MECHANICS OF MATERIALS

Size: px
Start display at page:

Download "MECHANICS OF MATERIALS"

Transcription

1 00 The McGraw-Hill Copanies, Inc. All rights reserved. T Edition CHAPTER MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University Principle Stresses Under a Given Loading

2 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8 - Principle Stresses Under a Given Loading Introduction Principle Stresses in a Bea Saple Proble 8.1 Saple Proble 8. Design of a Transission Shaft Saple Proble 8.3 Stresses Under Cobined Loadings Saple Proble 8.5

3 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-3 Introduction In Chaps. 1 and, you learned how to deterine the noral stress due to centric loads In Chap. 3, you analyzed the distribution of shearing stresses in a circular eber due to a twisting couple In Chap. 4, you deterined the noral stresses caused by bending couples In Chaps. 5 and 6, you evaluated the shearing stresses due to transverse loads In Chap. 7, you learned how the coponents of stress are transfored by a rotation of the coordinate axes and how to deterine the principal planes, principal stresses, and axiu shearing stress at a point. In Chapter 8, you will learn how to deterine the stress in a structural eber or achine eleent due to a cobination of loads and how to find the corresponding principal stresses and axiu shearing stress

4 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-4 Principle Stresses in a Bea Prisatic bea subjected to transverse loading τ x xy My I VQ It τ Mc I VQ It Principal stresses deterined fro ethods of Chapter 7 Can the axiu noral stress within the cross-section be larger than Mc I

5 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-5 Principle Stresses in a Bea

6 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-6 Principle Stresses in a Bea Cross-section shape results in large values of τ xy near the surface where x is also large. ax ay be greater than

7 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-7 Saple Proble 8.1 SOLUTION: Deterine shear and bending oent in Section A-A Calculate the noral stress at top surface and at flange-web junction. A 160-kN force is applied at the end of a W00x5 rolled-steel bea. Neglecting the effects of fillets and of stress concentrations, deterine whether the noral stresses satisfy a design specification that they be equal to or less than 150 MPa at section A-A. Evaluate the shear stress at flangeweb junction. Calculate the principal stress at flange-web junction

8 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-8 Saple Proble 8.1 SOLUTION: Deterine shear and bending oent in Section A-A M V A A ( 160kN)( 0.375) 160kN 60kN - Calculate the noral stress at top surface and at flange-web junction. a b M 60kN A S MPa a y c b 10.9 MPa 3 ( 117. MPa)

9 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-9 Saple Proble 8.1 Evaluate shear stress at flange-web junction. Q τ b ( ) V Q A It 95.5MPa ( )( 3) 160kN ( )( ) Calculate the principal stress at flange-web junction ( 1 ) 1 ax + + b b τb ( 95.5) MPa 3 ( > 150 MPa) Design specification is not satisfied. 3

10 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8. SOLUTION: Deterine reactions at A and D. The overhanging bea supports a uniforly distributed load and a concentrated load. Knowing that for the grade of steel to used all 4 ksi and τ all 14.5 ksi, select the wideflange bea which should be used. Deterine axiu shear and bending oent fro shear and bending oent diagras. Calculate required section odulus and select appropriate bea section. Find axiu noral stress. Find axiu shearing stress.

11 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8. SOLUTION: Deterine reactions at A and D. M M Calculate required section odulus and select appropriate bea section. S in A D 0 0 M ax all R R D 59 kips 41kips select W1 6 bea section A Deterine axiu shear and bending oent fro shear and bending oent diagras. M V ax ax 39.4 kip in 43kips with V 4kip in in 4ksi 1. kips

12 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-1 Saple Proble 8. Find axiu shearing stress. Assuing unifor shearing stress in web, V 43 kips τ ax ax 5.1 ksi < 14.5ksi 8.40 in A web Find axiu noral stress. M ax 60kip in a ksi S 3 17in τ b b a V A y c web b (.6 ksi) kips 1.45ksii 8.40in 1.3ksi ax 1.3ksi 1.3ksi + + ( 1.45ksi) 1.4 ksi < 4ksi

13 00 The McGraw-Hill Copanies, Inc. All rights reserved Design of a Transission Shaft If power is transferred to and fro the shaft by gears or sprocket wheels, the shaft is subjected to transverse loading as well as shear loading. Noral stresses due to transverse loads ay be large and should be included in deterination of axiu shearing stress. Shearing stresses due to transverse loads are usually sall and contribution to axiu shear stress ay be neglected.

14 00 The McGraw-Hill Copanies, Inc. All rights reserved Design of a Transission Shaft At any section, τ Mc I Tc J where M M y + M z Maxiu shearing stress, τ ax ax c J M + + T ( τ ) Mc I Tc + J for a circular or annular cross - section, I τ Shaft section requireent, J c in M + T τ all ax J

15 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8.3 SOLUTION: Deterine the gear torques and corresponding tangential forces. Find reactions at A and B. Solid shaft rotates at 480 rp and transits 30 kw fro the otor to gears G and H; 0 kw is taken off at gear G and 10 kw at gear H. Knowing that all 50 MPa, deterine the sallest perissible diaeter for the shaft. Identify critical shaft section fro torque and bending oent diagras. Calculate iniu allowable shaft diaeter.

16 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8.3 SOLUTION: Deterine the gear torques and corresponding tangential forces. P 30kW TE 597 N πf π 80Hz F T T E C D T r E E 0kW π ( 80Hz) 10kW π ( 80Hz) ( ) 597 N kN 398N 199 N Find reactions at A and B. A B y y 0.93 kn.80 kn A B z z 6. kn.90 kn F F C D 6.63kN.49 kn

17 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8.3 Identify critical shaft section fro torque and bending oent diagras. M + T ax ( ) N + 597

18 00 The McGraw-Hill Copanies, Inc. All rights reserved Saple Proble 8.3 Calculate iniu allowable shaft diaeter. J c For a solid circular shaft, J c π c 3 M + T τ all N 50MPa c d 3 c

19 00 The McGraw-Hill Copanies, Inc. All rights reserved Stresses Under Cobined Loadings Wish to deterine stresses in slender structural ebers subjected to arbitrary loadings. Pass section through points of interest. Deterine force-couple syste at centroid of section required to aintain equilibriu. Syste of internal forces consist of three force coponents and three couple vectors. Deterine stress distribution by applying the superposition principle.

20 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-0 Stresses Under Cobined Loadings Axial force and in-plane couple vectors contribute to noral stress distribution in the section. Shear force coponents and twisting couple contribute to shearing stress distribution in the section.

21 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-1 Stresses Under Cobined Loadings Noral and shearing stresses are used to deterine principal stresses, axiu shearing stress and orientation of principal planes. Analysis is valid only to extent that conditions of applicability of superposition principle and Saint-Venant s principle are et.

22 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8 - Saple Proble 8.5 SOLUTION: Deterine internal forces in Section EFG. Evaluate noral stress at H. Evaluate shearing stress at H. Three forces are applied to a short steel post as shown. Deterine the principle stresses, principal planes and axiu shearing stress at point H. Calculate principal stresses and axiu shearing stress. Deterine principal planes.

23 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-3 Saple Proble 8.5 SOLUTION: Deterine internal forces in Section EFG. V M M x x y 30 kn 0 ( 50kN)( ) ( 75kN)( 0.00 ) 8.5kN M z P 50kN Note: Section properties, A I I x z ( )( ) V 75kN ( 30kN)( ) 3kN ( )( ) ( )( ) z

24 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-4 Saple Proble 8.5 Evaluate noral stress at H. y + 50kN P A + M I z z a + ( 8.5kN )( 0.05) M I ( 3kN )( 0.00 ) x x ( ) MPa 66.0MPa Evaluate shearing stress at H. Q τ yz V I A y z Q t x 17.5 MPa b 4 [( )( 0.045) ]( ) 3 ( )( 3) 75kN ( )( ) 4

25 00 The McGraw-Hill Copanies, Inc. All rights reserved. 8-5 Saple Proble 8.5 Calculate principal stresses and axiu shearing stress. Deterine principal planes. τ tan θ θ ax ax in p OC OC p R τ θ p R R CY CD ax ax in MPa MPa MPa MPa 70.4 MPa 7.4 MPa θ p 7.96

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 00 The cgraw-hill Copanies, Inc. All rights reserved. Third E CHAPTER 8 Principle ECHANICS OF ATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University

More information

MECHANICS OF MATERIALS Design of a Transmission Shaft

MECHANICS OF MATERIALS Design of a Transmission Shaft Design of a Transission Shaft If power is transferred to and fro the shaft by ygears or sprocket wheels, the shaft is subjected to transverse loading as well as shear loading. Noral stresses due to transverse

More information

MECHANICS OF MATERIALS Design of a Transmission Shaft

MECHANICS OF MATERIALS Design of a Transmission Shaft Design of a Transmission Shaft If power is transferred to and from the shaft by gears or sprocket wheels, the shaft is subjected to transverse loading as well as shear loading. Normal stresses due to transverse

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHATER MECHANICS OF MATERIAS Ferdinand. Beer E. Russell Johnston, Jr. John T. DeWolf Energy Methods ecture Notes: J. Walt Oler Teas Tech niversity 6 The McGraw-Hill Copanies, Inc. All rights reserved.

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third E CHAPTER 6 Shearing MECHANCS OF MATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University Stresses in Beams and Thin- Walled Members Shearing

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHAPTER MECHANCS OF MATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University Shearing Stresses in Beams and Thin- Walled Members 006 The McGraw-Hill

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHAPTER 6 MECHANCS OF MATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt Oler Texas Tech University Shearing Stresses in Beams and Thin- Walled Members

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third E CHAPTER 1 Introduction MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University Concept of Stress Contents Concept of Stress

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 2009 The McGraw-Hill Companies, Inc. All rights reserved. Fifth SI Edition CHAPTER 3 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Torsion Lecture Notes:

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 009 The McGraw-Hill Companies, Inc. All rights reserved. Fifth SI Edition CHAPTER 7 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Transformations of

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 2009 The McGraw-Hill Companies, Inc. All rights reserved. Fifth SI Edition CHAPTER 6 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J.

More information

PROBLEM 7.1 SOLUTION. σ = 5.49 ksi. τ = ksi

PROBLEM 7.1 SOLUTION. σ = 5.49 ksi. τ = ksi PROBLEM 7.1 For the given state of stress, determine the normal and shearing stresses exerted on the oblique face of the shaded triangular element shon. Use a method of analysis based on the equilibrium

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHAPTER MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Teas Tech Universit Transformations of Stress and Strain 006 The McGraw-Hill Companies,

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third E CHAPTER 2 Stress MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University and Strain Axial Loading Contents Stress & Strain:

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 00 The Graw-Hill Copanies, n. All rights reserved. Third E CHAPTER Pure ECHANCS OF ATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Bending Leture Notes: J. Walt Oler Teas Teh Universit

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 009 The McGraw-Hill Companies, nc. All rights reserved. Fifth S E CHAPTER 6 MECHANCS OF MATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt Oler Texas

More information

Stress Analysis Lecture 4 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Stress Analysis Lecture 4 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy Stress Analysis Lecture 4 ME 76 Spring 017-018 Dr./ Ahmed Mohamed Nagib Elmekawy Shear and Moment Diagrams Beam Sign Convention The positive directions are as follows: The internal shear force causes a

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

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS GE SI CHAPTER 3 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Torsion Lecture Notes: J. Walt Oler Texas Tech University Torsional Loads on Circular Shafts

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 006 The Graw-Hill Copanies, n. ll rights reserved. Fourth E CHTER ure ECHNCS OF TERLS Ferdinand. Beer E. Russell Johnston, Jr. John T. DeWolf Bending Leture Notes: J. Walt Oler Teas Teh Universit ECHNCS

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Fifth SI Edition CHTER 1 MECHNICS OF MTERILS Ferdinand. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Introduction Concept of Stress Lecture Notes: J. Walt Oler Teas Tech University Contents

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third CHTR Stress MCHNICS OF MTRIS Ferdinand. Beer. Russell Johnston, Jr. John T. DeWolf ecture Notes: J. Walt Oler Texas Tech University and Strain xial oading Contents Stress & Strain: xial oading Normal

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 00 The McGraw-Hill Companies, Inc. All rights reserved. T Edition CHAPTER MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Teas Tech Universit

More information

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL (Del I, teori; 1 p.) 1. In fracture echanics, the concept of energy release rate is iportant. Fro the fundaental energy balance of a case with possible crack growth, one usually derives the equation where

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 00 The Graw-Hill Copanies, n. All rights reserved. Third E CHAPTER 4 Pure ECHANCS OF ATERALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Bending Leture Notes: J. Walt Oler Teas Teh Universit

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS STATICS AND MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr, John T. DeWolf David E Mazurek \Cawect Mc / iur/» Craw SugomcT Hilt Introduction 1 1.1 What is Mechanics? 2 1.2 Fundamental

More information

Module 5: Theories of Failure

Module 5: Theories of Failure Module 5: Theories of Failure Objectives: The objectives/outcomes of this lecture on Theories of Failure is to enable students for 1. Recognize loading on Structural Members/Machine elements and allowable

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 Objectives At the end of this lesson, the students should be able to understand Power screw echanis. The thread fors used in power screws. Torque required to raise and lower a load in a power

More information

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy Stress Analysis Lecture 3 ME 276 Spring 2017-2018 Dr./ Ahmed Mohamed Nagib Elmekawy Axial Stress 2 Beam under the action of two tensile forces 3 Beam under the action of two tensile forces 4 Shear Stress

More information

Chapter 8. Lecture Notes Dr. Rakhmad Arief Siregar Kolej Universiti Kejuruteraan Utara Malaysia

Chapter 8. Lecture Notes Dr. Rakhmad Arief Siregar Kolej Universiti Kejuruteraan Utara Malaysia Chapter 8 Screw, Fasteners and the Design of Nonperanent Joint Lecture Notes Dr. Rakhad Arief Siregar Kolej Universiti Kejuruteraan Utara Malaysia Mechanical Engineering Design Sixth Metric Edition J.E.

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS For updated version, please click on http://ocw.ump.edu.my MECHANICS OF MATERIALS COURSE INFORMATION by Nur Farhayu Binti Ariffin Faculty of Civil Engineering and Earth Resources farhayu@ump.edu.my MECHANICS

More information

PHYSICS 2210 Fall Exam 4 Review 12/02/2015

PHYSICS 2210 Fall Exam 4 Review 12/02/2015 PHYSICS 10 Fall 015 Exa 4 Review 1/0/015 (yf09-049) A thin, light wire is wrapped around the ri of a unifor disk of radius R=0.80, as shown. The disk rotates without friction about a stationary horizontal

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third CHTR Stress MCHNICS OF MTRIS Ferdinand. Beer. Russell Johnston, Jr. John T. DeWolf ecture Notes: J. Walt Oler Texas Tech University and Strain xial oading Contents Stress & Strain: xial oading Normal

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 6 Shearing Stress in Beams & Thin-Walled Members

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 6 Shearing Stress in Beams & Thin-Walled Members EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 6 Shearing Stress in Beams & Thin-Walled Members Beams Bending & Shearing EMA 3702 Mechanics & Materials Science Zhe Cheng (2018)

More information

Stress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y.

Stress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y. 014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyright laws as they currently 9 7. Determine the normal stress and shear stress acting

More information

STATICS. Distributed Forces: Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

STATICS. Distributed Forces: Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr. 007 The McGraw-Hill Companies, nc. All rights reserved. Eighth E CHAPTER 9 VECTOR MECHANCS FOR ENGNEERS: STATCS Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University

More information

Mass Efficiency in Mechanical Design

Mass Efficiency in Mechanical Design Proceedings of the World Congress on Engineering 008 Vol II WCE 008, July - 4, 008, London, U.K. Mass Efficiency in Mechanical Design Subbiah Raalinga Abstract Using the axiu strain energy density in a

More information

材料力學 Mechanics of Materials

材料力學 Mechanics of Materials 材料力學 Mechanics of Materials 林峻立博士 國立陽明大學生物醫學工程系教授 Chun-Li Lin, PhD., Professor, Department of Biomedical Engineering National Yang-Ming University 1-1 Cortical bone: 10-20GPa Load Cross section b Moment

More information

Chapter 8 Deflection. Structural Mechanics 2 Dept of Architecture

Chapter 8 Deflection. Structural Mechanics 2 Dept of Architecture Chapter 8 Deflection Structural echanics Dept of rchitecture Outline Deflection diagras and the elastic curve Elastic-bea theory The double integration ethod oent-area theores Conjugate-bea ethod 8- Deflection

More information

Chapter 3. Load and Stress Analysis. Lecture Slides

Chapter 3. Load and Stress Analysis. Lecture Slides Lecture Slides Chapter 3 Load and Stress Analysis 2015 by McGraw Hill Education. This is proprietary material solely for authorized instructor use. Not authorized for sale or distribution in any manner.

More information

STATICS. Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Seventh Edition CHAPTER. Ferdinand P. Beer

STATICS. Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Seventh Edition CHAPTER. Ferdinand P. Beer 00 The McGraw-Hill Companies, nc. All rights reserved. Seventh E CHAPTER VECTOR MECHANCS FOR ENGNEERS: 9 STATCS Ferdinand P. Beer E. Russell Johnston, Jr. Distributed Forces: Lecture Notes: J. Walt Oler

More information

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015 Physics 2210 Fall 2015 sartphysics 20 Conservation of Angular Moentu 21 Siple Haronic Motion 11/23/2015 Exa 4: sartphysics units 14-20 Midter Exa 2: Day: Fri Dec. 04, 2015 Tie: regular class tie Section

More information

SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling.

SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling. SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling. Find: Determine the value of the critical speed of rotation for the shaft. Schematic and

More information

ME 025 Mechanics of Materials

ME 025 Mechanics of Materials ME 025 Mechanics of Materials General Information: Term: 2019 Summer Session Instructor: Staff Language of Instruction: English Classroom: TBA Office Hours: TBA Class Sessions Per Week: 5 Total Weeks:

More information

Mechanics of Solids I. Transverse Loading

Mechanics of Solids I. Transverse Loading Mechanics of Solids I Transverse Loading Introduction o Transverse loading applied to a beam results in normal and shearing stresses in transverse sections. o Distribution of normal and shearing stresses

More information

TORSION INCLUDING WARPING OF OPEN SECTIONS (I, C, Z, T AND L SHAPES)

TORSION INCLUDING WARPING OF OPEN SECTIONS (I, C, Z, T AND L SHAPES) Page1 TORSION INCLUDING WARPING OF OPEN SECTIONS (I, C, Z, T AND L SHAPES) Restrained warping for the torsion of thin-wall open sections is not included in most commonly used frame analysis programs. Almost

More information

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along

1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along (40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass

More information

Strength of Materials

Strength of Materials Strength of Materials Session Pure Bending 04 Leture note : Praudianto, M.Eng. g{ V ä Ä tçw ÄtÇÇ Çz XÇz ÇÜ Çz Xwâvtà ÉÇ WÑtÜàÅÇà g{ V ä Ä tçw ÄtÇÇ Çz XÇz ÇÜ Çz Xwâvtà ÉÇ WÑtÜàÅÇà Pure Bending: Prisati

More information

6. Bending CHAPTER OBJECTIVES

6. Bending CHAPTER OBJECTIVES CHAPTER OBJECTIVES Determine stress in members caused by bending Discuss how to establish shear and moment diagrams for a beam or shaft Determine largest shear and moment in a member, and specify where

More information

(Tech. Specification) Total Tank Height of Shell, H1 m 14.1 Maximum Design Liquid Level, H 2 m Net Design Liquid Height, H 2 m 13.

(Tech. Specification) Total Tank Height of Shell, H1 m 14.1 Maximum Design Liquid Level, H 2 m Net Design Liquid Height, H 2 m 13. A.1.0. Input Design Data Quantity of Tank Nos. 2 Diaeter, D 12 (Tech. Specification) Total Tank Height of Shell, H1 14.1 Maxiu Design Liquid Level, H 2 13.634 Net Design Liquid Height, H 2 13.27 Refer

More information

Advanced Structural Analysis EGF Section Properties and Bending

Advanced Structural Analysis EGF Section Properties and Bending Advanced Structural Analysis EGF316 3. Section Properties and Bending 3.1 Loads in beams When we analyse beams, we need to consider various types of loads acting on them, for example, axial forces, shear

More information

Module 2 Stresses in machine elements. Version 2 ME, IIT Kharagpur

Module 2 Stresses in machine elements. Version 2 ME, IIT Kharagpur Module Stresses in machine elements Lesson Compound stresses in machine parts Instructional Objectives t the end of this lesson, the student should be able to understand Elements of force system at a beam

More information

STATICS. Bodies VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

STATICS. Bodies VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr. N E 4 Equilibrium CHAPTER VECTOR MECHANICS FOR ENGINEERS: STATICS Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University of Rigid Bodies 2010 The McGraw-Hill Companies,

More information

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection Mechanics of Materials II Chapter III A review of the fundamental formulation of stress, strain, and deflection Outline Introduction Assumtions and limitations Axial loading Torsion of circular shafts

More information

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY Spring 2006 Final Examination STUDENT S NAME (please print) STUDENT S SIGNATURE STUDENT NUMBER IDE 110 CLASS SECTION INSTRUCTOR S NAME Do not turn this page until instructed to start. Write your name on

More information

Montgomery County Community College EGR 213 Mechanics of Materials 3-2-2

Montgomery County Community College EGR 213 Mechanics of Materials 3-2-2 Montgomery County Community College EGR 213 Mechanics of Materials 3-2-2 COURSE DESCRIPTION: This course covers the deformation of beams and shafts using energy methods and structural analysis, the analysis

More information

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)?

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)? IDE 110 S08 Test 1 Name: 1. Determine the internal axial forces in segments (1), (2) and (3). (a) N 1 = kn (b) N 2 = kn (c) N 3 = kn 2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at

More information

Actuators & Mechanisms Actuator sizing

Actuators & Mechanisms Actuator sizing Course Code: MDP 454, Course Nae:, Second Seester 2014 Actuators & Mechaniss Actuator sizing Contents - Modelling of Mechanical Syste - Mechaniss and Drives The study of Mechatronics systes can be divided

More information

MECHANICS OF MATERIALS. Analysis of Beams for Bending

MECHANICS OF MATERIALS. Analysis of Beams for Bending MECHANICS OF MATERIALS Analysis of Beams for Bending By NUR FARHAYU ARIFFIN Faculty of Civil Engineering & Earth Resources Chapter Description Expected Outcomes Define the elastic deformation of an axially

More information

DESIGN OF BEAMS AND SHAFTS

DESIGN OF BEAMS AND SHAFTS DESIGN OF EAMS AND SHAFTS! asis for eam Design! Stress Variations Throughout a Prismatic eam! Design of pristmatic beams! Steel beams! Wooden beams! Design of Shaft! ombined bending! Torsion 1 asis for

More information

ENT345 Mechanical Components Design

ENT345 Mechanical Components Design 1) LOAD AND STRESS ANALYSIS i. Principle stress ii. The maximum shear stress iii. The endurance strength of shaft. 1) Problem 3-71 A countershaft carrying two-v belt pulleys is shown in the figure. Pulley

More information

Modeling Diaphragms in 2D Models with Linear and Nonlinear Elements

Modeling Diaphragms in 2D Models with Linear and Nonlinear Elements Modeling Diaphrags in 2D Models with Linear and Nonlinear Eleents Vesna Terzic UC Berkeley October 2011 Introduction to the proble (1) Floor diaphrag need to be axially rigid to assure proper distribution

More information

Kernel Methods and Support Vector Machines

Kernel Methods and Support Vector Machines Intelligent Systes: Reasoning and Recognition Jaes L. Crowley ENSIAG 2 / osig 1 Second Seester 2012/2013 Lesson 20 2 ay 2013 Kernel ethods and Support Vector achines Contents Kernel Functions...2 Quadratic

More information

PROBLEM 5.1 SOLUTION. Reactions: Pb L Pa L. From A to B: 0 < x < a. Pb L Pb L Pb L Pbx L. From B to C: a < x < L Pa L. Pa L. L Pab At section B: M = L

PROBLEM 5.1 SOLUTION. Reactions: Pb L Pa L. From A to B: 0 < x < a. Pb L Pb L Pb L Pbx L. From B to C: a < x < L Pa L. Pa L. L Pab At section B: M = L PROBEM 5.1 For the beam and loading shown, (a) draw the shear and bending-moment diagrams, (b) determine the equations of the shear and bending-moment curves. SOUTION Reactions: From A to B: 0 < x < a

More information

[8] Bending and Shear Loading of Beams

[8] Bending and Shear Loading of Beams [8] Bending and Shear Loading of Beams Page 1 of 28 [8] Bending and Shear Loading of Beams [8.1] Bending of Beams (will not be covered in class) [8.2] Bending Strain and Stress [8.3] Shear in Straight

More information

4. SHAFTS. A shaft is an element used to transmit power and torque, and it can support

4. SHAFTS. A shaft is an element used to transmit power and torque, and it can support 4. SHAFTS A shaft is an element used to transmit power and torque, and it can support reverse bending (fatigue). Most shafts have circular cross sections, either solid or tubular. The difference between

More information

(48) CHAPTER 3: TORSION

(48) CHAPTER 3: TORSION (48) CHAPTER 3: TORSION Introduction: In this chapter structural members and machine parts that are in torsion will be considered. More specifically, you will analyze the stresses and strains in members

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHAPER MECHANICS OF MAERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John. DeWolf orsion Leture Notes: J. Walt Oler exas eh University 006 he MGraw-Hill Companies, In. All rights reserved. Contents

More information

Equilibrium. Rigid Bodies VECTOR MECHANICS FOR ENGINEERS: STATICS. Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

Equilibrium. Rigid Bodies VECTOR MECHANICS FOR ENGINEERS: STATICS. Eighth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr. Eighth E 4 Equilibrium CHAPTER VECTOR MECHANICS FOR ENGINEERS: STATICS Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University of Rigid Bodies Contents Introduction

More information

STATICS. Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr.

STATICS. Moments of Inertia VECTOR MECHANICS FOR ENGINEERS: Ninth Edition CHAPTER. Ferdinand P. Beer E. Russell Johnston, Jr. N E 9 Distributed CHAPTER VECTOR MECHANCS FOR ENGNEERS: STATCS Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Teas Tech Universit Forces: Moments of nertia Contents ntroduction

More information

EVALUATION OF DESIGN PROVISIONS FOR IN-PLANE SHEAR IN MASONRY WALLS COURTNEY LYNN DAVIS

EVALUATION OF DESIGN PROVISIONS FOR IN-PLANE SHEAR IN MASONRY WALLS COURTNEY LYNN DAVIS EVALUATION OF DESIGN PROVISIONS FOR IN-PLANE SHEAR IN MASONRY WALLS By COURTNEY LYNN DAVIS A thesis subitted in partial fulfillent of the requireents for the degree of MASTER OF SCIENCE IN CIVIL ENGINEERING

More information

CHAPTER 4: BENDING OF BEAMS

CHAPTER 4: BENDING OF BEAMS (74) CHAPTER 4: BENDING OF BEAMS This chapter will be devoted to the analysis of prismatic members subjected to equal and opposite couples M and M' acting in the same longitudinal plane. Such members are

More information

SOFTWARE FOR AASHTO LRFD COMBINED SHEAR AND TORSION COMPUTATIONS USING MODIFIED COMPRESSION FIELD THEORY AND 3D TRUSS ANALOGY

SOFTWARE FOR AASHTO LRFD COMBINED SHEAR AND TORSION COMPUTATIONS USING MODIFIED COMPRESSION FIELD THEORY AND 3D TRUSS ANALOGY Report No. K-TRAN: KSU-08-5 FINAL REPORT October 2011 SOFTWARE FOR AASHTO LRFD COMBINED SHEAR AND TORSION COMPUTATIONS USING MODIFIED COMPRESSION FIELD THEORY AND 3D TRUSS ANALOGY Abdul Hali Hali Hayder

More information

STATICS. Bodies. Vector Mechanics for Engineers: Statics VECTOR MECHANICS FOR ENGINEERS: Design of a support

STATICS. Bodies. Vector Mechanics for Engineers: Statics VECTOR MECHANICS FOR ENGINEERS: Design of a support 4 Equilibrium CHAPTER VECTOR MECHANICS FOR ENGINEERS: STATICS Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University of Rigid Bodies 2010 The McGraw-Hill Companies,

More information

Subject Code: R13110/R13 I B. Tech I Semester Regular Examinations Jan./Feb ENGINEERING MECHANICS

Subject Code: R13110/R13 I B. Tech I Semester Regular Examinations Jan./Feb ENGINEERING MECHANICS Set No - 1 I B. Tech I Seester Regular Exainations Jan./Feb. 2015 ENGINEERING MECHANICS (Coon to CE, ME, CSE, PCE, IT, Che E, Aero E, AME, Min E, PE, Metal E) Tie: 3 hours Max. Marks: 70 What is the principle

More information

WORCESTER POLYTECHNIC INSTITUTE

WORCESTER POLYTECHNIC INSTITUTE WORCESTER POLYTECHNIC INSTITUTE MECHANICAL ENGINEERING DEPARTMENT STRESS ANALYSIS ES-2502, C 2012 Lecture 17: 10 February 2012 General information Instructor: Cosme Furlong HL-151 (508) 831-5126 cfurlong@wpi.edu

More information

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4.

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4. PHYSICS 151 Notes for Online Lecture.4 Springs, Strings, Pulleys, and Connected Objects Hook s Law F = 0 F = -k x 1 x = 0 x = x 1 Let s start with a horizontal spring, resting on a frictionless table.

More information

Feature Extraction Techniques

Feature Extraction Techniques Feature Extraction Techniques Unsupervised Learning II Feature Extraction Unsupervised ethods can also be used to find features which can be useful for categorization. There are unsupervised ethods that

More information

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE 1 Chapter 3 Load and Stress Analysis 2 Chapter Outline Equilibrium & Free-Body Diagrams Shear Force and Bending Moments in Beams Singularity Functions Stress Cartesian Stress Components Mohr s Circle for

More information

Department of Physics Preliminary Exam January 3 6, 2006

Department of Physics Preliminary Exam January 3 6, 2006 Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHAPTER 2 MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt Oler Texas Tech University Stress and Strain Axial Loading 2.1 An Introduction

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science Zhe Cheng (2018) 2 Stress & Strain - Axial Loading Statics

More information

3 Hours/100 Marks Seat No.

3 Hours/100 Marks Seat No. *17304* 17304 14115 3 Hours/100 Marks Seat No. Instructions : (1) All questions are compulsory. (2) Illustrate your answers with neat sketches wherever necessary. (3) Figures to the right indicate full

More information

Downloaded from Downloaded from / 1

Downloaded from   Downloaded from   / 1 PURWANCHAL UNIVERSITY III SEMESTER FINAL EXAMINATION-2002 LEVEL : B. E. (Civil) SUBJECT: BEG256CI, Strength of Material Full Marks: 80 TIME: 03:00 hrs Pass marks: 32 Candidates are required to give their

More information

Comb resonator design (2)

Comb resonator design (2) Lecture 6: Comb resonator design () -Intro Intro. to Mechanics of Materials School of Electrical l Engineering i and Computer Science, Seoul National University Nano/Micro Systems & Controls Laboratory

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHATR Stress MCHANICS OF MATRIALS and Strain Axial Loading Stress & Strain: Axial Loading Suitability of a structure or machine may depend on the deformations in the structure as well as the stresses induced

More information

Seismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi.

Seismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi. Seisic Analysis of Structures by K Dutta, Civil Departent, II Delhi, New Delhi. Module 5: Response Spectru Method of Analysis Exercise Probles : 5.8. or the stick odel of a building shear frae shown in

More information

Monitoring and system identification of suspension bridges: An alternative approach

Monitoring and system identification of suspension bridges: An alternative approach Monitoring and syste identification of suspension bridges: An alternative approach Erdal Şafak Boğaziçi University, Kandilli Observatory and Earthquake Reseach Institute, Istanbul, Turkey Abstract This

More information

CLASSICAL TORSION AND AIST TORSION THEORY

CLASSICAL TORSION AND AIST TORSION THEORY CLASSICAL TORSION AND AIST TORSION THEORY Background The design of a crane runway girder has not been an easy task for most structural engineers. Many difficult issues must be addressed if these members

More information

Supplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators

Supplementary Information for Design of Bending Multi-Layer Electroactive Polymer Actuators Suppleentary Inforation for Design of Bending Multi-Layer Electroactive Polyer Actuators Bavani Balakrisnan, Alek Nacev, and Elisabeth Sela University of Maryland, College Park, Maryland 074 1 Analytical

More information

FEM-Design. Verification Examples. version Motto: ,,There is singularity between linear and nonlinear world. (Dr.

FEM-Design. Verification Examples. version Motto: ,,There is singularity between linear and nonlinear world. (Dr. FEM-Design version.3 8 Motto:,,There is singularity between linear and nonlinear world. (Dr. Ire Bojtár) StruSoft AB Visit the StruSoft website for copany and FEM-Design inforation at www.strusoft.co Copyright

More information

Physical Science and Engineering. Course Information. Course Number: ME 100

Physical Science and Engineering. Course Information. Course Number: ME 100 Physical Science and Engineering Course Number: ME 100 Course Title: Course Information Basic Principles of Mechanics Academic Semester: Fall Academic Year: 2016-2017 Semester Start Date: 8/21/2016 Semester

More information

7 TRANSVERSE SHEAR transverse shear stress longitudinal shear stresses

7 TRANSVERSE SHEAR transverse shear stress longitudinal shear stresses 7 TRANSVERSE SHEAR Before we develop a relationship that describes the shear-stress distribution over the cross section of a beam, we will make some preliminary remarks regarding the way shear acts within

More information

5. What is the moment of inertia about the x - x axis of the rectangular beam shown?

5. What is the moment of inertia about the x - x axis of the rectangular beam shown? 1 of 5 Continuing Education Course #274 What Every Engineer Should Know About Structures Part D - Bending Strength Of Materials NOTE: The following question was revised on 15 August 2018 1. The moment

More information

) = slugs/ft 3. ) = lb ft/s. ) = ft/s

) = slugs/ft 3. ) = lb ft/s. ) = ft/s 1. Make use of Tables 1. in the text book (See the last page in this assignent) to express the following quantities in SI units: (a) 10. in./in, (b) 4.81 slugs, (c).0 lb, (d) 7.1 ft/s, (e) 0.04 lb s/ft.

More information

APPENDIX (LECTURE #2) :

APPENDIX (LECTURE #2) : APPENDIX (LECTURE #) : I. Review / Suary of Cantilever Bea Theory II. Suary of Haronic Motion III. Liits of orce Detection IV. Excerpts fro Vibrations and Waves, A.P. rench, W. W. Norton and Copany, 97

More information

Sub. Code:

Sub. Code: Important Instructions to examiners: ) The answers should be examined by key words and not as word-to-word as given in the model answer scheme. ) The model answer and the answer written by candidate may

More information

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10 There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference

More information

2. Polar moment of inertia As stated above, the polar second moment of area, J is defined as. Sample copy

2. Polar moment of inertia As stated above, the polar second moment of area, J is defined as. Sample copy GATE PATHSHALA - 91. Polar moment of inertia As stated above, the polar second moment of area, is defined as z π r dr 0 R r π R π D For a solid shaft π (6) QP 0 π d Solid shaft π d Hollow shaft, " ( do

More information

Chapter 29 Solutions

Chapter 29 Solutions Chapter 29 Solutions 29.1 (a) up out of the page, since the charge is negative. (c) no deflection (d) into the page 29.2 At the equator, the Earth's agnetic field is horizontally north. Because an electron

More information