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Teora de Estructuras y Construcciones Industriales. 2014-2015
CHAPTER 1. Introduction to Structural Analysis
Teora de Estructuras y Construcciones Industriales. 2014-2015
Lesson 1. Introduction to Structural Analysis
1.1. Objectives of structural analysis.
1.2. Structural models.
1.3. Structural forms.
1.4. Simplified structural models.
1.5. Types of internal forces.
1.6. Types of external loading.
1.7. Types of supports and reactions.
1.8. Determinacy and freedom degrees.
1.9. Design hypothesis: first and second order theories.
Teora de Estructuras y Construcciones Industriales. 2014-2015
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Structure could be a load-bearing element or a group of load-bearing elements with functional requirements.
The main objective of structural analysis is to determine how a structure responds to specified loads and actions.
1.1. Objectives of structural analysis
Teora de Estructuras y Construcciones Industriales. 2014-2015
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Conceptual and preliminary stages (types of structure,
materials and loading),
Calculation stage (internal forces and displacements),
Final stage (design drawings with written
specifications of materials and
pertinent codes to be
employed),
Construction stage.
The structural design process:
1.1. Objectives of structural analysis
Teora de Estructuras y Construcciones Industriales. 2014-2015
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Structural model
(elements, materials,
supports)
Loading analysis
Calculation of
stresses and strains
Checking limit states
(design codes)
Final design
New structural
design
Calculation of
displacements
Calculatin of
internal forces
YES
NO
1.1. Objectives of structural analysis
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1.2. Simplified structural models
(Idealization)
Variables to define:
Materials,
Structural forms,
Elements types,
Joints (connections) types,
Supports,
External loading,
Type of calculation (static,
dynamic, etc.)
Type of structural analysis
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1.3. Structural forms
Clasification by structural funtion:
Houses, offices and industrial buildings.
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1.3. Structural forms
Industrial equipment (cranes,
pressure vessels, silos)
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1.3. Structural forms
Gateways, bridges and slabs.
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1.4. Simplified structural models
Classification of structures: Rigid and pin joint structures.
Rigid joint: same angle before and after deformation.
2D and 3D Rigid joint structures (Frames)
Before
deformation
After
deformation
Teora de Estructuras y Construcciones Industriales. 2014-2015
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Pin Joint: free rotation (hinge)
1.4. Simplified structural models
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Element types:
1D elements (bar elements)
2D elements:
- Membranes,
- Plates,
- Shells,
- Shear walls.
3D elements.
1.4. Simplified structural models
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1.5. Types of internal forces
b)
1D elements: bars elements
2D and 3D Rigid elements
(Axial and Shear Forces and
Bending and Torsion Moments)
Cables
(Axial Force: Tension)
Pin joint elements
(Axial Force: Tension and Compression)
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2D elements: Membranes
1.5. Types of internal forces
Membranes examples
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2D elements: Plates
1.5. Types of internal forces
Plates examples
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2D elements: Shells
1.5. Types of internal forces
placamembranaMembrane Plate
Shells examples
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2D elements: Shear walls
1.5. Types of internal forces
Shear wall example
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3D elements
1.5. Types of internal forces
Dam example
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1.6. Types of external loading
Classification (actions):
Surface and volume loads. Static and dynamic loads. Permanent and variable loads.
Point and distributed loads. Thermal load. Enforced displacements. Fitting defects.
Classification (actions): own weight load snow load
wind load
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Support clasification:
Pin and roller (rocker) supports
Fixed or clamped (encastre) support
Guide
Spring supports: linear ad torsional springs.
1.7. Types of supports and reactions
Pin support
Spring support
Roller support
Fixed support
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1.7. Types of supports and reactions
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3 linear displacements (u, v, w )
3 rotations (Fx, Fy, Fz)
3D element section
(6 degrees of freedom)
Fixed: Restriction of 6 FD 6 Reactions (Unknowns)
Pin: Restriction of 3 FD 3 Reactions (Unknowns)
1.7. Types of supports and reactions
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1.7. Types of supports and reactions
1 rotation (Fz)
2D element section
(3 degrees of freedom)
2 linear displacements (u, v)
Pin support Roller support Fixed support Guide
Schematic representation
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Spring supports: partially limitation of linear and rotation
displacements. The reactions depend on the rigid constant (k = sm).
RV
Linear spring support Torsional spring support
1.7. Types of supports and reactions
RH
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1.8. Determinacy grade: DG ( = GH) = r - 3
If DG < 0 Unstable structures (mechanisms) (No. unknowns < No. available equilibrium equations)
If DG = 0 Statically determinate structures (No. unknowns = No. available equilibrium equations)
If DG > 0 Statically indeterminate structures
(No. unknowns > No. available equilibrium equations)
DG=1 DG=3
Teora de Estructuras y Construcciones Industriales. 2014-2015
Rigid joint open structures:
DG = DGext + DGint = r - 3 ao
DGext = r 3 ao
DGint = 0
r = No. reactions
ao = bo 1 = hinge equations (open contours)
Rigid joint closed structures:
DG = DGext + DGint = r + 3 cc - 3 (ao + ac)
DGext = r 3 - aa
DGint = 3 cc ac
r = No. reactions,
cc = No. closed contours,
ao = bo - 1= hinge equations (open contours)
ac = bc 1 = hinge equations (closed contours)
DG = DGext = 3 DG = DGext = 2
DG = 3+3=6
DGext = 3
DGint = 3
DG = 3+2=5
DGext = 3
DGint = 2
1.8.a) Statically indeterminate rigid joint structures.
Teora de Estructuras y Construcciones Industriales. 2014-2015
DG = DGext + DGint = r + b 2n
DGext = r - 3
DGint = DG - DGext = b 2n + 3
b = No. bars, r = No. reactions, n = No. joints
b = 17
r = 3
n = 10
b = 17
r = 3
n = 10
b = 18
r = 3
n = 10 A
Sm
50kN
50kN
4m 4m
3m
C
D
B
b = 5
r = 4
n = 4 d)
DG=0 DG=0
DG=DGint=1 DG=DGext=1
1.8.b) Statically indeterminate pin joint structures.
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Structures without sidesway: If AE = (axial deformations, e = 0), kinematic unknowns
(freedom degrees) are rotation of joints (NR) only, because bar rotation are cero (BR = 0).
A B C DA B C D
jB jC
CIR
1.8.c) Kinematically indeterminate structures:
Degrees of freedom FD (= GL) = NR + BR
FD = NR = 2 (jB , jC)
Structures with sidesway: If AE= (axial
deformations, e = 0), kinematic unknowns
(freedom degrees) are both joint rotations (NR)
and bar rotations (BR).
A
B C
D
UB UC
VB VCjB
jC
q q
yAB yDC
yBC
FD = NR + BR = 3 (jB , jC , yAB)
yBC = f (yAB)
yDC = f (yAB)
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Requirements of first order theory:
Linear-elastic material behaviour.
Small strain and displacements
These conditions permit:
Equilibrium applied to undeformed structure geometry.
Linear equation systems solution.
Superposition principle.
1.9. Design hypothesis: First and second order theories
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First order theory:
1.9. Design hypothesis: First and second order theories
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Second order theory:
1.9. Design hypothesis: First and second order theories