Module 9 Thin and thick cylinders

Similar documents
ME311 Machine Design

Parametric Examination including Brief Survey of Composite and Homogenous Closed Ended Cylindrical Pressure Vessels

is needed and this can be established by multiplying A, obtained in step 3, by, resulting V = A x y =. = x, located in 1 st quadrant rotated about 2

SHAKEDOWN BEHAVIOUR OF COMPOSITE CYLINDERS WITH CROSS HOLE

A. Thicknesses and Densities

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

Wp/Lmin. Wn/Lmin 2.5V

Hotelling s Rule. Therefore arbitrage forces P(t) = P o e rt.

CHAPTER 24 GAUSS LAW

Electric potential energy Electrostatic force does work on a particle : Potential energy (: i initial state f : final state):

Example

Cork Institute of Technology. Spring 2005 DCE 3.5 Thermodynamics & Heat Transfer (Time: 3 Hours) Section A

LEAP FROG TECHNIQUE. Operational Simulation of LC Ladder Filters ECEN 622 (ESS) TAMU-AMSC

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set

A criterion of warpage about center-anchored deformable focusing micromirrors

Chapter 3, Solution 1C.

Derivation of the Differential Forms of the Conservation Laws Momentum

T-model: - + v o. v i. i o. v e. R i

Shakedown Analysis of a Composite Cylinder with a Cross-hole

Introduction of Two Port Network Negative Feedback (Uni lateral Case) Feedback Topology Analysis of feedback applications

Work, Energy, and Power. AP Physics C

Analysis of the chemical equilibrium of combustion at constant volume

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Chapter 12 Equilibrium and Elasticity

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Molecular Dynamic Simulations of Nickel Nanowires at Various Temperatures

Lecture 2 Feedback Amplifier

5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:

Conduction Heat Transfer

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

Set of square-integrable function 2 L : function space F

Transient Conduction: Spatial Effects and the Role of Analytical Solutions

Physics 1501 Lecture 19

CHAPTER GAUSS'S LAW

CIRCLE YOUR DIVISION: Div. 1 (9:30 am) Div. 2 (11:30 am) Div. 3 (2:30 pm) Prof. Ruan Prof. Naik Mr. Singh

1. Starting with the local version of the first law of thermodynamics q. derive the statement of the first law of thermodynamics for a control volume

55:041 Electronic Circuits

A) 100 K B) 150 K C) 200 K D) 250 K E) 350 K

Chapter 8. Linear Momentum, Impulse, and Collisions

Thermoelastic Problem of a Long Annular Multilayered Cylinder

ME 3600 Control Systems Frequency Domain Analysis

Electric Charge. Electric charge is quantized. Electric charge is conserved

Example 11: The man shown in Figure (a) pulls on the cord with a force of 70

24-2: Electric Potential Energy. 24-1: What is physics

Review of Vector Algebra and Vector Calculus Operations

CTN 2/23/16. EE 247B/ME 218: Introduction to MEMS Design Lecture 11m2: Mechanics of Materials. Copyright 2016 Regents of the University of California

Consider the simple circuit of Figure 1 in which a load impedance of r is connected to a voltage source. The no load voltage of r

(5) Furthermore, the third constraint implies the following equation: (6)

8 Baire Category Theorem and Uniform Boundedness

Lecture 12. Heat Exchangers. Heat Exchangers Chee 318 1

The International Association for the Properties of Water and Steam

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

a v2 r a' (4v) 2 16 v2 mg mg (2.4kg)(9.8m / s 2 ) 23.52N 23.52N N

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

6. Cascode Amplifiers and Cascode Current Mirrors

Remember: When an object falls due to gravity its potential energy decreases.

ANALOG ELECTRONICS DR NORLAILI MOHD NOH

Lucas Imperfect Information Model

LASER ABLATION ICP-MS: DATA REDUCTION

Scalars and Vectors Scalar

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

P 365. r r r )...(1 365

On Accurate Stress Determination in Laminated Finite Length Cylinders Subjected to Thermo Elastic Load

A) N B) 0.0 N C) N D) N E) N

Stellar Astrophysics. dt dr. GM r. The current model for treating convection in stellar interiors is called mixing length theory:

Section 4.2 Radians, Arc Length, and Area of a Sector

Rigid Bodies: Equivalent Systems of Forces

Optimization of the Electron Gun with a Permanent Ion Trap

UNIT10 PLANE OF REGRESSION

Spring 2002 Lecture #17

Module 11 Design of Joints for Special Loading. Version 2 ME, IIT Kharagpur

Section 3: Detailed Solutions of Word Problems Unit 1: Solving Word Problems by Modeling with Formulas

EEE2146 Microelectronics Circuit Analysis and Design. MIC2: Investigation of Amplifier Parameters of a Common-Collector Amplifier

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

A) (0.46 î ) N B) (0.17 î ) N

Contact, information, consultations

Optimization Frequency Design of Eddy Current Testing

Stress Distribution on a Single-Walled Carbon Nanohorn Embedded in an Epoxy Matrix Nanocomposite Under Axial Force

Review for the Mid-Term Exam

Analysis The characteristic length of the junction and the Biot number are

PHYS 1443 Section 003 Lecture #21

OBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470

Active Load. Reading S&S (5ed): Sec. 7.2 S&S (6ed): Sec. 8.2

Physics Exam II Chapters 25-29

5.1 Moment of a Force Scalar Formation

APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS

WYSE Academic Challenge 2004 Sectional Physics Solution Set

CS579 - Homework 2. Tu Phan. March 10, 2004

Exercises for Frequency Response. ECE 102, Fall 2012, F. Najmabadi

Drawing of Hollow Multilayered All-Polymer Fibers

I have not received unauthorized aid in the completion of this exam.

hitt Phy2049: Magnetism 6/10/2011 Magnetic Field Units Force Between Two Parallel Currents Force Between Two Anti-Parallel Currents

Summary of DLT method for stereo camera calibration, 3D reconstruction and robot-camera integration

Summary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating:

(8) Gain Stage and Simple Output Stage

element k Using FEM to Solve Truss Problems

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

Multistage Median Ranked Set Sampling for Estimating the Population Median

Electric Fields and Electric Forces

Transcription:

Mdule 9 Thn and thck cylndes Vesn 2 ME, IIT Khaagu

Lessn 3 Desgn ncles f thck cylndes Vesn 2 ME, IIT Khaagu

Instuctnal Objectves: At the end f ths lessn, the students shuld have the knwledge f: Falue thees aled t thck walled essue vessels. Vaatn f wall thckness wth ntenal essue based n dffeent falue thees. Falue cten f estessed thck cylndes. Cmasn f wall thckness vaatn wth ntenal essue f sld wall, sngle jacket and lamnated thck walled cylndes. Falue cten f thck walled cylndes wth autfettage. 9.3.1 Alcatn f thees f falue f thck walled essue vessels. Havng dscussed the stesses n thck walled cylndes t s mtant t cnsde the falue cten. The fve falue thees wll be cnsdeed n ths egad and the vaatn f wall thckness t ntenal adus at t/ adus at / wth / y f dffeent falue thees wuld be dscussed. A numbe f cases such as =0, =0 bth nn-ze and ae ssble but hee nly the cylndes wth clsed ends and subjected t an ntenal essue nly wll be cnsdeed, f an examle. 9.3.1.1 Maxmum Pncal Stess they Accdng t ths they falue ccus when maxmum ncal stess exceeds the stess at the tensle yeld nt. The falue envele accdng t ths falue mde s shwn n fgue-9.3.1.1.1 and the falue ctea ae gven by 1 = 2 = ± y. If =0 the maxmum values f ccumfeental and adal stesses ae gven by = θ(max) = + = (1) (max) = Vesn 2 ME, IIT Khaagu

Hee bth θ and ae the ncal stesses and θ s lage. Thus the cndtn f falue s based n θ and we have + =y whee y s the yeld stess. Ths gves (2) t = 1 1+ y y 1 2 + y - y + y 1 - y 9.3.1.1.1F- Falue envele accdng t Maxmum Pncal Stess They. 9.3.1.2 Maxmum Shea Stess they Accdng t ths they falue ccus when maxmum shea stess exceeds the maxmum shea stess at the tensle yeld nt. The falue envele accdng t ths cten s shwn n fgue- 9.3.1.2.1 and the maxmum shea stess s gven by τ max = 2 1 2 whee the ncal stesses 1 and 2 ae gven by Vesn 2 ME, IIT Khaagu

= = 1 θ 2 = = + Hee 1 s tensle and 2 s cmessve n natue. τ max may theefe be gven by τ = 2 max (3) and snce the falue cten s τ max = y / 2 we may wte t 1 = 1 2 y 1 (4) 2 1 yc - =1 yt - yc + yt 2 2 = yt 1 = yt + yt 1 1 = yc 2 = yc - yc 1 2 yt - =1 yc 9.3.1.2.1F- Falue envele accdng t Maxmum Shea Stess they. 9.3.1.3 Maxmum Pncal Stan they Accdng t ths they falue ccus when the maxmum ncal stan exceeds the stan at the tensle yeld nt. Vesn 2 ME, IIT Khaagu

1 ε1 1 ν 2 3 ε E = { ( + )} = y and ths gves ν ( ) + = 1 2 3 y whee ε y and y ae the yeld stan and stess esectvely. Fllwng ths the falue envele s as shwn n fgue-9.3.1.3.1. Hee the thee ncle stesses can be gven as fllws accdng t the standad 3D slutns: = = 1 θ (5) +, 2 = = and The falue cten may nw be wtten as 2 + ν + ν = y and ths gves 2 = = 3 z ( ) ( ) t 1+ 1 2ν y = 1 1 1+ν y (6) 2 + y + y - y 1 - y 9.3.1.3.1F- Falue envele accdng t Maxmum Pncal Stan they Vesn 2 ME, IIT Khaagu

9.3.1.4 Maxmum Dsttn Enegy They Accdng t ths they f the maxmum dsttn enegy exceeds the dsttn enegy at the tensle yeld nt falue ccus. The falue envele s shwn n fgue-9.3.1.4.1 and the dsttn enegy E d s gven by {( ) 2 ( ) 2 2 ( 1 ) } 1+ ν Ed = 1 2 + 2 3 + 3 6E Snce at the unaxal tensle yeld nt 2 = 3 = 0 and 1 = y E d at the tensle yeld nt = 1+ ν 3E We cnsde 1 = θ, 2 = and 3 = z and theefe = 1 + 2 y = (7) 2 = z The falue cten theefe educes t 1 = 2 3 y t 1 = 1 3 y 1 whch gves (8) Vesn 2 ME, IIT Khaagu

2 y - y y 1 - y 9.3.1.4.1F- Falue envele accdng t Maxmum Dsttn Enegy They 9.3.1.4.2. Plts f / y and t/ f dffeent falue ctea ae shwn n fgue- 1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 Maxmum ncal stess they Dsttn enegy they Maxmum stan they Maxmum shea stess they 1 2 3 4 5 6 7 8 t 9.3.1.4.2F- Cmasn f vaatn f aganst t f dffeent falue cten. The ctea develed and the lts aly t thck walled cylndes wth ntenal essue nly but smla ctea f cylndes wth extenal Vesn 2 ME, IIT Khaagu

essue nly n case whee bth ntenal and extenal essues exst may be develed. Hweve, n the bass f these esults we nte that the ate f ncease n / y s small at lage values f t/ f all the falue mdes cnsdeed. Ths means that at hghe values f small ncease n essue eques lage ncease n wall thckness. But snce the stesses nea the ute adus ae small, mateal at the ute adus f vey thck wall cylndes ae neffectvely used. It s theefe necessay t select mateals s that / y s easnably small. When ths s nt ssble estessed cylndes may be used. All the abve thees f falue ae based n the edctn f the begnnng f nelastc defmatn and these ae stctly alcable f ductle mateals unde statc ladng. Maxmum ncal stess they s wdely used f bttle mateals whch nmally fal by bttle factue. In sme alcatns f thck cylndes such as, gun baels n nelastc defmatn can be emtted f e functnng and thee desgn based n maxmum shea stess they maxmum dsttn enegy they ae accetable. F sme essue vessels a satsfacty functn s mantaned untl nelastc defmatn that stats fm the nne adus and seads cmletely thugh the wall f the cylnde. Unde such ccumstances nne f the falue thees wuld wk satsfactly and the cedue dscussed n sectn lessn 9.2 s t be used. 9.3.1.5 Falue ctea f e-stessed thck cylndes Falue ctea based n the thee methds f e-stessng wuld nw be dscussed. The adal and ccumfeental stesses develed dung shnkng a hllw cylnde ve the man cylnde ae shwn n fgue- 9.3.1.5.1. Vesn 2 ME, IIT Khaagu

s s Jacket Cylnde θ s 9.3.1.5.1F- Dstbutn f adal and ccumfeental stesses n a cmste thck walled cylnde subjected t an ntenal essue. Fllwng the analyss n sectn 9.2 the maxmum ntal (esdual) ccumfeental stess at the nne adus f the cylnde due t the cntact essue s s = 2 s θ s = s 2 and the maxmum ntal (esdual) ccumfeental stess at the nne adus f the jacket due t cntact essue s s + s θ s = s s = Suesng the ccumfeental stesses due t (cnsdeng the cmste cylnde as ne) the ttal ccumfeental stesses at the nne adus f the cylnde and nne adus f the jacket ae esectvely Vesn 2 ME, IIT Khaagu

= 2 + + s θ s = s 2 s s + s + θ = 2 s s s = + 2 These maxmum stesses shuld nt exceed the yeld stess and theefe we may wte 2 + 2s + s s = y (9) s + + + s s 2 s s 2 = y (10) It was shwn n sectn-9.2 that the cntact essue s s gven by Eδ = + + + s s s s s s (11) Fm (9), (10) and (11) t s ssble t elmnate s and exess t/ n tems f / y and ths s shwn gahcally n fgue-9.3.1.5.2. Lamnated 3.0 2.0 Sngle jacket Sld wall 1.0 0 0 1 2 3 4 5 6 7 8 t Vesn 2 ME, IIT Khaagu

9.3.1.5.2F- Plt f / y vs t/ f lamnated multlayeed, sngle jacket and sld wall cylndes. Ths shws that even wth a sngle jacket thee s a cnsdeable eductn n wall thckness and thus t cntbutes t an ecnmc desgn. As dscussed eale autfettage causes yeldng t stat at the nne be and wth the ncease n essue t seads utwads. If nw the essue s eleased the ute elastc laye exets adal cmessve essue n the nne tn and ths n tun causes adal cmessve stess nea the nne tn and tensle stess at the ute tn. F a gven flud essue dung autfettage a gven amunt f nelastc defmatn s duced and theefe n sevce the same flud essue may be used wthut causng any addtnal elastc defmatn. The self hng effect eaches ts maxmum value when yeldng just begns t sead t the ute wall. Unde ths cndtn the cylnde s sad t have eached a fully lastc cndtn and the cesndng ntenal flud essue s knwn as fully lastc essue, say, f. Ths essue may be fund by usng the educed equlbum equatn (3) n sectn- 9.2.1 whch s educed hee f cnvenence d θ = + d (12) Anthe equatn may be btaned by cnsdeng that when the maxmum shea stess at a nt n the cylnde wall eaches shea yeld value τ y t emans cnstant even afte futhe yeldng. Ths s gven by 1 2 ( ) θ =τ y (13) Hweve exements shw that fully lastc essue s eached befe nelastc defmatn has sead t evey nt n the wall. In fact Lude s lnes aea fst. Lude s lnes ae sal bands acss the cylnde wall such that the mateal between the bands etans elastcty. If the cylnde Vesn 2 ME, IIT Khaagu

s ket unde fully lastc essue f seveal hus unfm yeldng acss the cylnde wall wuld ccu. Ths gves d d = 2τ ylg+ c = 2 τ y / and n ntegatn we have Alyng the bunday cndtn at = = 0 we have and = 2τylg (14) θ = τ + 2 y 1 lg Als alyng the bunday cndtn at = = - f we have 2 lg f = τy (15) Snce the basc equatns ae ndeendent f whethe the cylndes ae en clsed ends, the exessns f and θ aly t bth the cndtns. The stess dstbutns ae shwn n fgue- 9.3.1.5.3. θ τ τ Tensle τ τ Cmessve 9.3.1.5.3F- Stess dstbutn n a thck walled cylnde wth autfettage If we ughly assume that 2τ y = y we have Vesn 2 ME, IIT Khaagu

f = lg y (16) The esults f maxmum ncal stess they and maxmum shea stess they alng wth the fully lastc esults ae eltted n fgue 9.3.1.5.4 whee we may cmae the elatve mets f dffeent falue ctea. It can be seen that cylndes wth autfettage may endue lage ntenal essue at elatvely lw wall thckness. 2.0 Maxmum autfettage 1.6 1.2 Maxmum ncal stess they 0.8 Maxmum shea stess they 0.4 0 1 2 3 4 5 6 7 8 9.3.1.5.4F- Plts f / y vs f maxmum shea stess they, maxmum ncal stess they and maxmum autfettage. Vesn 2 ME, IIT Khaagu

Fnally t must be emembeed that f tue essue vessel desgn t s essental t cnsult Ble Cdes f me cmlete nfmatn and gudelnes. Pessue vessels can be extemely dangeus even at elatvely lw essue and theefe the methdlgy stated hee s a ugh gude and shuld nt be cnsdeed t be a cmlete desgn methdlgy. 9.3.2 Pblems wth Answes Q.1: Detemne the necessay thckness f the shell lates f 2.5m damete ble wth the ntenal essue f 1MPa. The mateal s mld steel wth a tensle stength f 500MPa. Assumng an effcency f the lngtudnal welded jnt t be 75% and a fact f safety f 5 fnd the stess n the efated steel late. A.1: Cnsdeng that the ble desgn s based n thn cylnde ncles the shell thckness s gven by t = whee s the ble adus and η s the jnt effcency. η ty Ths gves t = 6 10 x1.25 500 x10 6 x0.75 5 = 0.0166m = 16.6 mm,say 20mm. The stess n the efated late s theefe gven by =.e. 62.5MPa t Q.2: A hydaulc cylnde wth an ntenal damete 250mm s subjected t an ntenal essue f 10 MPa. Detemne the wall thckness based n (a) Maxmum ncal stess they, b) Maxmum shea stess they and c) Vesn 2 ME, IIT Khaagu

A.2: Maxmum dsttn enegy they f falue. Cmae the esults wth wall thckness calculated based n thn cylnde assumtn. Assume the yeld stess f the cylnde mateal t be 60 MPa. Cnsdeng that the hydaulc cylndes ae nmally desgned n the thck cylnde assumtn we have fm sectn 9.3.1.1 f Maxmum Pncal stess They we have t = Hee 1+ 1 y y y 1 =10 / 60 0.167 and = 125 mm. Ths gves t = 22.9mm, say 23 mm Fm sectn 9.3.1.2 f Maxmum Shea Stess they we have t = Wth 1 1 2 y y 1 0.167 and = 125 mm, t = 28.2 mm, say 29 mm. Fm sectn 9.3.1.4 f maxmum dsttn enegy they we have 1 t = 1 1 3 y wth y 0.167 and = 125mm t = 23.3 mm, say 24 mm. Vesn 2 ME, IIT Khaagu

Cnsdeng a thn cylnde t = y and ths gves t = 20.875mm, say 21 mm. The thn cylnde aach yelds the lwest wall thckness and ths s bably nt safe. The lagest wall thckness f 29mm edcted usng the maxmum shea stess they s theefe adted. Q.3: A cylnde wth extenal damete 300mm and ntenal damete 200mm s subjected t an ntenal essue f 25 MPa. Cmae the elatve mets f a sngle thck walled cylnde and a cmste cylnde wth the nne cylnde whse ntenal and extenal dametes ae 200mm and 250 mm esectvely. A tube f 250 mm ntenal damete and 300mm extenal damete s shunk n the man cylnde. The safe tensle yeld stess f the mateal s 110 MPa and the stess set u at the junctn due t shnkage shuld nt exceed 10 MPa. A.3: We fst cnsde the stesses set u n a sngle cylnde and then n a cmste cylnde. Sngle cylnde The bunday cndtns ae at = 150mm = 0 and at = 100mm = - 20MPa Usng equatn (10) n sectn 9.2.1 C2 C 1 + 0 0.0225 = and C C2 1 + 20 0.01 = Ths gves C 1 = 16 and C 2 = -0.36 The h stess at = 100mm and = 150 mm ae 52 MPa and 32 MPa esectvely. Vesn 2 ME, IIT Khaagu

Stess n the cmste cylnde The stesses n the cylnde due t shnkage nly can be fund usng the fllwng bunday cndtns at = 150mm = 0 and at = 125mm = -10MPa Fllwng the abve cedue the h stess at = 150 mm and = 125mm ae 45.7MPa and 55.75MPa esectvely. The stess n the nne cylnde due t shnkage nly can be fund usng the fllwng bunday cndtns at = 100mm = 0 and at = 125mm = -10MPa Ths gves the h stess at = 100mm and = 125mm t be - 55.55 MPa and 45.55 MPa esectvely. Cnsdeng the ntenal essue nly n the cmlete cylnde the bunday cndtns ae at = 150mm = 0 and at = 100mm = -25 MPa Ths gves ( θ ) =150mm = 40MPa ( θ ) =125mm = 49 MPa ( θ ) =100mm = 65MPa. Resultant stess due t bth shnkage and ntenal essue Oute cylnde ( θ ) =150mm = 40 +45.7 = 85.7 MPa ( θ ) =125mm = 49+55.75 = 104.75 MPa Inne cylnde ( θ ) =125mm = 49-45.7 = 3.3 MPa ( θ ) =100mm = 65-55.75 = 9.25 MPa The stesses n bth the sngle cylnde and the cmste ae wthn the safe tensle stength f the mateal. Hweve n the sngle cylnde the stess gadent s lage acss the wall thckness wheeas n the cmste cylnde the stess vaatn s gentle. These esults ae llustated n fgue- 9.3.2.1 Vesn 2 ME, IIT Khaagu

104 MPa 85.7 MPa 54.67 MPa 3.3 MPa 38.24 MPa 9.25 MPa 200 mm 250 mm 300 mm 9.3.2.1F- Stess gadents (ccumfeental) n the nne and ute cylndes as well as the gadent acss the wall f a sngle cylnde. 9.3.3 Summay f ths Lessn The lessn ntally dscusses the alcatn f dffeent falue thees n thck walled essue vessels. Falue cten n tems f the at f wall thckness t the ntenal adus and the at f ntenal essue t yeld stess have been deved f dffeent falue cten. Falue cten f estessed cmste cylndes and cylndes wth autfettage have als been deved. Fnally cmasns f dffeent falue cten have been dscussed. 9.3.4 Refeences f Mdule-9 1) Desgn f machne elements by M.F.Stts, Pentce hall f Inda, 1991. 2) Machne desgn-an ntegated aach by Rbet L. Ntn, Peasn Educatn Ltd, 2001. Vesn 2 ME, IIT Khaagu

3) A textbk f machne desgn by P.C.Shama and D.K.Agawal, S.K.Kataa and sns, 1998. 4) Mechancal engneeng desgn by Jseh E. Shgley, McGaw Hll, 1986. 5) Fundamentals f machne cmnent desgn, 3 d edtn, by Rbet C. Juvnall and Kut M. Mashek, Jhn Wley & Sns, 2000. 6) Advanced stength and aled stess analyss, 2 nd Edtn, by Rchad G. Budynas, McGaw Hll Publshes, 1999. 7) Mechancs f Mateals by E.J. Hean, Pegamn Pess, 1977. Vesn 2 ME, IIT Khaagu