Beauheim 1987 - Waste Isolation Pilot Plant - U.S. Department of ...
Beauheim 1987 - Waste Isolation Pilot Plant - U.S. Department of ...
Beauheim 1987 - Waste Isolation Pilot Plant - U.S. Department of ...
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102<br />
I I 1 1<br />
1<br />
W<br />
K<br />
3<br />
v)<br />
v)<br />
W<br />
K<br />
n<br />
v)<br />
W<br />
J<br />
2<br />
v)<br />
2<br />
W<br />
10'<br />
v) 100<br />
0<br />
z<br />
a io-'<br />
MATCH PARAMETERS<br />
AP<br />
= 1.0 psi<br />
t<br />
= 1.0 hr<br />
PD = 0.1<br />
tdCo =31<br />
tC,,ezs), = 0.4<br />
(CDezs)t-m = 4.0 x 10-3<br />
e-2s = 0.9<br />
Pi<br />
= 44.87 psig<br />
NO-FLOW<br />
BOUNDARY<br />
AT Do = SO00<br />
-<br />
0 PRESSURE DATA<br />
* PRESSURE-DERIVATlVE DATA<br />
SIMULATIONS<br />
10-2<br />
I 1 I I<br />
10-2 io-' 109 10' 102 103 104<br />
DIMENSIONLESS TIME GROUP, t,/Co<br />
Figure 5-21. H-8b/Culebra Pumping Test Drawdown Log-Log Plot with INTERPRET Simulation<br />
well with a smaller radius. Conversely, a well with a<br />
negative skin factor should behave like a well with a<br />
larger radius. H-8b, with a skin factor <strong>of</strong> -7.2 and an<br />
actual radius <strong>of</strong> 0.255 ft, behaves like a well with a<br />
radius <strong>of</strong> about 340 ft.<br />
The reason for the two-fold discrepancy between the<br />
transmissivity reported by Mercer (1983) and that<br />
obtained from this test is not clear. The hydraulic<br />
boundary indicated by this test analysis was either<br />
not felt by the earlier, shorter test, or was not<br />
recognized. Without either data from multiple<br />
observation wells or independent<br />
geologicfgeophysical information, the orientation <strong>of</strong><br />
the boundary cannot be determined.<br />
Figure 5-22 shows a log-log plot <strong>of</strong> the H-8b recovery<br />
data along with an INTERPRET simulation using<br />
exactly the same model as was used in the<br />
drawdown simulation (Figure 5-21). In an ideal<br />
system, this model should fit both the drawdown and<br />
recovery data identically. In general, the fit is<br />
excellent until extreme late time, at which point<br />
apparent "over-recovery" on the order <strong>of</strong> 1 psi is<br />
observed (most clearly in the rise <strong>of</strong> the pressure<br />
derivative). This over-recovery may be related to<br />
residua1 recovery from some pre-test pumping<br />
activities associated with checking the pump and<br />
filling the discharge lines (INTERA Technologies,<br />
1986). Figure 5-23, a linear-linear plot <strong>of</strong> both the<br />
drawdown (compensated for the initial 3.2psi pump<br />
loss) and recovery data along with an INTERPRETgenerated<br />
simulation, also shows the generally<br />
excellent tit between the data and the simulation, as<br />
well as the over-recovery beginning about 70 hr into<br />
the recovery period.<br />
In general, the H-8b response was very similar to the<br />
responses observed at wells H-3b2. H-3b3, and<br />
WIPP-13 when those wells were pumped (<strong>Beauheim</strong>,<br />
<strong>1987</strong>a and <strong>1987</strong>b). At these locations, the Culebra<br />
exhibits unrestricted interporosity flow with rapid<br />
transition between flow from the fractures only and<br />
flow from both the fractures and the matrix This type<br />
<strong>of</strong> response contrasts with the responses observed<br />
during pumping tests at wells DOE-1 (see Section<br />
64