ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER /15 PAPER A

Size: px
Start display at page:

Download "ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER /15 PAPER A"

Transcription

1 SSOCITE DEGREE IN ENGINEERING EXMINTIONS SEMESTER /15 PPER COURSE NME: ENGINEERING MECHNICS - STTICS CODE: ENG 2008 GROUP: D ENG II DTE: May 2015 TIME: DURTION: 2 HOURS INSTRUCTIONS: 1. This paper consists of SIX questions. 2. Candidates must attempt NY FOUR questions on this paper. 3. ll working MUST be CLERLY shown. 4. Keep all parts of the same question together. 5. The use of programmable calculators is permitted. DO NOT TURN THIS PGE UNTIL YOU RE TOLD TO DO SO

2 [Question 1] (a) Figure 1.1 below shows four forces acting on a particle at the origin. Determine the magnitude of P and the orientation of the 800 N force so that the particle is in equilibrium. [10 marks] 800 N y 700 N 60 0 P Figure N (b) Epress the force F in Figure 1.2 in Cartesian vector form. [7 marks] z F y 100 N Figure 1.2 (c) Determine the moment of the couple formed by the two forces F and F acting on the bar B. z [8 marks] F = {-6 i + 3 j + 3k } N -F = {6 i - 3 j - 3k } N B y Figure 1.3

3 [Total = 25 Marks] [Question 2] (a) The loading on the beam B in Figure 2.1 consists of three point loads and a couple moment. Replace the loading on the beam by a single resultant force. Specify where the force acts measured from. [15 marks] 450 N 300 N 700 N 60 0 B m 4 m 3 m 1500 Nm Figure 2.1 (b) Find the magnitude of the projected component of the force F along the cable C in Figure 2.2. [10 marks] z C 4 m 2 m B 6 m F = 500 N y 4 m Figure 2.2 [Total = 25 marks]

4 [Question 3] (a) girder B shown in Figure 3.1 has four concentrated loads acting on it. 7 kn 7 kn 7 kn 7 kn 2 m 2 m 2 m 2 m 1 m B Figure 3.1 Neglecting the weight of the girder, determine: (i) the reactions at and B. [5 marks] (ii) Draw the shear force diagram. [8 marks] (iii) Draw the bending moment diagram. Indicate the maimum value of the bending moment. [12 marks] [Total = 25 marks] [Question 4] Figure 4.1 shows a plane frame which is simply supported. 12 kn 6 kn 6 kn H G F E 2 m B C D 2 m 2m 2m Figure 4.1 (a) Determine the reactions at and D. [6 marks] (b) Identify the zero-force member(s) and justify your answer. [3 marks] (c) Using the method of sections determine the forces in the members BC, GC and GF. [16 marks]

5 [Total = 25 marks] 5. (a) uniform crate has a mass of 40 kg and rests on a floor for which s = The crate is pushed with a force F at an angle of 30 0 above the horizontal as shown in Figure 5.1. F 30 0 crate Figure 5.1 floor Determine the smallest force F required to move the crate. [13 marks] (b) crate of weight 200 lb is supported by a cord which wraps over a pipe as shown in Figure 5.2. F 200 lb Figure 5.2 (i) Determine the minimum force F which is required to prevent the crate from slipping downwards if the cord passes once over the pipe ( = ). [8 marks]

6 (ii) What tension is required to allow the crate to move downwards at constant velocity when = [4 marks] s = 0.25 and k = 0.2. [Total = 25 marks] [Question 6] (a) Eplain the meaning of the term moment of inertia. [2 marks] (b) With the aid of a diagram eplain the parallel ais theorem. [4 marks] (c) The cross-section of a beam is shown in Figure 6.1. y 120 mm 20 mm 50 mm 125 mm 20 mm Figure 6.1 (i) Determine the location of the centroid of the beam from the -ais. [8 marks] (ii) Compute the moment of inertia of the area about the -ais. [11 marks]

7 [Total = 25 marks] END OF EXM SSOCITE DEGREE IN ENGINEERING SOLUTIONS SEMESTER MY COURSE NME: ENGINEERING STTICS CODE: GROUP: D-ENG 2 DTE: MY 2015 TIME: DURTION: 2 HOURS SOLUTIONS: 1. (a) F = 0; 700 cos cos = 0... (1) [2] F y = 0; 700 sin sin - P = 0...(2) [2] From (1): 800 cos = 700 cos = 650 cos = 650/800 = = cos -1 (0.8125) = [3] Substituting into ((2):

8 P = 700 sin sin = 700 sin sin P = = 1093 N [3] (b) F = 100 N F cos 40 0 = F = 100 F = 100/cos40 0 = 131 N [2] F = 100 cos 60 0 = 50 N [1] F y = 100 cos 30 0 = 86.6 N [1] F z = 131 cos 50 0 = 84.2 N [2] F = { 50 i j k} N [1] (c) M = r F = (0.6 k j) (- 6 i + 3 j + 3 k) = [3] i j k [1] = i j k [2] = i ( ) - j (0-3.6) + k ( ) M = {4.2 i j k} Nm [2] 2. (a) 450 N 300 N 700 N 60 0 B m 4 m 3 m 1500 Nm F = 450 cos cos 60 0 = = -125 N [3] F y = -450 sin sin N = N F = N R [3] F R = [( ) + (-1296) 2 ] = 1302 N

9 = tan -1 (1296/125) = [2] M = sin sin = M = Nm [3] d N M = d sin = 9535 d = 9535/(1302 sin ) d = 7.36 m [4] (b) C 2 m B F = 500 N 4 m 6 m 4 m r B = {- 6 i + 2 k} m [1] r C = {- 4 j + 4 k} m [1] u B = (- 6 i + 2 k)/ ( ) = (- 6 i + 2 k)/6.32 [2] u C = (- 4 j + 4 k)/ ( ) = (- 4 j + 4 k)/5.66 [2] F = (500) (- 6 i + 2 k)/6.32 [1] The projected component of F along C is given by F. u C.

10 F. u C = (500/6.23) (- 6 i + 2 k).(- 4 j + 4 k)/5.66 = = 113 N [3] 3. 7 kn 7 kn 7 kn 7 kn 2 m 2 m 2 m 2 m 1 m B (a) M = 0; R B 9 = R B = R B = 0 R B = 140/9 = 15.6 kn M B = 0; -R = 0-9 R = 0 R = 112/9 = 12.4 kn [5] (b)

11 7 kn 7 kn 7 kn 7 kn 2 m 2 m 2 m 2 m 1 m B V(kN) 12.4 kn 24.8 knm 5.4 kn 10.8 knm -1.6 kn -8.6 kn -3.2 knm knm knm kn M(kNm) 24.8 knm 15.2 knm 35.6 knm 32.4 knm

12 M ma = 35.6 knm 4. (a) R 12 kn 6 kn 6 kn 2 m 2 m 2m D R D M = 0; R B 6 = R B = 0 R B = 84/6 = 14 kn [3] M D = 0; -R = 0 6 R = = 60 R = 60/6 = 10 kn [3] (b) Zero force members are : B and FE. [3 ] (c) 12 kn H G 45 0 F GF 2 m F GC 10 kn 2 m B F BC [4] Using the section shown above:

13 F y = 0; F GC sin 45 0 = 0 F GC = (10-12)/ sin 45 0 = kn (S) [4] M G = 0; F BC = 0 F BC = 20/2 = 10 kn (T) [4] F = 0; F GF + F BC + F GC cos45 0 = 0 F GF (-2.83) cos45 0 = 0 F GF = cos45 0 = -8.0 kn (S) [4] 5. (a) F 30 0 crate [3] f floor N mg Equation of equilibrium: F = 0; F cos N = 0 F cos N = (1) [3] F y = 0; -Fsin g + N = 0... (2) [2] From (1): N = Fcos 30 0 / (3) Substituting equation (3) into (2) gives: -Fsin (9.8) + Fcos 30 0 /0.25 = F F = 0 or 2.96 F = 392 F = 132 N [5] (b) (i) T 2 = 200 lb = and = 0.25

14 T 2 = T 1 e 200 = T 1 ep( 0.25 ) T 1 = 200/ ep( 0.25 ) T 1 = 91.2 lb [6] (ii) T 1 = 200/ ep( 0.2 ) = 107 lb [3] 6. (a) Moment of inertia is the second moment of area of a cross-section about a given ais. [2] (b) rea = G d Consider the figure shown above with and centroid at point G. The centroidal ais is -. The moment of inertia about the centroidal ais is I. The moment of inertia about the new ais - which is at a perpendicular distance d from the centroidal ais is given by I = I + d 2 [4] (c) y 120 mm 2 20 mm 50 mm mm

15 Divide the cross-section in parts 1 and 2 as shown in the diagram: (i) 1 = = 2500 mm 2 ; y 1 = 125/2 = 62.5 mm [2] 2 = = 2400 mm 2 ; y 1 = /2 = 135 mm [2] ( ) ŷ = 1 y y 2 ( ) ŷ = [2] 4900 ŷ = = ŷ = /4900 = mm [2] (ii) I 1 = (1/12) (125/2) 2 = I 1 = mm 4 [5] I 2 = (1/12) (135) 2 = I 2 = mm 4 [5] I = I 1 + I 2 = ( ) 10 6 mm 4 I = mm 4 [1]

16 Eamination Paper nalysis ssociate of pplied Science Degree Module: Engineering Mechanics (Statics) Eaminer: Noel Brown pril 2, 2015 Syllabus Objectives Question B C D E F G H I J 1 X X X 2 X X 3 X X 4 X 5 X 6 X Question 1 Question is adequate for this level. Question 2 Question is adequate for this level. Question 3 Question is adequate for this level. Question 4 Question is adequate for this level. Question 5 Question is adequate for this level. Question 6 Question is adequate for this level.

17 The paper need to be formatted properly. I have included some of the formatting. Please ensure that the paper is proofread before it is sent to the second eaminer. Overall both papers are provides good coverage of the syllabus objectives. The time allotted is also adequate for the student to safely complete four questions. ny of the papers could be used as the final.

ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER /13

ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER /13 ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER 2 2012/13 COURSE NAME: ENGINEERING MECHANICS - STATICS CODE: ENG 2008 GROUP: AD ENG II DATE: May 2013 TIME: DURATION: 2 HOURS INSTRUCTIONS: 1. This

More information

ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS. SEMESTER 2 May 2013

ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS. SEMESTER 2 May 2013 ASSOCIATE DEGREE IN ENGINEERING EXAMINATIONS SEMESTER 2 May 2013 COURSE NAME: CODE: Mechanical Engineering Science [8 CHARACTER COURSE CODE] GROUP: AD-ENG 1 DATE: TIME: DURATION: "[EXAM DATE]" "[TIME OF

More information

PORTMORE COMMUNITY COLLEGE ASSOCIATE DEGREE IN ENGINEERING TECHNOLOGY

PORTMORE COMMUNITY COLLEGE ASSOCIATE DEGREE IN ENGINEERING TECHNOLOGY PORTMORE COMMUNITY COLLEGE ASSOCIATE DEGREE IN ENGINEERING TECHNOLOGY RESIT EXAMINATIONS SEMESTER 2 JUNE 2011 COURSE NAME: Mechanical Engineering Science CODE: GROUP: ADET 1 DATE: JUNE 28 TIME: DURATION:

More information

PORTMORE COMMUNITY COLLEGE

PORTMORE COMMUNITY COLLEGE PORTMORE COMMUNITY COLLEGE ASSOCIATE DEGREE IN ENGINEERING TECHNOLOGY RESIT EXAMINATIONS SEMESTER 2 July 2012 COURSE NAME: Mechanical Engineering Science CODE: GROUP: ADET 1 DATE: July 3, 2012 TIME: DURATION:

More information

Check Homework. Reading Quiz Applications Equations of Equilibrium Example Problems Concept Questions Group Problem Solving Attention Quiz

Check Homework. Reading Quiz Applications Equations of Equilibrium Example Problems Concept Questions Group Problem Solving Attention Quiz THREE-DIMENSIONAL FORCE SYSTEMS Today s Objectives: Students will be able to solve 3-D particle equilibrium problems by a) Drawing a 3-D free body diagram, and, b) Applying the three scalar equations (based

More information

CHAPTER 2: EQUILIBRIUM OF RIGID BODIES

CHAPTER 2: EQUILIBRIUM OF RIGID BODIES For a rigid body to be in equilibrium, the net force as well as the net moment about any arbitrary point O must be zero Summation of all external forces. Equilibrium: Sum of moments of all external forces.

More information

Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3

Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3 Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3 2 3 Determine the magnitude of the resultant force FR = F1 + F2 and its direction, measured counterclockwise from the

More information

Engineering Mechanics: Statics in SI Units, 12e

Engineering Mechanics: Statics in SI Units, 12e Engineering Mechanics: Statics in SI Units, 12e 5 Equilibrium of a Rigid Body Chapter Objectives Develop the equations of equilibrium for a rigid body Concept of the free-body diagram for a rigid body

More information

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns, and, b) Recognize two-force members. In-Class

More information

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns, and b) Recognize two-force members. In-Class

More information

== Delft University of Technology == Give on the upper right. Exam STATICS /

== Delft University of Technology == Give on the upper right. Exam STATICS / == elft University of Technology == Give on the upper right University ourse pplied Mechanics corner of each sheet your NME STUY NUMER and ISIPLINE Exam STTIS 2003.08.26 / 09.00-12.00 The work of a student

More information

Chapter 2. Shear Force and Bending Moment. After successfully completing this chapter the students should be able to:

Chapter 2. Shear Force and Bending Moment. After successfully completing this chapter the students should be able to: Chapter Shear Force and Bending Moment This chapter begins with a discussion of beam types. It is also important for students to know and understand the reaction from the types of supports holding the

More information

Module 6. Approximate Methods for Indeterminate Structural Analysis. Version 2 CE IIT, Kharagpur

Module 6. Approximate Methods for Indeterminate Structural Analysis. Version 2 CE IIT, Kharagpur Module 6 Approximate Methods for Indeterminate Structural Analysis Lesson 35 Indeterminate Trusses and Industrial rames Instructional Objectives: After reading this chapter the student will be able to

More information

RIN: Monday, May 16, Problem Points Score Total 100

RIN: Monday, May 16, Problem Points Score Total 100 RENSSELER POLYTEHNI INSTITUTE TROY, NY FINL EXM INTRODUTION TO ENGINEERING NLYSIS ENGR-00) NME: Solution Section: RIN: Monda, Ma 6, 06 Problem Points Score 0 0 0 0 5 0 6 0 Total 00 N.B.: You will be graded

More information

8.3 Shear and Bending-Moment Diagrams Constructed by Areas

8.3 Shear and Bending-Moment Diagrams Constructed by Areas 8.3 Shear and ending-moment Diagrams Constructed by reas 8.3 Shear and ending-moment Diagrams Constructed by reas Procedures and Strategies, page 1 of 3 Procedures and Strategies for Solving Problems Involving

More information

BTECH MECHANICAL PRINCIPLES AND APPLICATIONS. Level 3 Unit 5

BTECH MECHANICAL PRINCIPLES AND APPLICATIONS. Level 3 Unit 5 BTECH MECHANICAL PRINCIPLES AND APPLICATIONS Level 3 Unit 5 FORCES AS VECTORS Vectors have a magnitude (amount) and a direction. Forces are vectors FORCES AS VECTORS (2 FORCES) Forces F1 and F2 are in

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

Ishik University / Sulaimani Architecture Department. Structure. ARCH 214 Chapter -5- Equilibrium of a Rigid Body

Ishik University / Sulaimani Architecture Department. Structure. ARCH 214 Chapter -5- Equilibrium of a Rigid Body Ishik University / Sulaimani Architecture Department 1 Structure ARCH 214 Chapter -5- Equilibrium of a Rigid Body CHAPTER OBJECTIVES To develop the equations of equilibrium for a rigid body. To introduce

More information

8.1 Internal Forces in Structural Members

8.1 Internal Forces in Structural Members 8.1 Internal Forces in Structural Members 8.1 Internal Forces in Structural Members xample 1, page 1 of 4 1. etermine the normal force, shear force, and moment at sections passing through a) and b). 4

More information

1. The horizontal beam represented in Examination Figure 6 carries three loads P 1. and R 2

1. The horizontal beam represented in Examination Figure 6 carries three loads P 1. and R 2 Student ID: 52573847 Exam: 286037RR - Engineering Mechanics, Part 2 When you have completed your exam and reviewed your answers, click Submit Exam. Answers will not be recorded until you hit Submit Exam.

More information

ARCH 631 Note Set 2.1 F2010abn. Statics Primer

ARCH 631 Note Set 2.1 F2010abn. Statics Primer RCH 631 Note Set.1 F010abn Statics Primer Notation: a = name for acceleration = area (net = with holes, bearing = in contact, etc...) (C) = shorthand for compression d = perpendicular distance to a force

More information

INTI INTERNATIONAL UNIVERSITY FOUNDATION PROGRAMME (ENGINEERING/SCIENCE) (CFSI) EGR 1203: ENGINEERING MECHANICS FINAL EXAMINATION: AUGUST 2015 SESSION

INTI INTERNATIONAL UNIVERSITY FOUNDATION PROGRAMME (ENGINEERING/SCIENCE) (CFSI) EGR 1203: ENGINEERING MECHANICS FINAL EXAMINATION: AUGUST 2015 SESSION i) (0.005 mm) 2 (1 mark) EGR1203(F)/Page 1 of 14 INTI INTERNATIONAL UNIVERSITY FOUNDATION PROGRAMME (ENGINEERING/SCIENCE) (CFSI) EGR 1203: ENGINEERING MECHANICS FINAL EXAMINATION: AUGUST 2015 SESSION Instructions:

More information

Delft Applied Mechanics Course: Statics AE1-914-I. 18 August 2004, 9:00 12:00

Delft Applied Mechanics Course: Statics AE1-914-I. 18 August 2004, 9:00 12:00 Delft pplied Mechanics Course: Statics E1-914-I 18 ugust 2004, 9:00 12:00 This is the English exam. Only the answer forms will be collected ny other sheets will be rejected. Write down your name and student

More information

M D P L sin x FN L sin C W L sin C fl cos D 0.

M D P L sin x FN L sin C W L sin C fl cos D 0. 789 roblem 9.26 he masses of the ladder and person are 18 kg and 90 kg, respectively. he center of mass of the 4-m ladder is at its midpoint. If D 30, what is the minimum coefficient of static friction

More information

Shear Force and Bending Moment Diagrams for a Beam Steven Vukazich San Jose State University

Shear Force and Bending Moment Diagrams for a Beam Steven Vukazich San Jose State University Shear Force and Bending oment Diagrams for a Beam Steven ukazich San Jose State University General procedure for the construction of internal force diagrams 1. Find all of the eternal forces and draw the

More information

ENGR-1100 Introduction to Engineering Analysis. Lecture 13

ENGR-1100 Introduction to Engineering Analysis. Lecture 13 ENGR-1100 Introduction to Engineering Analysis Lecture 13 EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS Today s Objectives: Students will be able to: a) Identify support reactions, and, b) Draw a free-body

More information

STATICS. FE Review. Statics, Fourteenth Edition R.C. Hibbeler. Copyright 2016 by Pearson Education, Inc. All rights reserved.

STATICS. FE Review. Statics, Fourteenth Edition R.C. Hibbeler. Copyright 2016 by Pearson Education, Inc. All rights reserved. STATICS FE Review 1. Resultants of force systems VECTOR OPERATIONS (Section 2.2) Scalar Multiplication and Division VECTOR ADDITION USING EITHER THE PARALLELOGRAM LAW OR TRIANGLE Parallelogram Law: Triangle

More information

7 STATICALLY DETERMINATE PLANE TRUSSES

7 STATICALLY DETERMINATE PLANE TRUSSES 7 STATICALLY DETERMINATE PLANE TRUSSES OBJECTIVES: This chapter starts with the definition of a truss and briefly explains various types of plane truss. The determinancy and stability of a truss also will

More information

Engineering Mechanics Statics

Engineering Mechanics Statics Mechanical Systems Engineering -2016 Engineering Mechanics Statics 3. Force Vectors; Position Vector & Dot product Position Vector A position vector is a fixed vector that locates a point in space relative

More information

Eng Sample Test 4

Eng Sample Test 4 1. An adjustable tow bar connecting the tractor unit H with the landing gear J of a large aircraft is shown in the figure. Adjusting the height of the hook F at the end of the tow bar is accomplished by

More information

SLOPE-DEFLECTION METHOD

SLOPE-DEFLECTION METHOD SLOPE-DEFLECTION ETHOD The slope-deflection method uses displacements as unknowns and is referred to as a displacement method. In the slope-deflection method, the moments at the ends of the members are

More information

F R. + F 3x. + F 2y. = (F 1x. j + F 3x. i + F 2y. i F 3y. i + F 1y. j F 2x. ) i + (F 1y. ) j. F 2x. F 3y. = (F ) i + (F ) j. ) j

F R. + F 3x. + F 2y. = (F 1x. j + F 3x. i + F 2y. i F 3y. i + F 1y. j F 2x. ) i + (F 1y. ) j. F 2x. F 3y. = (F ) i + (F ) j. ) j General comments: closed book and notes but optional one page crib sheet allowed. STUDY: old exams, homework and power point lectures! Key: make sure you can solve your homework problems and exam problems.

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

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd Chapter Objectives To develop the equations of equilibrium for a rigid body. To introduce the concept of the free-body diagram for a rigid body. To show how to solve rigid-body equilibrium problems using

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

Types of Structures & Loads

Types of Structures & Loads Structure Analysis I Chapter 4 1 Types of Structures & Loads 1Chapter Chapter 4 Internal lloading Developed in Structural Members Internal loading at a specified Point In General The loading for coplanar

More information

MOMENT OF A COUPLE. Today s Objectives: Students will be able to. a) define a couple, and, b) determine the moment of a couple.

MOMENT OF A COUPLE. Today s Objectives: Students will be able to. a) define a couple, and, b) determine the moment of a couple. Today s Objectives: Students will be able to MOMENT OF A COUPLE a) define a couple, and, b) determine the moment of a couple. In-Class activities: Check Homework Reading Quiz Applications Moment of a Couple

More information

SOLUTION 8 1. a+ M B = 0; N A = 0. N A = kn = 16.5 kn. Ans. + c F y = 0; N B = 0

SOLUTION 8 1. a+ M B = 0; N A = 0. N A = kn = 16.5 kn. Ans. + c F y = 0; N B = 0 8 1. The mine car and its contents have a total mass of 6 Mg and a center of gravity at G. If the coefficient of static friction between the wheels and the tracks is m s = 0.4 when the wheels are locked,

More information

TUTORIAL SHEET 1. magnitude of P and the values of ø and θ. Ans: ø =74 0 and θ= 53 0

TUTORIAL SHEET 1. magnitude of P and the values of ø and θ. Ans: ø =74 0 and θ= 53 0 TUTORIAL SHEET 1 1. The rectangular platform is hinged at A and B and supported by a cable which passes over a frictionless hook at E. Knowing that the tension in the cable is 1349N, determine the moment

More information

EQUATIONS OF MOTION: RECTANGULAR COORDINATES

EQUATIONS OF MOTION: RECTANGULAR COORDINATES EQUATIONS OF MOTION: RECTANGULAR COORDINATES Today s Objectives: Students will be able to: 1. Apply Newton s second law to determine forces and accelerations for particles in rectilinear motion. In-Class

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

Chapter 04 Equilibrium of Rigid Bodies

Chapter 04 Equilibrium of Rigid Bodies Chapter 04 Equilibrium of Rigid Bodies Application Engineers designing this crane will need to determine the forces that act on this body under various conditions. 4-2 Introduction For a rigid body, the

More information

P.E. Civil Exam Review:

P.E. Civil Exam Review: P.E. Civil Exam Review: Structural Analysis J.P. Mohsen Email: jpm@louisville.edu Structures Determinate Indeterminate STATICALLY DETERMINATE STATICALLY INDETERMINATE Stability and Determinacy of Trusses

More information

Module 3. Analysis of Statically Indeterminate Structures by the Displacement Method

Module 3. Analysis of Statically Indeterminate Structures by the Displacement Method odule 3 Analysis of Statically Indeterminate Structures by the Displacement ethod Lesson 21 The oment- Distribution ethod: rames with Sidesway Instructional Objectives After reading this chapter the student

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

Easy. P5.3 For equilibrium: f = F and n = F g. Also, f = n, i.e., f n F F g. (a) 75.0 N N N N (b) ma y.

Easy. P5.3 For equilibrium: f = F and n = F g. Also, f = n, i.e., f n F F g. (a) 75.0 N N N N (b) ma y. Chapter 5 Homework Solutions Easy P5.3 For equilibrium: f = F and n = F g. Also, f = n, i.e., (a) f n F F g s k 75.0 N 25.09.80 N 0.306 60.0 N 25.09.80 N 0.245 ANS. FIG. P5.3 P5.4 F y ma y : n mg 0 f s

More information

3.1 CONDITIONS FOR RIGID-BODY EQUILIBRIUM

3.1 CONDITIONS FOR RIGID-BODY EQUILIBRIUM 3.1 CONDITIONS FOR RIGID-BODY EQUILIBRIUM Consider rigid body fixed in the x, y and z reference and is either at rest or moves with reference at constant velocity Two types of forces that act on it, the

More information

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method Module 2 Analysis of Statically Indeterminate Structures by the Matrix Force Method Lesson 8 The Force Method of Analysis: Beams Instructional Objectives After reading this chapter the student will be

More information

EQUILIBRIUM OF RIGID BODIES

EQUILIBRIUM OF RIGID BODIES EQUILIBRIUM OF RIGID BODIES Equilibrium A body in equilibrium is at rest or can translate with constant velocity F = 0 M = 0 EQUILIBRIUM IN TWO DIMENSIONS Case where the force system acting on a rigid

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

However, the friction forces are limited in magnitude and will not prevent motion if sufficiently large forces are applied.

However, the friction forces are limited in magnitude and will not prevent motion if sufficiently large forces are applied. FRICTION 1 Introduction In preceding chapters, it was assumed that surfaces in contact were either frictionless (surfaces could move freely with respect to each other) or rough (tangential forces prevent

More information

Final Examination Study Set 1. (Solutions will be in the Solutions Manual of Textbook)

Final Examination Study Set 1. (Solutions will be in the Solutions Manual of Textbook) Final Examination Study Set 1 (Solutions will be in the Solutions Manual of Textbook) Final Examination Study Set 2 (Solutions will be in the Solutions Manual of Textbook) 3/86 The shaft, lever,

More information

APPLIED MECHANICS I Resultant of Concurrent Forces Consider a body acted upon by co-planar forces as shown in Fig 1.1(a).

APPLIED MECHANICS I Resultant of Concurrent Forces Consider a body acted upon by co-planar forces as shown in Fig 1.1(a). PPLIED MECHNICS I 1. Introduction to Mechanics Mechanics is a science that describes and predicts the conditions of rest or motion of bodies under the action of forces. It is divided into three parts 1.

More information

EGN 3310 Practice Final Spring 2017

EGN 3310 Practice Final Spring 2017 EGN 3310 Practice Final Spring 2017 *Try finishing each problem in 15 minutes or less to practice test-like time contraints. The topics on the practice exam are what I feel have been stressed in class,

More information

Announcements. Equilibrium of a Particle in 2-D

Announcements. Equilibrium of a Particle in 2-D nnouncements Equilibrium of a Particle in 2-D Today s Objectives Draw a free body diagram (FBD) pply equations of equilibrium to solve a 2-D problem Class ctivities pplications What, why, and how of a

More information

Name ME 270 Summer 2006 Examination No. 1 PROBLEM NO. 3 Given: Below is a Warren Bridge Truss. The total vertical height of the bridge is 10 feet and each triangle has a base of length, L = 8ft. Find:

More information

Physics B Newton s Laws AP Review Packet

Physics B Newton s Laws AP Review Packet Force A force is a push or pull on an object. Forces cause an object to accelerate To speed up To slow down To change direction Unit: Newton (SI system) Newton s First Law The Law of Inertia. A body in

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

Announcements. Equilibrium of a Rigid Body

Announcements. Equilibrium of a Rigid Body Announcements Equilibrium of a Rigid Body Today s Objectives Identify support reactions Draw a free body diagram Class Activities Applications Support reactions Free body diagrams Examples Engr221 Chapter

More information

where x and y are any two non-parallel directions in the xy-plane. iii) One force equation and one moment equation.

where x and y are any two non-parallel directions in the xy-plane. iii) One force equation and one moment equation. Concurrent Force System ( of Particles) Recall that the resultant of a concurrent force system is a force F R that passes through the point of concurrency, which we label as point O. The moment equation,

More information

two structural analysis (statics & mechanics) Structural Requirements Structure Requirements Structure Requirements serviceability efficiency

two structural analysis (statics & mechanics) Structural Requirements Structure Requirements Structure Requirements serviceability efficiency LIED RCHITECTURL STRUCTURES: STRUCTURL NLYSIS ND SYSTEMS DR. NNE NICHOLS SRING 018 lecture two structural analysis (statics & mechanics) nalysis 1 pplied rchitectural Structures 009abn Structural Requirements

More information

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method Module 2 Analysis of Statically Indeterminate Structures by the Matrix Force Method Lesson 11 The Force Method of Analysis: Frames Instructional Objectives After reading this chapter the student will be

More information

Beams. Beams are structural members that offer resistance to bending due to applied load

Beams. Beams are structural members that offer resistance to bending due to applied load Beams Beams are structural members that offer resistance to bending due to applied load 1 Beams Long prismatic members Non-prismatic sections also possible Each cross-section dimension Length of member

More information

S in. S in 40 M s = (20.35)(30.0) M s = 611 in-lb clockwise = 2.12 m with a negative action. The moment about B is

S in. S in 40 M s = (20.35)(30.0) M s = 611 in-lb clockwise = 2.12 m with a negative action. The moment about B is Problem 4.14 The moment eerted about point E b the weight is 299 in-lb. What moment does the weight eert about point S? S 30 13 in. 12 in. E 40 The ke is the geometr rom trigonometr, cos 40 = d 2 13 in,

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

5. Plane Kinetics of Rigid Bodies

5. Plane Kinetics of Rigid Bodies 5. Plane Kinetics of Rigid Bodies 5.1 Mass moments of inertia 5.2 General equations of motion 5.3 Translation 5.4 Fixed axis rotation 5.5 General plane motion 5.6 Work and energy relations 5.7 Impulse

More information

E 490 FE Exam Prep. Engineering Mechanics

E 490 FE Exam Prep. Engineering Mechanics E 490 FE Exam Prep Engineering Mechanics 2008 E 490 Course Topics Statics Newton s Laws of Motion Resultant Force Systems Moment of Forces and Couples Equilibrium Pulley Systems Trusses Centroid of an

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

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd Chapter Objectives To generalize the procedure by formulating equations that can be plotted so that they describe the internal shear and moment throughout a member. To use the relations between distributed

More information

Bending Stress. Sign convention. Centroid of an area

Bending Stress. Sign convention. Centroid of an area Bending Stress Sign convention The positive shear force and bending moments are as shown in the figure. Centroid of an area Figure 40: Sign convention followed. If the area can be divided into n parts

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

ENG202 Statics Lecture 16, Section 7.1

ENG202 Statics Lecture 16, Section 7.1 ENG202 Statics Lecture 16, Section 7.1 Internal Forces Developed in Structural Members - Design of any structural member requires an investigation of the loading acting within the member in order to be

More information

Chapter 5. The Laws of Motion

Chapter 5. The Laws of Motion Chapter 5 The Laws of Motion Sir Isaac Newton 1642 1727 Formulated basic laws of mechanics Discovered Law of Universal Gravitation Invented form of calculus Many observations dealing with light and optics

More information

ES226 (01) Engineering Mechanics: Statics Spring 2018 Lafayette College Engineering Division

ES226 (01) Engineering Mechanics: Statics Spring 2018 Lafayette College Engineering Division ES226 (01) Engineering Mechanics: Statics Spring 2018 Lafayette College Engineering Division Exam 1 Study Guide Exam 1: Tuesday, February 6, 2018 7:30 to 8:30pm Kirby Room 104 Exam Format: 50 minute time

More information

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 2016/2017 ENGINEERING PRINCIPLES 2

UNIVERSITY OF BOLTON WESTERN INTERNATIONAL COLLEGE FZE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 2016/2017 ENGINEERING PRINCIPLES 2 UNIVERSITY OF BOLTON OCD15 WESTERN INTERNATIONAL COLLEGE FZE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 016/017 ENGINEERING PRINCIPLES MODULE NO: AME4053 Date: Wednesday 4 May 017 Time:

More information

CHAPTER 6: Shearing Stresses in Beams

CHAPTER 6: Shearing Stresses in Beams (130) CHAPTER 6: Shearing Stresses in Beams When a beam is in pure bending, the only stress resultants are the bending moments and the only stresses are the normal stresses acting on the cross sections.

More information

if the initial displacement and velocities are zero each. [ ] PART-B

if the initial displacement and velocities are zero each. [ ] PART-B Set No - 1 I. Tech II Semester Regular Examinations ugust - 2014 ENGINEERING MECHNICS (Common to ECE, EEE, EIE, io-tech, E Com.E, gri. E) Time: 3 hours Max. Marks: 70 Question Paper Consists of Part- and

More information

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

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

More information

B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering)

B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) I B.Tech. Civil (Construction Management) / B.Tech. Civil (Water Resources Engineering) Term-End Examination 00 December, 2009 Co : ENGINEERING MECHANICS CD Time : 3 hours Maximum Marks : 70 Note : Attempt

More information

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns, and, b) Recognize two-force members. APPLICATIONS

More information

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC. BENDING STRESS The effect of a bending moment applied to a cross-section of a beam is to induce a state of stress across that section. These stresses are known as bending stresses and they act normally

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

PROBLEMS ON EQUILIBRIUM OF PARTICLES

PROBLEMS ON EQUILIBRIUM OF PARTICLES O EQUILIBRIUM O PRICLES 1. ind the angle of tilt q with the horiontal so that the contact force at B will be one-half that at for the smooth clinder. (3/15) q?, contact force at B will be one-half that

More information

Chapter 4.1: Shear and Moment Diagram

Chapter 4.1: Shear and Moment Diagram Chapter 4.1: Shear and Moment Diagram Chapter 5: Stresses in Beams Chapter 6: Classical Methods Beam Types Generally, beams are classified according to how the beam is supported and according to crosssection

More information

Name. ME 270 Fall 2005 Final Exam PROBLEM NO. 1. Given: A distributed load is applied to the top link which is, in turn, supported by link AC.

Name. ME 270 Fall 2005 Final Exam PROBLEM NO. 1. Given: A distributed load is applied to the top link which is, in turn, supported by link AC. Name ME 270 Fall 2005 Final Exam PROBLEM NO. 1 Given: A distributed load is applied to the top link which is, in turn, supported by link AC. Find: a) Draw a free body diagram of link BCDE and one of link

More information

3.032 Problem Set 1 Fall 2007 Due: Start of Lecture,

3.032 Problem Set 1 Fall 2007 Due: Start of Lecture, 3.032 Problem Set 1 Fall 2007 Due: Start of Lecture, 09.14.07 1. The I35 bridge in Minneapolis collapsed in Summer 2007. The failure apparently occurred at a pin in the gusset plate of the truss supporting

More information

Module 3. Analysis of Statically Indeterminate Structures by the Displacement Method

Module 3. Analysis of Statically Indeterminate Structures by the Displacement Method odule 3 Analysis of Statically Indeterminate Structures by the Displacement ethod Lesson 16 The Slope-Deflection ethod: rames Without Sidesway Instructional Objectives After reading this chapter the student

More information

PHYS 111 K SECOND HOUR EXAM 2015

PHYS 111 K SECOND HOUR EXAM 2015 PHYS 111 K SECOND HOUR EXAM 2015 This is a closed book closed note exam. Do all your writing in your blue book (s) and be sure to put your name on each blue book you use. You will not need nor are permitted

More information

Chapter 9- Static Equilibrium

Chapter 9- Static Equilibrium Chapter 9- Static Equilibrium Changes in Office-hours The following changes will take place until the end of the semester Office-hours: - Monday, 12:00-13:00h - Wednesday, 14:00-15:00h - Friday, 13:00-14:00h

More information

Equilibrium of Rigid Bodies

Equilibrium of Rigid Bodies Equilibrium of Rigid Bodies 1 2 Contents Introduction Free-Bod Diagram Reactions at Supports and Connections for a wo-dimensional Structure Equilibrium of a Rigid Bod in wo Dimensions Staticall Indeterminate

More information

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS Today s Objectives: Students will be able to: a) Apply equations of equilibrium to solve for unknowns b) Identify support reactions c) Recognize

More information

PROBLEMS. m s TAC. m = 60 kg/m, determine the tension in the two supporting cables and the reaction at D.

PROBLEMS. m s TAC. m = 60 kg/m, determine the tension in the two supporting cables and the reaction at D. 1. he uniform I-beam has a mass of 60 kg per meter of its length. Determine the tension in the two supporting cables and the reaction at D. (3/62) A( 500) m (5 23) m m = 60 kg/m determine the tension in

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

MARKS DISTRIBUTION AS PER CHAPTER (QUESTION ASKED IN GTU EXAM) Name Of Chapter. Applications of. Friction. Centroid & Moment.

MARKS DISTRIBUTION AS PER CHAPTER (QUESTION ASKED IN GTU EXAM) Name Of Chapter. Applications of. Friction. Centroid & Moment. Introduction Fundamentals of statics Applications of fundamentals of statics Friction Centroid & Moment of inertia Simple Stresses & Strain Stresses in Beam Torsion Principle Stresses DEPARTMENT OF CIVIL

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

UNIT II 1. Sketch qualitatively the influence line for shear at D for the beam [M/J-15]

UNIT II 1. Sketch qualitatively the influence line for shear at D for the beam [M/J-15] UNIT II 1. Sketch qualitatively the influence line for shear at D for the beam [M/J-15] 2. Draw the influence line for shear to the left of B for the overhanging beam shown in Fig. Q. No. 4 [M/J-15] 3.

More information

7.6 Journal Bearings

7.6 Journal Bearings 7.6 Journal Bearings 7.6 Journal Bearings Procedures and Strategies, page 1 of 2 Procedures and Strategies for Solving Problems Involving Frictional Forces on Journal Bearings For problems involving a

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

0.3 m. 0.4 m. 0.3 m. A 2 kn. 0.4 m. tan γ = 7. (BC = kn) γ = Fx = BC cos θ + AC cos γ =0

0.3 m. 0.4 m. 0.3 m. A 2 kn. 0.4 m. tan γ = 7. (BC = kn) γ = Fx = BC cos θ + AC cos γ =0 Problem 6.4 etermine the aial forces in the members of the truss. kn 0.3 m 0.4 m 0.6 m 1. m Solution: irst, solve for the support reactions at and, and then use the method of joints to solve for the forces

More information

Chapter 5. The Laws of Motion

Chapter 5. The Laws of Motion Chapter 5 The Laws of Motion The Laws of Motion The description of an object in motion included its position, velocity, and acceleration. There was no consideration of what might influence that motion.

More information