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Response parameters in model settings of 4.a, 2.a, 4.b, 4.c, 4.d, 4.e, 4.f, 4.g and 4.h. a) Maximum outflowing water temperature, b) area of the thermal water reservoir (T > 30 • C) in proportion to the whole model domain and average water temperature, c) Péclet number plotted against horizontal hydraulic conductivity and d) location and horizontal extent of thermal water (T > 30 • C) discharge. Scenarios with recharge>1 m/yr are indicated by grey colour.

Response parameters in model settings of 4.a, 2.a, 4.b, 4.c, 4.d, 4.e, 4.f, 4.g and 4.h. a) Maximum outflowing water temperature, b) area of the thermal water reservoir (T > 30 • C) in proportion to the whole model domain and average water temperature, c) Péclet number plotted against horizontal hydraulic conductivity and d) location and horizontal extent of thermal water (T > 30 • C) discharge. Scenarios with recharge>1 m/yr are indicated by grey colour.

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Extensional domain type geothermal plays, as fertile targets for future resource development, consist of an orogen and an adjoining sedimentary basin of asymmetric physiographic and geologic setting. Preliminary geothermal potential, i.e. prospective geothermal regions, basin-scale flow patterns, heat transfer processes, temperature distribution an...

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Context 1
... portrayed very similar curves. The maximum temperature of discharging water (T max ) was not more than ~32 • C, except for one model geometry (4.g), where this value was a bit under 30 • C, i.e. without thermal water discharge. Water temperatures higher than 30 • C were mostly restricted to hydraulic conductivities of 2⋅10 6 to 5⋅10 5 m/s (Fig. 4.a). The portion of the thermal water reservoir (A% (T > 30 • C)) and average temperature (T av ) had the same plateau, starting at K = 2⋅10 8 m/s with values of ~79% of A% and ~ 58 • C of T av . There were only minor changes regarding A% and T av in the studied cases: their minima were ~ 4% and ~ 13 • C, respectively (Fig. 4.b). Minor ...
Context 2
... 2⋅10 6 to 5⋅10 5 m/s (Fig. 4.a). The portion of the thermal water reservoir (A% (T > 30 • C)) and average temperature (T av ) had the same plateau, starting at K = 2⋅10 8 m/s with values of ~79% of A% and ~ 58 • C of T av . There were only minor changes regarding A% and T av in the studied cases: their minima were ~ 4% and ~ 13 • C, respectively (Fig. 4.b). Minor differences could be observed in the values of Pe reflecting changes in the magnitude of groundwater flow due to water table variations: slightly higher Pe numbers were characteristic for cases (4.b, 4.e and 4.h) with higher water table maxima (1000 ft./304.8 m), i.e. groundwater flow was more intense. Otherwise, the critical ...
Context 3
... in the values of Pe reflecting changes in the magnitude of groundwater flow due to water table variations: slightly higher Pe numbers were characteristic for cases (4.b, 4.e and 4.h) with higher water table maxima (1000 ft./304.8 m), i.e. groundwater flow was more intense. Otherwise, the critical value of Pe = 1 was reached at K ≈ 5⋅10 8 m/s (Fig. 4.c). The location of thermal water discharge on the surface was controlled by the water table configuration. In cases (2.a and 4.d), where the regional slope was c' = 0.02 and the sine amplitude was a' ≈ 50 and 100 ft. (15.24 and 30.48 m), the thermal water discharged at the "regular" place of ~5800 m, i.e. at the discharge area of the ...
Context 4
... ~200 ft. (~60.96 m) (model 4.f), the location of discharge moved farther to ~8700 m because of local-scale variation of the water table and consequent shallow penetration depth of the flow paths. The width of the thermal water plume gradually decreased as the discharge location migrated along the x-axis and as the water table gradient decreased (Fig. ...

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