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8/3/2019 Seismic Response Analysis-3
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SEISMIC RESPONSE ANALYSISOF
STRUCTUTRES
KAUSHIK CHATTERJEE
DCE (CIVIL), NPCIL
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Uncoupled Equations of motionUncoupled Equations of motion
unun--dampeddampedEquation of motion of an un-damped MDOF
system is
Substituting from eq. (1), we get,
Pre-multiplying by the transpose of the nth mode
shape vector, Tn ,we get,
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Uncoupled Equations of motionUncoupled Equations of motion
unun--dampeddampedNow let us introduce new symbols as,
These are called the normal coordinate
generalized mass
, generalized stiffness and
generalized loadfor mode n respectively.
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Uncoupled Equations of motionUncoupled Equations of motion
unun--dampeddamped
Thus the eqn. of motion of the MDOF system
can be written as,
Which is a SDOF system equation of motion for
mode n.
We have learnt earlier that,
Multiplying both sides by we get,
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Uncoupled Equations of motionUncoupled Equations of motion
unun--dampeddamped
Hence, a set of N simultaneous differentialequations which are coupled by the off-diagonalterms in the mass and stiffness matrices, gets
converted into a set of N independent normal-coordinates equations.
The dynamic response can be obtained bysolving separately for the response of eachnormal (modal) coordinate and thensuperposing these by eq. 1 to obtain theresponse in the original coordinates. This is
called ModalSuperposition Method.
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Uncoupled Equations of motionUncoupled Equations of motion
dampeddamped
The damped eqn. of motion is,
Normal coordinates transformation can be used to
uncouple the damped equation of motion.
Using eqn. (1) and pre-multiplying by the transpose
of the nth mode shape vector, Tn ,we get,
The orthogonality property causes all componentsexcept the nth mode term in the mass and stiffness
expressions of the eqn. to vanish.
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Uncoupled Equations of motionUncoupled Equations of motion
dampeddampedIf it is assumed that the corresponding
orthogonality condition applies to the damping
matrix also, then the above eqn. can be written
as,
Or,
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Uncoupled Equations of motionUncoupled Equations of motion
dampeddamped
Where,
n is the generalized damping ratio for mode n.
n = cn/cc = cn/2Mn n
The normal coordinate generalized mass,
stiffness and load are identical to those for the
un-damped system.
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
Required to : Obtain time varying response of structures
due to dynamic excitation. (Example Turbo-
generator foundation subjected to dynamic
machine load)
Generate floor time history & corresponding
floor response spectra at various floor levels
of multistoried buildings, which are used toseismically qualify equipments located on that
particular floor.
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS.
Ug U
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
In case of seismic excitation of a MDOF system
(say a multistoried building) the forces
generated by the seismic excitation within the
structural members are due to relativedisplacementbetween the stories.
No external force is applied on the structure assuch.
.
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
Hence.
Substituting this in the equation of motion, we
get
As the negative sign on the RHS has no real
significance in case of seismic analysis, it is
omitted in the subsequent equations.
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
Applying the concept of generalized coordinatesu=z and pre multiplying by
.
we get the equation of motion in generalized
coordinates as
Where, is called theModal earthquake excitation factor
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
If the natural mode of vibration isthe natural frequency of vibration is
and the damping ratio is
The equation of motion for the nth
mode ofvibration of the idealized multi-storey building
can be expressed as
.
The ratio Ln/Mn is called
Modal participation factor
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
The solution to this equation can be written interms of the Duhamel integral (damped system)
Thus the modal displacement is
The contribution of the nth mode to the
displacement at jth floor is given by
, j=1, 2, 3, ., N
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
The deformation or drift in storey j is given by
the difference of displacements of the floors
above and below
Now find out the equivalent lateral force fn(t),
which, if applied as static forces, would cause
structural displacements un(t). Thus
i.e.,
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
If we express the forces in terms of the massmatrix, then
Thus, the equivalent force at jth floor, which
causes lateral displacement ujn(t), is
The inertial force in the structure can be
determined by a static analysis, applying these
equivalent lateral forces.
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TIME HISTORY ANALYSISTIME HISTORY ANALYSIS
Then the earthquake response of the structureis obtained by combining the modal responses
in all the modes of vibration.
The total value of any response r(t), is thecombination of the contribution of all the
vibration modes to that response quantity
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
Response spectra is a plot of the maximumresponse of a series SDOF system having
different natural frequencies, for a particular
value of damping.
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
As the response in each vibration mode can bemodeled by the response of a SDOF system, the
maximum response in the mode can be directly
computed from the response spectra.
In design Max. response, rather than response
history is required.
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
To evaluate the earthquake response of a MDOF
system at any time:
Evaluate the earthquake response integral at
that time for each significant response mode.
To evaluate the maximum response:
Compute the modal response as before, for
each time during the earthquake history,
compare them and find the maximumresponse. ---- Time consuming calculation
involved.
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
Analysis based on ground motion responsespectra comes as an alternative handy tool.
For each individual mode of the structure, themaximum response can be obtained directly
from the response spectra.The maximum response in nth mode can beexpressed in terms ofSdn, Svn, and San which arethe ordinates of the displacement, pseudo
velocity and pseudo acceleration responsespectra respectively, corresponding to thevibration period and damping ratio of the mode.
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
The maximum modal displacement is
The maximum displacement at the jth floor is
The maximum drift in the jth storey is
The maximum lateral force at the j-th floor is
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
The base shear is given by
Substituting the value of fjn, we get
The relation between Sdn, Svn, and San is
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
Steps involved: Determine the response spectrum for the
ground motion if not already available.
Compute mass and stiffness matrices m and k. Estimate modal damping ratios.
Solve the eigen value problem to determine
the natural frequencies and mode shapes.
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RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS
Compute the maximum response in individualmodes of vibration by repeating the following
steps:
Corresponding to the period and damping
ratio, read the ordinates Sdn, and San of the
displacement and pseudo-acceleration
response spectra of the ground motion.
Compute floor displacements.
Compute storey drifts from floor
displacements.
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RESPONSERESPONSE SPECTRUM ANALYSISSPECTRUM ANALYSIS
Compute equivalent lateral forces.Compute internal forces storey shears and
moments by static analysis of the structuresubjected to equivalent lateral forces.
Determine an estimate of the maximum ofany response (displacement of a floor,deformation in storey, shear or moment in astorey, etc.) by combining the modal maximafor the response quantity