Part 08 - Response Spectra

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9/22/2014 1 Earthquake Response of Linear Systems Ch 6 Chopra Examples of Ground motions Earthquake Response of Linear Systems El Centro ground motions Ground acceleration Ground velocity Ground displacement

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Response Spectra

Transcript of Part 08 - Response Spectra

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Earthquake Response of Linear Systems Ch 6 Chopra

Examples of

Ground motions

Earthquake Response of Linear Systems

El Centro ground motions

Ground acceleration

Ground velocity

Ground displacement

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Earthquake Response of Linear Systems

Earthquake Response of Linear Systems

u(t) = displacement of the mass relative to the ground

Internal forces, like moments and shears in the beams and columns,

are linearly related to the displacement function.

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Earthquake Response of Linear Systems

For a given ground motion, the deformation response, u(t), depends only on the

natural vibration period of the system and its damping ratio.

Observations:

1. Period of the response is close

to the natural period.

2. Among the 3 systems, the

longer the vibration period, the

greater the peak deformation.

3. Systems with more damping

respond less than lightly

damped systems.

4. For the systems with the same

period, the times to reach the

maxima and minima are similar.

Earthquake Response of Linear Systems

The equivalent static force, fs , is related to the displacement u(t) as:

fs (t) = k u(t)

Expressing k in terms of the mass m gives:

where

A(t) = pseudo-acceleration

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Earthquake Response of Linear Systems

Earthquake Response of Linear Systems

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Response Spectra

Definition:

A plot of the peak value of a response quantity as a function of the natural

vibration period Tn of the system, or a related parameter such as circular

frequency �n or cyclic frequency fn, due to a given forcing function is called

the response spectrum of that quantity .

Construction of Response Spectrum Response Spectra

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Response Spectrum

To construct the Response Spectrum for the pseudo-velocity, we can use the

Response Spectrum for the displacement, D. We just apply the relationship

Response Spectrum

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Response Spectrum

Response Spectra

To construct the Response Spectrum for the pseudo-acceleration, we can use the

Response Spectrum for the displacement, D. We just apply the relationship

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Response Spectra

One of the reasons is that each of the spectrum provides a physically meaningful quantity:

1. The deformation spectrum provides the peak deformation of a system.

2. The pseudo-velocity spectrum is related directly to the peak strain energy stored

in the system during the earthquake (see Eq. 6.6.2)

3. The pseudo-acceleration spectrum is related directly to the peak value of the

equivalent static force and base shear (see Eq. 6.6.4)

Response Spectra

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Response Spectra

V = �D log V = log � + logD

A = � V log A = log V + log � (b)

These are linear

relationships in

the log scale

or log D = log V – log � (a)

Thus, a four-way log plot as shown in Fig. 6.6.3 allows all three types of

spectra to be illustrated on a single graph.

From these relations, it is seen that when a plot is made with log V as the

ordinate and log � as the abcissa, Eq (a) is a straigh line with slope of +450

for a constant value of log D, and Eq (b) is a straight line with slope of -450

for a constant value of log A.

Response Spectra

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Response Spectra

Response Spectra

6.7 PEAK STUCTURAL RESPONSE FROM THE RESPONSE SPECTRUM

Response quantities of interest can be expressed in terms of D, V, A, and the

vibration characteristics of the vibrating system.

peak deformation:

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Response Spectra

Response Spectra

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Response Spectra

Response Spectra

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Response Spectra

(Study Ex 6.4 and 6.5)

Response Spectra

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Response Spectra

Response Spectra

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Response Spectra

Response Spectra

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Response Spectra

Response Spectra Effect of Damping

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Response Spectra

Ground motions during earthquakes show jagged response spectra. Even for

the same site, the response spectra for different earthquakes may have

peaks and valleys not necessarily at the same periods. (See Fig. 6.9.1)

It is not possible to predict the jagged response spectrum in all its detail for

a future earthquake. Thus, the design spectrum should consist of a set of

smooth curves or a series of straight lines with one curve for each level of

damping.

Fig. 6.9.1 Response Spectra for the

el Centro earthquake in 1940, 1956,

and 1968, at * = 2%

Response Spectra

The design spectrum should be representative of ground motions at the

site during past earthquakes. If no records are available, it should be based

on other sites under similar conditions. The factors that we try to match

include:

1. magnitude

2. distance of site from earthquake source

3. fault mechanism

4. geology of the travel path of seismic waves

5. local soil condition at the site

The design spectrum is based on statistical analysis of the response spectra

for a set of ground motions. For each value of the period Tn the probability

distribution, its mean value and its standard deviation are determined.

Connecting all the mean values gives the mean response spectrum.

Similarly, connecting all the mean-plus-one-standard-deviation gives the

mean-plus-one-standard-deviation response spectrum. (See Fig. 6.9.2)

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Response Spectra

Observe that the two

response spectra are

much smoother than

the response spectrum

for an individual

ground motion.

This smoothed

response spectrum

lends itself to

idealization by a series

of straight lines

Response Spectra

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Response Spectra

Response Spectra

Example

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Response Spectra

Response Spectra

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Response Spectra

Examples of Design Spectra

Response Spectra

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Response Spectra

Response Spectra

Relative velocity response spectrum = a response spectrum for the peak

velocity of an SDOF system obtained from ,- (t)

Pseudo-velocity response spectrum = a response spectrum for the peak

displacement multiplied by �n

Pseudo-velocity =

Relative Displacement Response

Relative Velocity Response

Total acceleration Response

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Response Spectra

Difference between

Relative Velocity and

Pseudo-Velocity

Response Spectra

Total acceleration Response

Pseudo-acceleration Response

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Response Spectra