MECHANICS OF MATERIALS Design of a Transmission Shaft

Size: px
Start display at page:

Download "MECHANICS OF MATERIALS Design of a Transmission Shaft"

Transcription

1 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 loads ay be large and should be included in dt deterination ti of axiu shearing stress. Shearing stresses due to transverse loads are usually sall and contribution to axiu shear stress ay be neglected. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-1

2 Design of a Transission Shaft At any section, Mc σ where M M y + M I Tc τ J Maxiu shearing stress, τ ax σ + τ ( ) Mc I Tc + J for a circular or annular cross - section, I τ ax c J M + T Shaft section requireent, M + T J c τ all 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8 - in ax J

3 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 σ 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. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-3

4 Saple Proble 8.3 SOLUTION: Deterine the gear torques and corresponding tangential forces. T F E E P T r 30kW πfπ f π ( 8H ) E E 597 N 0.16 ( 8H) 597 N 3.73kN 0kW T C 398N FC π 10kW T D 199 N F π 8H D ( ) Find reactions at A and B. A B y y 0.93 kn.80 kn A B 6. kn.90 kn 6.63kN.49 kn 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-4

5 Saple Proble 8.3 Identify critical shaft section fro torque and bending oent diagras. ( ) M + M + T y ax N The McGraw-Hill Copanies, Inc. All rights reserved. 8-5

6 Saple Proble 8.3 Calculate iniu allowable shaft diaeter. J c M y + M + T τ all 1357 N MPa 6 3 For a solid circular shaft, J c c π 3 c d c The McGraw-Hill Copanies, Inc. All rights reserved. 8-6

7 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. Dt Deterine stress distribution ditibti by applying the superposition principle. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-7

8 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. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-8

9 Stresses Under Cobined Loadings Noral and shearing stresses are used to deterine principal p 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. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-9

10 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. 006 The McGraw-Hill Copanies, Inc. All rights reserved. 8-10

11 Saple Proble 8.5 SOLUTION: Deterine internal forces in Section EFG. V M x x 30 kn P 50kN 75kN ( 50kN)( ) ( 75kN)( 0.00 ) 8.5kN M y 0 M Note: Section properties, V ( 30kN)( ) 3kN 3 A ( )( ) I x I ( )( ) ( )( ) The McGraw-Hill Copanies, Inc. All rights reserved. 8-11

12 Saple Proble 8.5 Evaluate noral stress at H. σ y P + + A M I a 50kN M I x x b ( 3kN )( 0.00 ) ( 8.5kN )( 0.05) ( ) MPa 66.0MPa Evaluate shearing stress at H. Q τ y A y V I Q t x [( )( 0.045) ]( ) 17.5 MPa 3 ( )( 3) 75kN ( )( ) 006 The McGraw-Hill Copanies, Inc. All rights reserved

13 Saple Proble 8.5 Calculate principal stresses and axiu shearing stress. Deterine principal i planes. τ ax R MPa σ σ ax in tan θ θ p OC OC p R R CY CD τ ax σ σ θ p ax in MPa MPa MPa 70.4MPa 7.4 MPa θ p The McGraw-Hill Copanies, Inc. All rights reserved. 8-13

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS 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

More information

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 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

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

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

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

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

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

PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics

PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics Page1 PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [2910601] Introduction, Fundamentals of Statics 1. Differentiate between Scalar and Vector quantity. Write S.I.

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

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

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

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

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

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

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

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

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

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

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

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

In the session you will be divided into groups and perform four separate experiments:

In the session you will be divided into groups and perform four separate experiments: Mechanics Lab (Civil Engineers) Nae (please print): Tutor (please print): Lab group: Date of lab: Experients In the session you will be divided into groups and perfor four separate experients: (1) air-track

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

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

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

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

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

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

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. GTE 2016 Q. 1 Q. 9 carry one mark each. D : SOLID MECHNICS Q.1 single degree of freedom vibrating system has mass of 5 kg, stiffness of 500 N/m and damping coefficient of 100 N-s/m. To make the system

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

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - V PUMPS

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - V PUMPS CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - V PUMPS Centrifugal pups - Miniu speed to start the pup - NPSH - Cavitations in pups Operating characteristics - Multistage pups - Reciprocating pups - Negative

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

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 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

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

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

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

PROBLEM 3.3 ( )(45 10 ) T 5.17 kn m. A c c. 2 J c, (2)( ) 2 ( ) mm ( )

PROBLEM 3.3 ( )(45 10 ) T 5.17 kn m. A c c. 2 J c, (2)( ) 2 ( ) mm ( ) 0 mm PROEM..4 m 45 mm (a) Determine the torque that causes a maximum shearing stress of 45 MPa in the hollow cylindrical steel shaft shown. Determine the maximum shearing stress caused by the same torque

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

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

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

(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

APPENDIX 1 MODEL CALCULATION OF VARIOUS CODES

APPENDIX 1 MODEL CALCULATION OF VARIOUS CODES 163 APPENDIX 1 MODEL CALCULATION OF VARIOUS CODES A1.1 DESIGN AS PER NORTH AMERICAN SPECIFICATION OF COLD FORMED STEEL (AISI S100: 2007) 1. Based on Initiation of Yielding: Effective yield moment, M n

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

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

ELG3311: Assignment 3

ELG3311: Assignment 3 LG33: ssignent 3 roble 6-: The Y-connected synchronous otor whose naeplate is shown in Figure 6- has a perunit synchronous reactance of 0.9 and a per-unit resistance of 0.0. (a What is the rated input

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

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

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

) = 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

CIVL222 STRENGTH OF MATERIALS. Chapter 6. Torsion

CIVL222 STRENGTH OF MATERIALS. Chapter 6. Torsion CIVL222 STRENGTH OF MATERIALS Chapter 6 Torsion Definition Torque is a moment that tends to twist a member about its longitudinal axis. Slender members subjected to a twisting load are said to be in torsion.

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

EN40: Dynamics and Vibrations. Final Examination Monday May : 2pm-5pm

EN40: Dynamics and Vibrations. Final Examination Monday May : 2pm-5pm EN40: Dynaics and Vibrations Final Exaination Monday May 13 013: p-5p School of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on this exaination. You

More information

Helical Gears n A Textbook of Machine Design

Helical Gears n A Textbook of Machine Design 1066 n A Textbook of Machine Design C H A P T E R 9 Helical Gears 1. Introduction.. Terms used in Helical Gears. 3. Face Width of Helical Gears. 4. Formative or Equivalent Number of Teeth for Helical Gears.

More information

28 Innovative Solutions in the Field of Engineering Sciences

28 Innovative Solutions in the Field of Engineering Sciences Applied Mechanics and Materials ubitted: 14-5-1 IN: 166-748, Vol. 59, pp 7-1 Accepted: 14-5-1 doi:1.48/www.scientific.net/amm.59.7 Online: 14-6- 14 Trans Tech Publications, witerland The Vibration Based

More information

In this chapter we will start the discussion on wave phenomena. We will study the following topics:

In this chapter we will start the discussion on wave phenomena. We will study the following topics: Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical

More information

Influence lines for statically indeterminate structures. I. Basic concepts about the application of method of forces.

Influence lines for statically indeterminate structures. I. Basic concepts about the application of method of forces. Influence lines for statically indeterinate structures I. Basic concepts about the application of ethod of forces. The plane frae structure given in Fig. is statically indeterinate or redundant with degree

More information

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work. It is most beneficial to you to write this mock final exam UNDER EXAM CONDITIONS. This means: Complete the exam in 3 hours. Work on your own. Keep your textbook closed. Attempt every question. After the

More information

SECTION A. 8 kn/m. C 3 m 3m

SECTION A. 8 kn/m. C 3 m 3m SECTION Question 1 150 m 40 kn 5 kn 8 kn/m C 3 m 3m D 50 ll dimensions in mm 15 15 Figure Q1(a) Figure Q1(b) The horizontal beam CD shown in Figure Q1(a) has a uniform cross-section as shown in Figure

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

Internal Internal Forces Forces

Internal Internal Forces Forces Internal Forces ENGR 221 March 19, 2003 Lecture Goals Internal Force in Structures Shear Forces Bending Moment Shear and Bending moment Diagrams Internal Forces and Bending The bending moment, M. Moment

More information

Research on Power Output Characteristics of Magnetic Core in Energy Harvesting Devices

Research on Power Output Characteristics of Magnetic Core in Energy Harvesting Devices Sensors & Transducers Vol. 74 Issue 7 July 04 pp. 53-59 Sensors & Transducers 04 by IFSA Publishing S. L. http://www.sensorsportal.co Research on Power Output Characteristics of Magnetic Core in Energy

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

Torsion of shafts with circular symmetry

Torsion of shafts with circular symmetry orsion of shafts with circular symmetry Introduction Consider a uniform bar which is subject to a torque, eg through the action of two forces F separated by distance d, hence Fd orsion is the resultant

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

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

CHAPTER 15: Vibratory Motion

CHAPTER 15: Vibratory Motion CHAPTER 15: Vibratory Motion courtesy of Richard White courtesy of Richard White 2.) 1.) Two glaring observations can be ade fro the graphic on the previous slide: 1.) The PROJECTION of a point on a circle

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

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.

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

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 Mechanics of Materials 2. Introduction Dr. Rami Zakaria References: 1. Engineering Mechanics: Statics, R.C. Hibbeler, 12 th ed, Pearson 2. Mechanics of Materials: R.C. Hibbeler, 9 th ed, Pearson 3. Mechanics

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

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

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

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 10 ACSS Power

Chapter 10 ACSS Power Objectives: Power concepts: instantaneous power, average power, reactive power, coplex power, power factor Relationships aong power concepts the power triangle Balancing power in AC circuits Condition

More information

Chapter 16 Solutions

Chapter 16 Solutions Chapter 16 Solutions 16.1 Replace x by x vt = x 4.5t to get y = 6 [(x 4.5t) + 3] 16. y (c) y (c) y (c) 6 4 4 4 t = s t = 1 s t = 1.5 s 0 6 10 14 x 0 6 10 14 x 0 6 10 14 x y (c) y (c) 4 t =.5 s 4 t = 3

More information

PHYS 102 Previous Exam Problems

PHYS 102 Previous Exam Problems PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal

More information

Uniaxial Concrete Material Behavior

Uniaxial Concrete Material Behavior COMPUTERS AND STRUCTURES, INC., JULY 215 TECHNICAL NOTE MODIFIED DARWIN-PECKNOLD 2-D REINFORCED CONCRETE MATERIAL MODEL Overview This tehnial note desribes the Modified Darwin-Peknold reinfored onrete

More information

MTE 119 STATICS FINAL HELP SESSION REVIEW PROBLEMS PAGE 1 9 NAME & ID DATE. Example Problem P.1

MTE 119 STATICS FINAL HELP SESSION REVIEW PROBLEMS PAGE 1 9 NAME & ID DATE. Example Problem P.1 MTE STATICS Example Problem P. Beer & Johnston, 004 by Mc Graw-Hill Companies, Inc. The structure shown consists of a beam of rectangular cross section (4in width, 8in height. (a Draw the shear and bending

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

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

Sample Question Paper

Sample Question Paper Scheme I Sample Question Paper Program Name : Mechanical Engineering Program Group Program Code : AE/ME/PG/PT/FG Semester : Third Course Title : Strength of Materials Marks : 70 Time: 3 Hrs. Instructions:

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion Introduction Stress and strain in components subjected to torque T Circular Cross-section shape Material Shaft design Non-circular

More information

ME325 EXAM I (Sample)

ME325 EXAM I (Sample) ME35 EXAM I (Sample) NAME: NOTE: COSED BOOK, COSED NOTES. ONY A SINGE 8.5x" ORMUA SHEET IS AOWED. ADDITIONA INORMATION IS AVAIABE ON THE AST PAGE O THIS EXAM. DO YOUR WORK ON THE EXAM ONY (NO SCRATCH PAPER

More information

Static Failure (pg 206)

Static Failure (pg 206) Static Failure (pg 06) All material followed Hookeʹs law which states that strain is proportional to stress applied, until it exceed the proportional limits. It will reach and exceed the elastic limit

More information

Mechanics of Materials MENG 270 Fall 2003 Exam 3 Time allowed: 90min. Q.1(a) Q.1 (b) Q.2 Q.3 Q.4 Total

Mechanics of Materials MENG 270 Fall 2003 Exam 3 Time allowed: 90min. Q.1(a) Q.1 (b) Q.2 Q.3 Q.4 Total Mechanics of Materials MENG 70 Fall 00 Eam Time allowed: 90min Name. Computer No. Q.(a) Q. (b) Q. Q. Q.4 Total Problem No. (a) [5Points] An air vessel is 500 mm average diameter and 0 mm thickness, the

More information

PROBLEM 7.31 SOLUTION. β = τ max = 36.4 MPa. Solve Probs. 7.5 and 7.9, using Mohr s circle.

PROBLEM 7.31 SOLUTION. β = τ max = 36.4 MPa. Solve Probs. 7.5 and 7.9, using Mohr s circle. PROBLEM 7.1 Solve Probs. 7.5 an 7.9, using Mohr s circle. PROBLEM 7.5 through 7.8 For the given state of stress, etermine (a) the principal planes, (b) the principal stresses. PROBLEM 7.9 through 7.1 For

More information

Solution ME 323 EXAM #2 FALL SEMESTER :00 PM 9:30 PM Nov. 2, 2010

Solution ME 323 EXAM #2 FALL SEMESTER :00 PM 9:30 PM Nov. 2, 2010 Solution ME 33 EXAM # FALL SEMESTER 1 8: PM 9:3 PM Nov., 1 Instructions 1. Begin each problem in the space provided on the eamination sheets. If additional space is required, use the paper provided. Work

More information

UNIT-I Introduction & Plane Stress and Plane Strain Analysis

UNIT-I Introduction & Plane Stress and Plane Strain Analysis SIDDHARTH INSTITUTE OF ENGINEERING & TECHNOLOGY:: PUTTUR (AUTONOMOUS) Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code : Advanced Solid Mechanics (18CE1002) Year

More information

MECE 3321: MECHANICS OF SOLIDS CHAPTER 5

MECE 3321: MECHANICS OF SOLIDS CHAPTER 5 MECE 3321: MECHANICS OF SOLIDS CHAPTER 5 SAMANTHA RAMIREZ TORSION Torque A moment that tends to twist a member about its longitudinal axis 1 TORSIONAL DEFORMATION OF A CIRCULAR SHAFT Assumption If the

More information

Members Subjected to Combined Loads

Members Subjected to Combined Loads Members Subjected to Combined Loads Combined Bending & Twisting : In some applications the shaft are simultaneously subjected to bending moment M and Torque T.The Bending moment comes on the shaft due

More information

9. h = R. 10. h = 3 R

9. h = R. 10. h = 3 R Version PREVIEW Torque Chap. 8 sizeore (13756) 1 This print-out should have 3 questions. ultiple-choice questions ay continue on the next colun or page find all choices before answering. Note in the dropped

More information

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

Module 11 Design of Joints for Special Loading. Version 2 ME, IIT Kharagpur Module 11 Design of Joints for Special Loading Version ME, IIT Kharagpur Lesson Design of Eccentrically Loaded Welded Joints Version ME, IIT Kharagpur Instructional Objectives: At the end of this lesson,

More information

LECTURE 4 Stresses in Elastic Solid. 1 Concept of Stress

LECTURE 4 Stresses in Elastic Solid. 1 Concept of Stress V. DEMENKO MECHANICS OF MATERIALS 2015 1 LECTURE 4 Stresses in Elastic Solid 1 Concept of Stress In order to characterize the law of internal forces distribution over the section a measure of their intensity

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

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd Chapter Objectives To determine the torsional deformation of a perfectly elastic circular shaft. To determine the support reactions when these reactions cannot be determined solely from the moment equilibrium

More information