: A procor which proc h inpu ignal o produc h oupu dy ( n) ( n dy ( n) +
More informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationChapter 4 Longitudinal static stability and control Effect of acceleration (Lecture 15)
Chapr 4 Longiudinal saic sabiliy and conrol Effc of acclraion (Lcur 15) Kywords : Elvaor rquird in pull-up; sick-fixd manuvr poin; sick forc gradin in pull-up; manuvr poin sick-fr; ovrall limis on c.g.
More informationCOMPUTATIONAL VISCOELASTICITY OF AGING MATERIALS
ECCM 99 Europan Confrnc on Compuaional Mchanics Augus 31 Spmbr 3 Münchn, Grmany COMPUTATIONAL VISCOELASTICITY OF AGING MATERIALS B. Eirl and K. Schikora Insiu für Saik, Baumchanik und Bauinformaik Tchnisch
More informationFeedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System *
ISSN 746-7659 England UK Jornal of Informaion and Comping Scinc Vol. No. 6 pp. 9- Fdbac Conrol and Snchroniaion of Chaos for h Copld Dnamos Dnamical Ssm * Xdi Wang Liin Tian Shmin Jiang Liqin Y Nonlinar
More informationComputational prediction of high ZT of n-type Mg 3 Sb 2 - based compounds with isotropic thermoelectric conduction performance
Elcronic Supplnary Marial (ES for Physical Chisry Chical Physics. This journal is h Ownr Sociis 08 Supporing nforaion Copuaional prdicion of high ZT of n-yp Mg 3 Sb - basd copounds wih isoropic hrolcric
More information46. Let y = ln r. Then dy = dr, and so. = [ sin (ln r) cos (ln r)
98 Scion 7.. L w. Thn dw d, so d dw w dw. sin d (sin w)( wdw) w sin w dw L u w dv sin w dw du dw v cos w w sin w dw w cos w + cos w dw w cos w+ sin w+ sin d wsin wdw w cos w+ sin w+ cos + sin +. L w +
More informationChemistry 988 Part 1
Chmisry 988 Par 1 Radiaion Dcion & Masurmn Dp. of Chmisry --- Michigan Sa Univ. aional Suprconducing Cycloron Lab DJMorrissy Spring/2oo9 Cours informaion can b found on h wbsi: hp://www.chmisry.msu.du/courss/cm988uclar/indx.hml
More informationStability of an ideal (flat) plate. = k. critical stresses σ* (or N*) take the. Thereof infinitely many solutions: Critical stresses are given as:
. Buckling of plaes Linear and nonlinear heor of uckling, uckling under direc sresses (class secions), uckling under shear, local loading and Eurocode approach. Saili of an ideal (fla) plae various loading
More informationPROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS
Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra
More information1 Isoparametric Concept
UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric
More informationMidterm exam 2, April 7, 2009 (solutions)
Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions
More informationCopyright 2012 Pearson Education, Inc. Publishing as Prentice Hall.
Chapr Rviw 0 6. ( a a ln a. This will qual a if an onl if ln a, or a. + k an (ln + c. Thrfor, a an valu of, whr h wo curvs inrsc, h wo angn lins will b prpnicular. 6. (a Sinc h lin passs hrough h origin
More informationINVESTIGATION ON APPLICABILITY OF SUBSTITUTE BEAM - COLUMN FRAME FOR DESIGN OF REINFORCED CONCRETE SWAY FRAMES
INVESTIGATION ON APPLICABILITY OF SUBSTITUTE BEAM - COLUMN FRAME FOR DESIGN OF REINFORCED CONCRETE SWAY FRAMES Abrham Ewnti and *Girma Zrayohanns School of Civil and Environmntal Enginring, Addis Ababa
More informationUnfired pressure vessels- Part 3: Design
Unfird prssur vssls- Part 3: Dsign Analysis prformd by: Analysis prformd by: Analysis vrsion: According to procdur: Calculation cas: Unfird prssur vssls EDMS Rfrnc: EF EN 13445-3 V1 Introduction: This
More informationHomotopy perturbation technique
Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,
More informationMECHANICS OF MATERIALS Poisson s Ratio
Poisson s Raio For a slender bar subjeced o axial loading: ε x x y 0 The elongaion in he x-direcion i is accompanied by a conracion in he oher direcions. Assuming ha he maerial is isoropic (no direcional
More informationS.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]
S.Y. B.Sc. (IT) : Sm. III Applid Mahmaics Tim : ½ Hrs.] Prlim Qusion Papr Soluion [Marks : 75 Q. Amp h following (an THREE) 3 6 Q.(a) Rduc h mari o normal form and find is rank whr A 3 3 5 3 3 3 6 Ans.:
More information14.02 Principles of Macroeconomics Fall 2005 Quiz 3 Solutions
4.0 rincipl of Macroconomic Fall 005 Quiz 3 Soluion Shor Quion (30/00 poin la a whhr h following amn ar TRUE or FALSE wih a hor xplanaion (3 or 4 lin. Each quion coun 5/00 poin.. An incra in ax oday alway
More informationA Condition for Stability in an SIR Age Structured Disease Model with Decreasing Survival Rate
A Condiion for abiliy in an I Ag rucurd Disas Modl wih Dcrasing urvival a A.K. upriana, Edy owono Dparmn of Mahmaics, Univrsias Padjadjaran, km Bandung-umng 45363, Indonsia fax: 6--7794696, mail: asupria@yahoo.com.au;
More informationDecline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.
Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.
More informationLagrangian for RLC circuits using analogy with the classical mechanics concepts
Lagrangian for RLC circuis using analogy wih h classical mchanics concps Albrus Hariwangsa Panuluh and Asan Damanik Dparmn of Physics Educaion, Sanaa Dharma Univrsiy Kampus III USD Paingan, Maguwoharjo,
More informationREPETITION before the exam PART 2, Transform Methods. Laplace transforms: τ dτ. L1. Derive the formulas : L2. Find the Laplace transform F(s) if.
Tranform Mhod and Calculu of Svral Variabl H7, p Lcurr: Armin Halilovic KTH, Campu Haning E-mail: armin@dkh, wwwdkh/armin REPETITION bfor h am PART, Tranform Mhod Laplac ranform: L Driv h formula : a L[
More informationTHE SHORT-RUN AGGREGATE SUPPLY CURVE WITH A POSITIVE SLOPE. Based on EXPECTATIONS: Lecture. t t t t
THE SHORT-RUN AGGREGATE SUL CURVE WITH A OSITIVE SLOE. Basd on EXECTATIONS: Lcur., 0. In Mankiw:, 0 Ths quaions sa ha oupu dvias from is naural ra whn h pric lvl dvias from h xpcd pric lvl. Th paramr a
More informationSOLUTIONS. 1. Consider two continuous random variables X and Y with joint p.d.f. f ( x, y ) = = = 15. Stepanov Dalpiaz
STAT UIUC Pracic Problms #7 SOLUTIONS Spanov Dalpiaz Th following ar a numbr of pracic problms ha ma b hlpful for compling h homwor, and will lil b vr usful for suding for ams.. Considr wo coninuous random
More informationEffect of sampling on frequency domain analysis
LIGO-T666--R Ec sampling n rquncy dmain analysis David P. Nrwd W rviw h wll-knwn cs digial sampling n h rquncy dmain analysis an analg signal, wih mphasis n h cs upn ur masurmns. This discussin llws h
More informationLecture 4: Laplace Transforms
Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions
More informationGeneral Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract
Applicaion of Diffrnial... Gnral Aricl Applicaion of diffrnial uaion in - and C- circui analysis by classical mhod. ajndra Prasad gmi curr, Dparmn of Mahmaics, P.N. Campus, Pokhara Email: rajndraprasadrgmi@yahoo.com
More information