Chapter 4 Pure Bending

Size: px
Start display at page:

Download "Chapter 4 Pure Bending"

Transcription

1 Chapter Pure endg INTRODUCTION endg tress W W L endg of embers made of everal aterials 0 5 lumum 0.5 TYP rass teel rass lumum Cross-section, Cross-section, tress Concentrations r r D d D d 2r Introduction -1

2 Eccentric ial Loadg a Plane of mmetr P Unsmmetric endg -2 Introduction

3 ENDING TRE L endg tress -

4 ENDING TRE- contued z z σ = I - endg tress

5 ECTION ODULU σ 2 c2 c1 z σ 1 h b σ = = I ection odulus -5

6 Eample Fd the maimum bendg stress at section a-a ( m from ) of the W beam. Units: N, m a 000 a W mm 6mm mm 2 mm rea, = 790 mm Depth, d = 157 mm Flange Width, bf = 15 Flange Thickness, tf = 9. Web Thickness, t = 6.6 I = I = = = mm w mm mm -6

7 Eample Fd the bendg stresses at the wall at pots and for a 6" pipe with a wall thickness of 0.125". Units: lb, ft Cross-section -7

8 Eample Fd the bendg stresses at the wall at pots and for the W620 beam. Units: lb, ft W620 Cross-section 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 w -8

9 Eample Fd the bendg stresses at the wall at pots and for the C61 beam. Units: lb, ft. 200 C61 Cross-section 2 rea, =.8 Depth, d = 6.00 Flange Width, bf = 2.16 Flange Thickness, tf = 0. Web Thickness, t = 0.7 I = 17. I = 1.05 = 5.80 = 0.62 = 0.51 w -9

10 Eample Fd the maimum bendg stress at section a-a ( m from ) of the W beam. Units: N/m, m a a 6 W mm 6mm mm 2 mm rea, = 790 mm Depth, d = 157 mm Flange Width, bf = 15 Flange Thickness, tf = 9. Web Thickness, t = 6.6 I = I = = = mm w mm mm -10

11 Eample The sign is subjected to a wd force of 250 lb at it s centroid 7' from the center of the column. The column has an outside diameter of 10" and a wall thickness of 0.25". Considerg onl this force, determe the maimum bendg stress. Units: ft. 7 ENGINEERING WY NEXT EXIT 0 Front View ide View -11

12 PRLLEL-XI THEORE OENT OF INERTI PRLLEL-XI THEORE I I d 2 = ( + ) I I d 2 = ( + ) EXPLE t (uniform thk.) a/2 a/2 b -12 Parallel-is Theorem

13 Eample The simpl-supported beam below has a cross-sectional area as shown. Determe the bendg stress that acts at pots c and d, located at section a-a ( m from ). Units: N/m, mm (uno) a a 6 m 20 c d -1

14 Eample The member is designed to resist a moment of 5 kip about the horizontal ais. Determe the maimum normal stress the member for the two similar cross-sections. Units:

15 Eample Compare the bendg stresses between the two cases for a moment about the horizontal ais. Case 1 is a simple solid cross-section, whereas case 2 is made up of identical boards. The boards aren t connected together and simpl rest on one another. Units:. 1.5 Case Case 2-15

16 Eample The two beams are connected b a th rigid plate on the top and bottom side of the flanges. Fd the bendg stresses at the wall at pots, and C for the W620 beam. Units: lb, ft, C 2000 C W620 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. Cross-section = 1. =.1 w -16

17 Eample The two beams are connected b a th rigid plate on the top and bottom side of the flanges. Fd the bendg stresses at the wall at pots, and C for the W620 beam. Units: lb, ft, C 2000 C 2000 W620 Cross-section 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 w -17

18 Eample The two beams are connected b bolts through the flanges. Fd the bendg stresses at the wall at pots and for the W620 beam. Units: lb, ft 2000 W620 Cross-section 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 w -18

19 Eample The two beams are connected b bolts through the flanges. Fd the bendg stresses at the wall at pots and for the W620 beam. Units: lb, ft W620 Cross-section 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 w -19

20 Eample The simpl-supported beam below has a cross-sectional area as shown. Determe the bendg stress that acts at pots c and d, located at section a-a ( m from ). Units: N/m, mm (UNO) a a 6 m 150 c d 2 Cross-section -20

21 ENDING OF EER DE OF EVERL TERIL N.. ε σ σ = n I endg of embers ade of everal aterials -21

22 Eample Fd the stress each of the three metals if a moment of 12 k- is applied about the horizontal ais. E (alumum)= 10E6, E(steel)= 0E6, E (brass)= 15E6 psi. Units:. lumum 0.5 TYP rass teel 2.5 rass lumum

23 Eample W wide flange beam is reforced with wood planks that are securel connected to the flanges. Esteel/Ewood= 20. If the allowable stresses the wood and steel are.5 Pa and 52 Pa, respectivel, determe the allowable distributed load w based on section a-a ( m from ). Units: N/m, mm (UNO) w a w a 6 m Cross-section W mm 6mm mm 2 mm rea, = 790 mm Depth, d = 157 mm Flange Width, bf = 15 Flange Thickness, tf = 9. Web Thickness, t = 6.6 I = I = = = mm w mm mm -2

24 Eample Two steel plates are securel fastened to a 6"10" wood beam. Esteel/Ewood= 20. Knowg that the beam is bent about the horizontal ais b a 125 kip- moment, determe the maimum stress (a) the wood, (b) the steel. Units:. 2 TYP 0.75 TYP Cross-section -2

25 Eample Determe the stress the concrete and steel if a moment of 1500 kip- is applied about the horizontal ais. rea of steel=.1 sq.. E (steel)= 0E6 psi, E (concrete)=.75e6 psi. Units: Cross-section 0 Cross-section -25

26 Eample Determe the required steel area for the beam to be balanced. llowable stress the steel and concrete are,000 and,000 psi respectivel. E (steel)= 29E6 psi, E (concrete)=.5e6 psi. Units: Cross-section Cross-section -26

27 TRE CONCENTRTION r r D d D d σ ma = k I 2r k D/d= D 1.1 r d k D 1.1 2r d r r/d tress-concentration factors for flat bars with fillets under pure bendg r/d tress-concentration factors for flat bars with groves under pure bendg Ref.: W.D. Pilke, Peterson s tress Concentration Factors, 2nd ed., John Wile and ons, New York, 1997 tress Concentrations -27

28 Eample For the 1 mm thick plate, determe the largest bendg moment that can be applied if the allowable bendg stress is 90 Pa. Units: mm. R k D/d= r/d tress-concentration factors for flat bars with fillets under pure bendg D r d Ref.: W.D. Pilke, Peterson s tress Concentration Factors, 2nd ed., John Wile and ons, New York,

29 Eample For the 7/8" thick plate, determe the largest bendg moment that can be applied if the allowable bendg stress is 2,000 psi. Units:. R k r/d tress-concentration factors for flat bars with groves under pure bendg Ref.: W.D. Pilke, Peterson s tress Concentration Factors, 2nd ed., John Wile and ons, New York, 1997 D 2r d r -29

30 ECCENTRIC XIL LODING IN PLNE OF YETRY P P In general, P σ = + I -0 Eccentric ial Loadg a Plane of mmetr

31 Eample For the solid rectangular bar, determe the largest load P that can be applied based on a maimum normal stress of 10 Pa. Ignore an stress concentrations. Units: mm. P P a P b a b ection a-a ection b-b P -1

32 Eample The three loads are applied at the end of the W620 beam. Fd the normal stress at the wall at pot for the beam, (a) if all three loads are applied, (b) the bottom load is removed. Units: lb, ft W620 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 Cross-section w -2

33 Eample The 100 mm diameter solid circular bar has an eccentric load P applied. Determe the maimum location that the load can be placed without ducg an tensile stresses. Units: mm. P -

34 Eample Compute the maimum tension and compression stresses located at section a-a. Units: N, mm (UNO). 2 m a 6 m a (uniform) 60 ection a-a a m a -

35 UNYETRIC ENDING z z σ = + Iz z I P z I I z σ = + z z z z Unsmmetric endg -5

36 Eample For the W620 section, determe the normal stresses at and. Units: kip W620 2 rea, = 5.87 Depth, d = 6.20 Flange Width, bf = 6.02 Flange Thickness, tf = 0.65 Web Thickness, t = I = 1. I = 1. = 1. =.1 w -6

37 Eample For the WT18150 section, determe the normal stresses at, and C. Units: k WT18150 C 2 rea, =.10 Depth, d = 18. Flange Width, bf = 16.7 Flange Thickness, tf = 1.68 Web Thickness, t = 0.95 I = 120 I = 68 = 86.1 = 77.8 =.1 w -7

38 Eample For the channel section, determe the normal stresses at and. Units: kn m, mm TYP -8

39 Eample For the L angle section, determe the normal stresses at and. Units: N m. z 2 mm rea, = 1770 mm d= b = 76 mm = = 2.6 Thickness, t = 12.7 I = I = r = 1.8 mm mm 6mm 00-9

40 URY endg tress W L σ = = I endg of embers made of everal aterials 0 5 lumum 0.5 TYP rass teel rass 2.5 σ = n I 2 lumum Cross-section, Cross-section, tress Concentrations r r D d D d.0 r 2.8 D/d= 2r 2.6 D d k r/d tress-concentration factors for flat bars with fillets under pure bendg -0 ummar

41 URY Eccentric ial Loadg a Plane of mmetr P σ = P I Unsmmetric endg z z z P z I I z σ = + z ummar -1

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

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 4 Pure Bending Homework Answers EA 3702 echanics & aterials Science (echanics of aterials) Chapter 4 Pure Bending Homework Answers 100 mm Homework 4.1 For pure bending moment of 5 kn m on hollow beam with uniform wall thickness of 10

More information

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. Please review the followg statement: I certify that I have not given unauthorized aid nor have I received aid the completion of this eam. Signature: INSTRUCTIONS Beg each problem the space provided on

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

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

MECHANICS OF MATERIALS Sample Problem 4.2

MECHANICS OF MATERIALS Sample Problem 4.2 Sample Problem 4. SOLUTON: Based on the cross section geometry, calculate the location of the section centroid and moment of inertia. ya ( + Y Ad ) A A cast-iron machine part is acted upon by a kn-m couple.

More information

CE 562 Structural Design I Midterm No. 2 Closed Book Portion (25 / 100 pts)

CE 562 Structural Design I Midterm No. 2 Closed Book Portion (25 / 100 pts) CE 56 Structural Design I Name: Midterm No. Closed Book Portion (5 / 100 pts) 1. ( pts) List all of the failure modes that should be checked for the followg bearg-tpe connection: P u ½ 7/8" dia bolts,

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

122 CHAPTER 2 Axially Loaded Numbers. Stresses on Inclined Sections

122 CHAPTER 2 Axially Loaded Numbers. Stresses on Inclined Sections 1 CHATER Aiall Loaded Numbers Stresses on Inclined Sections roblem.6-1 A steel bar of rectangular cross section (1.5 in..0 in.) carries a tensile load (see figure). The allowable stresses in tension and

More information

Properties of Sections

Properties of Sections ARCH 314 Structures I Test Primer Questions Dr.-Ing. Peter von Buelow Properties of Sections 1. Select all that apply to the characteristics of the Center of Gravity: A) 1. The point about which the body

More information

1. Given the shown built-up tee-shape, determine the following for both strong- and weak-axis bending:

1. Given the shown built-up tee-shape, determine the following for both strong- and weak-axis bending: 1. Given the shown built-up tee-shape, determe the followg for both strong- and weak-ais bendg: a. Location of the neutral ais b. Moment of ertia c. Section Moduli d. Radius of gration Solution: (a) Location

More information

Part 1 is to be completed without notes, beam tables or a calculator. DO NOT turn Part 2 over until you have completed and turned in Part 1.

Part 1 is to be completed without notes, beam tables or a calculator. DO NOT turn Part 2 over until you have completed and turned in Part 1. NAME CM 3505 Fall 06 Test 2 Part 1 is to be completed without notes, beam tables or a calculator. Part 2 is to be completed after turning in Part 1. DO NOT turn Part 2 over until you have completed and

More information

BEAMS: SHEAR AND MOMENT DIAGRAMS (FORMULA)

BEAMS: SHEAR AND MOMENT DIAGRAMS (FORMULA) LETURE Third Edition BEMS: SHER ND MOMENT DGRMS (FORMUL). J. lark School of Engineering Department of ivil and Environmental Engineering 1 hapter 5.1 5. b Dr. brahim. ssakkaf SPRNG 00 ENES 0 Mechanics

More information

Solid Mechanics Homework Answers

Solid Mechanics Homework Answers Name: Date: Solid Mechanics Homework nswers Please show all of your work, including which equations you are using, and circle your final answer. Be sure to include the units in your answers. 1. The yield

More information

Chapter 1 Introduction- Concept of Stress

Chapter 1 Introduction- Concept of Stress hapter 1 Introduction- oncept of Stress INTRODUTION Review of Statics xial Stress earing Stress Torsional Stress 14 6 ending Stress W W L Introduction 1-1 Shear Stress W W Stress and Strain L y y τ xy

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

This procedure covers the determination of the moment of inertia about the neutral axis.

This procedure covers the determination of the moment of inertia about the neutral axis. 327 Sample Problems Problem 16.1 The moment of inertia about the neutral axis for the T-beam shown is most nearly (A) 36 in 4 (C) 236 in 4 (B) 136 in 4 (D) 736 in 4 This procedure covers the determination

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

Determine the resultant internal loadings acting on the cross section at C of the beam shown in Fig. 1 4a.

Determine the resultant internal loadings acting on the cross section at C of the beam shown in Fig. 1 4a. E X M P L E 1.1 Determine the resultant internal loadings acting on the cross section at of the beam shown in Fig. 1 a. 70 N/m m 6 m Fig. 1 Support Reactions. This problem can be solved in the most direct

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

STRESS. Bar. ! Stress. ! Average Normal Stress in an Axially Loaded. ! Average Shear Stress. ! Allowable Stress. ! Design of Simple Connections

STRESS. Bar. ! Stress. ! Average Normal Stress in an Axially Loaded. ! Average Shear Stress. ! Allowable Stress. ! Design of Simple Connections STRESS! Stress Evisdom! verage Normal Stress in an xially Loaded ar! verage Shear Stress! llowable Stress! Design of Simple onnections 1 Equilibrium of a Deformable ody ody Force w F R x w(s). D s y Support

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

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

CH. 5 TRUSSES BASIC PRINCIPLES TRUSS ANALYSIS. Typical depth-to-span ratios range from 1:10 to 1:20. First: determine loads in various members

CH. 5 TRUSSES BASIC PRINCIPLES TRUSS ANALYSIS. Typical depth-to-span ratios range from 1:10 to 1:20. First: determine loads in various members CH. 5 TRUSSES BASIC PRINCIPLES Typical depth-to-span ratios range from 1:10 to 1:20 - Flat trusses require less overall depth than pitched trusses Spans: 40-200 Spacing: 10 to 40 on center - Residential

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

ES230 STRENGTH OF MATERIALS

ES230 STRENGTH OF MATERIALS ES230 STRENGTH OF MATERIALS Exam 1 Study Guide. Exam 1: Wednesday, February 8 th, in-class Updated 2/5/17 Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will

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

[5] Stress and Strain

[5] Stress and Strain [5] Stress and Strain Page 1 of 34 [5] Stress and Strain [5.1] Internal Stress of Solids [5.2] Design of Simple Connections (will not be covered in class) [5.3] Deformation and Strain [5.4] Hooke s Law

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

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

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

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

[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

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola MECHANICS OF MATERIALS Prepared by Engr. John Paul Timola Mechanics of materials branch of mechanics that studies the internal effects of stress and strain in a solid body. stress is associated with the

More information

Example 4: Design of a Rigid Column Bracket (Bolted)

Example 4: Design of a Rigid Column Bracket (Bolted) Worked Example 4: Design of a Rigid Column Bracket (Bolted) Example 4: Design of a Rigid Column Bracket (Bolted) Page : 1 Example 4: Design of a Rigid Column Bracket (Bolted) Determine the size of the

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

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

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

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering Mechanics Of Solids Suraj kr. Ray (surajjj2445@gmail.com) Department of Civil Engineering 1 Mechanics of Solids is a branch of applied mechanics that deals with the behaviour of solid bodies subjected

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

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS Unit 2: Unit code: QCF Level: Credit value: 15 Engineering Science L/601/10 OUTCOME 1 - TUTORIAL COLUMNS 1. Be able to determine the behavioural characteristics of elements of static engineering systems

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

3D Force Couple System and Resultant. Q.No.1: Replace the force system by an equivalent force and couple moment at point A.

3D Force Couple System and Resultant. Q.No.1: Replace the force system by an equivalent force and couple moment at point A. 3D Force Couple System and Resultant Q.No.1: Replace the force system by an equivalent force and couple moment at point A. Q.No.2: Handle forces F1 and F2 are applied to the electric drill. Replace this

More information

COLUMNS: BUCKLING (DIFFERENT ENDS)

COLUMNS: BUCKLING (DIFFERENT ENDS) COLUMNS: BUCKLING (DIFFERENT ENDS) Buckling of Long Straight Columns Example 4 Slide No. 1 A simple pin-connected truss is loaded and supported as shown in Fig. 1. All members of the truss are WT10 43

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

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

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR:

CIVIL DEPARTMENT MECHANICS OF STRUCTURES- ASSIGNMENT NO 1. Brach: CE YEAR: MECHANICS OF STRUCTURES- ASSIGNMENT NO 1 SEMESTER: V 1) Find the least moment of Inertia about the centroidal axes X-X and Y-Y of an unequal angle section 125 mm 75 mm 10 mm as shown in figure 2) Determine

More information

db = 23.7 in B C D 96 k bf = 8.97 in tf = in k = 1.09 in 13 Fy = 50 ksi Fu = 65 ksi Member A-B, Interior column: A E

db = 23.7 in B C D 96 k bf = 8.97 in tf = in k = 1.09 in 13 Fy = 50 ksi Fu = 65 ksi Member A-B, Interior column: A E line B1, second floor. t = thickness of connected part Pu = factored load to be resisted d = diameter of the bolt eb = one-half the depth of the beam, in. ec = one-half the depth of the column, in. Hub

More information

ENGINEERING SCIENCE H1 OUTCOME 1 - TUTORIAL 4 COLUMNS EDEXCEL HNC/D ENGINEERING SCIENCE LEVEL 4 H1 FORMERLY UNIT 21718P

ENGINEERING SCIENCE H1 OUTCOME 1 - TUTORIAL 4 COLUMNS EDEXCEL HNC/D ENGINEERING SCIENCE LEVEL 4 H1 FORMERLY UNIT 21718P ENGINEERING SCIENCE H1 OUTCOME 1 - TUTORIAL COLUMNS EDEXCEL HNC/D ENGINEERING SCIENCE LEVEL H1 FORMERLY UNIT 21718P This material is duplicated in the Mechanical Principles module H2 and those studying

More information

The plastic moment capacity of a composite cross-section is calculated in the program on the following basis (BS 4.4.2):

The plastic moment capacity of a composite cross-section is calculated in the program on the following basis (BS 4.4.2): COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIFORNIA SEPTEMBER 2002 COMPOSITE BEAM DESIGN BS 5950-90 Technical Note Composite Plastic Moment Capacity for Positive Bending This Technical Note describes

More information

Shear Stress. Horizontal Shear in Beams. Average Shear Stress Across the Width. Maximum Transverse Shear Stress. = b h

Shear Stress. Horizontal Shear in Beams. Average Shear Stress Across the Width. Maximum Transverse Shear Stress. = b h Shear Stre Due to the preence of the hear force in beam and the fact that t xy = t yx a horizontal hear force exit in the beam that tend to force the beam fiber to lide. Horizontal Shear in Beam The horizontal

More information

7.6 Stress in symmetrical elastic beam transmitting both shear force and bending moment

7.6 Stress in symmetrical elastic beam transmitting both shear force and bending moment 7.6 Stress in symmetrical elastic beam transmitting both shear force and bending moment à It is more difficult to obtain an exact solution to this problem since the presence of the shear force means that

More information

GENERAL GEOMETRY LEFT SIDE BEAM RIGHT SIDE BS :2000/AC:2009. Ratio 0.17

GENERAL GEOMETRY LEFT SIDE BEAM RIGHT SIDE BS :2000/AC:2009. Ratio 0.17 Autodesk Robot Structural Analysis Professional 2015 Design of fixed beam-to-beam connection BS 5950-1:2000/AC:2009 Ratio 0.17 GENERAL Connection no.: 2 Connection name: Beam-Beam Structure node: 40 Structure

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

Lecture 7 Two-Way Slabs

Lecture 7 Two-Way Slabs Lecture 7 Two-Way Slabs Two-way slabs have tension reinforcing spanning in BOTH directions, and may take the general form of one of the following: Types of Two-Way Slab Systems Lecture 7 Page 1 of 13 The

More information

db = 23.7 in B C D 96 k bf = 8.97 in tf = in k = 1.09 in 13 Fy = 50 ksi Fu = 65 ksi Member A-B, Interior column: A E

db = 23.7 in B C D 96 k bf = 8.97 in tf = in k = 1.09 in 13 Fy = 50 ksi Fu = 65 ksi Member A-B, Interior column: A E le B1, second floor. t = thickness of connected part Pu = factored load to be resisted d = diameter of the bolt eb = one-half the depth of the beam, ec = one-half the depth of the column, Hub = factored

More information

Chapter 8 BIAXIAL BENDING

Chapter 8 BIAXIAL BENDING Chapter 8 BAXAL BENDN 8.1 DEFNTON A cross section is subjected to biaial (oblique) bending if the normal (direct) stresses from section are reduced to two bending moments and. enerall oblique bending is

More information

JUT!SI I I I TO BE RETURNED AT THE END OF EXAMINATION. THIS PAPER MUST NOT BE REMOVED FROM THE EXAM CENTRE. SURNAME: FIRST NAME: STUDENT NUMBER:

JUT!SI I I I TO BE RETURNED AT THE END OF EXAMINATION. THIS PAPER MUST NOT BE REMOVED FROM THE EXAM CENTRE. SURNAME: FIRST NAME: STUDENT NUMBER: JUT!SI I I I TO BE RETURNED AT THE END OF EXAMINATION. THIS PAPER MUST NOT BE REMOVED FROM THE EXAM CENTRE. SURNAME: FIRST NAME: STUDENT NUMBER: COURSE: Tutor's name: Tutorial class day & time: SPRING

More information

Mechanics in Energy Resources Engineering - Chapter 5 Stresses in Beams (Basic topics)

Mechanics in Energy Resources Engineering - Chapter 5 Stresses in Beams (Basic topics) Week 7, 14 March Mechanics in Energy Resources Engineering - Chapter 5 Stresses in Beams (Basic topics) Ki-Bok Min, PhD Assistant Professor Energy Resources Engineering i Seoul National University Shear

More information

Chapter Objectives. Design a beam to resist both bendingand shear loads

Chapter Objectives. Design a beam to resist both bendingand shear loads Chapter Objectives Design a beam to resist both bendingand shear loads A Bridge Deck under Bending Action Castellated Beams Post-tensioned Concrete Beam Lateral Distortion of a Beam Due to Lateral Load

More information

Moments of Inertia. Notation:

Moments of Inertia. Notation: RCH 1 Note Set 9. S015abn Moments of nertia Notation: b d d d h c Jo O = name for area = name for a (base) width = calculus smbol for differentiation = name for a difference = name for a depth = difference

More information

The University of Melbourne Engineering Mechanics

The University of Melbourne Engineering Mechanics The University of Melbourne 436-291 Engineering Mechanics Tutorial Four Poisson s Ratio and Axial Loading Part A (Introductory) 1. (Problem 9-22 from Hibbeler - Statics and Mechanics of Materials) A short

More information

Solution: The moment of inertia for the cross-section is: ANS: ANS: Problem 15.6 The material of the beam in Problem

Solution: The moment of inertia for the cross-section is: ANS: ANS: Problem 15.6 The material of the beam in Problem Problem 15.4 The beam consists of material with modulus of elasticity E 14x10 6 psi and is subjected to couples M 150, 000 in lb at its ends. (a) What is the resulting radius of curvature of the neutral

More information

Steel Cross Sections. Structural Steel Design

Steel Cross Sections. Structural Steel Design Steel Cross Sections Structural Steel Design PROPERTIES OF SECTIONS Perhaps the most important properties of a beam are the depth and shape of its cross section. There are many to choose from, and there

More information

3.5 Reinforced Concrete Section Properties

3.5 Reinforced Concrete Section Properties CHAPER 3: Reinforced Concrete Slabs and Beams 3.5 Reinforced Concrete Section Properties Description his application calculates gross section moment of inertia neglecting reinforcement, moment of inertia

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

CHAPTER II EXPERIMENTAL INVESTIGATION

CHAPTER II EXPERIMENTAL INVESTIGATION CHAPTER II EXPERIMENTAL INVESTIGATION 2.1 SCOPE OF TESTING The objective of this research is to determine the force distribution between the column web and stiffener when the column flanges are subjected

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

Strength of Material. Shear Strain. Dr. Attaullah Shah

Strength of Material. Shear Strain. Dr. Attaullah Shah Strength of Material Shear Strain Dr. Attaullah Shah Shear Strain TRIAXIAL DEFORMATION Poisson's Ratio Relationship Between E, G, and ν BIAXIAL DEFORMATION Bulk Modulus of Elasticity or Modulus of Volume

More information

By Dr. Mohammed Ramidh

By Dr. Mohammed Ramidh Engineering Materials Design Lecture.6 the design of beams By Dr. Mohammed Ramidh 6.1 INTRODUCTION Finding the shear forces and bending moments is an essential step in the design of any beam. we usually

More information

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

VERTICAL ARM AB M B. MAXIMUM STRESSES occur on opposite sides of the vertical arm. MAXIMUM TENSILE STRESS. s t P A M(d 2 2) 54 CHER 8 pplications of lane Stress Combined Loadings he problems for Section 8.5 are to be solved assuming that the structures behave linearl elasticall and that the stresses caused b two or more loads

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

Chapter 6: Cross-Sectional Properties of Structural Members

Chapter 6: Cross-Sectional Properties of Structural Members Chapter 6: Cross-Sectional Properties of Structural Members Introduction Beam design requires the knowledge of the following. Material strengths (allowable stresses) Critical shear and moment values Cross

More information

Homework 6.1 P = 1000 N. δ δ δ. 4 cm 4 cm 4 cm. 10 cm

Homework 6.1 P = 1000 N. δ δ δ. 4 cm 4 cm 4 cm. 10 cm Homework 6.1 Three thick and wide boards are connected together by two parallel rows of uniformly distributed nails separated by longitude distance δ to form a beam that is subject to constant vertical

More information

Free Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2

Free Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2 Problem 10.9 The angle β of the system in Problem 10.8 is 60. The bars are made of a material that will safely support a tensile normal stress of 8 ksi. Based on this criterion, if you want to design the

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

REDUCTION OF A SIMPLE DISTRIBUTED LOADING. Today s Objectives: Students will be able to determine an equivalent force for a distributed load.

REDUCTION OF A SIMPLE DISTRIBUTED LOADING. Today s Objectives: Students will be able to determine an equivalent force for a distributed load. REDUCTION OF A SIMPLE DISTRIBUTED LOADING Today s Objectives: Students will be able to determine an equivalent force for a distributed load. = READING QUIZ 1. The resultant force (F R ) due to a distributed

More information

Appendix J. Example of Proposed Changes

Appendix J. Example of Proposed Changes Appendix J Example of Proposed Changes J.1 Introduction The proposed changes are illustrated with reference to a 200-ft, single span, Washington DOT WF bridge girder with debonded strands and no skew.

More information

2. Supports which resist forces in two directions. Fig Hinge. Rough Surface. Fig Rocker. Roller. Frictionless Surface

2. Supports which resist forces in two directions. Fig Hinge. Rough Surface. Fig Rocker. Roller. Frictionless Surface 4. Structural Equilibrium 4.1 ntroduction n statics, it becomes convenient to ignore the small deformation and displacement. We pretend that the materials used are rigid, having the propert or infinite

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

Chapter 8: Bending and Shear Stresses in Beams

Chapter 8: Bending and Shear Stresses in Beams Chapter 8: Bending and Shear Stresses in Beams Introduction One of the earliest studies concerned with the strength and deflection of beams was conducted by Galileo Galilei. Galileo was the first to discuss

More information

INTRODUCTION TO STRAIN

INTRODUCTION TO STRAIN SIMPLE STRAIN INTRODUCTION TO STRAIN In general terms, Strain is a geometric quantity that measures the deformation of a body. There are two types of strain: normal strain: characterizes dimensional changes,

More information

Serviceability Deflection calculation

Serviceability Deflection calculation Chp-6:Lecture Goals Serviceability Deflection calculation Deflection example Structural Design Profession is concerned with: Limit States Philosophy: Strength Limit State (safety-fracture, fatigue, overturning

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

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3 MECE 3321 MECHANICS OF SOLIDS CHAPTER 3 Samantha Ramirez TENSION AND COMPRESSION TESTS Tension and compression tests are used primarily to determine the relationship between σ avg and ε avg in any material.

More information

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar

Design of Steel Structures Prof. S.R.Satish Kumar and Prof. A.R.Santha Kumar 5.4 Beams As stated previousl, the effect of local buckling should invariabl be taken into account in thin walled members, using methods described alread. Laterall stable beams are beams, which do not

More information

Mechanics of Materials CIVL 3322 / MECH 3322

Mechanics of Materials CIVL 3322 / MECH 3322 Mechanics of Materials CIVL 3322 / MECH 3322 2 3 4 5 6 7 8 9 10 A Quiz 11 A Quiz 12 A Quiz 13 A Quiz 14 A Quiz 15 A Quiz 16 In Statics, we spent most of our time looking at reactions at supports Two variations

More information

5.2 Rigid Bodies and Two-Dimensional Force Systems

5.2 Rigid Bodies and Two-Dimensional Force Systems 5.2 Rigid odies and Two-Dimensional Force Systems 5.2 Rigid odies and Two-Dimensional Force Systems Procedures and Strategies, page 1 of 1 Procedures and Strategies for Solving Problems Involving Equilibrium

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

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

Basic principles of steel structures. Dr. Xianzhong ZHAO

Basic principles of steel structures. Dr. Xianzhong ZHAO Basic principles of steel structures Dr. Xianzhong ZHAO.zhao@mail.tongji.edu.cn www.sals.org.cn 1 Introduction Resistance of cross-section Compression members Outlines Overall stabilit of uniform (solid

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

OUTCOME 1 - TUTORIAL 3 BENDING MOMENTS. You should judge your progress by completing the self assessment exercises. CONTENTS

OUTCOME 1 - TUTORIAL 3 BENDING MOMENTS. You should judge your progress by completing the self assessment exercises. CONTENTS Unit 2: Unit code: QCF Level: 4 Credit value: 15 Engineering Science L/601/1404 OUTCOME 1 - TUTORIAL 3 BENDING MOMENTS 1. Be able to determine the behavioural characteristics of elements of static engineering

More information

A Simply supported beam with a concentrated load at mid-span: Loading Stages

A Simply supported beam with a concentrated load at mid-span: Loading Stages A Simply supported beam with a concentrated load at mid-span: Loading Stages P L/2 L PL/4 MOMNT F b < 1 lastic F b = 2 lastic F b = 3 lastoplastic 4 F b = Plastic hinge Plastic Dr. M.. Haque, P.. (LRFD:

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

Chapter 9 BIAXIAL SHEARING

Chapter 9 BIAXIAL SHEARING 9. DEFNTON Chapter 9 BAXAL SHEARNG As we have seen in the previous chapter, biaial (oblique) shearing produced b the shear forces and, appears in a bar onl accompanied b biaial bending (we ma discuss about

More information

Appendix. A 1 Properties of areas.* *Symbols used are: A = area I = moment of inertia S = Section modulus

Appendix. A 1 Properties of areas.* *Symbols used are: A = area I = moment of inertia S = Section modulus Appendix A 1 Properties of areas.* *Symbols used are: A = area I = moment of inertia S = Section modulus r = radius of gyration = I/A J = polar moment of inertia Z p = polar section modulus Circle R D

More information

Errata Sheet for S. D. Rajan, Introduction to Structural Analysis & Design (1 st Edition) John Wiley & Sons Publication

Errata Sheet for S. D. Rajan, Introduction to Structural Analysis & Design (1 st Edition) John Wiley & Sons Publication S D Rajan, Introduction to Structural Analsis & Design ( st Edition) Errata Sheet for S D Rajan, Introduction to Structural Analsis & Design ( st Edition) John Wile & Sons Publication Chapter Page Correction

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

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

CHAPTER 5 Statically Determinate Plane Trusses

CHAPTER 5 Statically Determinate Plane Trusses CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS TYPES OF ROOF TRUSS ROOF TRUSS SETUP ROOF TRUSS SETUP OBJECTIVES To determine the STABILITY and DETERMINACY of plane trusses To analyse

More information