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Seoul National University Structural Design Laboratory Structural Design Lab.(Prof. Ho - Kyung Kim) Dept. of Civil & Environmental Eng. Seoul National University 457.649 Advanced Structural Analysis Part I: Fundamentals of d isplacement method

457.649 Advanced Structural Analysis Part I: Fundamentals

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Page 1: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

Structural Design Lab.(Prof. Ho-Kyung Kim)Dept. of Civil & Environmental Eng.

Seoul National University

457.649 Advanced Structural Analysis

Part I: Fundamentals of displacement method

Page 2: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ What is the degree of freedom?

1

Degree of Freedom

+→ +

++

Y

Z

X

+

←Yq

Y

Z

X

Y

Z

X

xd

Y

Z

X

yd

Y

Z

X

zd

Y

Z

X

Xq

Y

Z

X

zq

Y

Z

X

Page 3: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ If only in-plane motion available

2

Degree of Freedom

X

Y

xd

yd

Zq

Z

In-plane deformation xd

Y

Z

Xyd

Y

Z

X

zq

Y

Z

X

YqY

Z

X

zd

Y

Z

X

Xq

Y

Z

XOut-of-plane deformation

Page 4: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Plane frame

3

Idealization and Number of DOF

X

Y

Z

X

yd

zdxd

yq

zqxq

xd

yd

zq

Page 5: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Idealization of a plane frame

4

Idealization and Number of DOF

(a) (b) (c)

(d)(e)

Page 6: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ 1-DOF vs. Multi-DOF

5

Choices in Structural Modeling

Horizontal 1-DOF Vertical 1-DOF 2-DOF Multi-DOF1-DOF

Page 7: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

§ Any rigid body§ In equilibrium§ Resultant force = 0§ Resultant couple = 0

§ Hence, if given a small translational or rotational displacement:§ WE=Σ(Work done by R1, R2, …, R5) = Work done by resultant force = 0

Where WE: external work = work done by external forces.Later will consider work by internal forces.

▶ Point to note§ External forces on body must be in equilibrium.§ Displacement of body must be small – otherwise may not remain in equilibrium.§ Displacement is introduced for mathematical purposes only – i.e. it is an imaginary,

or virtual displacement.§ The forces are given - Hence real.

We create the displacement – Hence imaginary.We make the displacement small.

6

Virtual Displacement Principle for a Rigid Body

Page 8: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Extension to Mechanism§ If principle applies to a single rigid body, it also applies to a number of rigid bodies to

form a mechanism.

▶ Example 1. Find: RC; MD; VD

Procedure: 4 steps(1) Create a mechanism which is in equilibrium. The beam is statically determinate. To

create a mechanism we must introduce one or more “releases”.(2) Identify the real forces acting on the mechanism. Remember: the mechanism must

be in equilibrium.(3) Introduce a small(imaginary) displacement of the mechanism. Calculate the

displacements for each of the forces acting on the mechanism.(4) Write out and solve the work equations WE = 0.

7

Virtual Displacement Principle for a Rigid Body

Page 9: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory8

Virtual Displacement Principle for a Rigid Body

Page 10: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory9

Virtual Displacement Principle for a Rigid Body

Page 11: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Example 2. The loading and bending moment diagram for a frame are shown. Find the magnitude of load F.

(1) By Equilibrium Equations

10

Virtual Displacement Principle for a Rigid Body

Page 12: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

(2) By Virtual work on Equivalent Mechanism

11

Virtual Displacement Principle for a Rigid Body

Page 13: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

§ Structure in Equilibrium, as previously defined.§ Impose small, imaginary and compatible displacement, as previously defined. Nodes

displace as rigid bodies. Elements undergo rigid body displacement plus deformation.§ WE = work done by external forces moving through corresponding (node)

displacement.§ WI = work done by element actions moving through element deformations.§ WE=WI

12

Virtual Displacement Principle for a Deformable Body

Page 14: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Proof:(a) All joints are in equilibrium as rigid bodies.

Hence work by R’s +work by S’s on nodes=0True for any single node, hence for all nodes taken together.

(b) Forces S on elements are equal and opposite to forces S on nodes, and displacements of nodes, and element ends are same.

Hence work by S on nodes = - (work by S on elements)Work by R on nodes = WE(external)

Work by S on elements = WI(internal)Hence WE + (-WI)=0 or WE = WI

(c) Important to note that in calculating WI we can consider element deformations only - no need to consider rigid body displacements.

13

Virtual Displacement Principle for a Deformable Body

Page 15: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

§ In proceeding proof: forces and actions were REAL displacement and deformation were IMAGINARY.

§ But exactly the same proof applies if: • Forces and actions are IMAGINARY.• Displacements and deformations are REAL.

§ This is the virtual forces principle.

▶ Requirements(1) A REAL displacement – deformation system which is:

(a) Compatible(b) Small ← note

(2) An IMAGINARY force-action system which is:(a) In equilibrium

WE* = WI

* (use * to distinguish form virtual displacements principle)

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Virtual Forces Principle

Page 16: 457.649 Advanced Structural Analysis Part I: Fundamentals

Seoul National UniversityStructural Design Laboratory

▶ Geometry(Kinematics) of small angles and displacements

▶ Read carefully pp.420-428, pp.246-250 in “Elementary Structural Analysis, 4th Ed.” by Norris et al.

▶ Read carefully Chapter 3 in “Computer-Assisted Structural Analysis and Modeling” by Hoit.

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