DHARMCOMPRESSIBILITY AND CONSOLIDATION OF SOILS 229This solution enables the hydrostatic excess u to be computed for a soil mass under any
initial system of stress ui, at any depth z, and at any time t.
In particular, if ui is considered constant with respect to depth, this equation reduces tou =2
1
222 4 21u
nnnz
Hi enctH
nv
πππ π
(cos)sin− F /
HGI
KJL
NM
O
QP
−
=∞
∑ ...(Eq. 7.22)When n is even, (1 – cos nπ) vanishes; when n is odd, this factor becomes 2. Therefore it
is convenient to replace n by (2m + 1), m being an integer. Thus, we have
u =4
2121
0 2u 2122 42
mm
Hi e
mmctHv
()sin()()/
+L +
NMO
= QP∞
−+
∑ ππ
...(Eq. 7.23)It is convenient to use the symbol M to represent (π/2) (2m + 1), which occurs frequently:u =^2220u
MM
Hize MctH
mFsin v/
HGI
KJ−
=∞
∑ ...(Eq. 7.24)Three-dimensionless parameters are introduced for convenience in presenting the re-
sults in a form usable in practice. The first is z/H, relating to the location of the point at which
consolidation is considered, H being the maximum length of the drainage path. The second is
the consolidation ratio, Uz, defined in sec. 7.3, to indicate the extent of dissipation of the hydro-
static excess pressure in relation to the initial value:
Uz = (ui – u)/ui =^1 −F
HGI
KJu
ui ...(Eq. 7.16)
The subscript z is significant, since the extent of dissipation of excess pore water pres-
sure is different for different locations, except at the beginning and the end of the consolida-
tion process.
The third dimensionless parameter, relating to time, and called ‘Time-factor’, T, is de-
fined as follows:T =ct
Hv
2 ...(Eq. 7.25)where cv is the coefficient of consolidation,
H is the length drainage path,
and t is the elapsed time from the start of consolidation process.
In the context of consolidation process at a particular site, cv and H are constants, and
the time factor is directly proportional to time.
Introducing the time factor into Eq. 7.24, we haveu =2 2
0u
MMz
Hi e MT
mFsin
HGI
KJ−
=∞
∑ ...(Eq. 7.26)Introducing the consolidation ratio, Uz, we have:Uz = 1122
0−=− F
HGI
KJ−
=∞
∑u
uMMz
He
iMT
msin. ...(Eq. 7.27)