Digital Learning Tool

for

Engineering Mechanics

 

Developed by

Dr S.T. SMITH

Department of Civil Engineering

The University of Hong Kong

 

 

INTRODUCTION

 

This digital learning tool (DLT) has been created to facilitate in the learning of the engineering mechanics component of CIVL1013 Engineering Mechanics and Materials. CIVL1013 is one of the first courses in the structures stream that undergraduate students study who are enrolled in the Department of Civil Engineering at The University of Hong Kong (HKU).

 

Engineering mechanics is a core course and is of fundamental importance to the discipline of structural engineering in addition to other disciplines such as geotechnical engineering. The fundamental engineering mechanics knowledge learnt in CIVL1013, addition to the material learnt in ENGG1010 Foundations of Engineering Mechanics (i.e. HKU Faculty of Engineering Common Course), will form a solid foundation of knowledge to be used for the following structural engineering courses. The theory will also be used in elective courses and graduate courses in the structural discipline.

 

·   CIVL1007 Theory and Design of Structures I

·   CIVL2007 Theory and Design of Structures II

·   CIVL3007 Theory and Design of Structures III

 

As this learning tool is a working document, more tools may be added from time to time. Please therefore check it regularly. Also, please do email me any comments/suggestions of relevance you may have at stsmith@hku.hk. Finally, thanks are extended to Mr Jiaqi YANG (PhD candidate, HKU) for preparing the animations.

 

To facilitate your learning of CIVL1013, please confirm all the results given in this entire learning tool using the theory you have been presented with in class. You may wish to verify the results contained in each sub-topic as each sub-topic is presented in class. Reference will also be made regularly to this document throughout the lectures.

 

I hope this digital learning tool will be helpful to your learning. Enjoy your digital learning experience!

 

Scott SMITH

January 2012

 

 

 

COURSE TOPICS

 

The mechanics component of CIVL1013 is divided into the following 5 sub-topics and is delivered in the first half of the second semester of the academic year. The latest version of the course is offered in Semester 2 of the 2011-12 academic year.

 

Topic

Title

A

Bending Moment, Shear and Axial Force Diagrams

B

Stresses in Beams and Shear Centre

C

Deflections of Beams

D

Analysis of Stress and Strain and Stress-Strain Transformation

E

Buckling of Columns

 

 

 

DIGITAL RESOURCES

 

There are several digital resources available to undertake calculations which vary considerably in complexity. The following resource is suitable for the level of CIVL1013. It is also freely available and hence reference will be made to it herein.

 

xcalcs: http://www.xcalcs.com

 

It is important to note that digital tools are merely tools. They produce an answer based on the information that is provided. As an engineer (in training), you need to verify that the computer results are correct. Verification for you as a student means you need to calculate the results from first principles using the theory that you have been taught in class. You are strongly encouraged to supplement your knowledge with independent learning.

 

The program ABAQUS, which utilizes the finite element method, has been used to create some of the following animations. Note that finite element analysis is outside the scope of CIVL1013 but students will have the opportunity to learn about it in more advanced undergraduate and graduate courses. Linear-elastic behaviour has been assumed and maintained for all cases herein.

 

 

 

TOPIC A: Bending Moment, Shear and Axial Force Diagrams

 

Note the following terminology:

BMD = Bending Moment Diagram

SFD = Shear Force Diagram

AFD = Axial Force Diagram

 

Animations

The following animations show the development of bending moment and shear force (and axial force for one case) for a variety of beams, support conditions and load cases for varying levels of load. Notice in the animations that the shape of the BMD, SFD and AFD’s do not change but their magnitude does.

 

·   Simply-supported beam subjected to central load (3-point bending)

Case 1

Case 2

 

 

·   Cantilevered beam subjected to free-end load

 

Case 1

Case 2

 

 

·   Simply-supported beam subjected to uniformly distributed load (UDL)

Case 1

Case 2

 

 

·   Simply-supported beam subjected to central couple

Case 1

Case 2

 

 

·   Simply-supported beam with overhang subjected to point load at overhang tip

Case 1

Case 2

 

 

·   Simply-supported beam subjected to inclined load

Case 1

Case 2

 

 

 

Superposition

 

 

 

 

 

 

BMD for UDL

 

 

 

BMD for Point Load

 

 

 

BMD for UDL + Point Load

 

 

 

 

 

 

SFD for UDL

 

 

 

 

SFD for Point Load

 

 

 

SFD for UDL + Point Load

 

 

 

Digital Resource

Utilising xcalcx, analyse the following beam scenarios. For each scenario, calculate the bending moment (BM) and shear force (SF) values at mid-span as well as quarter span positions. In addition, plot the distribution of BM and SF for each beam scenario.

 

  1. Simply supported beam of span 2 m subjected to a central load of 10 kN.
  2. Simply supported beam of span 2 m subjected to a uniformly distributed load (UDL) of intensity 10kN/m.
  3. Cantilever beam of span 2 m subjected to a free-end load of 10 kN.

 

 

For each beam scenario, assume the following:

Solid rectangular cross-section of 400 mm depth (h) and 200 mm width (b). The beam is made from steel of which the Elastic Modulus (E) is 200 GPa and Poisson’s Ratio (u) is 0.3. In addition, make sure to work in SI units.

 

Once you have completed the digital analysis, please confirm all numbers using the theory you have been taught in CIVL1013.

 

Once you are satisfied with all digital and hand-calculation results, then start to experiment with xcalcx, i.e. experiment with different support conditions and load types. Practice as many variations as you can and verify them with hand-calculations. Remember that practice makes perfect!

 

 

Note: Expected Answers from xcalcs for three beam scenarios: (all BM in kNm, all SF in kN) (on account of possible differences in sign convention, the absolute values of BM and SF have been given).

Case 1: BM (midspan)=5, BM (¼ span)=2.5, SF (midspan)=5, SF(¼ span) = 5.

Case 2: BM (midspan)=5, BM (¼ span)=3.75, SF (midspan)=0, SF(¼ span) =5.

Case 3: BM (support)=10, BM (¼ span from support)=7.5, SF (support)= 10, SF(¼ span from support) = 10.

 

 

 

TOPIC B: Stresses in Beams and Shear Centre

 

The following animations show development of longitudinal stress at the mid-span position (note that +’ve = tensile and -’ve = compressive stresses). The change in bending moment and shear force are also provided although only the bending moment information in needed to calculate the longitudinal stresses. Please verify all results using the theory you have been provided with in class. You may wish to supplement your knowledge by consultation of the open literature.

 

·   Simply-supported beam subjected to central load (3-point bending)

 

·   Simply-supported beam subjected to two point loads (4-point bending)

 

·   Cantilevered beam subjected to free-end load

·   Simply-supported beam subjected to uniformly distributed load (UDL)

 

The following animation shows the development of compressive and tensile stress at the mid-span of a beam subjected to uniform bending. Note the following:

·   Compressive stress act towards face (i.e. in top half of section)

·   Tensile stresses act away from section (i.e. in bottom half of section)

·   The neutral axis (i.e. position of zero bending) is located at the mid-depth of the section. (note that the neutral axis is located in this position for this example because the section is symmetric)

 

                                             

                             Mid-span section (Note: +’ve tensile stress, -‘ve compressive stress)

 

 

                                              

                                                            Shear-span section

 

Shear Centre

The following two animations show the physical reality of shear centre using a cantilevered C-section beam as an example in which load is applied to the free-end of the beam. Note the following:

(i) Load is applied through the centroid of the section. In this case, the beam is shown is shown to deflect vertically downwards WITH rotation.

(ii) Load is applied through the shear centre of the section. In this case, the beam is shown to deflect downwards WITHOUT rotation.

 

Appreciation of shear centre is therefore important for designers of structures because we would not want a member to twist if is was supporting say a wall or window.

 

(i) Load applied through centroid

(ii) Load applied through shear centre

 

Exercise: The centroid and shear centre of a section may be in the same location or they may not. As an exercise, calculate the positions of the centroid and shear centre of the following commonly used structural sections. What do you notice from your calculations?

(i) C-Section

(ii) Rectangular Hollow Section (RHS)

(iii) I-Section

 

(note: Use dimensions of standard sections which can be found in steel design handbooks)

 

 

 

TOPIC C: Deflections of Beams

 

The following animations show the relationship between vertical load and central or free-end vertical deflection. The deflected shape of the beam is also shown. As an exercise, please calculate all the results below using the theory that you have been presented with in class (note that the flexural rigidity EI = 1000 kNm2).

 

 

·   Simply-supported beam subjected to central load (3-point bending)

·   Simply-supported beam subjected to two point loads (4-point bending)

·   Cantilevered beam subjected to free-end load

·   Simply-supported beam subjected to uniformly distributed load (UDL)

TOPIC D: Analysis of Stress and Strain and Stress-Strain Transformations

 

The following diagrams are provided to explain the relationship between normal and shear stress on an element as it is rotated. Five different normal stress states have been provided as per the following table:

 

 

Maximum Principal Stress (MPa)

Minimum Principal Stress (MPa)

Case 1

3

1

Case 2

2

0

Case 3

1

-1

Case 4

-2

0

Case 5

-3

-1

Note: +’ve tensile normal stress, -‘ve compressive normal stress

 

·   Case 1

(Maximum Principal Stress = 3 MPa, Minimum Principal Stress = 1 MPa)

·   Case 2

(Maximum Principal Stress = 2 MPa, Minimum Principal Stress = 0 MPa)

·   Case 3

(Maximum Principal Stress = 1 MPa, Minimum Principal Stress = -1 MPa)

·   Case 4

(Maximum Principal Stress = -2 MPa, Minimum Principal Stress = 0 MPa)

·   Case 5

(Maximum Principal Stress = -3 MPa, Minimum Principal Stress = -1 MPa)

TOPIC E: Buckling of Columns

 

Buckling Modes

The following animations illustrate the concepts of (i) flexural buckling, (ii) torsional buckling, and (iii) flexural-torsional buckling. A pinned-pinned C-section strut is used as the example of which an axial load is applied. Note that the flexural buckling of (i) and (iii) is occurring about the minor (2-2) axis. As the 2-2 axis has a smaller second moment of area compared to the major (1-1) axis and as there are not intermediate restraints, the 2-2 axis is the critical buckling axis.

 

(i) Flexural Buckling

(ii) Torsional Buckling

(iii) Flexural-Torsional Buckling

 

 

 

Load versus Lateral Deflection Responses

The qualitative relationship between axial load (P) and lateral deflection of the following four column scenarios is provided herein. The first animation for each case represents a column with no initial (lateral) imperfection while the second animation represents the same column with initial imperfection. Initial imperfections will always exist and they can be induced during the manufacturing and installation stages of the column.

 

 

·   Buckling of Pinned-Pinned Column

Without Imperfection

With Imperfection

 

·   Buckling of Fixed-Free Column

Without Imperfection

With Imperfection

 

·   Buckling of Fixed-Fixed Column

Without Imperfection

With Imperfection

 

·   Buckling of Fixed-Pinned Column

Without Imperfection

With Imperfection

 

 

 

Euler Buckling Modes

The number of buckling half-wavelengths (n) which can be developed in a column will influence the critical Euler buckling load of the column as per  Pcr=n2p2EI/Le2. The following three animations show the first three buckling modes and the corresponding Euler buckling loads.

 

 

Pcr=p2EI/Le2

(1 Buckling Half Wavelength: n = 1)

 

Pcr=4p2EI/Le2

(2 Buckling Half Wavelengths: n = 2)

 

Pcr=9p2EI/Le2

(3 Buckling Half Wavelengths: n = 3)

 

 

 

Worked Example E-2 (Critical Buckling Stress) of Lecture Notes

The following I-section columns are pin supported at each end (i.e. pinned-pinned). In addition, the mid-height position is supported about the minor axis (2-2 axis) direction but not about the major axis (1-1 axis). Buckled shapes about the major and minor axes are shown in figures (i) and (ii), respectively, while buckling is prevented in figure (iii).

 

(i) Buckling about Major Axis

(i.e. 1-1 Axis)

(ii) Buckling about Minor Axis

(i.e. 2-2 Axis)

(iii) Yield of Material

(no buckling)