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Part I: Fundamentals of displacement method

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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

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What is the degree of freedom?

Degree of Freedom

→ + +

+ +

Y

Z

X

+

qY

Y

Z

X Y

Z

X

dx Y

Z

X

dy Y

Z

X

dz Y

Z

X

qX

Y

Z

X

qz

Y

Z

X

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If only in-plane motion available

Degree of Freedom

X Y

dx

dy qZ

Z

In-plane

deformation dx

Y

Z

X dy

Y

Z

X

qz

Y

Z

X

qY

Y

Z

X

dz

Y

Z

X

qX

Y

Z

Out-of-plane X

deformation

(4)

Plane frame

Idealization and Number of DOF

X Y

Z

X

dy

dz

dx

qy

qz x

q

dx dy

qz

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Idealization of a plane frame

Idealization and Number of DOF

(a) (b) (c)

(d) (e)

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1-DOF vs. Multi-DOF

Choices in Structural Modeling

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

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§ 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.

Virtual Displacement Principle for a Rigid Body

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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.

Virtual Displacement Principle for a Rigid Body

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Virtual Displacement Principle for a Rigid Body

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Virtual Displacement Principle for a Rigid Body

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

(1) By Equilibrium Equations

Virtual Displacement Principle for a Rigid Body

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(2) By Virtual work on Equivalent Mechanism

Virtual Displacement Principle for a Rigid Body

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§ 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

Virtual Displacement Principle for a Deformable Body

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Proof:

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

Hence work by R’s +work by S’s on nodes=0

True 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.

Virtual Displacement Principle for a Deformable Body

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§ 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)

Virtual Forces Principle

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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.

Assignments

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