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TS(HC)
G25(HC)
G50(HC)
G75(HC)
TS(LC)
G25(LC)
G50(LC)
G75(LC)
TKS(LC)
e min
500
Vs 0max
Vs 0min
Vs 0max
400
Hardin-Richart(1963)
Hardin-Richart(1963)
Quartz sand: Vs(e)=328-110e
Hardin-Richart(1963)
Quartz sand: Vs(e)=328-110e
Ottawa sand: Vs(e)=350-161e
Quartz sand: Vs(e)=328-110e
Ottawa sand: Vs(e)=350-161e
300
Ottawa sand: Vs(e)=350-161e
200
Vs 0min
100
e max
0
0
0.2
0.4
0.6
0.8
1
1.2
Void ratio: e
Fig. 8.7. Normalized S-wave velocity versus void ratiofor five tested soils
(modified fromKokusho and Yoshida, 1997)
Thus, it is obvious that the S-wave velocities of granular soils are not determined by a
unique function of void ratiobut highly variable witha difference inparticle gradation.
In order to formulate the S-wave velocity of granular soils with widely different particle
gradations,normalizedS-wavevelocitiescorrespondingto e max and e min (seeTable8.1),
denoted as Vs 0 min and Vs 0 max , respectively, were introduced. These values were deter-
mined at junctions of diagonal straight lines approximating the data points with vertical
linesof e max and e min (indicatedbythearrows)andplottedinFigure8.7withlargesolid
symbols; circles for Vs 0 min and squares for Vs 0 max , respectively. It should be noted in
Figure 8.7 that Vs 0 min , despite some scatters, tends to be almost stable, while Vs 0 max
obviouslyincreasesastheuniformitycoefficient Cu ofsoilincreasesfrompoorly-graded
sands to well-graded gravels. In other words, the minimum S-wave velocity of well-
gradedgravelswillremainatalmostthesamelevelasthatofpoorly-gradedsandsdespite
muchlowervoidratiothansands.ThisfindingmayhelptoexplainwhytheS-waveveloc-
ityinthedebrisflowgravelinMoricouldtakeaslowas60-90m/s(Kokushoetal.,1995).
In contrast, the maximum S-wave velocity of well-graded gravels tends to increase con-
siderablywithincreasing Cu .Thevaluesof Vs 0 min and Vs 0 max areplottedagainst Cu in
thesemi-logarithmicplotinFigure8.8.Theseplotscanbeapproximatedbysimpleequa-
tionsindicatedonthechart.Thepower m inEq.(8.1)obtainedbyregressionanalysiscan
be assumed almost constant as m
125 (Kokusho and Yoshida, 1997). Thus, S-wave
velocity of granular soils including poorly-graded sands and well-graded gravels may be
formulated by the next equation.
=
0
.
D r ] σ v /
p 0 σ h /
p 0 0 . 125
Vs
=
[136
+ {
440 Cu
/(
Cu
+
1
.
4
)
136
}
(8.2)
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