Influence of Mean Stress

Size: px
Start display at page:

Download "Influence of Mean Stress"

Transcription

1 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.

2 Men tresses Incresing en stress in the tensile direction results in reducing ftigue life (for constnt stress plitude). A constnt life digr ( versus ) or stress life digr ( x versus N f t different levels of R), etc. cn be used to understnd the influence of non-zero en stresses.

3 Constnt Life digr

4 tress life digr

5 Endurnce Liit Endurnce liit (Ftigue liit): hould be obtined by testing cn use the following e e = 0.5 ut = 740MP ut ut 1460MP > 1460MP e Endurnce Liit Rtio, s e / s ut 5

6

7 Modifying Fctors for Metl Ftigue A nuber of vribles cn hve significnt ipct on ftigue, such s: ize; Lrger coponents re ore likely to hve ftigue crcks initite, due to lrger volues of teril subject to high stresses, nd due to greter chnce of residul stresses (inherent processing difficulty). Effects inly seen t very long lives. Type of loding; Endurnce liits vry by loding condition (xil, bending, torsion) urfce finish; crtches, pits nd chining rks dd stress concentrtions. Fine grined terils (high strength steel) re ore ffected. Lrge effect, correction fctors usully presented grphiclly Teperture; Endurnce liits increse t low teperture (but frcture toughness decreses significntly) Endurnce liits dispper t high teperture 7

8 Modifying Fctors for Metl Ftigue urfce tretents. Ftigue crcks initite t free surfce, tretents cn be significnt Plting, therl or echnicl; ens to induce residul stress Copressive residul stresses re beneficil, tension is detrientl (reson why shot peening is benificil) The sensitivity of the surfce is ore higher for high strength terils Environent. Corrosion hs coplex interctive effect with ftigue (ttcks surfce nd cretes brittle oxide fil, which crcks nd pits to cuse stress concentrtions) Often in prctice, odifying fctors for the bove re plied to the eqution for the endurnce liit. 8

9 Clculting Endurnce liit using odifying fctors Endurnce liit odifying fctors = k k k k k k e b c d e f e k = urfce fctor k b = ize fctor k c = Lod odifiction fctor k d = Teperture fctor k e = Relibility fctor k f = Miscellneous effects fctor 9

10 urfce Fctor Ground k = 1.58 ut Mchined or cold rolled k 0.65 = 4.51 ut higley, Mechnicl Engineering Design, 1 st etric ed Hot rolled k As-forged = 57.7 ut k = ut Note: ut is in GP 10

11 ize Fctor For bending nd torsion (round brs) d.79 < d 51 k b = d 51 < d < 54 Equivlent dieter for nonrotting squre d = 0.808( hb) 1/ For xil loding: k b =1 11

12 Lod nd Teperture The endurnce liit differ if tests re crried out using rotting be, xil (push pull) nd torsion loding 1.00 Bending k c = 0.85 Axil 0.59 Torsion Use k c =1 for cobined loding Teperture effects Tepertures below roo teperture - brittle filure At high tepertures there is no ftigue liit. 1

13 Modifying Fctors Relibility fctor (bsed on 8% stndrd devition) Relibility % Relibility Fctor k e higley, Mechnicl Engineering Design, 7 th ed 13

14 Miscellneous Fctor Corrosion (k f ) Benh & Wrnock, Mechnics of olids nd tructures,

15 tress concentrtions At sudden chnges in section the stress distribution cn no longer be clculted by the stndrd equtions for stress This phenoenon is known s stress concentrtion, nd the chnge in section is referred to s stress riser tress concentrtion fctor, K t, is defined s the increse in stress over the noinl stress = K x t 0 Where K t is the theoreticl stress concentrtion fctor 15

16 Notch ensitivity oe terils not fully sensitive for the presence of notches A reduced vlue of K t cn be used for these terils The xiu stress in these terils is: x = K f 0 x fs 0 This fctor, K f. is clled ftigue stress concentrtion fctor τ = K τ K f = t 1+ q( K 1) Where q is clled the notch sensitivity, 16

17 Notch ensitivity For steels nd 04 Aluiniu lloys in reversed bending: Fig 7-0:higley, Mechnicl Engineering Design, 7 th ed 17

18 Notch ensitivity Estition of q by Peterson q 1 = 1 +α r α [] ut [MP] Eq 4.4 Bnnntine 1990 For steel only α = 0.5 for norlized or nneled steels BHN 170 α = for quench nd tepered steels BHN 360 α = 0.05 for highly hrdened steels BHN 600 Modified Neuber q = 1+ 1 iplified nd odified Neuber epiricl fits to experientl dt for reltively ild notches shows tht, q, is relted to: Mteril Notch size / r Eq 6-34 :higley 008 Feture Trnsverse hole houlder Groove 174/ ut 139/ ut 104/ ut [] ut [MP] 18

19 Fluctuting stresses higley 008 : 6.11 Fluctuting stress re frequently not coplete stress reversls. N Curve only for coplete stress reversl (or stndrdized cses) hpe of wve not iportnt in periodic ptterns Only the peks (xiu nd iniu) re iportnt 19

20 in =iniu stress x =xiu stress =en stress =stress plitude r =stress rnge x = in x + = in 0

21 Ftigue trength under Fluctuting tress Copressive Men tress Filure occur t = e or x = yc 7-11 higley 005 1

22 Men tress Goodn + e u oderberg + Gerber n = 1 e n + ( n 1 e AME elliptic n n ( ) + ( e y = u n ) y = ) 1 = 1 higley nd Mischke, Mechnicl Engineering Design, 7 th ed 7-11 higley 005

23 Men tresses Goodn eqution: e + = 1 ut e is the endurnce strength. Conservtive nd sfe choice for design of ductile terils, for tensile en stresses. oewht non-conservtive (overly conservtive) for copressive en stresses. One possible pproch for copressive en stresses is to copletely disregrd the en stresses.

24 Men tresses If the su of norlized nd is less thn 1, then the prt hs infinite life. (norlised stresses: / e nd / ut ) However, if the su is ore thn 1, then the prt hs finite life. Goodn criteri is ost coonly used since it is esy to use nd slightly conservtive.

25 Gerber eqution: Men tresses e is the endurnce strength. Provides good fit for ductile terils, for tensile en stresses. Cnnot be used for copressive en stresses since it predicts hrful effect due to copressive stresses (which is never true in prctice, nd overly conservtive) e + = 1 ut

26 Morrow eqution: Men tresses + = 1 e f e is the endurnce strength. Provides good fit for brittle terils (such s cst iron), for tensile en stresses. Generlly results in good fit for copressive en stresses s well. ' f is often equl to the frcture strength.

27 Cobintion of Loding Modes Indentify the principl stresses Deterine the en nd lternting coponents x in τ = x τ τ in = τ x + τ x + τ = in in = Cobine the coponents for using either: Von Mises = + ( K f ) 3( K fsτ ) = + ( K f ) 3( K fsτ higley 008 : 6-14 ) Tresc = K ) + 4( K ( f fs τ ) = + τ ( K f ) 4( K fs ) 7

28 Cobined Loding (hfts) Alternting bending nd constnt torsion oents: My x = I 3M 3 πd = xy = 3 von Mises tress AME Elliptic = K = 3 K τ f x fs xy Tr 16T τ = J πd n ( e n + ( Tresc - oderberg = ) y ) = 1 x = τ xy n e n + y =1 8

29 Coputing Ftigue Life Re-writing Goodn criteri: e + = ut = For infinite life with N N = FO e ut Fro -N curve 1 + = For finite life with N N ut N = FO

30 Coputing Ftigue Life elect n plitude-en odel Goodn criteri ost coonly used. elect FO, if needed. Deterine if life is infinite. If not, use the FO nd the criteri to deterine the equivlent stress plitude for zero en stress, N.

31 Coputing Ftigue Life Use the en stress odel to copute equivlent stress plitude. N = 1 Use the -N curve nd N to copute ftigue life. ut N = AN B f

32 Finite Life Region N Infinite Life Region e ut

33 Typicl exple For n un-notched sple de of AII 4340 steel subject to cyclic stress with = 00 MP nd = 450 MP, deterine the nuber of cycles to filure using Goodn criteri, Gerber criteri nd Morrow criteri. Copre results nd coent on the estited life. Following dt is given: ut = 117 MP, A = 1643 MP, B = , ' f = 1758 MP

Some History. Over the Next Several Days. Three Stages of Fatigue Failure. Identifying Fatigue Fractures. Three Approaches. Low vs.

Some 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 information

NONLINEAR CONSTANT LIFE MODEL FOR FATIGUE LIFE PREDICTION OF COMPOSITE MATERIALS

NONLINEAR 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 information

Design Against Fatigue Failure 2/3/2015 1

Design 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 information

Ideal Gas behaviour: summary

Ideal Gas behaviour: summary Lecture 4 Rel Gses Idel Gs ehviour: sury We recll the conditions under which the idel gs eqution of stte Pn is vlid: olue of individul gs olecules is neglected No interctions (either ttrctive or repulsive)

More information

Strength of materials II- Fatigue failure

Strength 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 information

Contact Analysis on Large Negative Clearance Four-point Contact Ball Bearing

Contact 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 information

ME311 Machine Design

ME311 Machine Design ME11 Mchine Design Lecture 10: Springs (Chpter 17) W Dornfeld 9Nov018 Firfield University School of Engineering A Free Body Digrm of coil spring (cutting through nywhere on the coil) shows tht there must

More information

CHAPTER 5 Newton s Laws of Motion

CHAPTER 5 Newton s Laws of Motion CHAPTER 5 Newton s Lws of Motion We ve been lerning kinetics; describing otion without understnding wht the cuse of the otion ws. Now we re going to lern dynics!! Nno otor 103 PHYS - 1 Isc Newton (1642-1727)

More information

Materials 337. Lecture 7. Topics covered Introduction to fracture mechanics The elastic stress field Superposition principle Fracture toughness

Materials 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 information

AN EXPERIMENTAL INVESTIGATION OF PENETRATION FAILURE MODES IN COMPOSITE LAMINATES

AN 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 information

Towards a probabilistic concept of the Kitagawa-Takahashi diagram

Towards a probabilistic concept of the Kitagawa-Takahashi diagram 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,

More information

The Atwood Machine OBJECTIVE INTRODUCTION APPARATUS THEORY

The Atwood Machine OBJECTIVE INTRODUCTION APPARATUS THEORY The Atwood Mchine OBJECTIVE To derive the ening of Newton's second lw of otion s it pplies to the Atwood chine. To explin how ss iblnce cn led to the ccelertion of the syste. To deterine the ccelertion

More information

7-1: Zero and Negative Exponents

7-1: 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 information

ADVANCEMENT 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 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 information

Effects of peripheral drilling moment on delamination using special drill bits

Effects 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 information

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER)

Lesson 8. Thermomechanical Measurements for Energy Systems (MENR) Measurements for Mechanical Systems and Production (MMER) Lesson 8 Thermomechnicl Mesurements for Energy Systems (MEN) Mesurements for Mechnicl Systems nd Production (MME) A.Y. 205-6 Zccri (ino ) Del Prete Mesurement of Mechnicl STAIN Strin mesurements re perhps

More information

Progressive failure analysis of compression-loaded composite flat panel with cutout

Progressive failure analysis of compression-loaded composite flat panel with cutout Interntionl Journl on Theoreticl nd Applied Reserch in Mechnicl Engineering (IJTARME) Progressive filure nlysis of compression-loded composite flt pnel with cutout 1 Guspir S. Mkndr, 2 N.K. Chhpkhne, 3

More information

ECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model

ECONOMETRIC 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 information

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system Complex Numbers Section 1: Introduction to Complex Numbers Notes nd Exmples These notes contin subsections on The number system Adding nd subtrcting complex numbers Multiplying complex numbers Complex

More information

ESTIMATION OF THE MODULUS OF ELASTICITY FOR DAM CONCRETE

ESTIMATION 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 information

PHY 5246: Theoretical Dynamics, Fall Assignment # 5, Solutions. θ = l mr 2 = l

PHY 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 information

Week 10: Line Integrals

Week 10: Line Integrals Week 10: Line Integrls Introduction In this finl week we return to prmetrised curves nd consider integrtion long such curves. We lredy sw this in Week 2 when we integrted long curve to find its length.

More information

Phys101 Lecture 4,5 Dynamics: Newton s Laws of Motion

Phys101 Lecture 4,5 Dynamics: Newton s Laws of Motion Phys101 Lecture 4,5 Dynics: ewton s Lws of Motion Key points: ewton s second lw is vector eqution ction nd rection re cting on different objects ree-ody Digrs riction Inclines Ref: 4-1,2,3,4,5,6,7,8,9.

More information

Kinetics of oriented crystallization of polymers in the linear stress-orientation range in the series expansion approach

Kinetics of oriented crystallization of polymers in the linear stress-orientation range in the series expansion approach express Polyer Letters Vol.1, No.4 (18) 48 Avilble online t www.expresspolylett.co https://doi.org/1.144/expresspolylett.18.9 Kinetics of oriented crystlliztion of polyers in the liner stress-orienttion

More information

Fundamentals of Analytical Chemistry

Fundamentals of Analytical Chemistry Homework Fundmentls of nlyticl hemistry hpter 9 0, 1, 5, 7, 9 cids, Bses, nd hpter 9(b) Definitions cid Releses H ions in wter (rrhenius) Proton donor (Bronsted( Lowry) Electron-pir cceptor (Lewis) hrcteristic

More information

ELE B7 Power Systems Engineering. Power System Components Modeling

ELE B7 Power Systems Engineering. Power System Components Modeling Power Systems Engineering Power System Components Modeling Section III : Trnsformer Model Power Trnsformers- CONSTRUCTION Primry windings, connected to the lternting voltge source; Secondry windings, connected

More information

DETERMINATION OF MECHANICAL PROPERTIES OF NANOSTRUCTURES WITH COMPLEX CRYSTAL LATTICE USING MOMENT INTERACTION AT MICROSCALE

DETERMINATION 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 information

Chapter 5 Bending Moments and Shear Force Diagrams for Beams

Chapter 5 Bending Moments and Shear Force Diagrams for Beams Chpter 5 ending Moments nd Sher Force Digrms for ems n ddition to illy loded brs/rods (e.g. truss) nd torsionl shfts, the structurl members my eperience some lods perpendiculr to the is of the bem nd will

More information

Pre-Session Review. Part 1: Basic Algebra; Linear Functions and Graphs

Pre-Session Review. Part 1: Basic Algebra; Linear Functions and Graphs Pre-Session Review Prt 1: Bsic Algebr; Liner Functions nd Grphs A. Generl Review nd Introduction to Algebr Hierrchy of Arithmetic Opertions Opertions in ny expression re performed in the following order:

More information

INVESTIGATION OF THERMAL PROPERTIES OF SOIL BY IMPULSE METHOD Juraj Veselský

INVESTIGATION 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 information

Intro to Nuclear and Particle Physics (5110)

Intro to Nuclear and Particle Physics (5110) Intro to Nucler nd Prticle Physics (5110) Feb, 009 The Nucler Mss Spectrum The Liquid Drop Model //009 1 E(MeV) n n(n-1)/ E/[ n(n-1)/] (MeV/pir) 1 C 16 O 0 Ne 4 Mg 7.7 14.44 19.17 8.48 4 5 6 6 10 15.4.41

More information

Study on the Calculation of Magnetic Force Based on the Equivalent Magnetic Charge Method

Study on the Calculation of Magnetic Force Based on the Equivalent Magnetic Charge Method Avilble online t www.sciencedirect.com Physics Procedi 4 () 9 97 Interntionl Conference on Applied Physics nd Industril Engineering Study on the Clcultion of Mgnetic Force Bsed on the Equivlent Mgnetic

More information

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that

( dg. ) 2 dt. + dt. dt j + dh. + dt. r(t) dt. Comparing this equation with the one listed above for the length of see that Arc Length of Curves in Three Dimensionl Spce If the vector function r(t) f(t) i + g(t) j + h(t) k trces out the curve C s t vries, we cn mesure distnces long C using formul nerly identicl to one tht we

More information

Solution Manual. for. Fracture Mechanics. C.T. Sun and Z.-H. Jin

Solution 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 information

Job 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 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 information

A - INTRODUCTION AND OVERVIEW

A - INTRODUCTION AND OVERVIEW MMJ5 COMPUTATIONAL METHOD IN SOLID MECHANICS A - INTRODUCTION AND OVERVIEW INTRODUCTION AND OVERVIEW M.N. Tmin, CSMLb, UTM MMJ5 COMPUTATIONAL METHOD IN SOLID MECHANICS Course Content: A INTRODUCTION AND

More information

Scientific notation is a way of expressing really big numbers or really small numbers.

Scientific notation is a way of expressing really big numbers or really small numbers. Scientific Nottion (Stndrd form) Scientific nottion is wy of expressing relly big numbers or relly smll numbers. It is most often used in scientific clcultions where the nlysis must be very precise. Scientific

More information

1. a) Describe the principle characteristics and uses of the following types of PV cell: Single Crystal Silicon Poly Crystal Silicon

1. a) Describe the principle characteristics and uses of the following types of PV cell: Single Crystal Silicon Poly Crystal Silicon 2001 1. ) Describe the principle chrcteristics nd uses of the following types of PV cell: Single Crystl Silicon Poly Crystl Silicon Amorphous Silicon CIS/CIGS Gllium Arsenide Multijunction (12 mrks) b)

More information

4 The dynamical FRW universe

4 The dynamical FRW universe 4 The dynmicl FRW universe 4.1 The Einstein equtions Einstein s equtions G µν = T µν (7) relte the expnsion rte (t) to energy distribution in the universe. On the left hnd side is the Einstein tensor which

More information

Vorticity. curvature: shear: fluid elements moving in a straight line but at different speeds. t 1 t 2. ATM60, Shu-Hua Chen

Vorticity. curvature: shear: fluid elements moving in a straight line but at different speeds. t 1 t 2. ATM60, Shu-Hua Chen Vorticity We hve previously discussed the ngulr velocity s mesure of rottion of body. This is suitble quntity for body tht retins its shpe but fluid cn distort nd we must consider two components to rottion:

More information

r = cos θ + 1. dt ) dt. (1)

r = 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 information

EFFECTIVE BUCKLING LENGTH OF COLUMNS IN SWAY FRAMEWORKS: COMPARISONS

EFFECTIVE 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 information

ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION

ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION 28 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES ENERGY-BASED METHOD FOR GAS TURBINE ENGINE DISK BURST SPEED CALCULATION Anton N. Servetnik Centrl Institute of Avition Motors, Moscow, Russi servetnik@cim.ru

More information

Effects of Micro-polar Fluids and the Tsann Roughness Model on Performance Characteristics of Two-lobe Bearings

Effects 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 information

1 Bending of a beam with a rectangular section

1 Bending of a beam with a rectangular section 1 Bending of bem with rectngulr section x3 Episseur b M x 2 x x 1 2h M Figure 1 : Geometry of the bem nd pplied lod The bem in figure 1 hs rectngur section (thickness 2h, width b. The pplied lod is pure

More information

Math 113 Exam 2 Practice

Math 113 Exam 2 Practice Mth Em Prctice Februry, 8 Em will cover sections 6.5, 7.-7.5 nd 7.8. This sheet hs three sections. The first section will remind you bout techniques nd formuls tht you should know. The second gives number

More information

1.1. Linear Constant Coefficient Equations. Remark: A differential equation is an equation

1.1. 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 information

An Introduction to Trigonometry

An Introduction to Trigonometry n Introduction to Trigonoetry First of ll, let s check out the right ngled tringle below. The LETTERS, B & C indicte the ngles nd the letters, b & c indicte the sides. c b It is iportnt to note tht side

More information

Fig. 1. Open-Loop and Closed-Loop Systems with Plant Variations

Fig. 1. Open-Loop and Closed-Loop Systems with Plant Variations ME 3600 Control ystems Chrcteristics of Open-Loop nd Closed-Loop ystems Importnt Control ystem Chrcteristics o ensitivity of system response to prmetric vritions cn be reduced o rnsient nd stedy-stte responses

More information

Chapter 1: Fundamentals

Chapter 1: Fundamentals Chpter 1: Fundmentls 1.1 Rel Numbers Types of Rel Numbers: Nturl Numbers: {1, 2, 3,...}; These re the counting numbers. Integers: {... 3, 2, 1, 0, 1, 2, 3,...}; These re ll the nturl numbers, their negtives,

More information

BME 207 Introduction to Biomechanics Spring 2018

BME 207 Introduction to Biomechanics Spring 2018 April 6, 28 UNIVERSITY O RHODE ISAND Deprtment of Electricl, Computer nd Biomedicl Engineering BME 27 Introduction to Biomechnics Spring 28 Homework 8 Prolem 14.6 in the textook. In ddition to prts -e,

More information

Reliability models of belt drive systems under slipping failure mode

Reliability 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 information

COMPARISON OF THE MODELS OF POLARIZATION USED TO SIMULATE I-V CURVES OF AlGaN/GaN STRUCTURES

COMPARISON OF THE MODELS OF POLARIZATION USED TO SIMULATE I-V CURVES OF AlGaN/GaN STRUCTURES OMARISON OF THE MODELS OF OLARIZATION USED TO SIMULATE I-V URVES OF Al/ STRUTURES Jurj Rcko, Alen Grnová, eter Benko, Ldislv Hrth, Miroslv Mikolášek, Mgdlén Kdlečíková, Jurj Brez Slovk University of Technology,

More information

CHEMICAL KINETICS

CHEMICAL KINETICS CHEMICAL KINETICS Long Answer Questions: 1. Explin the following terms with suitble exmples ) Averge rte of Rection b) Slow nd Fst Rections c) Order of Rection d) Moleculrity of Rection e) Activtion Energy

More information

OXFORD H i g h e r E d u c a t i o n Oxford University Press, All rights reserved.

OXFORD 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 information

A Brief Review on Akkar, Sandikkaya and Bommer (ASB13) GMPE

A Brief Review on Akkar, Sandikkaya and Bommer (ASB13) GMPE Southwestern U.S. Ground Motion Chrcteriztion Senior Seismic Hzrd Anlysis Committee Level 3 Workshop #2 October 22-24, 2013 A Brief Review on Akkr, Sndikky nd Bommer (ASB13 GMPE Sinn Akkr Deprtment of

More information

Each term is formed by adding a constant to the previous term. Geometric progression

Each term is formed by adding a constant to the previous term. Geometric progression Chpter 4 Mthemticl Progressions PROGRESSION AND SEQUENCE Sequence A sequence is succession of numbers ech of which is formed ccording to definite lw tht is the sme throughout the sequence. Arithmetic Progression

More information

UNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction

UNIT 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 information

V 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 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 information

fractions Let s Learn to

fractions Let s Learn to 5 simple lgebric frctions corne lens pupil retin Norml vision light focused on the retin concve lens Shortsightedness (myopi) light focused in front of the retin Corrected myopi light focused on the retin

More information

Math 113 Exam 1-Review

Math 113 Exam 1-Review Mth 113 Exm 1-Review September 26, 2016 Exm 1 covers 6.1-7.3 in the textbook. It is dvisble to lso review the mteril from 5.3 nd 5.5 s this will be helpful in solving some of the problems. 6.1 Are Between

More information

Department of Electrical and Computer Engineering, Cornell University. ECE 4070: Physics of Semiconductors and Nanostructures.

Department of Electrical and Computer Engineering, Cornell University. ECE 4070: Physics of Semiconductors and Nanostructures. Deprtment of Electricl nd Computer Engineering, Cornell University ECE 4070: Physics of Semiconductors nd Nnostructures Spring 2014 Exm 2 ` April 17, 2014 INSTRUCTIONS: Every problem must be done in the

More information

The Spring. Consider a spring, which we apply a force F A to either stretch it or compress it

The Spring. Consider a spring, which we apply a force F A to either stretch it or compress it The Spring Consider spring, which we pply force F A to either stretch it or copress it F A - unstretched -F A 0 F A k k is the spring constnt, units of N/, different for different terils, nuber of coils

More information

Improper Integrals. Type I Improper Integrals How do we evaluate an integral such as

Improper 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 information

V. DEMENKO MECHANICS OF MATERIALS LECTURE 6 Plane Bending Deformation. Diagrams of Internal Forces (Continued)

V. DEMENKO MECHANICS OF MATERIALS LECTURE 6 Plane Bending Deformation. Diagrams of Internal Forces (Continued) V. DEMENKO MECHNCS OF MTERLS 015 1 LECTURE 6 Plne ending Deformtion. Digrms of nternl Forces (Continued) 1 Construction of ending Moment nd Shering Force Digrms for Two Supported ems n this mode of loding,

More information

The steps of the hypothesis test

The steps of the hypothesis test ttisticl Methods I (EXT 7005) Pge 78 Mosquito species Time of dy A B C Mid morning 0.0088 5.4900 5.5000 Mid Afternoon.3400 0.0300 0.8700 Dusk 0.600 5.400 3.000 The Chi squre test sttistic is the sum of

More information

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!!

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!! Nme: Algebr II Honors Pre-Chpter Homework Before we cn begin Ch on Rdicls, we need to be fmilir with perfect squres, cubes, etc Try nd do s mny s you cn without clcultor!!! n The nth root of n n Be ble

More information

Rolling Contact Bearings (pg 599)

Rolling Contact Bearings (pg 599) Bering V9.xmcd [Pg / 6] Title [234] The Units used s stndrd: m, kg, N, P, sec, wtts N, kg, m, P, sec/min, wtts/kw Rolling Contct Berings (pg 599) This note is only guideline for using the text book. Detiled

More information

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

SUMMER KNOWHOW STUDY AND LEARNING CENTRE SUMMER KNOWHOW STUDY AND LEARNING CENTRE Indices & Logrithms 2 Contents Indices.2 Frctionl Indices.4 Logrithms 6 Exponentil equtions. Simplifying Surds 13 Opertions on Surds..16 Scientific Nottion..18

More information

Chapter 36. a λ 2 2. (minima-dark fringes) Diffraction and the Wave Theory of Light. Diffraction by a Single Slit: Locating the Minima, Cont'd

Chapter 36. a λ 2 2. (minima-dark fringes) Diffraction and the Wave Theory of Light. Diffraction by a Single Slit: Locating the Minima, Cont'd Chpter 36 Diffrction In Chpter 35, we sw how light bes pssing through ifferent slits cn interfere with ech other n how be fter pssing through single slit flres-iffrcts- in Young's experient. Diffrction

More information

Probabilistic Fatigue Life Prediction Method for Notched Specimens Based on the Weakest-link theory

Probabilistic 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 information

Lab Based Analysis of Speed Control of DC Motor by Using Different Semiconductor Power Converters

Lab Based Analysis of Speed Control of DC Motor by Using Different Semiconductor Power Converters Open Access Librry Journl Lb Bsed Anlysis of Speed Control of DC Motor by Using Different Seiconductor Power Converters Abdul Khlique Junejo, Ghull Mustf Bhutto, Munwr Ayz Meon, hsn Ali Buriro Deprtent

More information

2.4 Linear Inequalities and Interval Notation

2.4 Linear Inequalities and Interval Notation .4 Liner Inequlities nd Intervl Nottion We wnt to solve equtions tht hve n inequlity symol insted of n equl sign. There re four inequlity symols tht we will look t: Less thn , Less thn or

More information

ON THE THEORETICAL FRACTURE STATISTICS OF THE HERTZ INDENTATION TEST

ON 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 information

POLITECNICO DI TORINO Repository ISTITUZIONALE

POLITECNICO DI TORINO Repository ISTITUZIONALE OLITECNICO DI TORINO Repository ISTITUZIONALE A coupled stress nd energy criterion within finite frcture mechnics Originl A coupled stress nd energy criterion within finite frcture mechnics / A. CARINTERI;.

More information

approaches as n becomes larger and larger. Since e > 1, the graph of the natural exponential function is as below

approaches as n becomes larger and larger. Since e > 1, the graph of the natural exponential function is as below . Eponentil nd rithmic functions.1 Eponentil Functions A function of the form f() =, > 0, 1 is clled n eponentil function. Its domin is the set of ll rel f ( 1) numbers. For n eponentil function f we hve.

More information

Discussion Question 1A P212, Week 1 P211 Review: 2-D Motion with Uniform Force

Discussion Question 1A P212, Week 1 P211 Review: 2-D Motion with Uniform Force Discussion Question 1A P1, Week 1 P11 Review: -D otion with Unifor Force The thetics nd phsics of the proble below re siilr to probles ou will encounter in P1, where the force is due to the ction of n

More information

Lesson 1: Quadratic Equations

Lesson 1: Quadratic Equations Lesson 1: Qudrtic Equtions Qudrtic Eqution: The qudrtic eqution in form is. In this section, we will review 4 methods of qudrtic equtions, nd when it is most to use ech method. 1. 3.. 4. Method 1: Fctoring

More information

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac

ARITHMETIC 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 information

Read section 3.3, 3.4 Announcements:

Read section 3.3, 3.4 Announcements: Dte: 3/1/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: 1. f x = 3x 6, find the inverse, f 1 x., Using your grphing clcultor, Grph 1. f x,f

More information

1 Module for Year 10 Secondary School Student Logarithm

1 Module for Year 10 Secondary School Student Logarithm 1 Erthquke Intensity Mesurement (The Richter Scle) Dr Chrles Richter showed tht the lrger the energy of n erthquke hs, the lrger mplitude of ground motion t given distnce. The simple model of Richter

More information

ET 438a Control Systems Technology Laboratory 4 Modeling Control Systems with MATLAB/Simulink Position Control with Disturbances

ET 438a Control Systems Technology Laboratory 4 Modeling Control Systems with MATLAB/Simulink Position Control with Disturbances ET 438 Control Systes Technology bortory 4 Modeling Control Systes with MATAB/Siulink Position Control with Disturbnces bortory erning Objectives After copleting this lbortory you will be ble to:.) Convert

More information

Design Data 1M. Highway Live Loads on Concrete Pipe

Design Data 1M. Highway Live Loads on Concrete Pipe Design Dt 1M Highwy Live Lods on Concrete Pipe Foreword Thick, high-strength pvements designed for hevy truck trffic substntilly reduce the pressure trnsmitted through wheel to the subgrde nd consequently,

More information

f(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

f(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 information

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve Dte: 3/14/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: Use your clcultor to solve 4 7x =250; 5 3x =500; HW Requests: Properties of Log Equtions

More information

Conservation Law. Chapter Goal. 5.2 Theory

Conservation 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 information

DIRECT CURRENT CIRCUITS

DIRECT CURRENT CIRCUITS DRECT CURRENT CUTS ELECTRC POWER Consider the circuit shown in the Figure where bttery is connected to resistor R. A positive chrge dq will gin potentil energy s it moves from point to point b through

More information

STRENGTH AND FATIGUE LIFE OF CARBON/EPOXY LAMINATES UNDER BIAXIAL LOADING

STRENGTH AND FATIGUE LIFE OF CARBON/EPOXY LAMINATES UNDER BIAXIAL LOADING STRENGTH AND FATIGUE LIFE OF CARBON/EPOXY LAMINATES UNDER BIAXIAL LOADING C. S. Lee, W. Hwng, H. C. Prk, nd K. S. Hn Deprtment o Mechnicl Engineering Pohng University o Science nd Technology, Pohng 79-784,

More information

FATIGUE MECHANISM OF BOLTED JOINTS UNDER MULTI-AXIAL VIBRATION

FATIGUE MECHANISM OF BOLTED JOINTS UNDER MULTI-AXIAL VIBRATION Proceedings of the 5th Interntionl Conference on Integrity-Relibility-Filure, Porto/Portugl 24-28 July 2016 Editors J.F. Silv Gomes nd S.A. Meguid Publ. INEGI/FEUP (2016) PAPER REF: 6299 FATIGUE MECHANISM

More information

Topics Covered AP Calculus AB

Topics Covered AP Calculus AB Topics Covered AP Clculus AB ) Elementry Functions ) Properties of Functions i) A function f is defined s set of ll ordered pirs (, y), such tht for ech element, there corresponds ectly one element y.

More information

Project A: Active Vibration Suppression of Lumped-Parameters Systems using Piezoelectric Inertial Actuators *

Project 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 information

13: Diffusion in 2 Energy Groups

13: 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 information

Numerical Analysis: Trapezoidal and Simpson s Rule

Numerical Analysis: Trapezoidal and Simpson s Rule nd Simpson s Mthemticl question we re interested in numericlly nswering How to we evlute I = f (x) dx? Clculus tells us tht if F(x) is the ntiderivtive of function f (x) on the intervl [, b], then I =

More information

WELCOME TO THE LECTURE

WELCOME TO THE LECTURE WELCOME TO THE LECTURE ON DC MOTOR Force on conductor If conductor is plced in mgnetic field nd current is llowed to flow through the conductor, the conductor will experience mechnicl force. N S Electric

More information

Expectation and Variance

Expectation and Variance Expecttion nd Vrince : sum of two die rolls P(= P(= = 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12 P(=2) = 1/36 P(=3) = 1/18 P(=4) = 1/12 P(=5) = 1/9 P(=7) = 1/6 P(=13) =? 2 1/36 3 1/18 4 1/12 5 1/9 6 5/36 7 1/6

More information

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by.

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by. NUMERICAL INTEGRATION 1 Introduction The inverse process to differentition in clculus is integrtion. Mthemticlly, integrtion is represented by f(x) dx which stnds for the integrl of the function f(x) with

More information

Physics 1402: Lecture 7 Today s Agenda

Physics 1402: Lecture 7 Today s Agenda 1 Physics 1402: Lecture 7 Tody s gend nnouncements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW ssignments, solutions etc. Homework #2: On Msterphysics tody: due Fridy Go to msteringphysics.com Ls:

More information

Chapter 1: Logarithmic functions and indices

Chapter 1: Logarithmic functions and indices Chpter : Logrithmic functions nd indices. You cn simplify epressions y using rules of indices m n m n m n m n ( m ) n mn m m m m n m m n Emple Simplify these epressions: 5 r r c 4 4 d 6 5 e ( ) f ( ) 4

More information

1.2. 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.

1.2. 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 information

MATH20812: PRACTICAL STATISTICS I SEMESTER 2 NOTES ON RANDOM VARIABLES

MATH20812: PRACTICAL STATISTICS I SEMESTER 2 NOTES ON RANDOM VARIABLES MATH20812: PRACTICAL STATISTICS I SEMESTER 2 NOTES ON RANDOM VARIABLES Things to Know Rndom Vrible A rndom vrible is function tht ssigns numericl vlue to ech outcome of prticulr experiment. A rndom vrible

More information