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PLASTIC ANALYSIS
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
PLASTIC ANALYSIS
IntroductionFundamentals of plastic theoryBending of beams symmetrical aboutboth axes
General Requirements for utilisingplastic design concepts
Plastic hinges2Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
PLASTIC ANALYSIS - 2
Fundamental conditions for plasticanalysis
Rigid plastic AnalysisStabilityEffect of axial load and shearPlastic analysis for more than onecondition of loading
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
INTRODUCTION
Elastic design method limits the usefulness to theallowable stress of the material, which is well below the
elastic limit
In plastic design method, the ultimate load is regardedas the design criterion.
Plastic design method is rapid and provides a rationalapproach for the analysis.
Plastic design method can be easily applied in theanalysis and design of statically indeterminate framed
structures.
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Basis of Plastic Theory
Ductility of Steel
fy
A
B
Stress f
O
Strain
Idealised stress strain curve for steel in tension
Strain hardening commences
Strain hardening
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Stress - Strain Curve for perfectly plastic materials
Basis of plastic theory - 2
Perfectly Elastic Material
Stress
Strain
Compression
Tension
fy
fy
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Fully Plastic Moment of a Section
Assumptions
Material obeys Hooke's law until the stress reaches the upper yield value; on further straining, the stress drops to the lower yield value and thereafter remains constant.
Homogeneous and isotropic in both the elastic
and plastic states.
Plane transverse sections remain plane and
normal to the longitudinal axis after bending.
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Fully Plastic Moment of a Section- 2
The yield stresses and the modulus of elasticity have the same value in compression and tension.
No resultant axial force on the beam.
Cross section of the beam is symmetrical aboutan axis through its centroid parallel to plane of
bending.
Every layer of the material is free to expand andcontract longitudinally and laterally under stress.
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Fully Plastic Moment of a Section- 3
Total compression , C = Total tension , T
C = fy .A1
T = fy . A2
fy
fy
A2
G2
A1
G1
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Elastic stresses in beams
Bending of Beams Symmetrical about both Axes
Neutral
Axis
f
f fy
f
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Bending of Beams Symmetrical about both Axes - 2
Stresses in partially plastic beams
Plastic Zone (Compression)
Plastic Zone (Tension)
Neutral
Axis
(a)Rectangular
section
(b) I - section
(c) Stress distribution
for (a) or (b)
fy
fy
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Bending of Beams Symmetrical about both Axes - 3
b
d
fy
fy
Neutral
Axis
(b) I - section
Stresses in fully plastic beams
(a) Rectangular
section
(c) Stress distribution
for (a) or (b)
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
General Requirements for Utilising
Plastic Design Concepts
Shape factor varies from 1.15 to 1.8
S= (Plastic Modulus)/(Elastic Modulus)
1.00
0.87
0.67
o
Rotation
a
b
(S 1.00)
(S 1.15)
(S 1.50)
(S 1.80)
Moment rotation curves
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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rotation can take place at a constant plastic moment.
Theoretically, a plastic hinge is assumed to format a point of plastic rotation.
There is a constant moment at the Plastic hinge, witha value equal to Plastic moment Capacity of the
cross section
Plastic Hinges
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Hinged Length of a Simply Supported Beam with
Central Concentrated Load
Plastic Hinges
It has been shown that
My = 2/3Mp and
L/2
L/2
MY
MY
Mp
W
x
b
h
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
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Mechanism condition
The ultimate or collapse load is reached when a mechanism is formed.
Equilibrium conditionFx = 0, Fy = 0, Mxy = 0
Plastic moment conditionBending moment should not be more than the plastic moment.
Fundamental Conditions for Plastic Analysis
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Mechanism
- Beam Mechanism
- Panel or Sway Mechanism
- Gable Mechanism
- Joint Mechanism
- Combined Mechanism
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
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Mechanism - 2
Beam Mechanism
Simply supported beam
(fails due to formation of one hinge)
Propped cantilever beam
(fails when 2 hinges are formed)
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
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Beam Mechanism
Mechanism - 3
1
3
2
Fixed beam
Three hinges are formed in the following order as shown:
1, 2, 3
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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Mechanism - 4
Panel, Gable and Joint Mechanisms
(a) Panel Mechanism
(b) Gable Mechanism
(c) Joint Mechanism
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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Mechanism - 5
Combined Mechanism
(Two hinges on the beam + 2 hinges at the base)
Combined Mechanism
Two hinges developed on the beam
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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Lower Bound or Static Theorem
A load factor (s ) computed on the basis of an arbitrarily assumed bending moment diagram which is in equilibrium with the applied loads and where the fully plastic moment of resistance is nowhere exceeded will always be less than (or at best equal to) the load factor at rigid plastic collapse, (p).
Load Factor and Theorems of
Plastic Collapse
Plastic analysis is governed by three theorems
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Upper Bound or Kinematic Theorem
A load factor (k) computed on the basis of an arbitrarily assumed mechanism will always be greater than, (or at
best equal to) the load factor at rigid plastic collapse (p )
Uniqueness Theorem
If both the above criteria are satisfied, then the resulting load factor corresponds to its value at rigid plastic collapse (p).
Load factor and theorems of plastic collapse - 2
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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Rigid plastic analysis
W
Plastic zone
Yield zone
Stiff length
2
M
Simply supported beam at plastic hinge stage
L
B. M. D.
Moment rotation curve
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Rigid plastic analysis - 2
P=0
P=0
MB
A
B
C
W / unit length
L
Loading
MP
MP
MP
MP
2
Collapse
Encastre Beam
MA
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Continuous Beams
Rigid Plastic Analysis - 3
10W
10W
6W
2L
2L
3L
2L
2L
3L
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Collapse pattern 3:
Collapse pattern 2:
Collapse pattern 1:
Rigid Plastic Analysis - 4
10W
2
10W
6W
10W
6W
10W
2
3
5
10W
10W
6W
2
3
5
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
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Mechanism Method
In this method, various alternative plastic failuremechanisms are evaluated.
The plastic collapse loads are obtained by equatingthe internal work to the external work done by
loads.
For gabled frames and other such frames, thekinematics of collapse is somewhat complex.
Rigid Plastic Analysis - 5
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Rigid Plastic Analysis - 6
Therefore it is convenient to use the instantaneous centres of rotation of the rigid elements of the frame to evaluate displacements corresponding to different mechanisms.Rigid Body Rotation
x
y
o
x
F
P
P
r
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Rectangular Portal Framework and Interaction Diagrams
Rigid Plastic Analysis - 8
H
a
a
a
V
(a)
H
V
H
V
(c)
2
(d)
H
V
2
(b)
Possible Failure Mechanisms
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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Rigid Plastic Analysis - 9
Interaction Diagram
0
2
4
6
2
4
6
Va / Mp
A
B
C
D
Ha / Mp
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Frames not of Constant Section Throughout
Rigid Plastic Analysis - 10
H
a
a
a
V
(a)
H
V
(b)
H
(c)
V
2
(d)
H
2
V
2
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Rigid Plastic Analysis - 11
0
2
4
6
2
4
6
Interaction Diagrams
8
8
A
B
C
D
Va / Mp
Ha / Mp
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
For plastically designed frames three stability criteria to be considered for ensuring the safety of the frame.
General Frame Stability Local Buckling Criterion RestraintsStability
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If a member is subjected to the combined action of bending moment and axial force, the plastic moment capacity will be reduced.
Effect of Axial Load and Shear
Effect of axial force on plastic moment capacity
C
T
fy
fy
C
fy
b
d
C
T
fy
fy
d/2
y1
Total stresses = Bending + Axial
compression
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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It is necessary to perform separate calculations, one for each loading condition, the section being determined by the solution requiring the largest plastic moment.
This is because the principle of Superposition doesNOT hold for plastic Analysis
Plastic Analysis for more than one condition of loading
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
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- Basic concepts on Plastic Analysis have been
discussed
- methods of computation of ultimate load causing
plastic collapse have been outlined
- Theorems of plastic collapse and alternative
patterns of hinge formation triggering plastic
collapse have been discussed.
Concluding Remarks
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
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THANK YOU
Teaching Resources IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
Teaching Resources for Steel Structures
IIT Madras, SERC Madras, Anna Univ., INSDAG Calcutta
1
y
S
1
2
y
p
y
M
S
1
M
=
L
3
1
x
=