ME 323 Examination #2

Size: px
Start display at page:

Download "ME 323 Examination #2"

Transcription

1 ME 33 Eamination # SOUTION Novemer 14, 17 ROEM NO. 1 3 points ma. The cantilever eam D of the ending stiffness is sujected to a concentrated moment M at C. The eam is also supported y a roller at. Using Castigliano s theorem: a) Determine the reaction force at the roller. ) Determine the rotation angle of the eam aout z ais at the end. Ignore the shear energy due to ending. Epress your answers in terms of M, E, and I. M d M M D SOUTION Eternal reactions Using FD of entire eam: M D F y = y + D y = = M y ( ) + M d + M D = rolem is INDETERMINTE. Will choose y as the redundant reaction: M D = y M D y = y (1) () C (3) D M d M d H y D y M 1 V 1 K M Strain energy From FD with cut through section (1): M H = M 1 + M d = M 1 = From FD with cut through section (): M H = M + M d y ( ) = ( ) M = + y From FD with cut through section (3): M H = M 3 + M d y M 3 = + y ( ) M ( ) + M = M d y V C y M Q M 3 V 3

2 From this, we have: U = U 1 +U +U 3 = 1 d y ( ) d y ( ) M d age of 1 Castigliano s theorem Since y is our redundant reaction, we can write: = U y = + 1 = y = y Md = + y ( ) ( + )d + 1 Md = 3 ( )d y ( + )d M 1 ( 3 )3 3 ( ) + = y M = 8 y 3 3 M 3 Therefore: y = 9 16 M 3 3 ( ) M ( )d ( ) + 1 ( 3 3 ) 3 ( ) 3 M Md = ( ) ( ) ( ) ( ) ( )d + ( 3 ) 3

3 lso: U θ = M d = 1 = y M d = M d d + 1 Md = ( )d y y ( ) Md ( 1 )d + 1 = ( ) M d = y 1 ( ) ( ) y 1 3 = y = y = 9 16 = 1 8 M 3 1 y + M M + M M ( ) ( ) 3 + y ( 3 ) + M age 3 of 1 ( ) M Md ( 1 )d = ( 3 )

4 ME 33 Eamination # age 4 of 1 SOUTION Novemer 14, 17 ROEM NO. 5 points ma. t a point aove the neutral ais of the eam shown in the figure, the state of plane stress can e descried y the insert on the right-hand side of the figure. The maimum in-plane shear stress at this point is τ!"# = 13Ma, the normal stress in the -direction is σ! = Ma, and normal stress in the y-direction is σ! = Ma. a) Determine the magnitude of the shear stress, τ!", on the and y faces. ) Determine the sign of the shear stress τ!". HINT: Determine first the direction of the shear force acting on the cross-section with normal at point. c) Draw Mohr s circle corresponding to the state of stress at point. Clearly indicate the location of the center of the circle, the radius of the circle and point X (which represents the stress state on the -face) in this drawing. d) Determine the two in-plane principal stresses at this point. Determine the rotation angle of the stress element for each principal stress. e) Show the locations of the principal stresses and of the in-plane maimum shear stress on your Mohr s circle in c) aove. y y + State of stress at point SOUTION Internal resultants = +V = V = F y M V Stress transformation results: σ ave = σ +σ y = = 1 Ma R = σ σ y + τ y = + τ = 1 + τ

5 Since: we can write: τ ma,in plane = R = τ = 13 τ = ± 13 1 = ± 69 Choose the - sign ased on the direction of the applied force. age 5 of 1 Mohr s circle and principal stresses The Mohr s circle is centered at σ ave, ( ) = ( 1,) Ma and has a radius of R = 13 Ma, as shown. From this, the principal components of stress are: σ 1 = σ ave + R = = 3 Ma σ = σ ave R = 1 13 = 3 Ma The location X of the -ais on Mohr s circle is: (, 69) Ma. From the figure, we see that the rotation angles from the -ais to the aove principal components of stress are: θ = 18 tan = θ = 7.1 θ θ 1 = θ +18 θ 1 = θ + 9 = 16.1 θ S = θ + 9 θ S = θ + 45 = σ = 3 τ X R = 13 σ = ais τ ma = 13 τ y = 69 σ θ 1 τ ma = 13 θ S σ ave = 1 σ 1 = 3

6 ME 33 Eamination # age 6 of 1 SOUTION Novemer 14, 17 ROEM NO. 3 5 points ma. The propped cantilever in the figure is simply supported at end and fied at end. It supports a linearly distriuted load of maimum intensity w! on the span. a) Draw a free ody diagram of the structure. ssume the reactions forces act in the direction of positive and y aes, and the reaction moments act counterclockwise. ) State the equations of equilirium of the structure and indicate whether it is statically determinate or indeterminate. c) Indicate all the oundary conditions that correspond to this prolem. d) Use the second-order integration method (or the fourth-order integration method) to determine an epression for the reaction(s) at the support. Epress the result as a sole function of, w! and. e) Determine an epression for the deflection of the eam as a sole function of, w! and. f) Sketch the deflection curve. w / w M y y 1 w SOUTION Equilirium From FD of entire eam: M = 1 w 3 + y + M = y y + M = 1 3 w C V M F y = y + y 1 w = y + y = 1 w From FD with cut through eam at location : M C = y + 1 w M = M() = y 1 w 3 6

7 Integrations Will need to enforce the following oundary conditions: v() = v() = θ ( ) =. θ() = θ() + 1 M ( )d = θ + 1 = θ y 1 w 4 4 y 1 w 3 d 6 v() = v() + θ ( )d = + θ y 1 w 4 4 d = θ y 3 1 w 5 1 age 7 of 1 Enforcing the oundary conditions at : = θ() = θ y 1 4 w 3 θ = 1 1 y w 3 = v() = θ y w 4 θ = y w 3 Equating the aove two epressions for θ : 1 1 y w 3 = y w 3 1 y w = 1 6 y w y = w y = w 1 and: θ = 1 1 y w 3 = 1 1 w w 3 = 1 w 3 1 Therefore: v() = 1 w w w 4 = w eam deflec)on w

8 ME 33 Eamination # age 8 of 1 SOUTION Novemer 14, 17 ROEM NO. 4 - RT 4 points ma. y y h / 4 h z h / 4 h / 4 / / h / 4 C D eam cross sec*on at C Consider the cantilevered eam aove with the concentrated load at end D. Determine the shear stress on the neutral surface of the eam at location C along the eam. SOUTION Internal resultant shear force F y = +V = V = M V Shear stress with: Therefore, τ = V* y * It * y * = h h h 4 I = 1 1 h3 1 h 1 t = 4 = τ = 7h / 64 15h 3 / 19 = 14 / 5 3 3h 8 = h3 h + 4 h h 4 = 7 64 h

9 ME 33 Eamination # age 9 of 1 SOUTION Novemer 14, 17 ROEM NO. 4 - RT 3 points ma. y a / / C D eam cross sec*on at C Consider the cantilevered eam aove with the concentrated load at end D. Consider the aial components of stress at points a and (σ a and σ, respectively) at location C along the eam. Circle the response elow that most accurately descries the relative sizes of the magnitudes of these two stresses: a) σ a > σ ) σ a = σ y c) σ a < σ SOUTION et O e the centroid of the cross section. Therefore, σ a σ = Mh / I Md / I = h d > 1 σ a > σ z h d a O

10 ME 33 Eamination # age 1 of 1 SOUTION Novemer 14, 17 ROEM NO. 4 - RT C 4 points ma. t r g C W Consider the thin-walled pressure vessel aove that contains a gas under a pressure of p. The vessel is attached to a fied support at and has a plate of weight W attached to it at end C. Ignore the weight of the vessel. Determine the weight W of the plate for which the maimum in-plane shear stress in the vessel at point is zero. SOUTION σ h = pr t σ a = pr t + W πrt For zero maimum in-plane shear stress: R = = pr t σ σ y = pr t + W πrt + τ y = W = π pr σ h σ a + = σ h σ a σ h = σ a

11 ME 33 Eamination # age 11 of 1 SOUTION Novemer 14, 17 ROEM NO. 4 - RT D 4 points ma. y σ y =? σ =? σ 4 ksi τ ksi 1 ksi Consider the state of plane stress shown aove left where the two normal components of stress, σ and σ y, are unknown. The Mohr s circle for this state of stress is provided in the figure aove right. Determine numerical values for the two normal components of stress σ and σ y. There may e more than one set of answers; you need only find one set. SOUTION From the aove Mohr s circle, we see that: σ ave = 1 + = 7 ksi R = 1 = 5 ksi Therefore: σ ave = σ +σ y R = σ σ y σ σ y = ± σ +σ y = σ ave = 14 ksi + τ y σ σ y + τ y = R R τ y = ± 5 ( 4) = ± 6ksi Choosing the + sign and solving gives: σ = 1 ksi and σ y = 4 ksi. Choosing the - sign and solving gives: σ = 4 ksi and σ y = 1 ksi.

12 ME 33 Eamination # age 1 of 1 SOUTION Novemer 14, 17 ROEM NO. 4 - RT E 5 points ma. d d d C D H rod is made up of three circular cross-section components: C,CD and DH. The material for all components have a Young s modulus of E. Suppose you are to develop a finite element model for the rod using one element for each component. If the equilirium equations after the enforcement of oundary conditions are to e written as: K { u} = { F} determine the stiffness matri Spring stiffnesses: ( ) k 1 = Eπ d / ( ) ( ) Eπ d / k = k 3 = Eπ d / = π 4 = π = π 8 K and the load vector { F}. Ed Ed Ed F C D H Stiffness and forcing Therefore the gloal stiffness matri and forcing vector efore enforcing Cs are: F K 6 4 = π Ed and { F} = F H Eliminating the first and last row and column of [K] and the first and last row of {F}: K 6 4 = π Ed and { F} = F H

ME 323 Examination #2 April 11, 2018

ME 323 Examination #2 April 11, 2018 ME 2 Eamination #2 April, 2 PROBLEM NO. 25 points ma. A thin-walled pressure vessel is fabricated b welding together two, open-ended stainless-steel vessels along a 6 weld line. The welded vessel has an

More information

ME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft.

ME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft. ME 323 - Final Exam Name December 15, 2015 Instructor (circle) PROEM NO. 4 Part A (2 points max.) Krousgrill 11:30AM-12:20PM Ghosh 2:30-3:20PM Gonzalez 12:30-1:20PM Zhao 4:30-5:20PM M (x) y 20 kip ft 0.2

More information

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323 Problem 9.1 Two beam segments, AC and CD, are connected together at C by a frictionless pin. Segment CD is cantilevered from a rigid support at D, and segment AC has a roller support at A. a) Determine

More information

FINAL EXAMINATION. (CE130-2 Mechanics of Materials)

FINAL EXAMINATION. (CE130-2 Mechanics of Materials) UNIVERSITY OF CLIFORNI, ERKELEY FLL SEMESTER 001 FINL EXMINTION (CE130- Mechanics of Materials) Problem 1: (15 points) pinned -bar structure is shown in Figure 1. There is an external force, W = 5000N,

More information

Stress and Strain ( , 3.14) MAE 316 Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering

Stress and Strain ( , 3.14) MAE 316 Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering (3.8-3.1, 3.14) MAE 316 Strength of Mechanical Components NC State Universit Department of Mechanical & Aerospace Engineering 1 Introduction MAE 316 is a continuation of MAE 314 (solid mechanics) Review

More information

Conceptual question Conceptual question 12.2

Conceptual question Conceptual question 12.2 Conceptual question 12.1 rigid cap of weight W t g r A thin-walled tank (having an inner radius of r and wall thickness t) constructed of a ductile material contains a gas with a pressure of p. A rigid

More information

Solution: (a) (b) (N) F X =0: A X =0 (N) F Y =0: A Y + B Y (54)(9.81) 36(9.81)=0

Solution: (a) (b) (N) F X =0: A X =0 (N) F Y =0: A Y + B Y (54)(9.81) 36(9.81)=0 Prolem 5.6 The masses of the person and the diving oard are 54 kg and 36 kg, respectivel. ssume that the are in equilirium. (a) Draw the free-od diagram of the diving oard. () Determine the reactions at

More information

CHAPTER 7 DEFLECTIONS OF BEAMS

CHAPTER 7 DEFLECTIONS OF BEAMS CHPTER 7 DEFLECTIONS OF EMS OJECTIVES Determine the deflection and slope at specific points on beams and shafts, using various analytical methods including: o o o The integration method The use of discontinuity

More information

PROBLEM #1.1 (4 + 4 points, no partial credit)

PROBLEM #1.1 (4 + 4 points, no partial credit) PROBLEM #1.1 ( + points, no partial credit A thermal switch consists of a copper bar which under elevation of temperature closes a gap and closes an electrical circuit. The copper bar possesses a length

More information

Outline. Organization. Stresses in Beams

Outline. Organization. Stresses in Beams Stresses in Beams B the end of this lesson, ou should be able to: Calculate the maimum stress in a beam undergoing a bending moment 1 Outline Curvature Normal Strain Normal Stress Neutral is Moment of

More information

σ = Eα(T T C PROBLEM #1.1 (4 + 4 points, no partial credit)

σ = Eα(T T C PROBLEM #1.1 (4 + 4 points, no partial credit) PROBLEM #1.1 (4 + 4 points, no partial credit A thermal switch consists of a copper bar which under elevation of temperature closes a gap and closes an electrical circuit. The copper bar possesses a length

More information

Name (Print) ME Mechanics of Materials Exam # 2 Date: March 29, 2017 Time: 8:00 10:00 PM - Location: WTHR 200

Name (Print) ME Mechanics of Materials Exam # 2 Date: March 29, 2017 Time: 8:00 10:00 PM - Location: WTHR 200 Name (Print) (Last) (First) Instructions: ME 323 - Mechanics of Materials Exam # 2 Date: Time: 8:00 10:00 PM - Location: WTHR 200 Circle your lecturer s name and your class meeting time. Koslowski Zhao

More information

1 of 7. Law of Sines: Stress = E = G. Deformation due to Temperature: Δ

1 of 7. Law of Sines: Stress = E = G. Deformation due to Temperature: Δ NME: ES30 STRENGTH OF MTERILS FINL EXM: FRIDY, MY 1 TH 4PM TO 7PM Closed book. Calculator and writing supplies allowed. Protractor and compass allowed. 180 Minute Time Limit GIVEN FORMULE: Law of Cosines:

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

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 20, 2011 Professor A. Dolovich

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 20, 2011 Professor A. Dolovich UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 20, 2011 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS LAST NAME (printed): FIRST NAME (printed): STUDENT

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

Chapter 3. Load and Stress Analysis

Chapter 3. Load and Stress Analysis Chapter 3 Load and Stress Analysis 2 Shear Force and Bending Moments in Beams Internal shear force V & bending moment M must ensure equilibrium Fig. 3 2 Sign Conventions for Bending and Shear Fig. 3 3

More information

7.4 The Elementary Beam Theory

7.4 The Elementary Beam Theory 7.4 The Elementary Beam Theory In this section, problems involving long and slender beams are addressed. s with pressure vessels, the geometry of the beam, and the specific type of loading which will be

More information

2 marks Questions and Answers

2 marks Questions and Answers 1. Define the term strain energy. A: Strain Energy of the elastic body is defined as the internal work done by the external load in deforming or straining the body. 2. Define the terms: Resilience and

More information

Cover sheet and Problem 1

Cover sheet and Problem 1 over sheet and Problem nstructions M 33 FNL M FLL SMSTR 0 Time allowed: hours. There are 4 problems, each problem is of equal value. The first problem consists of three smaller sub-problems. egin each

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

Section 6: PRISMATIC BEAMS. Beam Theory

Section 6: PRISMATIC BEAMS. Beam Theory Beam Theory There are two types of beam theory aailable to craft beam element formulations from. They are Bernoulli-Euler beam theory Timoshenko beam theory One learns the details of Bernoulli-Euler beam

More information

4.5 The framework element stiffness matrix

4.5 The framework element stiffness matrix 45 The framework element stiffness matri Consider a 1 degree-of-freedom element that is straight prismatic and symmetric about both principal cross-sectional aes For such a section the shear center coincides

More information

Homework No. 1 MAE/CE 459/559 John A. Gilbert, Ph.D. Fall 2004

Homework No. 1 MAE/CE 459/559 John A. Gilbert, Ph.D. Fall 2004 Homework No. 1 MAE/CE 459/559 John A. Gilbert, Ph.D. 1. A beam is loaded as shown. The dimensions of the cross section appear in the insert. the figure. Draw a complete free body diagram showing an equivalent

More information

Chapter 5 Elastic Strain, Deflection, and Stability 1. Elastic Stress-Strain Relationship

Chapter 5 Elastic Strain, Deflection, and Stability 1. Elastic Stress-Strain Relationship Chapter 5 Elastic Strain, Deflection, and Stability Elastic Stress-Strain Relationship A stress in the x-direction causes a strain in the x-direction by σ x also causes a strain in the y-direction & z-direction

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

2 Axially Loaded Numbers

2 Axially Loaded Numbers xially oaded Numers hanges in engths of xially oaded Memers rolem.-1 The T-shaped arm shown in the figure lies in a vertical plane and pivots aout a horizontal pin at. The arm has constant cross-sectional

More information

M. Vable Mechanics of Materials: Chapter 5. Torsion of Shafts

M. Vable Mechanics of Materials: Chapter 5. Torsion of Shafts Torsion of Shafts Shafts are structural members with length significantly greater than the largest cross-sectional dimension used in transmitting torque from one plane to another. Learning objectives Understand

More information

December 10, PROBLEM NO points max.

December 10, PROBLEM NO points max. PROBLEM NO. 1 25 points max. PROBLEM NO. 2 25 points max. B 3A A C D A H k P L 2L Given: Consider the structure above that is made up of rod segments BC and DH, a spring of stiffness k and rigid connectors

More information

Rigid and Braced Frames

Rigid and Braced Frames RH 331 Note Set 12.1 F2014abn Rigid and raced Frames Notation: E = modulus of elasticit or Young s modulus F = force component in the direction F = force component in the direction FD = free bod diagram

More information

Planar Rigid Body Kinematics Homework

Planar Rigid Body Kinematics Homework Chapter 2: Planar Rigid ody Kinematics Homework Chapter 2 Planar Rigid ody Kinematics Homework Freeform c 2018 2-1 Chapter 2: Planar Rigid ody Kinematics Homework 2-2 Freeform c 2018 Chapter 2: Planar

More information

Comb Resonator Design (2)

Comb Resonator Design (2) Lecture 6: Comb Resonator Design () -Intro. to Mechanics of Materials Sh School of felectrical ti lengineering i and dcomputer Science, Si Seoul National University Nano/Micro Systems & Controls Laboratory

More information

LECTURE 13 Strength of a Bar in Pure Bending

LECTURE 13 Strength of a Bar in Pure Bending V. DEMENKO MECHNCS OF MTERLS 015 1 LECTURE 13 Strength of a Bar in Pure Bending Bending is a tpe of loading under which bending moments and also shear forces occur at cross sections of a rod. f the bending

More information

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A DEPARTMENT: CIVIL SUBJECT CODE: CE2201 QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A (2 Marks) 1. Define longitudinal strain and lateral strain. 2. State

More information

ragsdale (zdr82) HW7 ditmire (58335) 1 The magnetic force is

ragsdale (zdr82) HW7 ditmire (58335) 1 The magnetic force is ragsdale (zdr8) HW7 ditmire (585) This print-out should have 8 questions. Multiple-choice questions ma continue on the net column or page find all choices efore answering. 00 0.0 points A wire carring

More information

1 of 12. Law of Sines: Stress = E = G. Deformation due to Temperature: Δ

1 of 12. Law of Sines: Stress = E = G. Deformation due to Temperature: Δ NAME: ES30 STRENGTH OF MATERIALS FINAL EXAM: FRIDAY, MAY 1 TH 4PM TO 7PM Closed book. Calculator and writing supplies allowed. Protractor and compass allowed. 180 Minute Time Limit GIVEN FORMULAE: Law

More information

Exact Free Vibration of Webs Moving Axially at High Speed

Exact Free Vibration of Webs Moving Axially at High Speed Eact Free Viration of Wes Moving Aially at High Speed S. HATAMI *, M. AZHARI, MM. SAADATPOUR, P. MEMARZADEH *Department of Engineering, Yasouj University, Yasouj Department of Civil Engineering, Isfahan

More information

9. Stress Transformation

9. Stress Transformation 9.7 ABSOLUTE MAXIMUM SHEAR STRESS A pt in a body subjected to a general 3-D state of stress will have a normal stress and shear-stress components acting on each of its faces. We can develop stress-transformation

More information

Cork Institute of Technology. Autumn 2007 Mechanics of Materials (Time: 3 Hours)

Cork Institute of Technology. Autumn 2007 Mechanics of Materials (Time: 3 Hours) Cork Institute of Technology Bachelor of Engineering (Honours) in Mechanical Engineering- Stage 2 (NFQ Level 8) Autumn 2007 Mechanics of Materials (Time: 3 Hours) Instructions Answer Five Questions Question

More information

MECHANICS OF MATERIALS REVIEW

MECHANICS OF MATERIALS REVIEW MCHANICS OF MATRIALS RVIW Notation: - normal stress (psi or Pa) - shear stress (psi or Pa) - normal strain (in/in or m/m) - shearing strain (in/in or m/m) I - area moment of inertia (in 4 or m 4 ) J -

More information

Chapter 5 Equilibrium of a Rigid Body Objectives

Chapter 5 Equilibrium of a Rigid Body Objectives Chapter 5 Equilibrium of a Rigid Bod Objectives Develop the equations of equilibrium for a rigid bod Concept of the free-bod diagram for a rigid bod Solve rigid-bod equilibrium problems using the equations

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

Review Lecture. AE1108-II: Aerospace Mechanics of Materials. Dr. Calvin Rans Dr. Sofia Teixeira De Freitas

Review Lecture. AE1108-II: Aerospace Mechanics of Materials. Dr. Calvin Rans Dr. Sofia Teixeira De Freitas Review Lecture AE1108-II: Aerospace Mechanics of Materials Dr. Calvin Rans Dr. Sofia Teixeira De Freitas Aerospace Structures & Materials Faculty of Aerospace Engineering Analysis of an Engineering System

More information

REVIEW FOR EXAM II. Dr. Ibrahim A. Assakkaf SPRING 2002

REVIEW FOR EXAM II. Dr. Ibrahim A. Assakkaf SPRING 2002 REVIEW FOR EXM II. J. Clark School of Engineering Department of Civil and Environmental Engineering b Dr. Ibrahim. ssakkaf SPRING 00 ENES 0 Mechanics of Materials Department of Civil and Environmental

More information

PES Institute of Technology

PES Institute of Technology PES Institute of Technology Bangalore south campus, Bangalore-5460100 Department of Mechanical Engineering Faculty name : Madhu M Date: 29/06/2012 SEM : 3 rd A SEC Subject : MECHANICS OF MATERIALS Subject

More information

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A (2 Marks) 1. Define longitudinal strain and lateral strain. 2. State Hooke s law. 3. Define modular ratio,

More information

ME 202 STRENGTH OF MATERIALS SPRING 2014 HOMEWORK 4 SOLUTIONS

ME 202 STRENGTH OF MATERIALS SPRING 2014 HOMEWORK 4 SOLUTIONS ÇANKAYA UNIVERSITY MECHANICAL ENGINEERING DEPARTMENT ME 202 STRENGTH OF MATERIALS SPRING 2014 Due Date: 1 ST Lecture Hour of Week 12 (02 May 2014) Quiz Date: 3 rd Lecture Hour of Week 12 (08 May 2014)

More information

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002 student personal identification (ID) number on each sheet. Do not write your name on any sheet. #1. A homogeneous, isotropic, linear elastic bar has rectangular cross sectional area A, modulus of elasticity

More information

Deflection of Beams. Equation of the Elastic Curve. Boundary Conditions

Deflection of Beams. Equation of the Elastic Curve. Boundary Conditions Deflection of Beams Equation of the Elastic Curve The governing second order differential equation for the elastic curve of a beam deflection is EI d d = where EI is the fleural rigidit, is the bending

More information

BME 207 Introduction to Biomechanics Spring Homework 9

BME 207 Introduction to Biomechanics Spring Homework 9 April 10, 2018 UNIVERSITY OF RHODE ISLAND Department of Electrical, Computer and Biomedical Engineering BME 207 Introduction to Biomechanics Spring 2018 Homework 9 Prolem 1 The intertrochanteric nail from

More information

Level 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method

Level 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method 9210-203 Level 7 Postgraduate Diploma in Engineering Computational mechanics using finite element method You should have the following for this examination one answer book No additional data is attached

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 4 Pure Bending

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 4 Pure Bending EA 3702 echanics & aterials Science (echanics of aterials) Chapter 4 Pure Bending Pure Bending Ch 2 Aial Loading & Parallel Loading: uniform normal stress and shearing stress distribution Ch 3 Torsion:

More information

KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS

KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS Chapter 8 KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS Figure 8.1: 195 196 CHAPTER 8. KINEMATIC RELATIONS IN DEFORMATION OF SOLIDS 8.1 Motivation In Chapter 3, the conservation of linear momentum for a

More information

Homework 6: Energy methods, Implementing FEA.

Homework 6: Energy methods, Implementing FEA. EN75: Advanced Mechanics of Solids Homework 6: Energy methods, Implementing FEA. School of Engineering Brown University. The figure shows a eam with clamped ends sujected to a point force at its center.

More information

Torsion of Shafts Learning objectives

Torsion of Shafts Learning objectives Torsion of Shafts Shafts are structural members with length significantly greater than the largest cross-sectional dimension used in transmitting torque from one plane to another. Learning objectives Understand

More information

dw 2 3(w) x 4 x 4 =L x 3 x 1 =0 x 2 El #1 El #2 El #3 Potential energy of element 3: Total potential energy Potential energy of element 1:

dw 2 3(w) x 4 x 4 =L x 3 x 1 =0 x 2 El #1 El #2 El #3 Potential energy of element 3: Total potential energy Potential energy of element 1: MAE 44 & CIV 44 Introduction to Finite Elements Reading assignment: ecture notes, ogan. Summary: Pro. Suvranu De Finite element ormulation or D elasticity using the Rayleigh-Ritz Principle Stiness matri

More information

x y plane is the plane in which the stresses act, yy xy xy Figure 3.5.1: non-zero stress components acting in the x y plane

x y plane is the plane in which the stresses act, yy xy xy Figure 3.5.1: non-zero stress components acting in the x y plane 3.5 Plane Stress This section is concerned with a special two-dimensional state of stress called plane stress. It is important for two reasons: () it arises in real components (particularl in thin components

More information

University of Pretoria Department of Mechanical & Aeronautical Engineering MOW 227, 2 nd Semester 2014

University of Pretoria Department of Mechanical & Aeronautical Engineering MOW 227, 2 nd Semester 2014 Universit of Pretoria Department of Mechanical & Aeronautical Engineering MOW 7, nd Semester 04 Semester Test Date: August, 04 Total: 00 Internal eaminer: Duration: hours Mr. Riaan Meeser Instructions:

More information

2. Determine the deflection at C of the beam given in fig below. Use principal of virtual work. W L/2 B A L C

2. Determine the deflection at C of the beam given in fig below. Use principal of virtual work. W L/2 B A L C CE-1259, Strength of Materials UNIT I STRESS, STRAIN DEFORMATION OF SOLIDS Part -A 1. Define strain energy density. 2. State Maxwell s reciprocal theorem. 3. Define proof resilience. 4. State Castigliano

More information

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS Name :. Roll No. :..... Invigilator s Signature :.. 2011 SOLID MECHANICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are required to give their answers

More information

R13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A

R13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A SET - 1 II B. Tech I Semester Regular Examinations, Jan - 2015 MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) Time: 3 hours Max. Marks: 70 Note: 1. Question Paper consists of two parts (Part-A and Part-B)

More information

Tutorial #1 - CivE. 205 Name: I.D:

Tutorial #1 - CivE. 205 Name: I.D: Tutorial # - CivE. 0 Name: I.D: Eercise : For the Beam below: - Calculate the reactions at the supports and check the equilibrium of point a - Define the points at which there is change in load or beam

More information

ESE TOPICWISE OBJECTIVE SOLVED PAPER I

ESE TOPICWISE OBJECTIVE SOLVED PAPER I C I V I L E N G I N E E R I N G ESE TOPICWISE OBJECTIVE SOLVED PAPER I FROM 1995-018 UPSC Engineering Services Eamination, State Engineering Service Eamination & Public Sector Eamination. Regd. office

More information

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV UNIT I STRESS, STRAIN DEFORMATION OF SOLIDS PART A (2 MARKS)

More information

Symmetric Bending of Beams

Symmetric Bending of Beams Symmetric Bending of Beams beam is any long structural member on which loads act perpendicular to the longitudinal axis. Learning objectives Understand the theory, its limitations and its applications

More information

, and M A , R B. , and then draw the shear-force and bending-moment diagrams, labeling all critical ordinates. Solution 10.

, and M A , R B. , and then draw the shear-force and bending-moment diagrams, labeling all critical ordinates. Solution 10. SETIN 0. ethod of Superposition 63 roblem 0.- The propped cantilever beam shown in the figure supports a uniform load of intensity on the left-hand half of the beam. Find the reactions R, R, and, and then

More information

UNIT 1 STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS 1. Define stress. When an external force acts on a body, it undergoes deformation.

UNIT 1 STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS 1. Define stress. When an external force acts on a body, it undergoes deformation. UNIT 1 STRESS STRAIN AND DEFORMATION OF SOLIDS, STATES OF STRESS 1. Define stress. When an external force acts on a body, it undergoes deformation. At the same time the body resists deformation. The magnitude

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

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich UNIVERSITY OF SASKATCHEWAN ME 313.3 MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich A CLOSED BOOK EXAMINATION TIME: 3 HOURS For Marker s Use Only LAST NAME (printed): FIRST

More information

PROBLEM 8.3. S F = 0: N -(250 lb)cos 30 -(50 lb)sin 30 = SOLUTION

PROBLEM 8.3. S F = 0: N -(250 lb)cos 30 -(50 lb)sin 30 = SOLUTION PROLEM 8. Determine whether the block shown is in equilibrium and find the magnitude and direction of the friction force when θ = and P = 5 lb. ssume equilibrium: S F = : F-(5 lb)sin + (5 lb)cos = S F

More information

Deflections. Deflections. Deflections. Deflections. Deflections. Deflections. dx dm V. dx EI. dx EI dx M. dv w

Deflections. Deflections. Deflections. Deflections. Deflections. Deflections. dx dm V. dx EI. dx EI dx M. dv w CIVL 311 - Conjugate eam 1/5 Conjugate beam method The development of the conjugate beam method has been atributed to several strucutral engineers. any credit Heinrich üller-reslau (1851-195) with the

More information

CHAPTER 4 Stress Transformation

CHAPTER 4 Stress Transformation CHAPTER 4 Stress Transformation ANALYSIS OF STRESS For this topic, the stresses to be considered are not on the perpendicular and parallel planes only but also on other inclined planes. A P a a b b P z

More information

both an analytical approach and the pole method, determine: (a) the direction of the

both an analytical approach and the pole method, determine: (a) the direction of the Quantitative Problems Problem 4-3 Figure 4-45 shows the state of stress at a point within a soil deposit. Using both an analytical approach and the pole method, determine: (a) the direction of the principal

More information

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2 Samantha Ramirez, MSE Stress The intensity of the internal force acting on a specific plane (area) passing through a point. Δ ΔA Δ z Δ 1 2 ΔA Δ x Δ y ΔA is an infinitesimal size area with a uniform force

More information

Math 216 Second Midterm 28 March, 2013

Math 216 Second Midterm 28 March, 2013 Math 26 Second Midterm 28 March, 23 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that

More information

Supplement: Statically Indeterminate Frames

Supplement: Statically Indeterminate Frames : Statically Indeterminate Frames Approximate Analysis - In this supplement, we consider another approximate method of solving statically indeterminate frames subjected to lateral loads known as the. Like

More information

MTE 119 STATICS LECTURE MATERIALS FINAL REVIEW PAGE NAME & ID DATE. Example Problem F.1: (Beer & Johnston Example 9-11)

MTE 119 STATICS LECTURE MATERIALS FINAL REVIEW PAGE NAME & ID DATE. Example Problem F.1: (Beer & Johnston Example 9-11) Eample Problem F.: (Beer & Johnston Eample 9-) Determine the mass moment of inertia with respect to: (a) its longitudinal ais (-ais) (b) the y-ais SOLUTION: a) Mass moment of inertia about the -ais: Step

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

NAME: Given Formulae: Law of Cosines: Law of Sines:

NAME: Given Formulae: Law of Cosines: Law of Sines: NME: Given Formulae: Law of Cosines: EXM 3 PST PROBLEMS (LESSONS 21 TO 28) 100 points Thursday, November 16, 2017, 7pm to 9:30, Room 200 You are allowed to use a calculator and drawing equipment, only.

More information

AE3160 Experimental Fluid and Solid Mechanics

AE3160 Experimental Fluid and Solid Mechanics AE3160 Experimental Fluid and Solid Mechanics Cantilever Beam Bending Claudio Di Leo 1 Learning Objectives 1. On Structural Mechanics: a) Mechanics of Slender Beams b) Strain Transformation Theory c) Principal

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

1.571 Structural Analysis and Control Prof. Connor Section 5: Non-linear Analysis of Members. π -- γ. v 2. v 1. dx du. v, x. u, x.

1.571 Structural Analysis and Control Prof. Connor Section 5: Non-linear Analysis of Members. π -- γ. v 2. v 1. dx du. v, x. u, x. 5. Deformation nalysis Y.57 Structural nalysis and Control rof. Connor Section 5: Non-linear nalysis of Members dy ( + ε y )dy π -- γ y ( + ε ) X 5.. Deformation of a fiber initially aligned with. u u

More information

ISHIK UNIVERSITY DEPARTMENT OF MECHATRONICS ENGINEERING

ISHIK UNIVERSITY DEPARTMENT OF MECHATRONICS ENGINEERING ISHIK UNIVERSITY DEPARTMENT OF MECHATRONICS ENGINEERING QUESTION BANK FOR THE MECHANICS OF MATERIALS-I 1. A rod 150 cm long and of diameter 2.0 cm is subjected to an axial pull of 20 kn. If the modulus

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

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

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3.

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3. ES230 STRENGTH OF MTERILS Exam 3 Study Guide Exam 3: Wednesday, March 8 th in-class Updated 3/3/17 Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on

More information

CE6306 STRENGTH OF MATERIALS TWO MARK QUESTIONS WITH ANSWERS ACADEMIC YEAR

CE6306 STRENGTH OF MATERIALS TWO MARK QUESTIONS WITH ANSWERS ACADEMIC YEAR CE6306 STRENGTH OF MATERIALS TWO MARK QUESTIONS WITH ANSWERS ACADEMIC YEAR 2014-2015 UNIT - 1 STRESS, STRAIN AND DEFORMATION OF SOLIDS PART- A 1. Define tensile stress and tensile strain. The stress induced

More information

March 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE

March 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE Chapter 4 Deflection and Stiffness 1 2 Chapter Outline Spring Rates Tension, Compression, and Torsion Deflection Due to Bending Beam Deflection Methods Beam Deflections by Superposition Strain Energy Castigliano

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

1 of 12. Given: Law of Cosines: C. Law of Sines: Stress = E = G

1 of 12. Given: Law of Cosines: C. Law of Sines: Stress = E = G ES230 STRENGTH OF MATERIALS FINAL EXAM: WEDNESDAY, MAY 15 TH, 4PM TO 7PM, AEC200 Closed book. Calculator and writing supplies allowed. Protractor and compass required. 180 Minute Time Limit You must have

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

BEAMS AND PLATES ANALYSIS

BEAMS AND PLATES ANALYSIS BEAMS AND PLATES ANALYSIS Automotive body structure can be divided into two types: i. Frameworks constructed of beams ii. Panels Classical beam versus typical modern vehicle beam sections Assumptions:

More information

Shear Stresses. Shear Stresses. Stresses in Beams Part 4

Shear Stresses. Shear Stresses. Stresses in Beams Part 4 Stresses in Beams Part 4 W do people order doule ceese urgers,large fries, and a diet Coke. UNQUE VEW OF HSTORY FROM THE 6 t GRDE ncient Egpt was inaited mummies and te all wrote in draulics. Te lived

More information

RODS: THERMAL STRESS AND STRESS CONCENTRATION

RODS: THERMAL STRESS AND STRESS CONCENTRATION RODS: HERML SRESS ND SRESS CONCENRION Example 5 rod of length L, cross-sectional area, and modulus of elasticity E, has been placed inside a tube of the same length L, but of cross-sectional area and modulus

More information

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points)

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points) ME 270 3 rd Sample inal Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points) IND: In your own words, please state Newton s Laws: 1 st Law = 2 nd Law = 3 rd Law = PROBLEM

More information

Lecture Slides. Chapter 4. Deflection and Stiffness. The McGraw-Hill Companies 2012

Lecture Slides. Chapter 4. Deflection and Stiffness. The McGraw-Hill Companies 2012 Lecture Slides Chapter 4 Deflection and Stiffness The McGraw-Hill Companies 2012 Chapter Outline Force vs Deflection Elasticity property of a material that enables it to regain its original configuration

More information

Experimental Lab. Principles of Superposition

Experimental Lab. Principles of Superposition Experimental Lab Principles of Superposition Objective: The objective of this lab is to demonstrate and validate the principle of superposition using both an experimental lab and theory. For this lab you

More information

SRI CHANDRASEKHARENDRA SARASWATHI VISWA MAHAVIDHYALAYA

SRI CHANDRASEKHARENDRA SARASWATHI VISWA MAHAVIDHYALAYA SRI CHANDRASEKHARENDRA SARASWATHI VISWA MAHAVIDHYALAYA (Declared as Deemed-to-be University under Section 3 of the UGC Act, 1956, Vide notification No.F.9.9/92-U-3 dated 26 th May 1993 of the Govt. of

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

RODS: STATICALLY INDETERMINATE MEMBERS

RODS: STATICALLY INDETERMINATE MEMBERS RODS: STTICLLY INDETERMINTE MEMERS Statically Indeterminate ackground In all of the problems discussed so far, it was possible to determine the forces and stresses in the members by utilizing the equations

More information