Towards a probabilistic concept of the Kitagawa-Takahashi diagram
|
|
- Arleen Manning
- 5 years ago
- Views:
Transcription
1 Tords probbilistic concept of the Kitg-Tkhshi digr Alfonso Fernández-Cnteli 1, Roberto Brighenti, Enrique Cstillo 3 1 Dept. of Construction nd Mnufcturing Engineering, University of Oviedo, Cpus de Viesques, 333 Gijón, Spin fc@uniovi.es Dept. of Civil-Environentl Engineering nd Architecture, University of Pr, Vile G.P. Usberti 181/A, 431 Pr, Itly brigh@unipr.it 3 Dept. of Applied Mthetics nd Coputtionl Sciences, University of Cntbri, Avd de los Cstros s/n, 395 Sntnder, Spin cstie@unicn.es ABSTRACT. The Kitg-Tkhshi (K-T digr, ipleented by the El Hddd eqution, reltes the conventionl ftigue liit to the crck size, enbling boundry for the cyclic stress rnge to be estblished, belo hich n infinite life of the structurl coponent y be, theoreticlly, ensured for ny crck size due to the non-propgtion of icro- nd crocrcks. In order to ccount for the inherent rndo chrcter of the ftigue phenoenon in rel terils nd the need of extending the K-T pplicbility to ny prefixed nuber of cycles, dvnced probbilistic S- odels should be considered to define the ftigue liit. In this y, ne bsis tords probbilistic Kitg-Tkhshi-El Hddd pproch is provided in greeent ith the syptotic tching proposed by Civrell-Monno. ITRODUCTIO AD MOTIVATIO The Kitg-Tkhshi (KT digr [1] represents boundry in ters of crck size nd stress rnge for hich infinite ftigue lifetie of structurl or echnicl coponents cn be sfely ensured due to non-propgting icro- nd crocrcks. Such ftigue life ssessent cn be relted to both the clssicl ftigue liit concept, resulting fro the experientl-bsed S- pproch, nd the threshold stress intensity fctor rnge, s defined by the crck propgtion l. Even fter the trnscendent iproveent provided by the intrinsic crck concept of El Hddd (EH [], to issues need to be delt ith: the extension of the KT-EH digr to ftigue liit for finite nuber of cycles, hich is not necessrily identified ith the endurnce liit for, nd b stochstic definition of the KT-EH digr s consequence of the vribility of the bsic ftigue functions being considered (S- nd crck groth rte curves. Both represent prcticl requireents relted to structurl integrity design. In this ork, ne pproch to the proble is supplied by considering the probbilistic S- developed by Cstillo nd Fernández-Cnteli [3], hich provides sound bsis in the definition of the KT-EH line, peritting lso the odel to be 141
2 extended fro infinite to ny finite life, s lredy proposed by Civrell nd Monno [4], hich provide n interesting lterntive to solve the first issue, heres the liittions of the siplistic S- field used, bsed on truncted Bsquin pproch ith bsence of probbilistic considertions, evidence the need of further enhnceent. Thus, the boundry beteen frcture nd non-frcture cn be optionlly referred to finite nuber of cycles for certin probbility of filure, becuse in the engineering prctice high, but finite, nuber of cycles, rther thn infinity, re usully ssued for ftigue life. PROBABIISTIC COCEPTS APPIED TO THE K-T APPROACH In this ork, only vribility of the S- field is considered, hile deterinistic concept of the crck groth rte curve is for the present ssued [5] s first ttept of introducing probbilistic considertions in the definition of the KT-EH digr. Figure 1. S- field ith percentile curves ccording to the regression odel[3]. The proposed probbilistic odel. According to the probbilistic regression odel proposed by Cstillo nd Fernández- Cnteli [3] the ftigue life given stress rnge, nd the stress rnge given lifetie re rndo vribles folloing Weibull distribution (Fig. 1: β (log B(log C λ p 1 exp δ, (1 here p is the probbility of filure, the lifetie in cycles, Δ σ the pplied stress rnge, B represents the threshold vlue of the lifetie nd C the endurnce liit, or ftigue liit for, nd β, δ nd λ re, respectively, the shpe, scle nd loction Weibull preters. As soon s the five preters re estited, the odel provides coplete nlyticl description of the probbilistic S- field being delt ith. The percentile curves re hyperbols shring the syptotes log B nd log C (see Fig. 1, the zero percentile curve represents the iniu possible required nuber of 14
3 cycles to chieve filure for different vlues of log. The percentile curves cn be interpreted s representing different initil fl sizes. Since the odel extends the Wöhler field up to n unliited nuber of cycles, n extrpoltion of the lifetie is possible outside the rnge of nuber of cycles tested in the experientl progr. The in liittion of the odel, consisting in the bsence of n upper bound in the CF region, y be overcoe by considering ne ftigue vrible, Δ σ ε x, s the reference preter controlling the ftigue process in the previous odel. Once the odel preters in ters of Δ σ ε x hve been estited, the S- field y be reconverted to the conventionl Δ σ vrible using the stress-strin cyclic digr of the teril, for instnce s Rberg-Osgood (R-O curve. K-T digr for finite nuber of cycles to filure Unless otherise specified, the S- curves re generlly relted to unique probbility of filure, p.5 or p.5, though the sctter of experientl dt requires the definition of the hole S- field s percentile curves bsed on sttisticl principles. The ftigue behviour of structurl coponent is inly governed by its surfce (or volue stte qulity, iplying roughness nd iperfections tht re preferentil sites for crck nucletion nd subsequent propgtion. According to [3], the percentile curves cn be ssued to be ssocited ith the probbility of the existence of crck being less thn certin initil crck size, i, initilly unknon. Consequently, the ftigue filure is governed by the xiu crck size present in the specien being tested so tht percentile curves ith incresing probbilities of filure re relted to diinishing crck sizes: the percentile curve p, corresponding to the gretest, or orst, of the xiu crck sizes of the popultion, i.e., i, x( x, hich is denoted xx crck size (Fig.. Siilrly, the upper percentile curve, p1, corresponds to the iniu, or best, of the xiu crck sizes of the popultion, i.e., i, b in( x, hich is denoted in-x crck size. For prcticl purposes, the definition of the ltter cn be relxed identifying, s n initil crck size relted to high probbility of i b filure, for instnce, p b.9 or.95. The to curves ssocited ith i, nd i,b represent the to liiting sizes of the initil xiu defect corresponding to the prticulr surfce finishing of the tested teril. According to [3], i,, relted to the percentile curve p, is deterined s here ΔKth 1 ΔK is the threshold SIF rnge, Y the geoetric fctor of the crck nd ( the endurnce liit. For given nuber of cycles to filure Δ σ b nd Δ σ ( Δ σ b > respectively. Consequently, for th i, π Y (, (, see Fig., to different stress rnges, re identified ith the best nd orst surfce defects s reference lifetie, n engineering SIF 143
4 threshold Δ K th, eng cn be found, prticulrly for the defect sizes i, nd i,b, but lso for ny crck size i, ( i, > i, > i,b, to be given by Δ Kth, eng, Y π i,, (3 here the stress rnge Δ σ results fro the percentile curve corresponding to (see Fig.. For, the Δ K th, eng becoes the true threshold vlue Δ Kth of the crck groth rte curve. ( ( ( Figure. Probbilistic concept pplied to n experientl S- curve for given teril. ote tht, ccording to El Hddd [], the intrinsic crck size is given s: 1 ΔK th, (4 π Y here Δ σ represents in this cse the ftigue liit for nuber of cycles, pointing out tht only for the intrinsic initil crck size coincides ith the orst crck size i,. Applying the El Hddd eqution to the evlution of testing sples ith vrying surfce sttes, i.e. intrinsic crck sizes, ould provide different ftigue liits Δ σ, i.e., unlike KT digrs, evidencing dependency ith respect to the prticulr surfce stte tested, thus, proving tht such KT digrs re not teril chrcteristic. On the contrry, unique KT digr is expected fro the proposed pproch despite the different endurnce liits, ssocited ith the orst crck sizes, obtined for the respective surfce sttes. The ssuption of deterinistic crck groth rte curve iplies deterinistic reltion beteen crck size nd nuber of cycles to filure ening tht the KT-EH digr is deterinistic too [5]. Accordingly, the sctter of the experientl dt re only relted to the initil surfce stte of the teril, iplying siply uncertinties relted to esureent precision or to teril heterogeneity. For certin initil crck size i,, the filure condition, K f K Ic, resulting for given nuber of cycles to filure,, is equivlent to 144
5 Δ K( Y π ( ΔK lloing us to express the finl crck size rtio, f f,, / s: f Ic f, > 1. (5 f, Assuing constnt geoetry fctor Y during the crck propgtion, the current crck size rtio r ( ( r (6 reins constnt long the hole propgtion process (see Fig. 3(b, in prticulr, fro the beginning of the ftigue process, i.e., for the initil crck sizes i, nd i,, up to the finl filure stte, proving tht on logrithic scle, the verticl distnce clog r beteen the curves relted to i, nd i, reins constnt ll long the propgtion process (see Fig. 3(b. ( (b Figure 3. Crck groth curves for the best nd orst initil defect cses for given teril ( plotted in nturl scle, nd (b plotted in logrithic scle. While the initil orst crck size i,, relted to p, is deterined fro Eq. (, nother crck size, i,, relted to given probbility p (prticulrly the best one i, b relted to p1, reining, in principle, unknon cn be obtined by integrtion of the crck groth rte l, d / d G( ΔK, due to its uniqueness, for generic nuber of cycles to filure, i.e.: f, d d f, f, ( i,,, G( ΔK(. (7 i, Since Eq. (6 pplies irrespective of the nuber of cycles considered, the bove quntities cn be used to rite syste of to equtions: 145
6 ( ( i,,, i,,, r nd f, f, f, f, ( ( i, i,,, r,, ith r ( /, the solution of hich provides the quntities i, nd i, tht cn be finlly ssocited ith the orst nd generic surfce stte of the teril, respectively. (8 APPICATIOS OF THE EXTEDED K-T DIAGRAM TO STEE 145 In order to deonstrte its utility for ftigue life ssessent of echnicl nd structurl coponents, the bove proposed pproch is pplied to the stndrd crbon steel 145 tking into ccount the echnicl nd ftigue properties s reported in Tble 1 [6]. Steel 145 Cheicl coposition Crbon Iron Mngnese Phosphorus Sulphur Blnce x.5 x Mechnicl properties E (GP σ y (MP σ u (MP K n E Ftigue properties Δ σ (MP ( K fc K th C (/cycle E-4 8 MP 7.1 MP 8.E Tble 1. Min cheicl, echnicl nd ftigue properties of the crbon steel 145 (fro [6]. In the present cse, rther thn using the probbilistic odel proposed by [3], the S- field is defined by deterining the percentile curves corresponding, respectively, to the probbilities of filure p nd p.9, fro the results of previous testing progr crried out for three different ftigue stress rnges ( 3, 4, 5 MP, s illustrted in Fig. 4. The quntities orst x( x nd best in( x re deterined ccording to 5 Eq. (6 by considering filure conditions relted to 1 cycles, heres, r ( b / (455/ (Fig. 4 or, equivlently, c ln r By dopting the crck groth rte l by Donhue et l. [7], expressed by: d G( ΔK C ( Y π ΔK th (9 d F ( the crck groth l ( e is ssessed nd used to get the expressions to be inserted into the syste given by Eqs (8. Since this syste of equtions is not esily solvble by nlyticl or nuericl stndrd techniques, it hs been tckled by using genetic lgorith (GA [8-9]. 146
7 Stress plitude, (MP E+1 1E+ 1E+3 p % p9% lo-cycle ft. energy pproch bsed on R-O odel 1E+4 1E+5 1E+6 Steel 145 1E+7 1E+8 1E+9 uber of cycles, Figure 4. S- curves corresponding to the p nd p.9 for the steel 145. b σy38 MP The ethod opertes by selecting, long the itertion process, the best solution ong different possibilities, trying to fulfil s better s possible the required vlue of the objective function, here identified s the knon rtio r ( / Δ b σ 1.79 for both the initil nd the finl crck sizes. After short nuber of itertions, the sought vlues for i, b nd i, re obtined. The GA process produces stble result for the to bove quntities, -4 nely, nd i b -4 i, , irrespectively of the stress rnge nd the finl nuber of cycles Stress plitude, (MP 1/ 1 1 dopted (see Eq.(8. σ 75 MP 1.E-4 1K 5K M 1M i,b i, ( 1.E-3 i ( Initil crck size, i ( Figure 5. Kitg-Tkhshi digr for the steel 145 for different vlues of cycles to filure ( ith probbility distribution relted to the finishing surfce stte (b. Finlly, the generlised Kitg-Tkhshi digr hs been obtined by integrting the Donhue eqution strting fro the initil crck size up to the fulfilent of the criticl condition ( Δ K I ( i, ΔK Ic for given nuber of cycles to filure; the initil crck size i hs been ssued to be siply uniforly distributed in the intervl i, b - i,. As cn be observed in Fig. 5, the initil crck size to be p( i 1 i,b (b i, 147
8 considered in the KT digr corresponds to the probbility of filure ssued, this being dependent on the finishing surfce stte. COCUSIOS The in conclusions to be drn fro the present study re the folloing: - A probbilistic concept is proposed for being ipleented in the Kitg- Tkhshi-El Hddd digr iing t providing higher relibility in prcticl design cses. - The pproch llos us to estblish connection beteen the probbilistic S- field nd the crck groth rte curve, the ltter being ssued for the present to be deterinistic. - The pproch cn be pplied indistinctly either for n infinite or finite liit nuber of cycles. - Further study is needed to llo n extension of the proposed pproch to define the KT digr for sll crcks. i.e., in the CF region, s ell s the considertion of stochstic crck groth rte curves, prticulrly in the threshold regie. ACKOWEGEDMETS The uthors cknoledge prtil support supplied by the Spnish Ministry of Science nd Innovtion MICI (Ref: BIA1-199 nd the Itlin Ministry for University nd Technologicl nd Scientific Reserch (MIUR. REFERECES [1] Kitg, H., Tkhshi, S. (1976 Proc. of the nd Int. Conf on Mech. Behviour of Mterils., ASM, [] El Hddd, M., Topper, T., Sith, K. (1979 Eng. Frct. Mech. 11, [3] Cstillo, E., Fernández-Cnteli, A. (1 Int. J. Frct. 17, [4] Civrell, M., Monno, F. (6 Int. J. Ft., 8, [5] Fernández-Cnteli A., Cstillo, E., Siegele, D. (1 18th Europen Conference on Frcture, ECF18, Dresden. [6] Mteril Reference. A Copendiu of Ftigue Thresholds nd Groth Rtes, EMAS, [7] Donhue, R.J., Clrk H.M., Atno P., et l. (197 Int J Frct Mech. 8, [8] Goldberg, D.E. (1989, Genetic lgoriths in serch, optiiztion, nd chine lerning. MA, Addison-Wesley Publishing Copny Inc. [9] Brighenti, R., Crpinteri, A., Vntdori, S. (6 Cop. Meth. App. Mech. nd Engng. 196,
Influence of Mean Stress
Influence of Men tress Discussion hs been liited to copletely reversible stress thus fr. Mening = 0 However, there re ny instnces of dynic loding when en stress is nonzero. Men tresses Incresing en stress
More informationUNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY
UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY YIFEI PAN, MEI WANG, AND YU YAN ABSTRACT We estblish soe uniqueness results ner 0 for ordinry differentil equtions of the
More informationStrength of materials II- Fatigue failure
Ftigue filure is one of the so clled cuultive liit sttes. In opposite to instntneous liit sttes, the cuultive ones re hereditry, they depend not only on the instntneous loding (stress-strin) stte of the
More informationNONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS
18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS NONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS T. Prk 1, M. Ki 1, B. Jng 1, J. Lee 2, J. Prk 3 * 1 Grdute School,
More informationUNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY
UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY YIFEI PAN, MEI WANG, AND YU YAN ABSTRACT We study ordinry differentil equtions of the type u n t = fut with initil conditions
More informationContact Analysis on Large Negative Clearance Four-point Contact Ball Bearing
Avilble online t www.sciencedirect.co rocedi ngineering 7 0 74 78 The Second SR Conference on ngineering Modelling nd Siultion CMS 0 Contct Anlysis on Lrge Negtive Clernce Four-point Contct Bll Bering
More informationAN EXPERIMENTAL INVESTIGATION OF PENETRATION FAILURE MODES IN COMPOSITE LAMINATES
16 TH INTRNATIONAL CONFRNC ON COMPOSIT MATRIALS AN XPRIMNTAL INVSTIGATION OF PNTRATION FAILUR MODS IN COMPOSIT LAMINATS Guiping Zho*, Zhengho Wng**, Jinxin Zhng**, Chongdu Cho*** *MO Key Lbortory for Strength
More informationECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model
ECONOMETRIC THEORY MODULE IV Lecture - 16 Predictions in Liner Regression Model Dr. Shlbh Deprtent of Mthetics nd Sttistics Indin Institute of Technology Knpur Prediction of vlues of study vrible An iportnt
More informationReview of Calculus, cont d
Jim Lmbers MAT 460 Fll Semester 2009-10 Lecture 3 Notes These notes correspond to Section 1.1 in the text. Review of Clculus, cont d Riemnn Sums nd the Definite Integrl There re mny cses in which some
More informationMaterials 337. Lecture 7. Topics covered Introduction to fracture mechanics The elastic stress field Superposition principle Fracture toughness
Mterils 337 Lecture 7 Topics covered Introduction to frcture mechnics The elstic stress field Superposition principle Frcture toughness Deprtment of Mechnicl Engineering Curtin University of Technology
More informationV E L O C I T Y a n d V E L O C I T Y P R E S S U R E I n A I R S Y S T E M S
V E L O C I T Y n d V E L O C I T Y R E S S U R E I n A I R S Y S T E M S A nlysis of fluid systes using ir re usully done voluetric bsis so the pressure version of the Bernoulli eqution is used. This
More informationOXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved.
Renshw: Mths for Econoics nswers to dditionl exercises Exercise.. Given: nd B 5 Find: () + B + B 7 8 (b) (c) (d) (e) B B B + B T B (where 8 B 6 B 6 8 B + B T denotes the trnspose of ) T 8 B 5 (f) (g) B
More informationENSC 461 Tutorial, Week#9 Non-Reacting Mixtures Psychrometrics Applied to a Cooling Tower
ENSC 61 Tutoril, Week#9 Non-Recting Mixtures Psychroetrics Applied to Cooling Toer Wter exiting the condenser of poer plnt t 5C enters cooling toer ith ss flo rte of 15000 kg/s. A stre of cooled ter is
More information99/105 Comparison of OrcaFlex with standard theoretical results
99/105 Comprison of OrcFlex ith stndrd theoreticl results 1. Introduction A number of stndrd theoreticl results from literture cn be modelled in OrcFlex. Such cses re, by virtue of being theoreticlly solvble,
More informationProbabilistic Fatigue Life Prediction Method for Notched Specimens Based on the Weakest-link theory
213 2 32 2 Mechnicl Science nd Technology for erospce Engineering Februry Vol. 32 213 o. 2 2116 Weibull Weibull Weibull - Weibull TC4 5% 1% 9% Weibull O346. 3 13-8728 213 2-164-6 Probbilistic Ftigue Life
More informationAN ORIGINAL METHOD FOR URBAN TRAFFIC NOISE PREDICTION
AN ORIGINA METHOD FOR URBAN TRAFFIC NOISE REDICTION Federico Rossi 1, Uberto Di Mtteo, Sofi Sioni 3 1 University of erugi Industril Engineering Deprtent oc. enti Bss 1, 05100, Terni, Itly frossi@unipg.it
More informationProject A: Active Vibration Suppression of Lumped-Parameters Systems using Piezoelectric Inertial Actuators *
Project A: Active Vibrtion Suppression of Luped-Preters Systes using Piezoelectric Inertil Actutors * A dynic vibrtion bsorber referred to s ctive resontor bsorber (ARA) is considered here, while exploring
More informationME 354 Tutorial, Week#11 Non-Reacting Mixtures Psychrometrics Applied to a Cooling Tower
ME 5 Tutoril, Week# Non-Recting Mixtures Psychroetrics Applied to Cooling Toer Wter exiting the condenser of poer plnt t 5 C enters cooling toer ith ss flo rte of 5000 kg/s. A stre of cooled ter is returned
More informationImproper Integrals. Type I Improper Integrals How do we evaluate an integral such as
Improper Integrls Two different types of integrls cn qulify s improper. The first type of improper integrl (which we will refer to s Type I) involves evluting n integrl over n infinite region. In the grph
More informationFamilies of Solutions to Bernoulli ODEs
In the fmily of solutions to the differentil eqution y ry dx + = it is shown tht vrition of the initil condition y( 0 = cuses horizontl shift in the solution curve y = f ( x, rther thn the verticl shift
More informationThe International Association for the Properties of Water and Steam. Release on the Ionization Constant of H 2 O
IAPWS R-7 The Interntionl Assocition for the Properties of Wter nd Stem Lucerne, Sitzerlnd August 7 Relese on the Ioniztion Constnt of H O 7 The Interntionl Assocition for the Properties of Wter nd Stem
More informationReview of basic calculus
Review of bsic clculus This brief review reclls some of the most importnt concepts, definitions, nd theorems from bsic clculus. It is not intended to tech bsic clculus from scrtch. If ny of the items below
More informationUNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction
Lesson : Logrithmic Functions s Inverses Prerequisite Skills This lesson requires the use of the following skills: determining the dependent nd independent vribles in n exponentil function bsed on dt from
More informationJob No. Sheet 1 of 8 Rev B. Made by IR Date Aug Checked by FH/NB Date Oct Revised by MEB Date April 2006
Job o. Sheet 1 of 8 Rev B 10, Route de Limours -78471 St Rémy Lès Chevreuse Cedex rnce Tel : 33 (0)1 30 85 5 00 x : 33 (0)1 30 5 75 38 CLCULTO SHEET Stinless Steel Vloristion Project Design Exmple 5 Welded
More informationEffects of peripheral drilling moment on delamination using special drill bits
journl of mterils processing technology 01 (008 471 476 journl homepge: www.elsevier.com/locte/jmtprotec Effects of peripherl illing moment on delmintion using specil ill bits C.C. Tso,, H. Hocheng b Deprtment
More informationPHY 5246: Theoretical Dynamics, Fall Assignment # 5, Solutions. θ = l mr 2 = l
PHY 546: Theoreticl Dynics, Fll 15 Assignent # 5, Solutions 1 Grded Probles Proble 1 (1.) Using the eqution of the orbit or force lw d ( 1 dθ r)+ 1 r = r F(r), (1) l with r(θ) = ke αθ one finds fro which
More informationChapter 3 The Schrödinger Equation and a Particle in a Box
Chpter 3 The Schrödinger Eqution nd Prticle in Bo Bckground: We re finlly ble to introduce the Schrödinger eqution nd the first quntum mechnicl model prticle in bo. This eqution is the bsis of quntum mechnics
More informationEffects of Micro-polar Fluids and the Tsann Roughness Model on Performance Characteristics of Two-lobe Bearings
Vol- Issue- 6 IJARIIE-ISSN(O)-95-96 Effects of Micro-polr Fluids nd the Tsnn Roughness Model on Perfornce Chrcteristics of Two-lobe Berings Rohollh Shfei, Mohd Hdi Shfei Mr., Engineering Deprtent, Yd University,
More informationSome History. Over the Next Several Days. Three Stages of Fatigue Failure. Identifying Fatigue Fractures. Three Approaches. Low vs.
Over the Next everl Dys Wht is Ftigue? Epiricl Dt Estiting Endurnce/Ftigue trength trtegies for Anlysis oe History Ril The cr xles ll-iportnt icrocrck Role of stress concentns ¾oet irplnes ¾ Unixil Fully
More informationPHYS 601 HW3 Solution
3.1 Norl force using Lgrnge ultiplier Using the center of the hoop s origin, we will describe the position of the prticle with conventionl polr coordintes. The Lgrngin is therefore L = 1 2 ṙ2 + 1 2 r2
More informationJim Lambers MAT 169 Fall Semester Lecture 4 Notes
Jim Lmbers MAT 169 Fll Semester 2009-10 Lecture 4 Notes These notes correspond to Section 8.2 in the text. Series Wht is Series? An infinte series, usully referred to simply s series, is n sum of ll of
More informationPhysics 116C Solution of inhomogeneous ordinary differential equations using Green s functions
Physics 6C Solution of inhomogeneous ordinry differentil equtions using Green s functions Peter Young November 5, 29 Homogeneous Equtions We hve studied, especilly in long HW problem, second order liner
More informationINVESTIGATION OF THERMAL PROPERTIES OF SOIL BY IMPULSE METHOD Juraj Veselský
THERMOPHYSICS 6 October 6 5 INVESTIGATION OF THERMAL PROPERTIES OF SOIL BY IMPULSE METHOD Jurj Veselský Fculty of Civil Engineering STU Brtislv, Rdlinského, 8 68 Brtislv Abstrct The therl properties of
More information7-1: Zero and Negative Exponents
7-: Zero nd Negtive Exponents Objective: To siplify expressions involving zero nd negtive exponents Wr Up:.. ( ).. 7.. Investigting Zero nd Negtive Exponents: Coplete the tble. Write non-integers s frctions
More informationTime Truncated Two Stage Group Sampling Plan For Various Distributions
Time Truncted Two Stge Group Smpling Pln For Vrious Distributions Dr. A. R. Sudmni Rmswmy, S.Jysri Associte Professor, Deprtment of Mthemtics, Avinshilingm University, Coimbtore Assistnt professor, Deprtment
More information1.2. Linear Variable Coefficient Equations. y + b "! = a y + b " Remark: The case b = 0 and a non-constant can be solved with the same idea as above.
1 12 Liner Vrible Coefficient Equtions Section Objective(s): Review: Constnt Coefficient Equtions Solving Vrible Coefficient Equtions The Integrting Fctor Method The Bernoulli Eqution 121 Review: Constnt
More informationON THE THEORETICAL FRACTURE STATISTICS OF THE HERTZ INDENTATION TEST
ON THE THEORETICA FRACTURE STATISTICS OF THE HERTZ INDENTATION TEST Gerrdo Díz R. () nd Pblo Kittl D. () () Deprtento de Cienci de los Mteriles, Fcultd de Ciencis Físics y Mteátics, Universidd de Chile,
More informationEFFECTIVE BUCKLING LENGTH OF COLUMNS IN SWAY FRAMEWORKS: COMPARISONS
IV EFFETIVE BUING ENGTH OF OUMN IN WAY FRAMEWOR: OMARION Ojectives In the present context, two different pproches re eployed to deterine the vlue the effective uckling length eff n c of colun n c out the
More informationSteady Sate Analysis of Self-Excited Induction Generator using Phasor-Diagram Based Iterative Model
WSS TNSTIONS on POW SYSTMS Knwrjit Singh Sndhu, Dheerj Joshi Stedy Ste nlysis of Self-xcited Induction Genertor using Phsor-Digr Bsed Itertive Model KNWJIT SINGH SNDHU & DHJ JOSHI Deprtent of lectricl
More informationVyacheslav Telnin. Search for New Numbers.
Vycheslv Telnin Serch for New Numbers. 1 CHAPTER I 2 I.1 Introduction. In 1984, in the first issue for tht yer of the Science nd Life mgzine, I red the rticle "Non-Stndrd Anlysis" by V. Uspensky, in which
More informationr = cos θ + 1. dt ) dt. (1)
MTHE 7 Proble Set 5 Solutions (A Crdioid). Let C be the closed curve in R whose polr coordintes (r, θ) stisfy () Sketch the curve C. r = cos θ +. (b) Find pretriztion t (r(t), θ(t)), t [, b], of C in polr
More informationGreen s Function Technique and Global Optimization in Reconstruction of Elliptic Objects in the Regular Triangle
Applied Mthetics,,, 94-3 doi:.436/..334 Published Online Mrch (http://www.scirp.org/journl/) Green s Function Technique nd Globl Optiiztion in Reconstruction of Elliptic Objects in the Regulr Tringle Abstrct
More informationTHIELE CENTRE. Linear stochastic differential equations with anticipating initial conditions
THIELE CENTRE for pplied mthemtics in nturl science Liner stochstic differentil equtions with nticipting initil conditions Nrjess Khlif, Hui-Hsiung Kuo, Hbib Ouerdine nd Benedykt Szozd Reserch Report No.
More informationMath 31S. Rumbos Fall Solutions to Assignment #16
Mth 31S. Rumbos Fll 2016 1 Solutions to Assignment #16 1. Logistic Growth 1. Suppose tht the growth of certin niml popultion is governed by the differentil eqution 1000 dn N dt = 100 N, (1) where N(t)
More information13: Diffusion in 2 Energy Groups
3: Diffusion in Energy Groups B. Rouben McMster University Course EP 4D3/6D3 Nucler Rector Anlysis (Rector Physics) 5 Sept.-Dec. 5 September Contents We study the diffusion eqution in two energy groups
More information1.1. Linear Constant Coefficient Equations. Remark: A differential equation is an equation
1 1.1. Liner Constnt Coefficient Equtions Section Objective(s): Overview of Differentil Equtions. Liner Differentil Equtions. Solving Liner Differentil Equtions. The Initil Vlue Problem. 1.1.1. Overview
More informationModule 6: LINEAR TRANSFORMATIONS
Module 6: LINEAR TRANSFORMATIONS. Trnsformtions nd mtrices Trnsformtions re generliztions of functions. A vector x in some set S n is mpped into m nother vector y T( x). A trnsformtion is liner if, for
More informationNOTE ON TRACES OF MATRIX PRODUCTS INVOLVING INVERSES OF POSITIVE DEFINITE ONES
Journl of pplied themtics nd Computtionl echnics 208, 7(), 29-36.mcm.pcz.pl p-issn 2299-9965 DOI: 0.752/jmcm.208..03 e-issn 2353-0588 NOE ON RCES OF RIX PRODUCS INVOLVING INVERSES OF POSIIVE DEFINIE ONES
More informationARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac
REVIEW OF ALGEBRA Here we review the bsic rules nd procedures of lgebr tht you need to know in order to be successful in clculus. ARITHMETIC OPERATIONS The rel numbers hve the following properties: b b
More informationCHAPTER 4a. ROOTS OF EQUATIONS
CHAPTER 4. ROOTS OF EQUATIONS A. J. Clrk School o Engineering Deprtment o Civil nd Environmentl Engineering by Dr. Ibrhim A. Asskk Spring 00 ENCE 03 - Computtion Methods in Civil Engineering II Deprtment
More informationSolution Manual. for. Fracture Mechanics. C.T. Sun and Z.-H. Jin
Solution Mnul for Frcture Mechnics by C.T. Sun nd Z.-H. Jin Chpter rob.: ) 4 No lod is crried by rt nd rt 4. There is no strin energy stored in them. Constnt Force Boundry Condition The totl strin energy
More informationChapter 3 Exponential and Logarithmic Functions Section 3.1
Chpter 3 Eponentil nd Logrithmic Functions Section 3. EXPONENTIAL FUNCTIONS AND THEIR GRAPHS Eponentil Functions Eponentil functions re non-lgebric functions. The re clled trnscendentl functions. The eponentil
More informationThe Fundamental Theorem of Calculus. The Total Change Theorem and the Area Under a Curve.
Clculus Li Vs The Fundmentl Theorem of Clculus. The Totl Chnge Theorem nd the Are Under Curve. Recll the following fct from Clculus course. If continuous function f(x) represents the rte of chnge of F
More informationPopulation Dynamics Definition Model A model is defined as a physical representation of any natural phenomena Example: 1. A miniature building model.
Popultion Dynmics Definition Model A model is defined s physicl representtion of ny nturl phenomen Exmple: 1. A miniture building model. 2. A children cycle prk depicting the trffic signls 3. Disply of
More informationDuality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below.
Dulity #. Second itertion for HW problem Recll our LP emple problem we hve been working on, in equlity form, is given below.,,,, 8 m F which, when written in slightly different form, is 8 F Recll tht we
More informationReliability models of belt drive systems under slipping failure mode
Specil Issue rticle Relibility models of belt drive systems under slipping filure mode dvnces in Mechnicl Engineering 1, Vol. 9(1) 1 1 Ó The uthor(s) 1 DOI: 1.11/11119 journls.sgepub.com/home/de Peng Go
More informationNumerical Integration
Chpter 5 Numericl Integrtion Numericl integrtion is the study of how the numericl vlue of n integrl cn be found. Methods of function pproximtion discussed in Chpter??, i.e., function pproximtion vi the
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES Introduction In rigid body kinemtics, e use the reltionships governing the displcement, velocity nd ccelertion, but must lso ccount for the rottionl motion of the body. Description
More informationf(x) dx, If one of these two conditions is not met, we call the integral improper. Our usual definition for the value for the definite integral
Improper Integrls Every time tht we hve evluted definite integrl such s f(x) dx, we hve mde two implicit ssumptions bout the integrl:. The intervl [, b] is finite, nd. f(x) is continuous on [, b]. If one
More information7.2 The Definite Integral
7.2 The Definite Integrl the definite integrl In the previous section, it ws found tht if function f is continuous nd nonnegtive, then the re under the grph of f on [, b] is given by F (b) F (), where
More informationDriving Cycle Construction of City Road for Hybrid Bus Based on Markov Process Deng Pan1, a, Fengchun Sun1,b*, Hongwen He1, c, Jiankun Peng1, d
Interntionl Industril Informtics nd Computer Engineering Conference (IIICEC 15) Driving Cycle Construction of City Rod for Hybrid Bus Bsed on Mrkov Process Deng Pn1,, Fengchun Sun1,b*, Hongwen He1, c,
More information38.2. The Uniform Distribution. Introduction. Prerequisites. Learning Outcomes
The Uniform Distribution 8. Introduction This Section introduces the simplest type of continuous probbility distribution which fetures continuous rndom vrible X with probbility density function f(x) which
More informationApproximate Large Deflection Analysis of Thin Rectangular Plates under Distributed Lateral Line Load
Second Interntionl Conference on Advnces in Engineering nd Technolog Approite Lrge eflection Anlsis of Thin Rectngulr Pltes under istriuted Lterl Line Lod Alln Okodi, Y N. Zir, Jckson A. Mkli Grdute Student,
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Statistical Physics I Spring Term Solutions to Problem Set #1
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Deprtment 8.044 Sttisticl Physics I Spring Term 03 Problem : Doping Semiconductor Solutions to Problem Set # ) Mentlly integrte the function p(x) given in
More informationDefinition of Continuity: The function f(x) is continuous at x = a if f(a) exists and lim
Mth 9 Course Summry/Study Guide Fll, 2005 [1] Limits Definition of Limit: We sy tht L is the limit of f(x) s x pproches if f(x) gets closer nd closer to L s x gets closer nd closer to. We write lim f(x)
More informationMain topics for the Second Midterm
Min topics for the Second Midterm The Midterm will cover Sections 5.4-5.9, Sections 6.1-6.3, nd Sections 7.1-7.7 (essentilly ll of the mteril covered in clss from the First Midterm). Be sure to know the
More information3 Conservation Laws, Constitutive Relations, and Some Classical PDEs
3 Conservtion Lws, Constitutive Reltions, nd Some Clssicl PDEs As topic between the introduction of PDEs nd strting to consider wys to solve them, this section introduces conservtion of mss nd its differentil
More informationTHERMAL EXPANSION COEFFICIENT OF WATER FOR VOLUMETRIC CALIBRATION
XX IMEKO World Congress Metrology for Green Growth September 9,, Busn, Republic of Kore THERMAL EXPANSION COEFFICIENT OF WATER FOR OLUMETRIC CALIBRATION Nieves Medin Hed of Mss Division, CEM, Spin, mnmedin@mityc.es
More informationMAT 168: Calculus II with Analytic Geometry. James V. Lambers
MAT 68: Clculus II with Anlytic Geometry Jmes V. Lmbers Februry 7, Contents Integrls 5. Introduction............................ 5.. Differentil Clculus nd Quotient Formuls...... 5.. Integrl Clculus nd
More informationA Compound of Geeta Distribution with Generalized Beta Distribution
Journl of Modern Applied Sttisticl Methods Volume 3 Issue Article 8 5--204 A Compound of Geet Distribution ith Generlized Bet Distribution Adil Rshid University of Kshmir, Sringr, Indi, dilstt@gmil.com
More informationDesign Against Fatigue Failure 2/3/2015 1
Design Aginst Ftigue Filure /3/015 1 Ftigue is the filure of mechnicl element by the growth of crck within mteril under vrible, repeted, lternting, or fluctuting stresses. Generlly, ftigue crck growth
More informationThe Predom module. Predom calculates and plots isothermal 1-, 2- and 3-metal predominance area diagrams. Predom accesses only compound databases.
Section 1 Section 2 The module clcultes nd plots isotherml 1-, 2- nd 3-metl predominnce re digrms. ccesses only compound dtbses. Tble of Contents Tble of Contents Opening the module Section 3 Stoichiometric
More informationADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS
ADVANCEMENT OF THE CLOSELY COUPLED PROBES POTENTIAL DROP TECHNIQUE FOR NDE OF SURFACE CRACKS F. Tkeo 1 nd M. Sk 1 Hchinohe Ntionl College of Technology, Hchinohe, Jpn; Tohoku University, Sendi, Jpn Abstrct:
More informationESTIMATION OF THE MODULUS OF ELASTICITY FOR DAM CONCRETE
ESTIMATION OF THE MODULUS OF ELASTICITY FOR DAM CONCRETE J. Vilrdell, A. Agudo, L. Agulló nd R. Gettu Universitt Politècnic de Ctluny, Deprtent of Construction Engineering, ETSECCPB-UPC, Edificio C-1,
More informationEFEFCTS OF GROUND MOTION UNCERTAINTY ON PREDICTING THE RESPONSE OF AN EXISTING RC FRAME STRUCTURE
13 th World Conference on Erthquke Engineering Vncouver, B.C., Cnd August 1-6, 2004 Pper No. 2007 EFEFCTS OF GROUND MOTION UNCERTAINTY ON PREDICTING THE RESPONSE OF AN EXISTING RC FRAME STRUCTURE Ftemeh
More informationTHE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS.
THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS RADON ROSBOROUGH https://intuitiveexplntionscom/picrd-lindelof-theorem/ This document is proof of the existence-uniqueness theorem
More informationMath 113 Exam 2 Practice
Mth 3 Exm Prctice Februry 8, 03 Exm will cover 7.4, 7.5, 7.7, 7.8, 8.-3 nd 8.5. Plese note tht integrtion skills lerned in erlier sections will still be needed for the mteril in 7.5, 7.8 nd chpter 8. This
More informationThe Thermodynamics of Aqueous Electrolyte Solutions
18 The Thermodynmics of Aqueous Electrolyte Solutions As discussed in Chpter 10, when slt is dissolved in wter or in other pproprite solvent, the molecules dissocite into ions. In queous solutions, strong
More informationAdvanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004
Advnced Clculus: MATH 410 Notes on Integrls nd Integrbility Professor Dvid Levermore 17 October 2004 1. Definite Integrls In this section we revisit the definite integrl tht you were introduced to when
More information19 Optimal behavior: Game theory
Intro. to Artificil Intelligence: Dle Schuurmns, Relu Ptrscu 1 19 Optiml behvior: Gme theory Adversril stte dynmics hve to ccount for worst cse Compute policy π : S A tht mximizes minimum rewrd Let S (,
More informationAQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions
Hperbolic Functions Section : The inverse hperbolic functions Notes nd Emples These notes contin subsections on The inverse hperbolic functions Integrtion using the inverse hperbolic functions Logrithmic
More informationOBSERVER DESIGN FOR OPEN AND CLOSED TROPHIC CHAINS
OBSERVER DESIGN FOR OPEN AND CLOSED TROPHIC CHAINS Z. Vrg M. Gáez b, I. López b Institute of Mthetics nd Infortics, Szent István University, Páter K. u.., H-3 Godollo, Hungry. (Vrg.Zoltn@gek.szie.hu) b
More informationThe First Fundamental Theorem of Calculus. If f(x) is continuous on [a, b] and F (x) is any antiderivative. f(x) dx = F (b) F (a).
The Fundmentl Theorems of Clculus Mth 4, Section 0, Spring 009 We now know enough bout definite integrls to give precise formultions of the Fundmentl Theorems of Clculus. We will lso look t some bsic emples
More informationConsequently, the temperature must be the same at each point in the cross section at x. Let:
HW 2 Comments: L1-3. Derive the het eqution for n inhomogeneous rod where the therml coefficients used in the derivtion of the het eqution for homogeneous rod now become functions of position x in the
More informationHow can we approximate the area of a region in the plane? What is an interpretation of the area under the graph of a velocity function?
Mth 125 Summry Here re some thoughts I ws hving while considering wht to put on the first midterm. The core of your studying should be the ssigned homework problems: mke sure you relly understnd those
More informationLinear predictive coding
Liner predictive coding Thi ethod cobine liner proceing with clr quntiztion. The in ide of the ethod i to predict the vlue of the current ple by liner cobintion of previou lredy recontructed ple nd then
More informationDETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE
Determintion RevAdvMterSci of mechnicl 0(009) -7 properties of nnostructures with complex crystl lttice using DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING
More information5.7 Improper Integrals
458 pplictions of definite integrls 5.7 Improper Integrls In Section 5.4, we computed the work required to lift pylod of mss m from the surfce of moon of mss nd rdius R to height H bove the surfce of the
More informationConservation Law. Chapter Goal. 5.2 Theory
Chpter 5 Conservtion Lw 5.1 Gol Our long term gol is to understnd how mny mthemticl models re derived. We study how certin quntity chnges with time in given region (sptil domin). We first derive the very
More information1 Online Learning and Regret Minimization
2.997 Decision-Mking in Lrge-Scle Systems My 10 MIT, Spring 2004 Hndout #29 Lecture Note 24 1 Online Lerning nd Regret Minimiztion In this lecture, we consider the problem of sequentil decision mking in
More informationChebyshev Functions and their use for two-dimensional electrostatic problems in elliptic coordinates
Chebyshev Functions nd their use for two-diensionl electrosttic probles in elliptic coordintes RAUL PEREZ-ENRIQUEZ, IVAN MARIN-ENRIQUEZ, J. L. MARIN AND R. RIERA Deprtento de Fisic Universidd de Sonor
More informationSongklanakarin Journal of Science and Technology SJST R1 Thongchan. A Modified Hyperbolic Secant Distribution
A Modified Hyperbolic Secnt Distribution Journl: Songklnkrin Journl of Science nd Technology Mnuscript ID SJST-0-0.R Mnuscript Type: Originl Article Dte Submitted by the Author: 0-Mr-0 Complete List of
More informationNUMERICAL INTEGRATION
NUMERICAL INTEGRATION How do we evlute I = f (x) dx By the fundmentl theorem of clculus, if F (x) is n ntiderivtive of f (x), then I = f (x) dx = F (x) b = F (b) F () However, in prctice most integrls
More informationSecond degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT
Ethiop. J. Sci. & Technol. 7( 5-, 0 5 Second degree generlized guss-seidel itertion ethod for solving liner syste of equtions Tesfye Keede Bhir Dr University, College of Science, Deprtent of Mthetics tk_ke@yhoo.co
More informationNon-Linear & Logistic Regression
Non-Liner & Logistic Regression If the sttistics re boring, then you've got the wrong numbers. Edwrd R. Tufte (Sttistics Professor, Yle University) Regression Anlyses When do we use these? PART 1: find
More information63. Representation of functions as power series Consider a power series. ( 1) n x 2n for all 1 < x < 1
3 9. SEQUENCES AND SERIES 63. Representtion of functions s power series Consider power series x 2 + x 4 x 6 + x 8 + = ( ) n x 2n It is geometric series with q = x 2 nd therefore it converges for ll q =
More informationContinuous Random Variables
STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 217 Néhémy Lim Continuous Rndom Vribles Nottion. The indictor function of set S is rel-vlued function defined by : { 1 if x S 1 S (x) if x S Suppose tht
More informationNew data structures to reduce data size and search time
New dt structures to reduce dt size nd serch time Tsuneo Kuwbr Deprtment of Informtion Sciences, Fculty of Science, Kngw University, Hirtsuk-shi, Jpn FIT2018 1D-1, No2, pp1-4 Copyright (c)2018 by The Institute
More informationEstimating a Bounded Normal Mean Under the LINEX Loss Function
Journl of Sciences, Islic Republic of Irn 4(): 57-64 (03) University of Tehrn, ISSN 06-04 http://jsciences.ut.c.ir Estiting Bounded Norl Men Under the LINEX Loss Function A. Krinezhd * Deprtent of Sttistics,
More informationProperties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives
Block #6: Properties of Integrls, Indefinite Integrls Gols: Definition of the Definite Integrl Integrl Clcultions using Antiderivtives Properties of Integrls The Indefinite Integrl 1 Riemnn Sums - 1 Riemnn
More information