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a
N/G res = 0.36
N/G res = 0.88
N/G res = 0.83
+146%
+131%
2%
kh net = 371md
kh net = 826md
kh net = 336md
-55%
-60%
kh simulator = 304md
kh true = 298md
k (md)
4504
Thin-bed
data
Logging
Filter
Blocking
Filter
4505
4506
N/G res > 1md
0.2m ave
0.5m grid
b
N/G logs = 0.36
N/G res = 0.365
Upscale
k v /k h
0.0004
kh true = 298md
Upscale
kh upscaled = 170md
k geom =74 < k est < k arith =299
k (md)
4504
Data
integration
Thin-bed
data
kh =
f(logs)
Upscaled
blocks
4505
4506
0.5m grid
4507
Fig. 3.36 Application of (
a
) the N/G approach and (
b
) the total property modelling approach to an example thin-bed
permeability dataset
discrete log by blocking the thin-bed data set
(using values for net and non-net reservoir).
The discrete-log N/G res estimate is quite accu-
rate, as smoothing has not been applied.
Upscaled cell values (k h and k v ) are then
estimated using functions proposed by Ringrose
et al. ( 2003 ) for permeability in heterolithic bed-
ding systems (described in Sect. 3.6 below).
These functions represent the numerical (single-
phase) upscaling step in the total-property-
modelling workflow. The TPM approach
preserves both an accurate estimate for N/G res
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