This model first introduced by Veletsos in 1973 for a circular rigid disk setting on a viscoelastic half space. Further studies were carried on to account for the effect of soil material damping and the effects of the footing embedment on the soil. The impedance terms introduced are frequency dependent and can be expressed in the form,
ki∗=ki+iωci
Eq. 2.4.1
In this expression, ki∗ is the frequency dependent impedance, ki is the static stiffness for the i-th degree of freedom, ω is the circular frequency of the vibration, ci is the damping constant for the i-th degree of freedom, and i is the complex numbers operator and is equal to −1. Expressions for vertical, horizontal, rocking, and torsional degrees of freedom will be presented in this section.
Dimensionless frequencyaoi
It is very common in the literature to develop the impedance expressions in terms of the dimensionless frequencyaoi defined as,
aoi=VsωRi=ωRiGρ
Eq. 2.4.2
Vertical Degree of Freedom v
The vertical degree of freedom impedance can be expressed as,
kv∗=GR[Cv1+iaovCv2]
Eq. 2.4.3
In Eq. 2.4.2, the terms Cv1 and Cv2 can be expressed as,
Cv1=(1−ν4)((1−χv−
2R′−1)γ4aov−γ3aov2)
Eq. 2.4.4
Cv2=(1−ν4)((2R′+1)γ4+
ψv+aovβm)
Eq. 2.4.5
R′ is a factor to account for material damping,
R′=1+βm2
Eq. 2.4.6
βm is the base soil damping ratio, and χv is defined as,
The constants in these equations are b1=0.425 and b2=0.687.
Effect of Foundation Embedment
Figure 2.1.1 Effect of Embedded Foundation
Because footing are normally embedded in the soil for normal construction methods, the effect of full or partial embedment in the soil must be studdied. The effect of embedment is a very complex topic with lots od studies in the literature. The most credible and somewhat straignforward to implement method is introduced in this section. This method estimates the impedance of the side layer in a similar fashion to the estimated impedance of the base soil then add the two quantities together to obtain the adjusted impedance of the overall foundation.
The complex dynamic empedance of the side layer can be expressed using the following equations, vertical impedance,
kev∗=Gsl[Sv1+iaovSv2]
Eq. 2.4.22
Horizontal impedance,
keu∗=Gsl[Su1+iaouSu2]
Eq. 2.4.23
Rocking impedance,
keψ∗=GsRψ2l[Sψ1+iaoψSψ2]
Eq. 2.4.24
Torsional impedance,
keη∗=GsRη2l[Sη1+iaoηSη2]
Eq. 2.4.25
In the above equations, the terms Si1 and Si2 can be determined approximately from Table 2.4.1, if the value of the dimensionless frequency aoi is less than 2 (aoi<2.0) for two categories of side layers, cohesive and granular.
DOF
Soil Type
Side Layer Si1
Side Layer Si2
Vertical
Cohesive
Sv1=2.7
Sv2=6.7
Vertical
Granular
Sv1=2.7
Sv2=6.7
Horizontal
Cohesive
Su1=4.1
Su2=10.6
Horizontal
Granular
Su1=4.0
Su2=9.1
Rocking
Cohesive
Sψ1=2.5
Sψ2=1.8
Rocking
Granular
Sψ1=2.5
Sψ2=1.8
Torsion
Cohesive
Sη1=10.2
Sη2=5.4
Torsion
Granular
Sη1=10.2
Sη2=5.4
For the broader range of aoi values, mathematical expressions involving Bessel functions of the first and second kinds are available in the literature. Due to the complexity of these expressions, they will not be introduced here, however, it is implemented in the impedance calculator provided in section 2.5 of this course.