7 Parameterisation


The groundwater models used in the Bioregional Assessment Programme have a relatively simple parameterisation. That is the hydrostratigraphic layers are generally assumed to be homogeneous with the properties having a depth dependence and are modified due to geomechanical deformation following longwall mining.

7.1 Assumption of homogeneity of aquifer parameters

In most groundwater models developed for BA purposes, spatial heterogeneity of hydraulic properties is not represented explicitly. Most hydrostratigraphic units are assigned a spatially uniform hydraulic property.

This section illustrates that by stochastically varying this uniform hydraulic property, the variation in predicted groundwater levels is at least as large as the variability that would arise from simulating spatial heterogeneity explicitly. This means that the stochastic predictions will be conservative (i.e. the range of the ensemble prediction will be larger compared to the range based on modelling heterogeneous hydraulic properties).

Figure 10

Figure 10 Conceptualisation of groundwater flow example (after Liang and Zhang, 2013)

The steady state solution for the groundwater level at a distance x from a no flow boundary, with a constant head boundary at x subscript N end subscript with constant head h subscript L end subscript , a spatially uniform diffuse recharge W and piecewise constant, spatially varying hydraulic conductivity K open parenthesis x close parenthesis equals K subscript i end subscript for x subscript i minus 1 end subscript is less than x is less than x subscript i end subscript open parenthesis i equals 1 comma 2 comma dot dot dot comma N can be expressed as (Figure 10 and equations 4 and 5 in Liang and Zhang, 2013):

h subscript x end subscript to the power of 2 end exponent equals h subscript L end subscript to the power of 2 end exponent plus fraction numerator W over denominator K subscript i end subscript end fraction open parenthesis C subscript i end subscript minus x to the power of 2 end exponent close parenthesis comma x is an element of open square bracket x subscript i minus 1 end subscript comma x subscript i end subscript close square bracket comma i equals 1 comma 2 comma dot dot dot comma N

(7)

C subscript i end subscript equals fraction numerator K subscript i end subscript over denominator K subscript N end subscript end fraction times x subscript N end subscript to the power of 2 end exponent plus upper case Theta open parenthesis N minus i close parenthesis sum from j equals i to N minus 1 of open parenthesis fraction numerator K subscript i end subscript over denominator K subscript j end subscript end fraction minus fraction numerator K subscript i end subscript over denominator K subscript j plus 1 end subscript end fraction close parenthesis times x subscript j end subscript to the power of 2 end exponent comma upper case Theta open parenthesis Theta symbol close parenthesis equals open curly bracket if Theta symbol is not equal to zero, the function result is 1, if Theta symbol is equal to zero, the function result is zero

(8)

These equations present a linear approximation to groundwater flow in a spatially variable field and yields the same results as a numerical model that is discretised in N grid cells. While this is a simplification of any field conditions, this general conceptual model resembles situations that are relevant to BA, such as groundwater mounding away from a river or groundwater level variation away from a mine that is drained to a fixed level.

Equations 7 and 8 are straightforward to implement numerically and are solved very quickly, which allows the exploration of the effects of spatial heterogeneity on groundwater level predictions.

Consider the log of hydraulic conductivity is normally distributed with a mean of 1 m/d and a standard deviation of 1:

natural log open parenthesis K close parenthesis equals N open parenthesis lower case Mu comma lower case Sigma to the power of 2 end exponent close parenthesis equals N open parenthesis 0 comma 1 close parenthesis

(9)

The spatial correlation can be described with an exponential variogram with correlation length lower case Lambda so that the variance between two locations a distance d apart is:

lower case Sigma subscript d end subscript to the power of 2 end exponent equals lower case Sigma to the power of 2 end exponent exp open parenthesis minus lower case Lambda d close parenthesis

(10)

Figure 11 shows the results of a comparison of groundwater levels predicted at a distance of 9000 m from the constant head boundary (x=1000 m). For the heterogeneous case, 1000 samples of ln(K) are generated from a multivariate normal distribution with mean equal to zero and a covariance governed by equation 10 with three different correlation lengths (100 m, 1000 m and 10,000 m). For the uniform K case, 1000 samples of ln(K) are taken from the normal distribution specified in equation 9. The latter approach is the approach that is taken in the stochastic sampling in the uncertainty analysis of BA groundwater models.

From Figure 11 it becomes clear that the resulting ensembles of groundwater level predictions are nearly identical between the heterogeneous and the uniform hydraulic conductivity fields for the three different correlation lengths.

Figure 12 shows the same analysis for groundwater level predictions 1000 m from the constant head boundary (x=9000 m). It is apparent that the uniform hydraulic conductivity field results in ensembles that have a similar mean and median to the heterogeneous case, but the spread in the distribution is underestimated. This effect is more pronounced for short correlation length.

While this is by no means a comprehensive study of the effects of spatial heterogeneity on groundwater level predictions, some general findings are:

  1. At regional scale, i.e. distances larger than a few kilometres, from a stress or boundary condition, spatial heterogeneity has little influence on groundwater level predictions. The uncertainty in groundwater level predictions can be captured by stochastically varying a spatially uniform hydraulic conductivity
  2. At a local scale, i.e. distance smaller than a few kilometres from a stress or boundary condition, spatial heterogeneity will have a distinct effect on groundwater level predictions. The differences between simulating spatial heterogeneity and varying a spatially uniform hydraulic conductivity increase for decreasing correlation length (i.e. higher spatial variability).

Figure 11

Figure 11 Single realisations of spatial variation in hydraulic conductivities (left column) for varying correlation lengths with the corresponding groundwater level predictions at x = 1000 m for 1000 realisations of the spatial varying field (heterogeneous K) and 1000 samples of spatially uniform hydraulic conductivity (uniform K) for a system with recharge W = 25 mm/year and xN = 10,000 m

Example only; do not use for analysis

Figure 12

Figure 12 Single realisations of spatial variation in hydraulic conductivities (left column) for varying correlation lengths with the corresponding groundwater level predictions at x = 9000 m for 1000 realisations of the spatial varying field (heterogeneous K) and 1000 samples of spatially uniform hydraulic conductivity (uniform K) for a system with recharge W = 25 mm/year and xN = 10,000 m

Example only; do not use for analysis

7.2 Depth dependence of hydraulic properties

Even though a simple parameterisation of the models is used that will generally see hydrostratigraphic layers treated as homogeneous, the hydraulic properties used in the groundwater modelling have a depth dependence that has been observed in many coal basins. An example is shown in Figure 13 for data from the Hunter subregion, Gloucester subregion and Sydney Basin bioregion (Parsons Brinkerhoff, 2015).

Figure 13

Figure 13 Relationship between depth and hydraulic conductivity for coal seams and interburden

Source: Figure 7.3 in Parsons Brinckerhoff (2015). This figure is not covered by a Creative Commons Attribution Licence, it has been reproduced with the permission of AGL.

7.3 Changes in hydraulic properties post-mining

Following longwall mining there are often changes in hydraulic properties observed due to geomechanical deformation. This can be represented in the groundwater models by enhancing the hydraulic conductivity after longwall mining. The hydraulic conductivity, K, above and below each mine working, is enhanced according to:

K open parenthesis x comma y comma z comma t close parenthesis equals 10 superscript delta end superscript times K subscript 0 end subscript open parenthesis x comma y comma z close parenthesis

(11)

where K0 is the base conductivity (both horizontal and vertical components), and parameterises the conductivity change. before mining of the seam commences, and at height, h, above the seam after mining commences. is calculated using the following piecewise-linear function of the height above the mining seam, h:

upper case Delta equals 0 for h greater than Z greater than or equal to 0

(12)

upper case Delta equals 0 for h less than z less than 0

(13)

upper case Delta equals M times open parenthesis Z minus h close parenthesis divided by Z for 0 less than or equal to h less than or equal to Z

(14)

upper case Delta equals m times open parenthesis h minus z close parenthesis divided by z for z less than h less than 0

(15)

The general form of the relationship is illustrated in Figure 14 where it is clear that conductivity change is M orders of magnitude directly above the seam, and m orders of magnitude directly below the seam, and that the conductivity changes occur between -z below the seam and Z above the seam.

Figure 14

Figure 14 Assumed relationship between the conductivity-change parameter, Δ, and the height above the mining seam, h

As discussed in Adhikary and Wilkins (2012), the effective conductivity in the immediate roof of longwall mines can be enhanced by up to 10 orders of magnitude. The enhancement of hydraulic conductivity can extend up to 500 m above and 250 m below the longwall panel.

Last updated:
8 June 2018