Strength of Materials

Size: px
Start display at page:

Download "Strength of Materials"

Transcription

1 Strngth of Matrials Sssion Column 08 ctur not : ramudiyanto, M.Eng.

2 Strngth of Matrials STBIITY OF STRUCTURE

3 In th dsign of columns, oss-sctional ara is slctd such that - allowabl strss is not xcdd all - dformation falls within spcifications E spc ftr ths dsign calculations, may discovr that th column is unstabl undr loading and that it suddnly bcoms sharply curvd or buckls.

4 Considr modl with two rods and torsional spring. ftr a small prturbation, K rstoring momnt sin dstabilizing momnt Column is stabl (tnds to rturn to alignd orintation) if K 4K

5 ssum that a load is applid. ftr a prturbation, th systm sttls to a nw quilibrium configuration at a finit dflction angl. sin K 4K sin Noting that sin <, th assumd configuration is only possibl if >.

6 Considr an axially loadd bam. ftr a small prturbation, th systm rachs an quilibrium configuration such that d y dx d y dx M EI EI EI y 0 Solution with assumd configuration can only b obtaind if EI y E r E r

7 Th valu of strss corrsponding to th itical load, rcding analysis is limitd to cntric loadings. r E r E r EI slndrnss ratio itical strss

8 column with on fixd and on fr nd, will bhav as th uppr-half of a pin-connctd column. Th itical loading is calculatd from Eulr s formula, EI E r quivalnt lngth

9

10 Sampl roblm 1 n aluminum column of lngth and rctangular oss-sction has a fixd nd at B and supports a cntric load at. Two smooth and roundd fixd plats rstrain nd from moving in on of th vrtical plans of symmtry but allow it to mov in th othr plan. a) Dtrmin th ratio a/b of th two sids of th oss-sction corrsponding to th most fficint dsign against buckling. = 0 in. E = 10.1 x 10 6 psi = 5 kips FS =.5 b) Dsign th most fficint oss-sction for th column.

11 SOUTION: Th most fficint dsign occurs whn th rsistanc to buckling is qual in both plans of symmtry. This occurs whn th slndrnss ratios ar qual. Buckling in xy lan: z 1 1 I ba r z z ab, z 0.7 r a 1 3 a 1, y ry b / 1 a 1 Buckling in xz lan: r y I y 1 1 ab ab 3 b 1 r r z y b 1 Most fficint dsign:, z, y r r z 0.7 a 1 a b b / 1 y 0.7 a b 0.35

12 = 0 in. E = 10.1 x 10 6 psi = 5 kips FS =.5 a/b = 0.35 Dsign: r y b 1 FS.55 kips 1500 lbs 0.35b b E r 1500 lbs 0.35b b 0 in b b b 1.60 in. a 0.35b in b psi 1.5 kips b 6 psi

13 Strngth of Matrials ECCENTRIC ODING: THE SECNT FORMU

14 Eccntric loading is quivalnt to a cntric load and a coupl. Bnding occurs for any nonzro ccntricity. Qustion of buckling bcoms whthr th rsulting dflction is xcssiv. Th dflction bcom infinit whn = d y y dx EI y max sc Maximum strss max 1 1 y max r c sc r 1 1 c E r EI

15 max 1 c sc r Y 1 E r

16 Sampl roblm E psi. Th uniform column consists of an 8-ft sction of structural tubing having th oss-sction shown. a) Using Eulr s formula and a factor of safty of two, dtrmin th allowabl cntric load for th column and th corrsponding normal strss. b) ssuming that th allowabl load, found in part a, is applid at a point 0.75 in. from th gomtric axis of th column, dtrmin th horizontal dflction of th top of th column and th maximum normal strss in th column.

17 SOUTION: Maximum allowabl cntric load: - Effctiv lngth, 8 ft 16 ft 19 in. - Critical load, EI 6.1 kips psi 8.0 in 19 in - llowabl load, all FS all 6.1 kips 31.1 kips 3.54 in all 31.1kips 8.79 ksi

18 Eccntric load: - End dflction, y m y m sc in sc in. 1 - Maximum normal strss, c m 1 sc r 31.1 kips in 0.75 in in 1.50 in sc m.0 ksi

19 Strngth of Matrials DESIGN OF COUMNS UNDER CENTRIC OD

20 rvious analyss assumd strsss blow th proportional limit and initially straight, homognous columns Exprimntal data dmonstrat - for larg /r, follows Eulr s formula and dpnds upon E but not Y. - for small /r, s is dtrmind by th yild strngth s Y and not E. - for intrmdiat /r, s dpnds on both s Y and E.

21 Structural Stl mrican Inst. of Stl Construction For /r > C c E / r all FS FS 1.9 For /r > C c / 1 r Y Cc FS / r C c 1 / r 8 Cc 3 all FS t /r = C c 1 Y C c E Y

22 luminum luminum ssociation, Inc. lloy 6061-T6 /r < 66: all /r > 66: all ksi / / r r ksi Ma / r / r Ma lloy 014-T6 /r < 55: all /r > 66: all ksi / r / r ksi Ma / r / r Ma

23 Sampl roblm Evaluat slndrnss ratio and vrify initial assumption. Rpat if ncssary. Using th aluminum alloy014-t6, dtrmin th smallst diamtr rod which can b usd to support th cntric load = 60 kn if a) = 750 mm, b) = 300 mm SOUTION: With th diamtr unknown, th slndrnss ration can not b valuatd. Must mak an assumption on which slndrnss ratio rgim to utiliz. Calculat rquird diamtr for assumd slndrnss ratio rgim.

24 For = 750 mm, assum /r > 55 Dtrmin cylindr radius: all 6010 c r N Ma Ma m c/ c mm c cylindr radius r radius of gyration I 4 c c 4 c Chck slndrnss ratio assumption: r c / 750mm mm assumption was corrct d c 36.9 mm

25 For = 300 mm, assum /r < 55 Dtrmin cylindr radius: 6010 all c 3 c 1.00 mm N r Ma 0.3 m / c Chck slndrnss ratio assumption: r c / 300 mm 1.00 mm assumption was corrct d c 4.0 mm a

26 Strngth of Matrials DESIGN OF COUMNS UNDER N ECCENTRIC OD

27 n ccntric load can b rplacd by a cntric load and a coupl M =. Normal strsss can b found from suprposing th strsss du to th cntric load and coupl, max cntric Mc I bnding llowabl strss mthod: Mc all I Intraction mthod: Mc all cntric all I bnding 1

28 That s for now THNK YOU

MECHANICS OF MATERIALS

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 information

682 CHAPTER 11 Columns. Columns with Other Support Conditions

682 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 information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHTER MECHNICS OF MTERILS 10 Ferdinand. Beer E. Russell Johnston, Jr. Columns John T. DeWolf cture Notes: J. Walt Oler Texas Tech University 006 The McGraw-Hill Companies, Inc. ll rights reserved. Columns

More information

4.2 Design of Sections for Flexure

4.2 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 information

Unfired pressure vessels- Part 3: Design

Unfired 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 information

VSMN30 FINITA ELEMENTMETODEN - DUGGA

VSMN30 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 information

Laboratory work # 8 (14) EXPERIMENTAL ESTIMATION OF CRITICAL STRESSES IN STRINGER UNDER COMPRESSION

Laboratory 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 information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle 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 information

ME311 Machine Design

ME311 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 information

Ultimate strength analysis & design of residential slabs on reactive soil

Ultimate strength analysis & design of residential slabs on reactive soil Ultimat strngth analysis & dsign of rsidntial slabs on ractiv soil This documnt prsnts an ovrviw of thory undrlying ultimat strngth analysis and dsign of stiffnd raft and waffl raft slabs, as commonly

More information

A New Approach to the Fatigue Life Prediction for Notched Components Under Multiaxial Cyclic Loading. Zhi-qiang TAO and De-guang SHANG *

A 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 information

A UNIFIED APPROACH FOR FIRE RESISTANCE PREDICTION OF STEEL COLUMNS AND FRAMES

A UNIFIED APPROACH FOR FIRE RESISTANCE PREDICTION OF STEEL COLUMNS AND FRAMES 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 4449244@ntu.du.sg Kang

More information

4.4 Design of Sections for Flexure (Part III)

4.4 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 information

At the end of this lesson, the students should be able to understand:

At the end of this lesson, the students should be able to understand: Instructional Objctivs: At th nd of this lsson, th studnts should b abl to undrstand: Dsign thod for variabl load Equivalnt strss on shaft Dsign basd on stiffnss and torsional rigidit Critical spd of shaft

More information

Design Formula for Rehabilitated Angle Steel Member Using Carbon Fiber Reinforced Plastic Plates

Design Formula for Rehabilitated Angle Steel Member Using Carbon Fiber Reinforced Plastic Plates Dsign Formula for Rhabilitatd Angl Stl Mmbr Using Carbon Fibr Rinforcd Plastic Plats Hiroyuki TAMAI Nagasaki Univrsity, Faculty of Enginring, Nagasaki, Japan Ako HATTORI & Yoshiyuki OZAWA & Tokuji HAITANI

More information

Mechanical Properties

Mechanical 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 information

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Division 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 information

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING

ME 354, MECHANICS OF MATERIALS LABORATORY COMPRESSION AND BUCKLING ME 354, MECHANICS OF MATERIALS LABATY COMPRESSION AND BUCKLING 01 January 000 / mgj PURPOSE Th purps f this xrcis is t study th ffcts f nd cnditins, clumn lngth, and matrial prprtis n cmprssiv bhaviur

More information

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: 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 information

INVESTIGATION 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 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 information

MATH 1080 Test 2-SOLUTIONS Spring

MATH 1080 Test 2-SOLUTIONS Spring MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =

More information

Plate Element Concrete Reinforcement Analysis

Plate Element Concrete Reinforcement Analysis Strand7 Rlas.4 Faturs Plat Elmnt oncrt Rinorcmnt Analsis Introduction oncrt is a widl usd construction matrial with high comprssiv t low tnsil strngths. Its poor prormanc in tnsion must thror b addrssd

More information

Module 7 Design of Springs. Version 2 ME, IIT Kharagpur

Module 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 information

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect

Instantaneous Cutting Force Model in High-Speed Milling Process with Gyroscopic Effect Advancd Matrials sarch Onlin: -8-6 ISS: 66-8985, Vols. 34-36, pp 389-39 doi:.48/www.scintific.nt/am.34-36.389 rans ch Publications, Switzrland Instantanous Cutting Forc Modl in High-Spd Milling Procss

More information

2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line

2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line //03 Ovrviw -owr Transmission Txt: 4.6-4.0 ECEGR 45 owr ystms Consrvation of Complx owr hort in owr Transmission owr Transmission isualization Radial in Mdium and ong in owr Transmission oltag Collaps

More information

Mechanical Design in Optical Engineering

Mechanical Design in Optical Engineering OPTI Buckling Buckling and Stability: As we learned in the previous lectures, structures may fail in a variety of ways, depending on the materials, load and support conditions. We had two primary concerns:

More information

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

The 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 information

AS 5850 Finite Element Analysis

AS 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 information

Finite Strain Elastic-Viscoplastic Model

Finite Strain Elastic-Viscoplastic Model Finit Strain Elastic-Viscoplastic Modl Pinksh Malhotra Mchanics of Solids,Brown Univrsity Introduction Th main goal of th projct is to modl finit strain rat-dpndnt plasticity using a modl compatibl for

More information

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems Daling with quantitati data and problm soling lif is a story problm! A larg portion of scinc inols quantitati data that has both alu and units. Units can sa your butt! Nd handl on mtric prfixs Dimnsional

More information

Performance of Seismic Design Aids for Nonlinear Pushover Analysis of Reinforced Concrete and Steel Bridges

Performance of Seismic Design Aids for Nonlinear Pushover Analysis of Reinforced Concrete and Steel Bridges Prormanc o Sismic Dsign Aids or Nonlinar Pushovr Analysis o Rinorcd Concrt and Stl Bridgs Franklin Y. Chng & Jry Gr issouri Univrsity o Scinc and Tchnology, Rolla, issouri, USA SUARY: Nonlinar static monotonic

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 10 Columns

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 10 Columns EMA 370 Mechanics & Materials Science (Mechanics of Materials) Chapter 10 Columns Columns Introduction Columns are vertical prismatic members subjected to compressive forces Goals: 1. Study the stability

More information

COLUMNS: BUCKLING (DIFFERENT ENDS)

COLUMNS: BUCKLING (DIFFERENT ENDS) COLUMNS: BUCKLING (DIFFERENT ENDS) Buckling of Long Straight Columns Example 4 Slide No. 1 A simple pin-connected truss is loaded and supported as shown in Fig. 1. All members of the truss are WT10 43

More information

2008 AP Calculus BC Multiple Choice Exam

2008 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 information

NTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II

NTHU ESS5850 Micro System Design F. G. Tseng Fall/2016, 7-2, p1. Lecture 7-2 MOSIS/SCNA Design Example- Piezoresistive type Accelerometer II F. G. Tsng Fall/016, 7-, p1 ctur 7- MOSIS/SCNA Dsign Exampl-!! Pizorsistivity Pizorsistiv typ Acclromtr II a Considr a conductiv lock of dimnsion a as shown in th figur. If a currnt is passd through th

More information

Dynamic Modelling of Hoisting Steel Wire Rope. Da-zhi CAO, Wen-zheng DU, Bao-zhu MA *

Dynamic 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 information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

CHAPTER 1. Introductory Concepts Elements of Vector Analysis Newton s Laws Units The basis of Newtonian Mechanics D Alembert s Principle

CHAPTER 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

Chapter 6: Polarization and Crystal Optics

Chapter 6: Polarization and Crystal Optics Chaptr 6: Polarization and Crystal Optics * P6-1. Cascadd Wav Rtardrs. Show that two cascadd quartr-wav rtardrs with paralll fast axs ar quivalnt to a half-wav rtardr. What is th rsult if th fast axs ar

More information

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0 unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr

More information

5 Chapter Capacitance and Dielectrics

5 Chapter Capacitance and Dielectrics 5 Chaptr Capacitanc and Dilctrics 5.1 Introduction... 5-3 5. Calculation of Capacitanc... 5-4 Exampl 5.1: Paralll-Plat Capacitor... 5-4 Exampl 5.: Cylindrical Capacitor... 5-6 Exampl 5.3: Sphrical Capacitor...

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE 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 information

UNIT I PARTIAL DIFFERENTIAL EQUATIONS PART B. 3) Form the partial differential equation by eliminating the arbitrary functions

UNIT 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 information

DIFFERENTIAL EQUATION

DIFFERENTIAL EQUATION MD DIFFERENTIAL EQUATION Sllabus : Ordinar diffrntial quations, thir ordr and dgr. Formation of diffrntial quations. Solution of diffrntial quations b th mthod of sparation of variabls, solution of homognous

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

Buried Corrugated Thermoplastic Pipe: Simulation and Design

Buried Corrugated Thermoplastic Pipe: Simulation and Design Schafr and M c Grath Burid Corrugatd Thrmoplastic Pip: Simulation and Dsign Schafr, B.W., M c Grath, T.J. B.W. Schafr, Ph.D., Assistant Profssor, schafr@jhu.du Johns Hopkins Univrsity, Latrob Hall, Baltimor,

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information

[1] (20 points) Find the general solutions of y y 2y = sin(t) + e t. Solution: y(t) = y c (t) + y p (t). Complementary Solutions: y

[1] (20 points) Find the general solutions of y y 2y = sin(t) + e t. Solution: y(t) = y c (t) + y p (t). Complementary Solutions: y [] (2 points) Find th gnral solutions of y y 2y = sin(t) + t. y(t) = y c (t) + y p (t). Complmntary Solutions: y c y c 2y c =. = λ 2 λ 2 = (λ + )(λ 2), λ =, λ 2 = 2 y c = C t + C 2 2t. A Particular Solution

More information

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination

University of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.

More information

Differential Equations

Differential 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 information

Dynamic response of a finite length euler-bernoulli beam on linear and nonlinear viscoelastic foundations to a concentrated moving force

Dynamic response of a finite length euler-bernoulli beam on linear and nonlinear viscoelastic foundations to a concentrated moving force Journal of Mchanical Scinc and Tchnology 2 (1) (21) 1957~1961 www.springrlink.com/contnt/1738-9x DOI 1.17/s1226-1-7-x Dynamic rspons of a finit lngth ulr-brnoulli bam on linar and nonlinar viscolastic

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI - 6. QUESTION WITH ANSWERS DEPARTMENT : CIVIL SEMESTER: V SUB.CODE/ NAME: CE 5 / Strngth of Matrials UNIT 4 STATE OF STRESS IN THREE DIMESIONS PART - A (

More information

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method

An Investigation on the Effect of the Coupled and Uncoupled Formulation on Transient Seepage by the Finite Element Method Amrican Journal of Applid Scincs 4 (1): 95-956, 7 ISSN 1546-939 7 Scinc Publications An Invstigation on th Effct of th Coupld and Uncoupld Formulation on Transint Spag by th Finit Elmnt Mthod 1 Ahad Ouria,

More information

Dynamic analysis of a Timoshenko beam subjected to moving concentrated forces using the finite element method

Dynamic 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 information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h.

1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h. NAME SUMMER ASSIGNMENT DUE SEPTEMBER 5 (FIRST DAY OF SCHOOL) AP CALC AB Dirctions: Answr all of th following qustions on a sparat sht of papr. All work must b shown. You will b tstd on this matrial somtim

More information

STRESSES FROM LOADING ON RIGID PAVEMENT COURSES

STRESSES FROM LOADING ON RIGID PAVEMENT COURSES bartosova.qxd 16.8.004 14:34 StrÆnka 3 003/1 PAGES 3 37 RECEIVED 5. 6. 00 ACCEPTED 15. 11. 00 ¼. BARTOŠOVÁ STRESSES FROM LOADING ON RIGID PAVEMENT COURSES ¼udmila Bartošová, Ing., PD. Assistant lcturr

More information

Differentiation of Exponential Functions

Differentiation of Exponential Functions Calculus Modul C Diffrntiation of Eponntial Functions Copyright This publication Th Northrn Albrta Institut of Tchnology 007. All Rights Rsrvd. LAST REVISED March, 009 Introduction to Diffrntiation of

More information

10. Limits involving infinity

10. 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 information

Nonlinear Bending of Strait Beams

Nonlinear Bending of Strait Beams Nonlinar Bnding of Strait Bams CONTENTS Th Eulr-Brnoulli bam thory Th Timoshnko bam thory Govrning Equations Wak Forms Finit lmnt modls Computr Implmntation: calculation of lmnt matrics Numrical ampls

More information

Impedance Transformation and Parameter Relations

Impedance Transformation and Parameter Relations 8/1/18 Cours nstructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 4 mpdanc Transformation and Paramtr Rlations mpdanc Ths Transformation

More information

EXPERIMENTAL AND THEORETICAL POST-BUCKLING STUDY OF STEEL SHEAR WALLS

EXPERIMENTAL 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 information

Mor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration

More information

COMPUTATIONAL NUCLEAR THERMAL HYDRAULICS

COMPUTATIONAL NUCLEAR THERMAL HYDRAULICS COMPUTTIONL NUCLER THERML HYDRULICS Cho, Hyoung Kyu Dpartmnt of Nuclar Enginring Soul National Univrsity CHPTER4. THE FINITE VOLUME METHOD FOR DIFFUSION PROBLEMS 2 Tabl of Contnts Chaptr 1 Chaptr 2 Chaptr

More information

St. Venants Torsion Constant of Hot Rolled Steel Profiles and Position of the Shear Centre

St. Venants Torsion Constant of Hot Rolled Steel Profiles and Position of the Shear Centre NSCC2009 St. Vnants Torsion Constant of Hot Rolld Stl Profils and Position of th Shar Cntr M. Kraus 1 & R. Kindmann 1 1 Institut for Stl and Composit Structurs, Univrsity of Bochum, Grmany BSTRCT: Th knowldg

More information

Performance of lightweight thin-walled steel sections: theoretical and mathematical considerations

Performance of lightweight thin-walled steel sections: theoretical and mathematical considerations Availal onlin at.plagiarsarchlirar.com lagia Rsarch Lirar Advancs in Applid Scinc Rsarch, 0, (5:847-859 ISSN: 0976-860 ODEN (USA: AASRF rformanc of lightight thin-alld stl sctions: thortical and mathmatical

More information

EAcos θ, where θ is the angle between the electric field and

EAcos θ, where θ is the angle between the electric field and 8.4. Modl: Th lctric flux flows out of a closd surfac around a rgion of spac containing a nt positiv charg and into a closd surfac surrounding a nt ngativ charg. Visualiz: Plas rfr to Figur EX8.4. Lt A

More information

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd 1. First you chck th domain of g x. For this function, x cannot qual zro. Thn w find th D domain of f g x D 3; D 3 0; x Q x x 1 3, x 0 2. Any cosin graph is going to b symmtric with th y-axis as long as

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 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 information

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Definition1: 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 information

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot

Determination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot 5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg

More information

Where k is either given or determined from the data and c is an arbitrary constant.

Where 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 information

A General Thermal Equilibrium Discharge Flow Model

A General Thermal Equilibrium Discharge Flow Model Journal of Enrgy and Powr Enginring 1 (216) 392-399 doi: 1.17265/1934-8975/216.7.2 D DAVID PUBLISHING A Gnral Thrmal Equilibrium Discharg Flow Modl Minfu Zhao, Dongxu Zhang and Yufng Lv Dpartmnt of Ractor

More information

6. The Interaction of Light and Matter

6. The Interaction of Light and Matter 6. Th Intraction of Light and Mattr - Th intraction of light and mattr is what maks lif intrsting. - Light causs mattr to vibrat. Mattr in turn mits light, which intrfrs with th original light. - Excitd

More information

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

Section 11.6: Directional Derivatives and the Gradient Vector

Section 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 information

CE 530 Molecular Simulation

CE 530 Molecular Simulation CE 53 Molcular Simulation Lctur 8 Fr-nrgy calculations David A. Kofk Dpartmnt of Chmical Enginring SUNY Buffalo kofk@ng.buffalo.du 2 Fr-Enrgy Calculations Uss of fr nrgy Phas quilibria Raction quilibria

More information

Response Sensitivity for Nonlinear Beam Column Elements

Response Sensitivity for Nonlinear Beam Column Elements Rspons Snsitivity for Nonlinar Bam Column Elmnts Michal H. Scott 1 ; Paolo Franchin 2 ; Grgory. Fnvs 3 ; and Filip C. Filippou 4 Abstract: Rspons snsitivity is ndd for simulation applications such as optimization,

More information

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology Bluchr Mchanical Enginring Procdings May 2014, vol. 1, num. 1 www.procdings.bluchr.com.br/vnto/10wccm TOPOLOGY DESIG OF STRUCTURE LOADED BY EARTHQUAKE P. Rosko 1 1 Cntr of Mchanics and Structural Dynamics,

More information

The Autonomous Underwater Vehicle (AUV) MAYA: General Description

The Autonomous Underwater Vehicle (AUV) MAYA: General Description Introduction h ocans and rivrs always hav bn and still ar an important sourc of rvnu and prosprity for mankind. Du to th grat importanc of ocans and rivrs, th scintific community maks us of Autonomous

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE HLKSH ENGNEENG COLLEGE TUCHPLL -. QUESTON WTH NSWES DEPTENT : CVL SEESTE: V SUB.CODE/ NE: CE / Strngt of atrials UNT DVNCED TOPCS N BENDNG OF BES PT - ( marks). Dfin Unsmmtrical nding T plan of loading

More information

Redesigning& Optimization of Conveyor Pulley

Redesigning& Optimization of Conveyor Pulley www.irjournal.org Intrnational Enginring Rsarch Journal (IERJ) Spcial Issu 2 Pag 5799-5804, 2015, ISSN 2395-1621 ISSN 2395-1621 Rdsigning& Optimization of Convyor Pully #1 Prasad C. Pol, #2 S. M. Jadhav

More information

Note 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.

Note 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 information

Massachusetts Institute of Technology Department of Mechanical Engineering

Massachusetts Institute of Technology Department of Mechanical Engineering Massachustts Institut of Tchnolog Dpartmnt of Mchanical Enginring. Introduction to Robotics Mid-Trm Eamination Novmbr, 005 :0 pm 4:0 pm Clos-Book. Two shts of nots ar allowd. Show how ou arrivd at our

More information

Sec 2.3 Modeling with First Order Equations

Sec 2.3 Modeling with First Order Equations Sc.3 Modling with First Ordr Equations Mathmatical modls charactriz physical systms, oftn using diffrntial quations. Modl Construction: Translating physical situation into mathmatical trms. Clarly stat

More information

Study of Buckling Stability on Tall Tower Truss Structure with All Loads

Study of Buckling Stability on Tall Tower Truss Structure with All Loads Intrnational Journal of Scinc, Tchnology and Socity 06; 4(4): 57-6 htt://www.scincublishinggrou.com/j/ijsts doi: 0.648/j.ijsts.060404. ISSN: 330-74 (rint); ISSN: 330-740 (Onlin) Study of Buckling Stability

More information

SME 3033 FINITE ELEMENT METHOD. Bending of Prismatic Beams (Initial notes designed by Dr. Nazri Kamsah)

SME 3033 FINITE ELEMENT METHOD. Bending of Prismatic Beams (Initial notes designed by Dr. Nazri Kamsah) Bnding of Prismatic Bams (Initia nots dsignd by Dr. Nazri Kamsah) St I-bams usd in a roof construction. 5- Gnra Loading Conditions For our anaysis, w wi considr thr typs of oading, as iustratd bow. Not:

More information

Abstract Interpretation. Lecture 5. Profs. Aiken, Barrett & Dill CS 357 Lecture 5 1

Abstract Interpretation. Lecture 5. Profs. Aiken, Barrett & Dill CS 357 Lecture 5 1 Abstract Intrprtation 1 History On brakthrough papr Cousot & Cousot 77 (?) Inspird by Dataflow analysis Dnotational smantics Enthusiastically mbracd by th community At last th functional community... At

More information

For official use only Doc. WRD 09(489) July 2007 BUREAU OF INDIAN STANDARDS. PRELIMINARY Indian Standard

For official use only Doc. WRD 09(489) July 2007 BUREAU OF INDIAN STANDARDS. PRELIMINARY Indian Standard For official us only Doc. WRD 09(489) July 007 BUREAU OF INDIAN STANDARDS PRELIMINARY Indian Standard STRUCTURAL DESIGN OF ENERGY DISSIPATORS FOR SPILLWAYS CRITERIA (First Rvision) (Not to b rproducd without

More information

PARTITION HOLE DESIGN FOR MAXIMIZING OR MINIMIZING THE FUNDAMENTAL EIGENFREQUENCY OF A DOUBLE CAVITY BY TOPOLOGY OPTIMIZATION

PARTITION 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 information

Dynamic behaviour of a rotating cracked beam

Dynamic behaviour of a rotating cracked beam Journal of Physics: Confrnc Sris PAPER OPEN ACCESS Dynamic bhaviour of a rotating crackd bam To cit this articl: Ahmd Yashar t al 6 J. Phys.: Conf. Sr. 744 57 Viw th articl onlin for updats and nhancmnts.

More information

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h

is an appropriate single phase forced convection heat transfer coefficient (e.g. Weisman), and h For t BWR oprating paramtrs givn blow, comput and plot: a) T clad surfac tmpratur assuming t Jns-Lotts Corrlation b) T clad surfac tmpratur assuming t Tom Corrlation c) T clad surfac tmpratur assuming

More information

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C

u r du = ur+1 r + 1 du = ln u + C u sin u du = cos u + C cos u du = sin u + C sec u tan u du = sec u + C e u du = e u + C Tchniqus of Intgration c Donald Kridr and Dwight Lahr In this sction w ar going to introduc th first approachs to valuating an indfinit intgral whos intgrand dos not hav an immdiat antidrivativ. W bgin

More information

1973 AP Calculus AB: Section I

1973 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 information

Module 8 Non equilibrium Thermodynamics

Module 8 Non equilibrium Thermodynamics Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis

More information

Search sequence databases 3 10/25/2016

Search 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 information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation 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 information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer 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 information

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

Synchronous machines

Synchronous machines Synchronous gnrator (altrnator): transorms mchanical nrgy into lctric nrgy; dsignd to gnrat sinusoidal oltags and currnts; usd in most powr plants, or car altrnators, tc. Synchronous motor: transorms lctric

More information