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13.4 Vibrations Due to Fluid – Structure Interaction
The principles of vibration due to fluids such as water are very similar to those of wind action presented
in the previous section. The fluid flow can significantly affect the vibrational characteristics of a structure.
The presence of a quiescent fluid decreases the natural frequencies and increases the damping of the
structure. Similar to wind, a turbulent fluid flow exerts random pressures on a structure, and these
random pressures induce a random response leading to large structural deformations or failure. More
details on fluid – structure interaction can be found in text books (e.g., Tiejens and Prandtl, 1957;
Milne-Thompson, 1968).
13.4.1 Added Mass and Inertial Coupling
A real fluid is viscous and compressible. In contrast, a perfect fluid is nonviscous and incompressible.
Fluid damping is absent in perfect fluids, and therefore, for a structure oscillating in a quiescent perfect
fluid, the fluid-force component is associated with the fluid inertia called the added mass. This is of
practical importance when the fluid density is comparable to the density of the structure, because then
the added mass becomes a significant fraction of the total mass in dynamic motion. Added mass and fluid
damping associated with single and multiple cylindrical structures are discussed in detail by Chen (1987).
For example, the added mass for a circular cylinder of radius a and height h is equal to pa2h: Added
masses for different cross-sectional shapes are presented by Milne-Thompson (1968).
13.4.2 Wave-Induced Vibration of Structure
This effect is similar to wind; however, the density is very much larger than wind, thus making
the structural damping less effective. Therefore, it is essential to ensure that resonance does not occur.
TABLE 13.6 Main Differences between Wind and Earthquake Loading
Characteristic Wind Earthquake
Source of loading External force due to wind pressures Applied base motion from
ground vibration
Type and duration
of loading
Wind storm of several hours duration.
Loads fluctuate, but are
predominantly in one direction
Transient cyclic loads of at most
a few minutes total duration.
Loads change repeatedly in direction
Predictability Good statistical basis is
generally available
Poor
Sensitivity of loading to
return period
Moderate; þ15% typical for
£ 10 on return period
High; maximum credible earthquake
often greatly in excess of “design” values
Influence of local
soil conditions
Little effect on dynamic sensitivity Soil conditions can be very important
Spectral peak input range Gust: , 0.1 Hz Usually 1 to 5 Hz
Main factors affecting
building response
External shape of building or structure.
Generally only global dynamic
properties are important.
Dynamic considerations affect
only a small fraction of
building structures
Response is governed by global dynamic
properties (fundamental period,
damping, and mass)
but plan and vertical regularity of
structure also important.
All structures are affected dynamically
Normal design basis Elastic response is required Inelastic response is usually permitted,
but ductility must be provided
Design of nonstructural
elements
Applied loading is concentrated
on external cladding
Entire building contents are shaken and
must be appropriately designed
Source: Data from Maguire, J.R. and Wyatt, T.A., 1999. Dynamics — An Introduction for Civil and Structural Engineers,
Thomas Telford, London.
Vibration and Shock Problems of Civil Engineering Structures 13-33
© 2005 by Taylor & Francis Group, LLC
The fluid forces which act in line with the
direction of wave propagation (Figure 13.19) can
be found using a generalized form of Morrison’s
equation comprising both drag (proportional to
area times velocity squared) and inertia forces
(proportional to immersed volume times acceleration).
More details can be found in Muga and
Wilson (1970).
Flexible structures will resonate with the wave if
the structural natural period equals the wave
period or a harmonic of the wave period. Since
the wave frequencies of importance are ordinarily
less than 0.2 Hz, such a resonance occurs only for
exceptionally flexible structures such as offshore platforms. The amplitude of structural response at
resonance is a balance between the wave force and the structural stiffness times the damping.
The above discussion considers only the in-line forces. These in-line forces produce an in-line
response. However, substantial transverse vibrations also occur for ocean flows around circular cylinders.
These vibrations are associated with periodic vortex shedding, which was discussed under wind-induced
vibration.
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