m sc steel-03-prof-zahid_siddiq
TRANSCRIPT
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Steel Structures
SE-505
Plastic Analysis and Design of Structures
M.Sc. Structural Engineering
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of Analysis
The objective is to find out a mechanism (independent or composite) such that M ≤Mp every where (or at lest at the selected points – answer may only be an upper bound and may not be the right answer.
1. Determine the location of all possible hinges and thus the number of these hinges (H). Hinges may form at concentrated load points, connections, and points of zero shear in case of members subjected to UDL.
2. Determine the total degree of indeterminacy of the structure (I).
3. The number of independent mechanisms (M) is calculated as under:
M = H − I
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Independent mechanisms include beam mechanism, panel or sway mechanism, gable mechanism and joint mechanism.
• Sketch each mechanism one by one and give convenient virtual deformation (displacement or rotation) to any point, assuming all the hinges of this mechanism to be just formed.
• Calculate the external and internal works done. External work done will be by the load multiplied with its corresponding deformation. Internal work will be done only at the plastic hinges and calculated as the plastic moment multiplied with the rotation.
External WD = Σ load × virtual displacement
Internal WD = ΣMoment at the hinge × virtual hinge rotation
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
6. Using the principle of virtual work, evaluate the collapse load for the mechanism under consideration.
WE = WI
7. Solve all the independent mechanisms and then form composite mechanisms by combining two or more independent and other composite mechanisms.
The composite mechanisms must be formed in such a way that plastic hinges are eliminated reducing the internal work done and hence the collapse load.
8. Find the lowest collapse load.
9. Check to see that M ≤Mp at all sections, if possible.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of Analysis
Example
L/2
P P
L/2 L/2 L/2
A B
CD
E
Determine the collapse Load.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution:
Mech-1
P P
L/2 L/2 L/2
A B
CD
E
θA θB
θC=2θ
θL/2
θ = θA = θB
Mech-2
L/2
θA is the virtual displacement given by us other displacements are as as a result of θA
I = 1
No. of Possible Hinges, H = 3
No. of Independent Mechanisms, M = H – I = 2
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
2LPθWE =
PPI MθM2θθ0W ×+×+×=
PI M3θW ×=
EI WW =Virtual Work Principle
2LPθθ3MP =
L6MP P
C =Same for other mechanism - 2
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisExample:
Mech-1
P P
Mech-2
I = 2
No. of Possible Hinges, H = 5
No. of Independent Mechanisms, M = H – I = 3
2MP MP
P
2m 2m 2m 5m 5m
Mech-3
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
3PθθP2θPWE =×+×=Beam Mechanism - 1
θ θ/2
3θ/2
2θ
2θM
23θ2Mθ2MW PPPI ×+×+×=
θ5.5MW PI =
EI WW =3Pθθ5.5MP =
P1.83MP =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
6Pθθ4P2θPWE =×+×=
Beam Mechanism - 2θ 2θ
3θ
4θ
2θM3θ2Mθ2MW PPPI ×+×+×=
θM01W PI =
EI WW =6Pθθ10MP =
PM67.1P =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
5Pθθ5PWE =×=
Beam Mechanism - 3θ θ
2θ
5θ
02θMθMW PPI +×+×=
θM3W PI =
EI WW =5Pθθ3MP =
PM6.0P =
Final answer is the smallest
PC M6.0P =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisExample:
Mech-1
P
θ θ
2θ
4.5θ
Mech-2
I = 2
H = 5
M = 3
4P4P4.5m4.5m 6m 6m 6m 6m
θθ
2θ
6θ
θθ
2θ
6θ
Mech-3
12Mp14Mp 16Mp
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
18Pθ4.5θP4WE =×=Beam Mechanism - 1
θ12M2θ2M10W PPI ×+×+=
θM63W PI =
EI WW =Pθ81θ36MP =
P2MP =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
Pθ426θP4WE =×=Beam Mechanism - 2
θ4M1θ2M41θ2M1W PPPI +×+=
θM54W PI =
EI WW =
Pθ24θ54MP =
P2.25MP =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
Pθ42WE =Beam Mechanism - 3
0θ2M61θM14W PPI +×+=
θM46W PI =
EI WW =
Pθ24θ46MP =
PM92.1P =
PC M92.1P =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
I for Rigid Frames
I for rigid frame = no. of closed loops x 3 – Releases at the bottom from fixed end – any real hinge in the super structure
( )70I
14355I=
−−××=
Real hinge
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Elimination of Hinges in Mechanism MethodCombined mechanisms are obtained in such a way that number of
plastic hinges are reduced.
There are two different ways in in which hinge can be eliminated:
1. If all members of the joint rotate through same angle in same direction in mechanisms to be added.
2. When a member rotates by equal amount but in opposite direction in the mechanisms to be combined.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Joint MechanismJoint mechanism shows the rotation of a joint w.r.t the structure.
Now this joint can rotate
2MP
MPHinge will be in column as its MPis smaller
2MP 4MP
MP
Hinge may not form in this column although it is the weakest, as it can’t take moment
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Joint Mechanism (contd…)
Location of hinge depends on loading and end conditions of other members
2MP 4MPLet, MP = 100 kN-m
MA = 100 x 4 = 400 kN-m = 4MP
Hinge will form in member AB although its strength is greater than other members.
4m
100kN
AB
MP
Joint mechanism determines location of hinges at joint of more than two members.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Joint Mechanism (contd…)
θ
θ
θ
θ
θ
θ
CW rotation of joint CCW rotation of joint
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisExample: Calculate the collapse load
3I =6H =
336M =−=2 Beam mechanism and 1 sway mechanism
Joint mechanism is not required as no joint is having more than 2 members.
P P
P 2m 2m 2m
4m
2MP
MP MP4m
Solution:
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
Beam2
Beam1
PCWIWEShape of MechType of
Mech
Mech#
θ θ/2
1.5θ
2θ
3PθθP2θP
=×
+×
θ4.5Mθ0.5M
1.5θ2MθM
P
P
P
P
=+
×+×
P1.5M
θ 2θ
3θ
4θ
6Pθθ2P
4θP
=×
+×
θ9M2θM
3θ2MθM
P
P
P
P
=×+×+×
P1.5M
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
Mech 1 +
Mech 3
4
Sway3
PCWIWEShape of MechType of
Mech
Mech#
4θP× θ4MP × P1.0M
7Pθ4Pθ3Pθ
=+
θM5.6θM-θM
-θ4Mθ4.5M
P
PP
P
P
=
×+
P0.93M
θ θθ
θ
P4θ P P
θθ
θ
4θθ/21.5θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisSolution: (contd…)
Mech 2 +
Mech 3
5
PCWIWEShape of MechType of
Mech
Mech#
10Pθ4Pθ6Pθ
=+
θM11θM-θM
θ13M
P
PP
P
=
−
P1.10M
Right hinge at the joint can’t be eliminated because column and beam are rotating in opposite directions.
PC M93.0P =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mechanism Method of AnalysisExample: Calculate the collapse load
632I =×=12H =
6621M =−=2 Beam mechanism and 2 sway mechanism2 Joint mechanism
Consider 1 hinge at the junction of 2-members and equal to no. of members at other joints.
1.5P
PMP
1.7MP 4m
Solution:
0.8MP0.8MP
2MP
1.7MP
4m
2P
4m 4m
1.8P
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
Beam2
Beam1
PCWIWEShape of MechType of
Mech
Mech#
6Pθ4θ1.5P
=×
θ3.6Mθ0.8M
2θMθ0.8M
P
P
P
P
=+
×+
P0.6M
Pθ2.74θ1.8P
=×
θ8MθM2
2θ2Mθ2M
P
P
P
P
=×+
×+×
P1.11M
2θ
θθ
4θ
2θ
θθ4θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
Sway of
bottom story
4
Sway of top story
3
PCWIWEShape of MechType of
Mech
Mech#
4θP× 4θ0.8MP ×P0.8M
12Pθθ42P
4θP
=×
+×
θ6.8Mθ41.7M
P
P
=×
P0.567M
θ
θ
θ θθ
4θ
θθθ
4θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
Right Joint Mech
6
Left Joint Mech
5
PCWIWEShape of MechType of
Mech
Mech#
0θ4.5M
θM7.1θ2Mθ0.8M
P
P
P
P
=
++
∞
0 θ4.5MP ∞
θ
Clockwise
θθ
θ
θ
θ
These joint mechanisms are fictitious & don’t occur independently, will occur in some combination
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
7+48
1 + 37
PCWIWEShape of MechType of
Mech
Mech#
10Pθ4Pθ6Pθ
=+
θ5.2MθM8.0
-θM8.0θ3.2Mθ3.6M
P
P
P
P
P
=
−+
We need not to combine mech – 1 & 4 as no hinge will be eliminated.
θθ
P.52M0
θθ
θθ
Pθ22Pθ2110Pθ
=+
θM12θ6.8Mθ5.2M
P
P
P
=+
P.545M0
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
9+610
8 + 59
PCWIWEShape of MechType of
Mech
Mech#
Pθ22022Pθ
=+
θM5.11θM7.12
-θM8.02θ4.5Mθ12M
P
P
P
P
P
=××
−+
P.523M0
θ
θ
θ
Pθ22 P.50M0
θ
θ
θ
θ θθ
θM11θM7.12
-θM8.02θ4.5Mθ11.5M
P
P
P
P
P
=××
−+
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresMechanism Method of AnalysisSolution: (contd…)
10 + 211
PCWIWEShape of MechType of
Mech
Mech#
Pθ2.92Pθ22
7.2Pθ=+
θM51θM22
θ11Mθ8M
P
P
P
P
=×
−+
P.514M0θ θ 2θ
2θ
2θ
PC 0.50MP =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Gable Mechanism
Gable Mechanism
• One hinge forms at crown and two at the beam joints.
• Somewhat similar to sway mechanism.
• wind ward side column does not move.
• The hinge formed at the crown sinks the frame.
• Gable mechanism is separate/independent mechanism.
θ
If an angle θ is known we cannot determine other angles by some simple method. For this we need to understand Instantaneous Center of Rotation
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Instantaneous Center of RotationThat center about which any part structure rotates
Gable Mechanism
θ
A
B
CD
E
For ED center of rotation is E, for BC C.O.R is B. for CD we have to find out the C.O.R.
If a point of a segment moves perpendicular to line passing through this point then center of rotation lies on this line.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Instantaneous Center of Rotation (contd…)
A
B B’ C
C’
D D’
E
L/2
F
L/2 L/2
L/2
Portion ABC has C.O.R at A
Portion DE has C.O.R at E
Portion CD
Point C is common with ABC. AC is perpendicular line to movement CC’. Point D is common with DE, center of rotation will lie on extension of DE.
Point F is ICOR for portion CD
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Instantaneous Center of Rotation (contd…)
L/2
F
L/2 L/2
L/2
θ
θ
θ
θ
2θθ
θ2θ
θL/2
2θθ θ θ
θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Example: 320kN 320kN
160kN10m
10m
15m 15m 15m 15m
MP Constant
Calculate MP
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Solution: 2P 2P
PL
L
1.5L
MP Constant
Let P = 160 kNL = 10 m
I = 1, H = 5, M = H – I = 4 2 Beam mech, 1 sway mech, 1 Gable mech.
1.5L 1.5L 1.5L
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution: (contd…)
Beam2
Beam1
PCWIWEShape of MechType of
Mech
Mech#
3PLθ1.5Lθ2P
=×
θ4MP
LM1.33
LM
34
P
P =θ θ2θ
Multiply rotation with Hz. Distance to
get vertical component of displacement
θθ
2θ
3PLθ1.5Lθ2P
=×
θ4MP
LM1.33
LM
34
P
P =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution: (contd…)
GableMech
4
Sway or
Panel
3
PCWIWEShape of MechType of
Mech
Mech#
PLθ θ2MPL
M2 P
3PθP
1.5L2θ2P
1.5L2θ2P
=
×+
×
++ 1.5θθ
2θMP
LMP
θθθθ
θL
θ/2θ/2 θ
θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution: (contd…)
2LLθ
2θ=
θ/2 θ
θ/2
Lθ
4- Gable Mechanism
θ
θ23
L
L
L
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution: (contd…)
1+36
1+45
PCWIWEShape of MechType of
Mech
Mech#
( )6PLθ
PLθ33=+ ( )
θM5θM2-34
P
P
=+
LM833.0 P
PLθ4( )
θM4θM2-24
P
P
=+
LM0.1 P
θ
1.5θ 1.5θ
θ θ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution: (contd…)
3+(2/3)57
PCWIWEShape of MechType of
Mech
Mech#
5PLθ
6PLθ32
PLθ
=
×+
( )
θM3
10θM-θM-
θ5M32θ2M
P
PP
PP
=
+
LM
32 P
θ θ32θ +
LM
32P P
C = 1023160MP ××=
m2400kNMP −=
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity
• In columns axial force is present simultaneous with moments.
• In beams of frames, smaller axial force in addition to moment may be present.
• Stresses are consumed by axial force hence plastic moment capacity reduces.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic Moment Capacity
+(-)
(-)
(+)
=
(-)
(+)
(-)
(+)
Fy
(-)
(+)
Fy
Fy
(-)
(+)
Fy
FyDue to axial compression, P
Due to sagging moment
P/A
N.A
ElasticPartially Inelastic
Inelastic
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity
(-)
(+)
Fy
Fy
(-)
(+)
= +(-)
Fy
Fy
yo
yo
Contribution of moment. Upper area is equal to lower area
Contribution of Axial force
Fy
(b)(c) (d)
N.A
(-)
(+)
Fy
(e)
(-)(+)
Fy
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity (contd…)
Case-I N.A Is Within The WebApplicable for smaller values of axial load, P.
From diagram “d”
yow F2ytP ××=
ywo F2t
Py =
If22t-dy f
o ≤ Then N.A. is with in Web
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-I N.A Is Within The Web (contd…)
Reduced moment capacity, MPC
FY x Area of diagram on top or bottom
= x Distance between centers of comp. & tension area.
Dia: (e)
MPC = FY (Z for total section – Z for central portion of 2yo height)
−×=
4)(2ytZFM
2ow
xyPC
( )2owxy ytZF −×=
2owyP ytF-M=
MP is full plastic moment capacity in the absence of Axial force
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-I N.A Is Within The Web (contd…)
2y
2w
2
wyPPC F4tPtF-MM =
yw
2
P F4tP-M=
( )yyw
2
P
PC
FzF4tP-1
MM
×=
( ) 2
2
yyw
2
AA
FzF4tP-1 ×
×=
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-I N.A Is Within The Web (contd…)
2
yw
2
P
PC
PP
z4tA-1
MM
×= yy FAP ×=Q
Py = Max. axial compressive load in the absence of bending moment& bucklingIf P = 0, P/Py = 0 then MPC/MP = 1, MPC = MP
(1)
Eq: 1 is applicable when 22tdy f
o−
≤
OR owy .2y.tFP ≤ ( )fwy 2t-d.tF=
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity (contd…)
Case-II N.A Is Within The FlangeApplicable when P is high and M is less.
(-)
Fy
(+)
= +
(-)
Fy
yo
Fy
(d) (e)
Fy
yo
(-)
(+) N.A
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-II N.A Is Within The Flange (contd…)
Lever arm in the diagram 2
2yd2y oo
−+=
2dyo +=
Let “A” be the total area of section
( )[ ]ofy 2ydbAFP −−=
[ ]fofy b2ydbAF −−=
−+= Adb
FP
2b1y f
yfo
2d
2bA
F2bPy
fyfo +−=
−−=
yfo P
P12bA
2dy
If yo = d/2, 1-P/Py=0 so P/Py = 1
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-II N.A Is Within The Flange (contd…)
−=
4)(2yb
4dbFM
2of
2f
yPC
−−−=
2
yff
2f
y PP1
2bA
2db
4dbF
ZZ
PP1
2dA
PP1
4bAF
y
2
yf
2
y ×
−
×+
−−=
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityCase-II N.A Is Within The Flange (contd…)
2
yf
2
yP
PC
PP1
Z4bA
PP1
Z2dA
MM
−+
−
××
=
This eq is valid for: fo t2dy −> ( )fwy 2td.tFP −>and
−+
−=
2
yfyP
PC
PP1
2bA
PP1d
2ZA
MM
(2)
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity
1MM
98
PP
P
PC
y
=+yP
P
2.0PP
y
=
0.1
P
PC
MM 0.1
Actual Curve, Eq:2
2.0PP
y
≥for
Actual Curve, Eq:1
1MM
2PP
P
PC
y
=+ 2.0PP
y
<for
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityActual curve is difficult to use so specifications allow to approximate the original equations by approximate equations.
For P/Py = 0.2 draw Hz. Line. Where this line cuts the original curve join that point with 1.0 value point on both axis. Then equation can be made for the straight lines.
AISC Interaction Equations
1.0MM
MM
98
PP
cy
ry
cx
rx
c
r ≤
++ For 2.0
PP
c
r ≥
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacity
1.0MM
MM
2PP
cy
uy
cx
rx
c
r ≤++ For 2.0PP
c
r <
Pr = required factored axial compressive strength (LRFD)= required allowable axial compressive strength (ASD)
Pc = design axial compressive strength (LRFD) = φcPn= allowable axial compressive strength (ASD) = Pn / Ω
Mr = required factored flexural strength (LRFD)= required allowable flexural strength (ASD)
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel Structures
Mt = Required nominal flexural strength for no axial load
= MPC/φb
Suppose 2.0P
P
nc
u >φ
1.0M
M98
PP
Pb
PC
nc
u =+φφ
Mc = design flexural strength (LRFD) = φbMn= allowable flexural strength (ASD) = Mn / Ω
φc = resistance factor for compression = 0.9φb = resistance factor for flexure = 0.9
Ωc = safety factor for compression = 1.67Ωb = safety factor for flexure = 1.67
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresInfluence of Axial Force On Plastic MomentCapacityAfter simplification
+= 0.889
PPMM
nc
utP φ
+= 0.889
PPZZ
nc
utx φ
For 2.0P
P
nc
u ≤φ
+= 00.1
PP5.0ZZ
nc
utx φ
Approximate interaction equations to reduce the trials
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresDesign Procedure For Column (beam column)
1. Select section without considering the axial force.
2. Calculate φcFcr & φ cPn for the trial section. Also calculatePu/ φ cPn and decide which interaction equation is applicable.
3. Find out increased value of Z. Because due to axial force there is reduction in plastic moment capacity so we need to calculate the reduction.
4. Select section for this plastic section modulus.
5. Apply interaction equations. If L.H.S < 1.01, section is O.K. If too much less than 1.0 , the section is uneconomical.
( )y
reqPt 0.9F
MZ =
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresExample:
Design a beam column having required plastic moment of 300 kN-m and an axial force (factored) of 500 kN. A-36 steel is to be used. Fy = 250 MPa. Effective length, KL = 2.0m
Solution:
( )2509.010300
0.9FM
Z6
y
reqPt ×
×==
33 mm101333×=From beam selection table
W 530 x 66
LP = 1.60m < Lu = 2.0 m
W 360 x 79
LP = 2.44m > Lu = 2.0 m In this way bracing is not required. In beams we can provide bracing but in case of column it may be difficult .
Trial Section W 360 x 79
A = 10,100 mm2 rx = 150mm, ry = 48.8mm
KLu/rmin = 2000/48.8 = 41 < 200 O.K.[Not better as a column]
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution:
MPa82.052Fcrc =φ
New value of “Z”
kN07921000
10,10082.052Pnc ≅×
=φ
0.224.02079500
PP
nc
u >==φ
+= 889.0
PPZZ
nc
ut φ
In this equation we can use the original value of Z.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution:
( )889.024.0103331Z 3 +×=
Now select the section according to this new value of Z
W 360 x 91, A = 11,500mm2, Z = 1671 x 103 mm3, φbMP = 376 kN-mrx = 152 mm, ry = 62.2 mm, Lp = 3.11 m
LP > Lu. Check local stability yourself.
33 mm101506×=
33rKL
min
u = 212.38MPaFcrc =⇒φ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Steel StructuresSolution:
Final Selection: W 360 x 91
2442kN1000
11500212.38Pnc =×
=φ
0.20.2052442500
PP
nc
u >==φ
01.1914.0M
M98
PP
nxb
ux
nc
u <=+φφ
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
TYPES OF COLUMNS DEPENDING ON BUCKLING BEHAVIOURElastic Critical Buckling Stress
The elastic critical buckling stress is defined as under:Fe = Elastic critical buckling (Euler) stress
= 2
2
rKL
Eπ
The critical slenderness ratio dividing the expected elastic and the inelastic buckling is denoted by Rcand is given below:
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
COLUMN STRENGTH FORMULAS
The design compressive strength (φc Pn) and the allowable compressive strength (Pn / Ωc) of compression members, whose elements do not exhibit elastic local instability (only compact and non-compact sections), are given below:
φc = 0.90 (LRFD) : Pn = Fcr AgΩc = 0.90 (ASD) : Pn = Fcr Ag
Fcr = critical or ultimate compressive strength based on the limit state of flexural buckling determined as under:
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Elastic Buckling
When KL / r > Rc or Fe < 0.44Fy
Fcr = 0.877 Fe (AISC Formula E3-2)
where Fe is the Euler’s buckling stress and 0.877 is a factor to estimate the effect of out-of-straightness of about 1/1500.
Inelastic Buckling and No BucklingWhen KL / r ≤ Rc or Fe > 0.44Fy
Fcr = Fy (AISC Formula E3-3)
e
y
FF
658.0
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Element
Width-Thickness
Ratio
λr λr For A36 Steel
Unstiffened1. Flanges of I-shaped sections in pure compression, plates projecting from compression elements, outstanding legs of pairs of angles in continuous contact, and flanges of channels in pure compression.
15.9
2. Legs of single angle struts, legs of double angle struts with separators and other un-stiffened elements supported along one edge.
12.8
3. Stems of tees. 21.3
4. Flanges of built-up I-sections with projecting plates or angles.
tb
tb
td
tb
yFE56.0
yFE45.0
yFE75.0
y
c
FEk64.0
ck1.18
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Element
Width-Thickness
Ratio
λr λr For A36 Steel
Stiffened1. Flanges of rectangular hollow sections of uniform thickness used for uniform compression.
39.7
2. Flexure in webs of doubly symmetric I-shaped sections and channels.
161.8
3. Uniform compression in webs of doubly symmetric I-shaped sections and uniform compression in all other stiffened elements.
42.3
4. Circular hollow sections in axial compression.D / t 0.11 (E / Fy) 88.6
bt
wth
bt
yFE40.1
yFE70.5
yFE49.1
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Beams:Lp = Limiting laterally unbraced length for full plastic bending capacity (Mp = Zx×Fy) in uniform moment case (Cb = 1.0).
For I-shaped members including hybrid sections and channels:
Lp = y
y FEr76.1 ≅ 50 ry (for A-36 Steel)
A section may develop yielding only at some points in case of inelastic buckling, when the unbraced length is between the two limiting lengths Lp and Lr, that is, when,
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Lp < Lb ≤ Lr
where Lr = limiting laterally unbraced length for inelastic torsional buckling, mm.
For doubly symmetric I-shaped members:
Lr = 27.0
76.6117.0
95.1
++
cJhS
EF
hScJ
FEr oxy
oxyts
≈y
ts FEr7.0
95.1 (very conservative estimate)
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Mr = limiting buckling moment dividing elastic and inelastic buckling for Cb = 1.0, Cbwill be defined later
= 0.7Fy Sx/106 kN-m2
tsrx
wy
SCI
x
oy
ShI
2= for doubly symmetric I-sections=
rts ≈ radius of gyration of the compression flange plus one-sixth of the web for doubly symmetric I-sections
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
+
ff
w
f
tbth
b
61112
rts =
c = 1.0 for a doubly symmetric I-shape
ho = distance between the flange centroids= d – tf / 2
Cw = warping torsional constant for the section, mm6
For symmetrical sections, Cw = 42
22oyof hIhI
≈
If = moment of inertia of one flange in lateral direction, mm4
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
J = torsional constant for the section, mm4
≈ ∑ 3bt31
For the above expression, b is the long dimension and t is the short dimension of any rectangular element of the section and summation is for all the elements of that section.
When Lb > Lr Mn = FcrSx ≤ Mp
Fcr = compression flange critical buckling stress
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Fcr =
+
ts
b
ox
ts
b
b
rL
hScJ
rL
EC078.012
2π
≈( )2
2
/ tsb
b
rLEC π
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
λp for compact section
1. Unstiffened flanges of I-shaped rolled beams, channels, tees and built-up doubly and single symmetric I-sections.
λp = = 10.8 for A-36 steelyFE /38.0
2. Unstiffened legs of single angles.
yFE /54.0λp = = 15.3 for A-36 steel
3. Stiffened flanges of HSS shapes
yFE /12.1λp = = 31.8 for A-36 steel
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Web local buckling criterionWeb is locally stable when the following condition is satisfied:
λ ≤ λp
where λ = wth
and assumed web depth for stability (h) is defined as under:h = twice the distance from the neutral
axis to the inside face of the compression flange less the fillet or corner radius for rolled sections
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
h = twice the distance from the neutral axis to the nearest line of fasteners at the compression flange or the inside face of the compression flange when welds are used.
λp for compact sectionFor webs of doubly symmetric I-sections and channels:
λp = = 107 for A-36 steelyFE /76.3For webs of rectangular HSS (λ = h / t):
λp = = 68.7 for A-36 steelyFE /42.2
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
FLEXURAL STRENGTH OF BEAMS
For a safe beam, the applied moment (service moment Ma in ASD and factored moment Mu in LRFD) must be lesser than or equal to the design strength of the beam.
Mu ≤ φbMn φb = 0.90 (LRFD)
Ma ≤ Mn / Ωb = 1.67 (ASD)
where Mn = nominal flexural strength as determined by the limit state of yielding, lateral torsional buckling, or local buckling.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Lm = Lp +( )( )
( )rpb
prppb
MMCLLMMC
−
−−
= Lp +( )
BFCMMC
b
ppb
×
−
= Lp + ≤ Lr
−
b
bp
CC
BFM 1
BF = slope of moment capacity versus unbraced length for inelastic lateral torsional buckling.
=pr
rp
LLMM
−
−
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
When Cb = 1.0, Lm = Lp
Design moment capacity (Mn) is determined for various cases of unbraced lengths as follows:
Case I: Compact Sections, Cb ≥ 1.0, Lb ≤ Lm
Mn = Mp = Z Fy / 106 (kN – m)
Case II: Compact Sections, Cb ≥ 1.0,
Lm < Lb ≤ Lr
Mn = ≤ Mp (kN – m)
−
−−−
pr
pbxyppb LL
LLSFMMC )7.0(
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Mn = Cb [Mp – BF(Lb – Lp)] ≤ Mp (kN – m)
Case III: Compact Sections, Cb ≥ 1.0,
Lb > Lr
For doubly symmetric I-shaped and channel section members:
Mn = CbFcrSx ≤ Mp
where Fcr = 2
2
2
078.01
+
ts
b
ox
ts
b
b
rL
hScJ
rL
EC π
The variables rts and others are as defined earlier.
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
The design shear strength of webs is φν Vnwith φν = 0.90 (LRFD) and the allowable shear strength is Vn / Ωv with Ωv = 1.67 (ASD).
For webs of rolled I-shaped members:
Vn = 0.6FyAwCv
wth
ywFE /Web Yielding:
For ≤ 2.24
(= 63.4 for A36 steel) Cv = 1.0
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Prof. Zahid Ahmad Siddiqi and Dr. Azhar Saleem
Concluded