performance based design by ashraf h
TRANSCRIPT
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Nonlinear Analysis & Performance Based Design
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Nonlinear Analysis & Performance Based Design
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Nonlinear Analysis & Performance Based Design
CALCULATED vs MEASURED
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Nonlinear Analysis & Performance Based Design
ENERGY DISSIPATION
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Nonlinear Analysis & Performance Based Design
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Nonlinear Analysis & Performance Based Design
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Nonlinear Analysis & Performance Based Design
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Nonlinear Analysis & Performance Based Design
IMPLICIT NONLINEAR BEHAVIOR
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Nonlinear Analysis & Performance Based Design
STEEL STRESS STRAIN RELATIONSHIPS
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Nonlinear Analysis & Performance Based Design
INELASTIC WORK DONE!
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Nonlinear Analysis & Performance Based Design
CAPACITY DESIGN
STRONG COLUMNS & WEAK BEAMS IN FRAMES
REDUCED BEAM SECTIONSLINK BEAMS IN ECCENTRICALLY BRACED FRAMES
BUCKLING RESISTANT BRACES AS FUSES
RUBBER-LEAD BASE ISOLATORS
HINGED BRIDGE COLUMNS
HINGES AT THE BASE LEVEL OF SHEAR WALLSROCKING FOUNDATIONS
OVERDESIGNED COUPLING BEAMS
OTHER SACRIFICIAL ELEMENTS
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Nonlinear Analysis & Performance Based Design
STRUCTURAL COMPONENTS
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Nonlinear Analysis & Performance Based Design
MOMENT ROTATION RELATIONSHIP
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Nonlinear Analysis
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Performance
Based
Design
IDEALIZED MOMENT ROTATION
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Nonlinear Analysis
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Performance
Based
Design
PERFORMANCE LEVELS
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Nonlinear Analysis
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Performance
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Design
IDEALIZED FORCE DEFORMATION CURVE
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Nonlinear Analysis
&
Performance
Based
Design 17
ASCE 41 BEAM MODEL
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Nonlinear Analysis
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Performance
Based
Design
• Linear Static Analysis
• Linear Dynamic
Analysis
(Response Spectrum or Time History Analysis)
• Nonlinear Static Analysis
(Pushover Analysis)
• Nonlinear Dynamic Time History Analysis(NDI or FNA)
ASCE 41 ASSESSMENT OPTIONS
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Nonlinear Analysis
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Performance
Based
Design
ELASTIC STRENGTH DESIGN ‐ KEY STEPS
CHOSE DESIGN CODE AND EARTHQUAKE LOADS
DESIGN CHECK PARAMETERS STRESS/BEAM MOMENT
GET ALLOWABLE STRESSES/ULTIMATE– PHI FACTORS
CALCULATE STRESSES – LOAD FACTORS (ST RS TH)
CALCULATE STRESS RATIOS
INELASTIC DEFORMATION BASED DESIGN ‐‐ KEY STEPS
CHOSE PERFORMANCE LEVEL AND DESIGN LOADS – ASCE 41
DEMAND CAPACITY MEASURES – DRIFT/HINGE ROTATION/SHEAR
GET DEFORMATION
AND
FORCE
CAPACITIES
CALCULATE DEFORMATION AND FORCE DEMANDS (RS OR TH)
CALCULATE D/C RATIOS – LIMIT STATES
STRENGTH vs DEFORMATION
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Nonlinear Analysis
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Performance
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Design
STRUCTURE and MEMBERS
• For a structure, F = load, D = deflection.
• For a component, F depends on the component type, D is the
corresponding deformation.
• The component F‐D relationships must be known.
• The structure F‐D relationship is obtained by structural analysis.
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Performance
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Design
FRAME COMPONENTS
• For each component type we need :
Reasonably accurate nonlinear F‐D relationships.
Reasonable deformation and/or strength capacities.
• We must choose realistic demand‐capacity measures, and it must be feasible to calculate the demand values.
• The best model is the simplest model that will do the job.
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Nonlinear Analysis
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Performance
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Design
Force (F)
Initiallylinear
StrainHardening
Ultimatestrength
Strength loss
Residual strength
Complete failure
First yield
Ductile limit
Hysteresis loopStiffness, strength and ductile limit mayall degrade under cyclic deformation
Deformation (D)
F-D RELATIONSHIP
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Performance
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Design
LATERALLOAD
Partially DuctileBrittle Ductile
DRIFT
DUCTILITY
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Performance
Based
Design
ASCE 41 - DUCTILE AND BRITTLE
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Performance
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Design
FORCE AND DEFORMATION CONTROL
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Performance
Based
Design
F
Relationship allowingfor cyclic deformation
Monotonic F-D relationship
Hysteresis loopsfrom experiment.
D
BACKBONE CURVE
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Performance
Based
Design
HYSTERESIS LOOP MODELS
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Performance
Based
Design
STRENGTH DEGRADATION
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Performance
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Design
ASCE 41 DEFORMATION CAPACITIES
• This can be used for components of all types.
• It can
be
used
if
experimental
results
are
available.
• ASCE 41 gives capacities for many different components.
• For beams and columns, ASCE 41 gives capacities only for the chord rotation model.
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Performance
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Design
θi θ j
Currentθ
Elasticθ
Plastic (hinge) θ
Totalrotation
Zero length hinges
Elastic beam
Plasticrotation
Elasticrotation
Similar atthis end
Mi M j
M or Mi j
M
θ θi jor
θ
BEAM END ROTATION MODEL
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Performance
Based
Design
PLASTIC HINGE MODEL
• It is
assumed
that
all
inelastic
deformation
is
concentrated
in
zero
‐
length plastic hinges.
• The deformation measure for D/C is hinge rotation.
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Design
PLASTIC ZONE MODEL
• The inelastic behavior occurs in finite length plastic zones.
• Actual plastic
zones
usually
change
length,
but
models
that
have
variable lengths are too complex.
• The deformation measure for D/C can be :
‐ Average curvature in plastic zone.
‐ Rotation over plastic zone ( = average curvature x plastic zone length).
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Design
ASCE 41 CHORD ROTATION CAPACITIES
IO LS CP
Steel Beam θp/θy = 1 θp/θy = 6 θp/θy = 8
RC Beam
Low shear
High shear
θp = 0.01
θp = 0.005
θp = 0.02
θp = 0.01
θp = 0.025
θp = 0.02
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Design
COLUMN AXIAL‐BENDING MODEL
Mi
P
PP
P
or
V
V
M j
MM
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Design
STEEL COLUMN AXIAL‐BENDING
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Performance
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Design
CONCRETE COLUMN AXIAL‐BENDING
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Performance
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Design
NodeZero-lengthshear "hinge"Elastic beam
SHEAR HINGE MODEL
PANEL ZONE ELEMENT
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Performance
Based
Design
PANEL ZONE ELEMENT
• Deformation, D = spring rotation = shear strain in panel zone.
• Force, F = moment
in
spring
= moment
transferred
from
beam
to
column elements.
• Also, F = (panel zone horizontal shear force) x (beam depth).
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Performance
Based
Design
BUCKLING-RESTRAINED BRACE
The BRB element includes “isotropic” hardening.
The D‐C measure is axial deformation.
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WALL FIBER MODEL
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Nonlinear Analysis
&
Performance
Based
Design
Steel
fibers
σ
σ
ε
ε
Concretefibers
WALL FIBER MODEL
ALTERNATIVE MEASURE STRAIN
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Design
ALTERNATIVE MEASURE - STRAIN
NONLINEAR SOLUTION SCHEMES
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Performance
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Design
∆ ƒ
ƒ
∆ u u
1 2
iteration
NEWTON – RAPHSON
ITERATION
∆ ƒ
ƒ
∆ u u
1 2
iteration
CONSTANT STIFFNESS
ITERATION
3 4 56
NONLINEAR SOLUTION SCHEMES
CIRCULAR FREQUENCY
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Nonlinear Analysis
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Performance
Based
Design
Y
+Y
-Y
0 Radius, R
θ
CIRCULAR FREQUENCY
THE D V & A RELATIONSHIP
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Performance
Based
Design
u.
t
ut1.
..
Slope = ut1..
t1
u
t1 t
Slope = ut1.
u
ut1..
t1 t
THE D, V & A RELATIONSHIP
UNDAMPED FREE VIBRATION
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Design
UNDAMPED FREE VIBRATION
)cos(0 t uut ω =
0ukum &&
m
k where =ω
RESPONSE MAXIMA
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Design
RESPONSE MAXIMA
ut )cos(0 t u ω =
)cos(02
t u ω ω −=ut &&
)sin(0 t u ω ω −=ut &
max2uω −=maxu&&
BASIC DYNAMICS WITH DAMPING
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Design
BASIC DYNAMICS WITH DAMPING
guuuu &&&&& −22
guMKuuCuM
KuuC
t
uM
&&&&&
&&&
−
= 0
gu&&
M
K
C
RESPONSE FROM GROUND MOTION
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ug..
2ug2..
ug1
..
1
t1 t2
Time t
&& A Bt u
g
= + = −&& &u u u+ +22ξω ω
RESPONSE FROM GROUND MOTION
DAMPED RESPONSE
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Design
{ [ & ] cos
[ (&
)] sin }
e uB
t
A u u
B
t
B
t
t d
dt t d
&ut = −
+ − − + +
−ξω
ωω
ω ω ξω ω ω ω
1 2
2
1 1 2 2
1
e A B
t
u u A B
t
A B Bt
t
t d
dt t d
ut = − +
+ + − +−
+ − +
−ξω
ω
ξ
ω
ω
ωξω
ξ
ω
ξ
ωω
ωξ
ω ω
{ [u ] cos
[ &( )
] sin }
[ ]
1 2 3
1 1
2
2
2 3 2
2
1 2 1
2
DAMPED RESPONSE
SDOF DAMPED RESPONSE
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Design
SDOF DAMPED RESPONSE
RESPONSE SPECTRUM GENERATION
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Design
RESPONSE SPECTRUM GENERATION
-0.40
-0.20
0.00
0.20
0.40
0.00 1.00 2.00 3.00 4.00 5.00 6.00
TIME, SECONDS
G R O
U N D
A C C , g
Earthquake Record
Displacement
Response Spectrum5% damping
-4.00
-2.00
0.002.00
4.00
0.00 1.00 2.00 3.00 4.00 5.00 6.00
D I S P L ,
i n .
-8.00
-4.00
0.00
4.00
8.00
0.00 1.00 2.00 3.00 4.00 5.00 6.00
D I S P
L , i n .
0
2
4
6
8
10
12
14
16
0 2 4 6 8 10
PERIOD, Seconds
D I S P L A C E M E N T ,
i n c h e s
T= 0.6 sec
T= 2.0 sec
SPECTRAL PARAMETERS
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0
4
8
12
16
0 2 4 6 8 10
PERIOD, sec
D I S P L
A C E M E N T , i n .
0
10
20
30
40
0 2 4 6 8 10
PERIOD, sec
V
E L O C I T Y , i n / s e c
0.00
0.20
0.40
0.60
0.80
1.00
0 2 4 6 8 10
PERIOD, sec
A C C E L E R A T I O N , g
dV SPS ω
va PSPS ω
SPECTRAL PARAMETERS
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ASCE 7 RESPONSE SPECTRUM
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Nonlinear Analysis
&
Performance
Based
Design
PUSHOVER
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Performance
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Design
THE LINEAR PUSHOVER
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Performance
Based
Design
EQUIVALENT LINEARIZATION
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Performance
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Design
How far to push? The Target Point!
DISPLACEMENT MODIFICATION
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DISPLACEMENT MODIFICATION
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Design
Calculating the Target Displacement
C0
Relates spectral to roof displacement
C1 Modifier for inelastic displacement
C2 Modifier for hysteresis loop shape
δ = C 0C
1C
2S
aT
e
2/ (4π
2)
LOAD CONTROL AND DISPLACEMENT CONTROL
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Performance
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Design
P-DELTA ANALYSIS
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P-DELTA DEGRADES STRENGTH
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P-DELTA EFFECTS ON F-D CURVES
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Design
STRUCTURESTRENGTH
The "over-ductility" is reduced,and is more uncertain.
P- e ects may reduce the dri t at which the"worst" component reaches its ductile limit.Δ
P- effects will reduce the drift atwhich the structure loses strength.Δ
DRIFT
THE FAST NONLINEAR ANALYSIS METHOD (FNA)
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Design
NON LINEAR FRAME AND SHEAR WALL HINGES
BASE ISOLATORS (RUBBER & FRICTION)
STRUCTURAL DAMPERS
STRUCTURAL UPLIFT
STRUCTURAL POUNDINGBUCKLING RESTRAINED BRACES
RITZ VECTORS
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Design
FNA KEY POINT
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Design
The Ritz modes generated by the
nonlinear
deformation
loads
are
used
to modify the basic structural modes
whenever the nonlinear elements go
nonlinear.
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MESH REFINEMENT
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Performance
Based
Design71
APPROXIMATING BENDING BEHAVIOR
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Nonlinear Analysis
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Performance
Based
Design72
This is for a coupling beam. A slender pier is similar.
ACCURACY OF MESH REFINEMENT
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Performance
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Design73
PIER / SPANDREL MODELS
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Performance
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Design74
STRAIN & ROTATION MEASURES
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Design75
STRAIN CONCENTRATION STUDY
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Design
76
Compare calculated strains and rotations for the 3 cases.
STRAIN CONCENTRATION STUDY
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Design
77
The strain over the story height is insensitive to the number of elements.
Also, the rotation over the story height is insensitive to the number of elements.
Therefore these are good choices for D/C measures.
No. of
elems
Roof
drift
Strain in bottom
element
Strain over story
height
Rotation over
story height
1 2.32% 2.39% 2.39% 1.99%
2 2.32% 3.66% 2.36% 1.97%
3 2.32% 4.17% 2.35% 1.96%
DISCONTINUOUS SHEAR WALLS
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PIER AND SPANDREL FIBER MODELS
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Nonlinear
Analysis
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Performance
Based
Design79
Vertical and horizontal fiber models
RAYLEIGH DAMPING
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Nonlinear
Analysis
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Performance
Based
Design 80
• The αM dampers
connect
the
masses
to
the
ground.
They
exert
external damping forces. Units of α are 1/T.
• The βK dampers act in parallel with the elements. They exert internal damping forces. Units of β are T.
• The
damping
matrix
is
C =
αM +
βK.
RAYLEIGH DAMPING
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Nonlinear
Analysis
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Performance
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Design 81
• For linear
analysis,
the
coefficients
α and
β can
be
chosen
to
give
essentially
constant damping over a range of mode periods, as shown.
• A possible method is as follows :
Choose TB = 0.9 times the first mode period.
Choose TA = 0.2 times the first mode period.
Calculate α and
β to
give
5%
damping
at
these
two
values.
• The damping ratio is essentially constant in the first few modes.
• The damping ratio is higher for the higher modes.
RAYLEIGH DAMPING
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KuuC &tuM && = 0
Kuu& + = 0
M +
K
u&& +
C
Mu&
MuK = 0
2uu& =
2 0 ω2 M
= C
ω2=
+
ω
2
ω2=CM 2
=
C
MMK =
2
C
MK 2 MK
M+
K=
tuM &&
u&&
;
2 MK
RAYLEIGH DAMPING
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Design
Higher Modes
(high
ω) = β
Lower Modes (low ω) = α
To get
ζ from
α &
β for
any
ω M
K=
To get α & β from two values of ζ1
& ζ2
; Τ 2πω
=
ζ1
= α 2ω
1
+
β ω1
2
ζ2 = α 2ω2
+
β ω22
Solve for α & β
DAMPING COEFFICIENT FROM HYSTERESIS
http://www.civil808.com/
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8/17/2019 performance based design by Ashraf H.
84/86
Nonlinear
Analysis
&
Performance
Based
Design
http://www.civil808.com/
-
8/17/2019 performance based design by Ashraf H.
85/86
A BIG THANK YOU!!!
-
8/17/2019 performance based design by Ashraf H.
86/86
Nonlinear
Analysis
&
Performance
Based
Design
http://www.civil808.com/