CYLINDER MADE FROM BRITTLE MATERIAL AND SUBJECT TO INTERNAL PRESSURE ONLY

Similar documents
OVERVIEW Using Similarity and Proving Triangle Theorems G.SRT.4

Chapter 3, Solution 1C.

The Laws of Sines and Cosines

SMARANDACHE GROUPOIDS

Intro to Nuclear and Particle Physics (5110)

Physic 231 Lecture 33

10 Vector Integral Calculus

11.2. Infinite Series

Math 259 Winter Solutions to Homework #9

Introduction to Three-phase Circuits. Balanced 3-phase systems Unbalanced 3-phase systems

Physics 107 HOMEWORK ASSIGNMENT #20

I1 = I2 I1 = I2 + I3 I1 + I2 = I3 + I4 I 3

CS 4758 Robot Kinematics. Ashutosh Saxena

378 Relations Solutions for Chapter 16. Section 16.1 Exercises. 3. Let A = {0,1,2,3,4,5}. Write out the relation R that expresses on A.

MA123, Chapter 10: Formulas for integrals: integrals, antiderivatives, and the Fundamental Theorem of Calculus (pp.

5. (±±) Λ = fw j w is string of even lengthg [ 00 = f11,00g 7. (11 [ 00)± Λ = fw j w egins with either 11 or 00g 8. (0 [ ffl)1 Λ = 01 Λ [ 1 Λ 9.

Wp/Lmin. Wn/Lmin 2.5V

QUADRATIC EQUATIONS OBJECTIVE PROBLEMS

September 13 Homework Solutions

7. SOLVING OBLIQUE TRIANGLES: THE LAW OF SINES

ME306 Dynamics, Spring HW1 Solution Key. AB, where θ is the angle between the vectors A and B, the proof

MAT 1275: Introduction to Mathematical Analysis

Farey Fractions. Rickard Fernström. U.U.D.M. Project Report 2017:24. Department of Mathematics Uppsala University

3.2.2 Kinetics. Maxwell Boltzmann distribution. 128 minutes. 128 marks. Page 1 of 12

Bridging the gap: GCSE AS Level

Interference is when two (or more) sets of waves meet and combine to produce a new pattern.

PRE-BOARD MATHEMATICS-1st (Held on 26 December 2017)

BME 207 Introduction to Biomechanics Spring 2018

Torsion, Thermal Effects and Indeterminacy

Static Failure (pg 206)

An Introduction to Robot Kinematics. Renata Melamud

MECHANICS OF SOLIDS TORSION TUTORIAL 2 TORSION OF THIN WALLED SECTIONS AND THIN STRIPS

( ) WYSE ACADEMIC CHALLENGE Regional Physics Exam 2009 Solution Set. 1. Correct answer: D. m t s. 2. Correct answer: A. 3.

Regular Language. Nonregular Languages The Pumping Lemma. The pumping lemma. Regular Language. The pumping lemma. Infinitely long words 3/17/15

Thin and Thick Cylinders and Spheres

Homework Assignment 3 Solution Set

Phys. 506 Electricity and Magnetism Winter 2004 Prof. G. Raithel Problem Set 1 Total 30 Points. 1. Jackson Points

SVMs for regression Non-parametric/instance based classification method

Path to static failure of machine components

Problem Solving 7: Faraday s Law Solution

Support vector machines for regression

,:,,i1iit. Metric SO-thread DIN 13 Tolerance zones screw-in group..n"(norma) British Standardfine threads BS 84 Gauge dimensions BS 919

The graphs of Rational Functions

Name: Period: Date: PERIODIC TABLE NOTES ADVANCED CHEMISTRY

Physics 102. Final Examination. Spring Semester ( ) P M. Fundamental constants. n = 10P

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.)

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

Name: Period: Date: PERIODIC TABLE NOTES HONORS CHEMISTRY

Physics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:

Bases for Vector Spaces

Nondeterminism and Nodeterministic Automata

WYSE Academic Challenge Regional Physics 2008 SOLUTION SET

2 Axially Loaded Numbers

ELG3150 DGD 6 P9.5; P9.7; P9.13; P9.18; AP9.5; DP9.2

1 Nondeterministic Finite Automata

Theory of a vertically loaded Suction Pile in SAND

Surface Integrals of Vector Fields

Technote 6. Op Amp Definitions. April 1990 Revised 11/22/02. Tim J. Sobering SDE Consulting

VERTICAL ARM AB M B. MAXIMUM STRESSES occur on opposite sides of the vertical arm. MAXIMUM TENSILE STRESS. s t P A M(d 2 2)

Chapter 1: Logarithmic functions and indices

We partition C into n small arcs by forming a partition of [a, b] by picking s i as follows: a = s 0 < s 1 < < s n = b.

4. Eccentric axial loading, cross-section core

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

and that at t = 0 the object is at position 5. Find the position of the object at t = 2.

( 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

UNIVERSITY OF IOANNINA DEPARTMENT OF ECONOMICS. M.Sc. in Economics MICROECONOMIC THEORY I. Problem Set II

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Matrix Eigenvalues and Eigenvectors September 13, 2017

Advanced Structural Analysis EGF Cylinders Under Pressure

set is not closed under matrix [ multiplication, ] and does not form a group.

The Fundamental Theorem of Calculus. The Total Change Theorem and the Area Under a Curve.

Lecture 3 ( ) (translated and slightly adapted from lecture notes by Martin Klazar)

. (7.1.1) This centripetal acceleration is provided by centripetal force. It is directed towards the center of the circle and has a magnitude

Calculus 2: Integration. Differentiation. Integration

12 TRANSFORMING BIVARIATE DENSITY FUNCTIONS

Lecture 13 - Linking E, ϕ, and ρ

p-adic Egyptian Fractions

PH2200 Practice Exam I Summer 2003

MATH FIELD DAY Contestants Insructions Team Essay. 1. Your team has forty minutes to answer this set of questions.

2.4 Linear Inequalities and Interval Notation

PHYSICS 211 MIDTERM I 21 April 2004

Stress Concentrations

Asynchronous Sequen<al Circuits

Automorphism Group of an Inverse Fuzzy Automaton

2 b. , a. area is S= 2π xds. Again, understand where these formulas came from (pages ).

MATH SPEAK - TO BE UNDERSTOOD AND MEMORIZED

Use 10 m/s 2 for the acceleration due to gravity.

Physics 2135 Exam 3 April 21, 2015

5.1 Properties of Inverse Trigonometric Functions.

Section 7.1 Integration by Substitution

MAE 322 Machine Design. Dr. Hodge Jenkins Mercer University

Improper Integrals. The First Fundamental Theorem of Calculus, as we ve discussed in class, goes as follows:

Sodium D-line doublet. Lectures 5-6: Magnetic dipole moments. Orbital magnetic dipole moments. Orbital magnetic dipole moments

The Trapezoidal Rule

1 Probability Density Functions

Chemistry 20 Lesson 11 Electronegativity, Polarity and Shapes

Part 3 Introduction to statistical classification techniques

CMPSCI 250: Introduction to Computation. Lecture #31: What DFA s Can and Can t Do David Mix Barrington 9 April 2014

Level I MAML Olympiad 2001 Page 1 of 6 (A) 90 (B) 92 (C) 94 (D) 96 (E) 98 (A) 48 (B) 54 (C) 60 (D) 66 (E) 72 (A) 9 (B) 13 (C) 17 (D) 25 (E) 38

Math 124B January 24, 2012

Transcription:

CYLINDER MADE FROM BRITTLE MATERIAL AND SUBJECT TO INTERNAL PRESSURE ONLY STRESS DISTRIBUTION ACROSS THE CYLINDER WALL The stresses n cyner suject t ntern ressure ny cn e etermne t tw ctns n the cyner w nmey, nner n uter surfce f the cyner w. Ths s ustrte n Fg. ew: STRESSES AT INNER SURFACE OF CYLINDER At ths ctn the stresses nuce re gven y the exressns [ ] Tngent stress + Lngtun stress t t * ( R stress r r STRESSES AT OUTER SURFACE OF CYLINDER At ths ctn the stresses nuce re gven y the exressns Tngent stress Lngtun stress R stress 0 r r t t * (

PRINCIPAL STRESSES AND PLANES The stresses entfe t nner n uter surfce re rnc stresses. Ths s ecuse t th surfces, the e s fu ressure whch s nrm tht gves rse t nrm stress. The nrm stress rsng ut f ressure t th surfces s therefre rnc stress. The tngent n ngtun rectns re erencur t the r ne, n re therefre s rnc nes; crryng rnc stresses whch re therefre s mxmum nrm stresses n thse nes. LOCATION OF EXTREME STRESSES The nner surfce s then the ctn f extreme stresses where fure s execte t ccur. Ths s ecuse [ ] The tngent stress t nner surfce + tngent stress t uter surfce s greter thn the t t t t * ( The ngtun stress s the sme vue t th nner n uter surfce The r stress r r t nner surfce s greter thn the r stress 0 r r CYLINDER FROM BRITTLE MATERIAL SUBJECT TO INTERNAL PRESSURE Fr rtte mter such s cst rn, the mxmum nrm stress thery f fure s e. Ths sys: When fure ccurs n ny mter, the mxmum nrm stress t the nt f fure equs r excees the mxmum nrm stress when fure ccurs n the tensn test secmen. PRINCIPAL STRESSES AT THE POINT OF FAILURE Mxmum n mnmum nrm stresses re,, where f f In the cse f cyner suject t ntern ressure ny, the stresses re extreme t the nner surfce, n re gven y t [ + ], * r (, Nyngs Pge /6/009

MAXIMUM NORMAL STRESS WHEN FAILURE OCCURS IN SIMPLE TENSION SPECIMEN When fure ccurs n the sme tensn secmen f rtte mter, the stress s gven y Sut, Or Suc Where S S ut uc Utmte tense strength f the mter Utmte cmressve strength f the mter STRESS CAUSING FAILURE AT THE INSIDE SURFACE OF CYLINDER At ths ctn Mxmum n mnmum nrm stresses re,, where But f f [ + ] t, n r The mxmum nrm stress t the ctn s tense whe the mnmum nrm stress s cmressve. Fure cu therefre e cuse y ether the mxmum tense stress, r the mnmum cmressve stress. Hwever, the cst rn mter hs cmressve strength whch s mny tmes hgher thn the tense strength. Fure w therefre e cuse y the hgher tense stress ctng n the wer tense strength f the mter. Fure w therefre ccur when t [ + ] Sut Ayng fctr f sfety n the strength f the mter Nyngs Pge /6/009

Ayng fctr f Sut, where f. s sfety Desgn stress fr the chsen rtte mter f. s Fctr f sfety The esgn equtn then ecmes [ + ] [ + ] ( ( + + Smfyng But t where + + + Extern meter f Intern meter f + t + + cyner cyner + t + ( + + t Where t w thckness f cyner The ve s Lme s equtn fr the esgn f cyner suject t ntern ressure ny n me frm rtte mter t + Lme' s equtn fr thck cyner f rtte mter Nyngs Pge 4 /6/009

THICK AND THIN CYLINDER-BRITTLE MATERIAL LAME'S EQUATION-WALL THICKNESS Inse Intern Desgn LAME Dmeter Pressure Stress mm. ( ( mm M M ( + t ( + + + + 00 7.5 6.5 8.5.05.0 0.0 50 4. 00 7.5 5.5 9.5..05 0.05 50 8. 00 7.5 4.5 40.5.7.08 0.08 50.5 00 4 7.5.5 4.5.4. 0. 50 7.0 00 5 7.5.5 4.5..4 0.4 50.5 00 6 7.5.5 4.5.8.8 0.8 50 6. 00 7 7.5 0.5 44.5.46. 0. 50. 00 8 7.5 9.5 45.5.54.4 0.4 50 6. 00 9 7.5 8.5 46.5.6.8 0.8 50 4.6 00 0 7.5 7.5 47.5.7. 0. 50 47. 00 7.5 5.5 49.5.94.9 0.9 50 59.0 00 7.5 4.5 50.5.06.44 0.44 50 65.4 00 4 7.5.5 5.5.9.48 0.48 50 7. 00 5 7.5.5 5.5..5 0.5 50 79. 00 6 7.5.5 5.5.49.58 0.58 50 86.6 00 7 7.5 0.5 54.5.66.6 0.6 50 94.6 00 8 7.5 9.5 55.5.85.69 0.69 50 0. 00 9 7.5 8.5 56.5.05.75 0.75 50.

THICK AND THIN CYLINDER-BRITTLE MATERIAL LAME'S EQUATION-WALL THICKNESS Inse Intern Desgn LAME Dmeter Pressure Stress mm. ( ( mm M M ( + t ( + + + + 600 7.5 6.5 8.5.05.0 0.0 00 8. 600 7.5 5.5 9.5..05 0.05 00 6.5 600 7.5 4.5 40.5.7.08 0.08 00 5.0 600 4 7.5.5 4.5.4. 0. 00.9 600 5 7.5.5 4.5..4 0.4 00 4. 600 6 7.5.5 4.5.8.8 0.8 00 5.5 600 7 7.5 0.5 44.5.46. 0. 00 6.4 600 8 7.5 9.5 45.5.54.4 0.4 00 7.6 600 9 7.5 8.5 46.5.6.8 0.8 00 8. 600 0 7.5 7.5 47.5.7. 0. 00 94. 600 7.5 5.5 49.5.94.9 0.9 00 8.0 600 7.5 4.5 50.5.06.44 0.44 00 0.7 600 4 7.5.5 5.5.9.48 0.48 00 44. 600 5 7.5.5 5.5..5 0.5 00 58. 600 6 7.5.5 5.5.49.58 0.58 00 7. 600 7 7.5 0.5 54.5.66.6 0.6 00 89. 600 8 7.5 9.5 55.5.85.69 0.69 00 06. 600 9 7.5 8.5 56.5.05.75 0.75 00 4. Nyngs Pge 6 /6/009