A UNIFIED APPROACH FOR FIRE RESISTANCE PREDICTION OF STEEL COLUMNS AND FRAMES
|
|
- Candice French
- 5 years ago
- Views:
Transcription
1 A UNIFIED APPROACH FOR FIRE RESISTANCE PREDICTION OF STEEL COLUMNS AND FRAMES Chu Yang TANG Nanang Tchnological Univrsit, School of Civil and Environmntal Enginring,N-B4-04, Singaor Kang Hai TAN Nanang Tchnological Univrsit, School of Civil and Environmntal Enginring,N-c-97, Singaor ABSTRACT For a long tim, th Rankin mthod has bn alid succssfull to stl columns and frams subjctd to incrasing loads but maintaind at constant ambint tmratur. This ar xtnds th Rankin formula to stl columns and frams undr fir conditions. Th authors rsnt a siml xrssion for buckling cofficint that can b usd for both columns and frams undr fir conditions, taking th dtrioration of stl rortis at lvatd tmratur into considration. Th Rankin rdictions ar comard to tst rsults of 34 axiall-loadd columns, 2 swa-frams and 6 non-swa frams. It is found that th rdictions agr vr wll with th tst rsults. For th 34 stl columns, th man of agrmnt of ratios of collas tmraturs T tst /T Rankin is 0.98 with a cofficint of variation (COV) of 5.4%. As for th 8 stl frams, th man is qual to 0.99 with a COV of 9.2%. KEYWORDS: fir rsistanc, fram, column, stl, fir tst 35
2 INTRODUCTION Th Rankin formula was originatd b Prof Rankin [] of Glassgow Univrsit in th lattr art of th 9 th cntur. It was latr modifid in th mid 20 th cntur [2] and was adotd in various dsign cods sinc thn. Th formula basicall involvd a linar intraction btwn two trms, th lastic buckling load factor λ and th lastic collas load factor λ as follows: = + () P P P R with P R Rankin load P lastic collas load P lastic critical load Th formula, whn usd for frams loadd to failur at ambint tmratur, ilds vr good agrmnt with tst rsults. Th ratio of th actual failur load factor λ c to th Rankin load factor λ R is around.00 to.20 [3]. In thir rcnt ar, Tang t al. [4] rovidd th thortical drivation of th Rankin formula and th furthr alid th Rankin formula to stl columns and frams undr fir conditions [4, 5]. Th currnt ar is to show that th Rankin formula is a unifid aroach for stl columns, swa and non-swa stl frams. RANKINE FORMULA IN FIRE CONDITIONS In fir conditions, th Rankin formula taks th following form: = + (2) R with T stl mmbr tmratur; T = 20 for ambint conditions. B adoting th matrial rduction factors for th rsctiv ild strngth (k ) and lastic modulus (k ) at lvatd tmraturs, th Rankin formula can xrssd as: P R (20) = + (3) k ( T) P (20) k ( T) P (20) Clarl, th Rankin formula rovids a linar intraction rlationshi btwn th lastic squashing load P and th lastic buckling load factor P. Th actual bhaviour of a column or a fram is dndnt on its normalizd slndrnss ratio [4, 5, 6]: Λ(20) = P 20) / P (20) (4) ( 36
3 For stl columns, th normalizd slndrnss ratio Λ(20) dnds on th mmbr slndrnss and nd conditions b th following rlationshi [4]: Λ(20 ) λ = (5) λ (20 ) E with λ slndrnss ratio; λ E transition slndrnss ratio. Hr, λ 20) = π E(20) / f (20) (6) E ( with E lastic modulus of stl; f ild strngth of stl. For frams, th trm Λ not onl dnds on th mmbr slndrnss and boundar conditions, but also on th loading attrns. Gnrall, non-swa frams hav smallr normalizd slndrnss ratio than swa frams; swa frams without latral loading hav smallr normalizd slndrnss ratio than thos with latral loading. Th normalizd slndrnss ratio is a vr imortant aramtr for both stl columns and frams. It dtrmins th rlativ imortanc of th lastic collas load and lastic critical load. From Equation (2), it can b sn that, for Λ << (vr stock columns or frams), th load caacit is dtrmind b th lastic collas load. On th othr hand, for Λ >> (vr slndr columns or frams), th load caacit is dtrmind b th lastic critical load. For Λ in th intrmdiat rang, both th lastic collas load and th lastic critical load ar imortant for dtrmining th failur load of th structur. B substituting Equation (4) into Equation (3), on obtains P 20) [ Λ(20)] = + k ( T) k ( T) R ( 2 At failur, P R (T) is qual to th alid load P. Thus, k ( T) N(20) = k ( T) + [ Λ(20)] k ( T) 2 (7) whr N is th buckling cofficint, givn b: P N (20) = (8) (20) P 37
4 Firgur shows th buckling curvs for both stl columns and frams at lvatd tmraturs basd on Equation (7). Hr, Eurocod 3 [7] is adotd for th matrial rduction factors k (T) and k E (T). Buckling Cofficint N(20) T = 20 C Normalizd Slndrnss Ratio Λ(20) FIGURE : Buckling cofficint for stl columns and frams at lvatd tmraturs Figur rovids a siml and unifid wa to dtrmin th fir rsistanc of both stl columns and frams. B rforming th ncssar analsis at ambint tmratur in ordr to dtrmin th normalizd slndrnss ratio for th structurs undr concrn, on can thn rad from Figur to dtrmin th structural fir rsistanc. CASE STUDIES Cas studis comrising axiall loadd columns, swa-frams, and non-swa frams, tstd undr standard fir ISO 834 [8] ar analsd to vrif th Rankin formula. Th first cas stud comriss 34 axiall loadd stl column, which ar summarizd in Tabl. Th comarisons of th Rankin rdictions with tst rsults for th 34 stl columns ar shown in Figur 2. For comarison uros, th N(T) - Λ(T) curv is lottd, whr P N( T) = (9) Λ(T) = / P ( T) (0) 38
5 Itms () Laboratoris Dscritions (2) Borhamhood, Braunschwig, CTICM, Gnt, LABEIN, Rnns, & Stuttgart. [9, 0, ] Stl grad S 235 & S 355. End conditions Pinnd-innd, inndfixd & fixd-fixd. Slndrnss ratios λ Var from 4 to 230. Man Tmraturs Var from 60 to 863 C. Load factors Var from % to 72 % with rsct to ild load at ambint tmratur. Loading ccntricitis Var from 0 to 650 mm. Tabl : tst conditions of th four cas studis Thus, from Equation (2), th Rankin formula can b xrssd b N( T) = () 2 + [ Λ( T)] Th normalizd squashing load N r (T) = and normalizd Eulr buckling load N r (T) = /Λ r (T) 2 ar also shown in th figur for comarison uros. Buckling Cofficint N(T) Plastic squashing curv N(T) = Eulr buckling curv N r (T) = / Λ(T) 2 Rankin curv (Eq. 27) N r (T) = / ( + Λ(T) 2 ) Normalizd Slndrnss Ratio Λ(Τ) FIGURE 2 : Comarison of rdictions and tst rsults for axiall-loadd stl columns 39
6 Th tst rsults agr wll with th Rankin rdictions for th 34 columns, with a man of agrmnt of T tst /T Rankin of 0.98 and a COV of 5.4%. Th scond cas stud comriss 6 non-swa frams (including th two EHR frams), and 2 swa-frams (including th singl-stor on-ba EGR frams and singl-stor two-ba ZSR frams) [6], as shown in Figur 3. F F 2 F F F2 h h l/2 l/2 EHR l EGR F F F F2 All cross-sctions: IPE 80, St 37 h l h l X: Stiffnr against tnsional dislacmnt rndicular to th fram lan ZSR FIGURE 3 : Ts of frams [2] Figur 4 shows th tst rsults of th 8 stl frams. Th man valu of T c Rankin /T c tst is.0 with a cofficint of variation of 9.2%. This accurac of rdictions for stl frams undr fir conditions is almost as good as th finit lmnt rsults [4]. Buckling Cofficint N(T) Plastic collas curv N(T) = EHR Frams EGR Frams ZSR Frams Elastic buckling curv N(T) = / Λ(T) 2 Rankin curv (Eq. 20) N(T) = / ( + Λ(T) 2 ) Normalizd Slndrnss Ratio Λ(T ) FIGURE 4 : Comarison of rdictions and tst rsults for swa and non-swa frams 40
7 CONCLUSIONS Th Rankin formula rovids a siml and unifid aroach to fir rsistanc calculation of stl columns and frams undr fir conditions. Th authors rsnts a siml xrssion for buckling cofficint that can b usd for both columns and frams undr fir conditions, taking th dtrioration of stl rortis at lvatd tmratur into considration. Good agrmnt with tst rsults is obtaind for th Rankin rdictions. REFERENCES [] Rankin, W. J. M., Usful Ruls and Tabls, London: C. Griffin & Co., Limitd, 908. [2] Mrchant, W., Th Failur Loads of Rigid Jointd Framworks as Influncd b Stabilit, Th Structural Enginr, 32, 85-90, 954. [3] Horn, M. R. & Mrchant, W, Th Stabilit of Frams, Oxford: Prgamon Prss Ltd, 965. [4] Tang, C. Y., Tan, K. H. and Ting, S. K., Basis and Alication of a Siml Intraction Formula for Stl Columns undr Fir Conditions, J. Struct. Engrg., ASCE, Octobr, Vol. 27, No. 0, , 200. [5] Tang, C. Y. and Tan, K. H., Basis and Alication of a Siml Intraction Formula for Stl Frams undr Fir Conditions, J. Struct. Engrg., ASCE, Octobr, Vol. 27, No. 0, , 200. [6] Rubrt, A., and Schaumann, P., Structural Stl and Plan Fram Assmblis undr Fir Action, Fir Saft J., 0, 73-84, 986. [7] CEN, Eurocod 3: Dsign of Stl Structurs. Part.2: Gnral Ruls Structural Fir Dsign, ENV 993--, Euroan Committ for Standardization, 995. [8] ISO 834, Fir Rsistanc Tats-Elmnts of Building Construction, Intrnational Standards Organisation, 975. [9] Janss, J., Statistical Analsis of Fir Tsts on Stl Bams and Columns to Eurocod 3, Part.2, J. Constr. Stl Rs., 33, 39 50, 995. [0] Talamona, D., Buckling Curvs in Cas of Fir ECSC 720 SA 36/55/93/68: Fir Rsistanc of Stl Columns with Eccntric Load, CTICM, Rort No. INC- 96/450-DT/VG Part, Saint-Rm-ls-Chvrus, Paris, 995. [] Schlich, J. B. & Cajot, L. G., Buckling Curvs in Cas of Fir: Draft Final Rort, Part I (Main Txt), CEC Agrmnt 720-SA 36/55/68/93, ProfilARBED- Rchrchs, Luxmbourg,
8 42
MECHANICS OF MATERIALS
00 Th McGraw-Hill Companis, Inc. ll rights rsrvd. T Edition CHTER MECHNICS OF MTERIS Frdinand. Br E. Russll Johnston, Jr. John T. DWolf Columns ctur Nots: J. Walt Olr Txas Tch Univrsit 00 Th McGraw-Hill
More informationStrength of Materials
Strngth of Matrials Sssion Column 08 ctur not : ramudiyanto, M.Eng. Strngth of Matrials STBIITY OF STRUCTURE In th dsign of columns, oss-sctional ara is slctd such that - allowabl strss is not xcdd all
More informationFiber Beam Element Model for the Collapse Simulation of Concrete Structures under Fire
Proc. Intrnational Smosium on Comutational Mchanics (ISCM7), Yao ZH & Yuan MW (ds.), Bijing: singhua Unirsit Prss & Sringr, Jul 3-August, 7, Bijing, China, 88 & CDROM. COMPUAIONA MECHANICS ISCM7, Jul 3-August,
More informationTheoretical and Experimental studying on simply supported Steel shear wall
Th 14 th World Confrnc on arthquak nginring Octobr 12-17, 28, Bijing, China Thortical and xrimntal studing on siml suortd Stl shar wall A.Sazgari 1 and H.Vladi 2 1 Lcturr, Dt. of Civil nginring, Islamic
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 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 informationThe Frequency Response of a Quarter-Wave Matching Network
4/1/29 Th Frquncy Rsons o a Quartr 1/9 Th Frquncy Rsons o a Quartr-Wav Matchg Ntwork Q: You hav onc aga rovidd us with conusg and rhas uslss ormation. Th quartr-wav matchg ntwork has an xact SFG o: a Τ
More information682 CHAPTER 11 Columns. Columns with Other Support Conditions
68 CHTER 11 Columns Columns with Othr Support Conditions Th problms for Sction 11.4 ar to b solvd using th assumptions of idal, slndr, prismatic, linarly lastic columns (Eulr buckling). uckling occurs
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 informationRESPONSE OF DUFFING OSCILLATOR UNDER NARROW-BAND RANDOM EXCITATION
Th rd Intrnational Confrnc on Comutational Mchanics and Virtual Enginring COMEC 9 9 OCTOBER 9, Brasov, Romania RESPONSE O DUING OSCILLATOR UNDER NARROW-BAND RANDOM EXCITATION Ptr STAN, Mtallurgical High
More informationFE Realization of Thermo-Visco-Plastic Constitutive Models using VUMAT in ABAQUS/Explicit Program
COMPUTATIONAL MECHANIC ICM2007, Jul 0-August 1, 2007, Bing, China 2007 Tsinghua Univrsit Prss & ringr FE Ralization of Thrmo-Visco-Plastic Constitutiv Modls using VUMAT in ABAQU/Exlicit Program C. Y. Gao*
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 informationDETERMINATION OF THE DISTORTION COEFFICIENT OF A 500 MPA FREE-DEFORMATION PISTON GAUGE USING A CONTROLLED-CLEARANCE ONE UP TO 200 MPA
XX IMEKO World Congrss Mtrology for Grn Growth Stmbr 9 14, 2012, Busan, Rublic of Kora DETERMINATION OF THE DISTORTION COEFFICIENT OF A 500 MPA FREE-DEFORMATION PISTON GAUGE USING A CONTROLLED-CLEARANCE
More informationHigher order derivatives
Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of
More information2008 AP Calculus BC Multiple Choice Exam
008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl
More informationThe van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012
Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor
More informationFinite Element Models for Steady Flows of Viscous Incompressible Fluids
Finit Elmnt Modls for Stad Flows of Viscous Incomprssibl Fluids Rad: Chaptr 10 JN Rdd CONTENTS Govrning Equations of Flows of Incomprssibl Fluids Mid (Vlocit-Prssur) Finit Elmnt Modl Pnalt Function Mthod
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More informationStrain-softening in continuum damage models: Investigation of MAT_058
9th Euroan LS-DYNA Confrnc 2013 Strain-softning in continuum damag modls: Invstigation of MAT_058 Karla Simon Gmkow, Rad Vignjvic School of Enginring, Cranfild Univrsity, Cranfild, Bdfordshir, MK43 0AL,
More informationCh. 24 Molecular Reaction Dynamics 1. Collision Theory
Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic
More informationDifferential Equations
UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs
More informationLaboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION
Laboratory wor # 8 (14) XPRIMNTAL STIMATION OF CRITICAL STRSSS IN STRINGR UNDR COMPRSSION At action of comprssing ffort on a bar (column, rod, and stringr) two inds of loss of stability ar possibl: 1)
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationDifferential Equations
Prfac Hr ar m onlin nots for m diffrntial quations cours that I tach hr at Lamar Univrsit. Dspit th fact that ths ar m class nots, th should b accssibl to anon wanting to larn how to solv diffrntial quations
More informationFirst derivative analysis
Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 4 Introduction to Finit Elmnt Analysis Chaptr 4 Trusss, Bams and Frams Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationAS 5850 Finite Element Analysis
AS 5850 Finit Elmnt Analysis Two-Dimnsional Linar Elasticity Instructor Prof. IIT Madras Equations of Plan Elasticity - 1 displacmnt fild strain- displacmnt rlations (infinitsimal strain) in matrix form
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 informationDynamic analysis of a Timoshenko beam subjected to moving concentrated forces using the finite element method
Shock and Vibration 4 27) 459 468 459 IOS Prss Dynamic analysis of a Timoshnko bam subjctd to moving concntratd forcs using th finit lmnt mthod Ping Lou, Gong-lian Dai and Qing-yuan Zng School of Civil
More informationA STUDY OF GEOPOTENTIAL GEOID IN THE PENINSULAR OF MALAYSIA Shahrum Ses Fakulti Ukur Universiti Teknologi Malay ia
ow stic iv han A STUDY OF GEOPOTENTAL GEOD N THE PENNSULAR OF MALAYSA Shahrum Ss Fakulti Ukur Univrsiti Tknologi Malay ia yno is Gcoidal hights can b comutd for a ingl oint valu or a grid of valu. A rogram
More informationA New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG *
2017 2nd Intrnational Conrnc on Applid Mchanics, Elctronics and Mchatronics Enginring (AMEME 2017) ISBN: 978-1-60595-497-4 A Nw Approach to th Fatigu Li Prdiction or Notchd Componnts Undr Multiaxial Cyclic
More information10. The Discrete-Time Fourier Transform (DTFT)
Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w
More informationCoupled Pendulums. Two normal modes.
Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron
More informationUNIT I PARTIAL DIFFERENTIAL EQUATIONS PART B. 3) Form the partial differential equation by eliminating the arbitrary functions
UNIT I PARTIAL DIFFERENTIAL EQUATIONS PART B 1) Form th artial diffrntial quation b liminating th arbitrar functions f and g in z f ( x ) g( x ) ) Form th artial diffrntial quation b liminating th arbitrar
More informationDESIGNING WITH ANISOTROPY.
DESIGNING WITH ANISOTOPY. PAT : QUASI-HOMOGENEOUS ANISOTOPIC LAMINATES. P. Vannucci, X. J. Gong & G. Vrchry. ISAT - Institut Suériur d l Automobil t ds Transorts, LMA - Laboratoir d chrch n Mécaniqu t
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 informationRational Approximation for the one-dimensional Bratu Equation
Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in
More informationINELASTIC BEHAVIOR OF MULTISTORY PARTIALLY RESTRAINED STEEL FRAMES. PART I
INELASTIC BEHAVIOR OF MULTISTORY PARTIALLY RESTRAINED STEEL FRAMES. PART I By Christohr M. Foly, 1 Associat Mmbr, ASCE, and Sriramulu Vinnakota, Fllow, ASCE ABSTRACT: This ar outlins th dvlomnt of a finit
More informationVSMN30 FINITA ELEMENTMETODEN - DUGGA
VSMN3 FINITA ELEMENTMETODEN - DUGGA 1-11-6 kl. 8.-1. Maximum points: 4, Rquird points to pass: Assistanc: CALFEM manual and calculator Problm 1 ( 8p ) 8 7 6 5 y 4 1. m x 1 3 1. m Th isotropic two-dimnsional
More informationCOHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.
MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function
More informationSCHUR S THEOREM REU SUMMER 2005
SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation
More informationUnit 6: Solving Exponential Equations and More
Habrman MTH 111 Sction II: Eonntial and Logarithmic Functions Unit 6: Solving Eonntial Equations and Mor EXAMPLE: Solv th quation 10 100 for. Obtain an act solution. This quation is so asy to solv that
More informationMechanical Properties
Mchanical Proprtis Elastic dformation Plastic dformation Fractur Mchanical Proprtis: Th Tnsion Tst s u P L s s y ΔL I II III For matrials proprtis, rplac load-dflction by strss-strain Enginring strss,
More informationThe Application of Phase Type Distributions for Modelling Queuing Systems
Th Alication of Phas Ty Distributions for Modlling Quuing Systms Eimutis VAAKEVICIUS Dartmnt of Mathmatical Rsarch in Systms Kaunas Univrsity of Tchnology Kaunas, T - 568, ithuania ABSTRACT Quuing modls
More informationChapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional
Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas
More informationNon-Linear Analysis of Interlaminar Stresses in Composite Beams with Piezoelectric Layers
7TH ITERATIOA OFEREE O OMPOSITE SIEE AD TEHOOGY on-inar Analysis of Intrlaminar Strsss in omosit Bams with Piolctric ayrs MASOUD TAHAI 1, AMIR TOOU DOYAMATI 1 Dartmnt of Mchanical Enginring, Faculty of
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 informationINTEGRATION BY PARTS
Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd
More informationELECTRON-MUON SCATTERING
ELECTRON-MUON SCATTERING ABSTRACT Th lctron charg is considrd to b distributd or xtndd in spac. Th diffrntial of th lctron charg is st qual to a function of lctron charg coordinats multiplid by a four-dimnsional
More informationThe graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the
Copyright itutcom 005 Fr download & print from wwwitutcom Do not rproduc by othr mans Functions and graphs Powr functions Th graph of n y, for n Q (st of rational numbrs) y is a straight lin through th
More informationSection 11.6: Directional Derivatives and the Gradient Vector
Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th
More informationEinstein Equations for Tetrad Fields
Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for
More informationWHAT LIES BETWEEN + AND (and beyond)? H.P.Williams
Working Par LSEOR 10-119 ISSN 2041-4668 (Onlin) WHAT LIES BETWEEN + AND (and byond)? HPWilliams London School of Economics hwilliams@lsacuk First ublishd in Grat Britain in 2010 by th Orational Rsarch
More information1973 AP Calculus AB: Section I
97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=
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 informationDivision of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.
Division of Mchanics Lund Univrsity MULTIBODY DYNMICS Examination 7033 Nam (writ in block lttrs):. Id.-numbr: Writtn xamination with fiv tasks. Plas chck that all tasks ar includd. clan copy of th solutions
More informationDynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *
17 nd Intrnational Confrnc on Mchanical Control and Automation (ICMCA 17) ISBN: 978-1-6595-46-8 Dynamic Modlling of Hoisting Stl Wir Rop Da-zhi CAO, Wn-zhng DU, Bao-zhu MA * and Su-bing LIU Xi an High
More informationThomas Whitham Sixth Form
Thomas Whitham Sith Form Pur Mathmatics Unit C Algbra Trigonomtr Gomtr Calculus Vctor gomtr Pag Algbra Molus functions graphs, quations an inqualitis Graph of f () Draw f () an rflct an part of th curv
More informationHuman vision is determined based on information theory:
Human vision is dtrmind basd on information thory: Supplmntary Information Alfonso Dlgado-Bonal,2 and F. Javir Martn Torrs,3 [] Instituto Andaluz d Cincias d la Tirra CSIC-UGR, Avda. d Las Palmras n 4,
More informationSearch sequence databases 3 10/25/2016
Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an
More informationTechnical Manual. S-Curve Tool
Tchnical Manual for S-Curv Tool Vrsion 1.0 (as of 09/1/1) Sonsord by: Naval Cntr for Cost Analysis (NCCA) Dvlod by: Tchnomics, Inc. 01 1 th Strt South, Suit 61 Arlington, VA 0 Points of Contact: Bruc Parkr,
More informationBroadband All-Angle Negative Refraction by Phononic Crystals
Supplmntar Information Broadband All-Angl Ngativ Rfraction b Phononic Crstals Yang Fan Li, Fi Mng, Shiwi Zhou, Ming-Hui Lu and Xiaodong Huang 1 Optimization algorithm and procss Bfor th optimization procss,
More informationImproved Prediction Method for Estimating Notch Elastic-Plastic Strains
Transactions, SMiRT 19, Toronto, August 007 Improvd Prdiction Mthod for Estimating Notch Elastic-Plastic Strains R. Adibi-Asl * and R. Sshadri Facult of Enginring and Applid Scinc, Mmorial Univrsit of
More informationAnswer Homework 5 PHA5127 Fall 1999 Jeff Stark
Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw
More informationScattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential
Commun. Thor. Phys. 66 06 96 00 Vol. 66, No., August, 06 Scattring Stats of l-wav Schrödingr Equation with Modifid Rosn Mors Potntial Wn-Li Chn í,, Yan-Wi Shi á, and Gao-Fng Wi Ôô, Gnral Education Cntr,
More informationAnalysis of the Monochloroacetic Acid Crystallization Process by Entropic Modeling
A ublication of 2071 VOL 32, 2013 CHEMICAL ENGINEERING TRANSACTIONS Chif Editors: Sauro Pirucci, Jiří J Klmš Coyright 2013, AIDIC Srvizi Srl, ISBN 978-88-95608-23-5; ISSN 1974-9791 Th Italian Association
More informationThe Transmission Line Wave Equation
1//5 Th Transmission Lin Wav Equation.doc 1/6 Th Transmission Lin Wav Equation Q: So, what functions I (z) and V (z) do satisfy both tlgraphr s quations?? A: To mak this asir, w will combin th tlgraphr
More informationPerformance analysis of some CFAR detectors in homogeneous Pearson-distributed clutter
SETIT 5 3 rd Intrnational Confrnc: Scincs of Elctronic, Tchnologis of Information and Tlcommunications arch 7-31, 5 TNISIA Prformanc analysis of som CFAR dtctors in homognous Parson-distributd cluttr iani
More informationPARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION
ICSV4 Cns Australia 9- July, 007 PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION Jin Woo L and Yoon Young Kim National Crativ
More informationMiddle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis
Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt
More informationEXPERIMENTAL AND THEORETICAL POST-BUCKLING STUDY OF STEEL SHEAR WALLS
4th Intrnational Confrnc on arthquak nginring Taipi, Taiwan Octobr 12-13, 2006 Papr No. 114 XPRIMNTAL AND THORTICAL POST-BUCKLING STUDY OF STL SHAR WALLS Abdolrahim. Jalali 1 and Arash.Sazgari 2 ABSTRACT
More informationSAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS
It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS
More informationModule 7 Design of Springs. Version 2 ME, IIT Kharagpur
Modul 7 Dsign of Springs Lsson Dsign of Hlical Springs for Variabl Load Instructional Objctivs: At th nd of this lsson, th studnts should b abl to undrstand: Natur of varying load on springs Modification
More informationOn the Hamiltonian of a Multi-Electron Atom
On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making
More informationCalculus Revision A2 Level
alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ
More informationLagrangian Analysis of a Class of Quadratic Liénard-Type Oscillator Equations with Exponential-Type Restoring Force function
agrangian Analysis of a Class of Quadratic iénard-ty Oscillator Equations wit Eonntial-Ty Rstoring Forc function J. Akand, D. K. K. Adjaï,.. Koudaoun,Y. J. F. Komaou,. D. onsia. Dartmnt of Pysics, Univrsity
More informationAnalysis of Folded H-Plane Tee Junction Using Multiple Cavity Modeling Technique
8 IEEE Rgion 1 Collouium and th Third Intrnational Confrnc on Industrial and Information Sstms Kharagur INDIA Dcmbr 8-1 8. > PAPER IDENTIFICATION NUMBER (14) < Analsis of Foldd -Plan T Junction Using Multil
More informationANALYSIS IN THE FREQUENCY DOMAIN
ANALYSIS IN THE FREQUENCY DOMAIN SPECTRAL DENSITY Dfinition Th spctral dnsit of a S.S.P. t also calld th spctrum of t is dfind as: + { γ }. jτ γ τ F τ τ In othr words, of th covarianc function. is dfind
More informationu x A j Stress in the Ocean
Strss in t Ocan T tratmnt of strss and strain in fluids is comlicatd and somwat bond t sco of tis class. Tos rall intrstd sould look into tis rtr in Batclor Introduction to luid Dnamics givn as a rfrnc
More informationNote If the candidate believes that e x = 0 solves to x = 0 or gives an extra solution of x = 0, then withhold the final accuracy mark.
. (a) Eithr y = or ( 0, ) (b) Whn =, y = ( 0 + ) = 0 = 0 ( + ) = 0 ( )( ) = 0 Eithr = (for possibly abov) or = A 3. Not If th candidat blivs that = 0 solvs to = 0 or givs an tra solution of = 0, thn withhold
More informationDesign of a New Soil-Tuber Separation Device on Potato Harvesters
Dsign of a Nw Soil-Tubr Saration Dvic on Potato Harvstrs Gaili Gao *, Dongxing Zhang, and Jun Liu Collg of Enginring, China Agricultural Univrsity, Bijing 83, P.R. China ggl965@6.com, ggl@cau.du.cn Abstract.
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More informationKCET 2016 TEST PAPER WITH ANSWER KEY (HELD ON WEDNESDAY 4 th MAY, 2016)
. Th maimum valu of Ë Ë c /. Th contraositiv of th convrs of th statmnt If a rim numbr thn odd If not a rim numbr thn not an odd If a rim numbr thn it not odd. If not an odd numbr thn not a rim numbr.
More information10. Limits involving infinity
. Limits involving infinity It is known from th it ruls for fundamntal arithmtic oprations (+,-,, ) that if two functions hav finit its at a (finit or infinit) point, that is, thy ar convrgnt, th it of
More informationSimulated Analysis of Tooth Profile Error of Cycloid Steel Ball Planetary Transmission
07 4th Intrnational Matrials, Machinry and Civil Enginring Confrnc(MATMCE 07) Simulatd Analysis of Tooth Profil Error of Cycloid Stl Ball Plantary Transmission Ruixu Hu,a, Yuquan Zhang,b,*, Zhanliang Zhao,c,
More informationFEM FOR HEAT TRANSFER PROBLEMS دانشگاه صنعتي اصفهان- دانشكده مكانيك
FEM FOR HE RNSFER PROBLEMS 1 Fild problms Gnral orm o systm quations o D linar stady stat ild problms: For 1D problms: D D g Q y y (Hlmholtz quation) d D g Q d Fild problms Hat transr in D in h h ( D D
More informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More informationWhere k is either given or determined from the data and c is an arbitrary constant.
Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is
More informationMulti-scale Analysis of Void Closure for Heavy Ingot Hot Forging
Modrn Applid Scinc; ol. 6, No. ; ISSN 9-844 E-ISSN 9-85 Publishd by Canadian Cntr of Scinc and Education Multi-scal Analysis of oid Closur for Havy Ingot Hot Forging Xiaoxun Zhang, Fang Ma, Kai Ma & Xia
More informationsurface of a dielectric-metal interface. It is commonly used today for discovering the ways in
Surfac plasmon rsonanc is snsitiv mchanism for obsrving slight changs nar th surfac of a dilctric-mtal intrfac. It is commonl usd toda for discovring th was in which protins intract with thir nvironmnt,
More informationSouthern Taiwan University
Chaptr Ordinar Diffrntial Equations of th First Ordr and First Dgr Gnral form:., d +, d 0.a. f,.b I. Sparabl Diffrntial quations Form: d + d 0 C d d E 9 + 4 0 Solution: 9d + 4d 0 9 + 4 C E + d Solution:
More informationII. MICROSTRUCTURES OF COPPER VIAS
Chnglin Wu, Tngfi Jiang, Ja Im, Knnth M. Lichti, Rui Huang and Paul S. Ho Dartmnt of Arosac Enginring and Enginring Mchanics, Univrsit of Txas, Austin, TX 78712, USA Microlctronics Rsarch Cntr and Txas
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationThe Matrix Exponential
Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!
More informationClassical Magnetic Dipole
Lctur 18 1 Classical Magntic Dipol In gnral, a particl of mass m and charg q (not ncssarily a point charg), w hav q g L m whr g is calld th gyromagntic ratio, which accounts for th ffcts of non-point charg
More informationSolution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:
APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding
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 informationDavisson Germer experiment
Announcmnts: Davisson Grmr xprimnt Homwork st 5 is today. Homwork st 6 will b postd latr today. Mad a good guss about th Nobl Priz for 2013 Clinton Davisson and Lstr Grmr. Davisson won Nobl Priz in 1937.
More informationGeneral Notes About 2007 AP Physics Scoring Guidelines
AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation
More informationCHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle
CHPTER 1 Introductory Concpts Elmnts of Vctor nalysis Nwton s Laws Units Th basis of Nwtonian Mchanics D lmbrt s Principl 1 Scinc of Mchanics: It is concrnd with th motion of matrial bodis. odis hav diffrnt
More information