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On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion
On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion
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On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion
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On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion
On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion
Journal Article

On Radial Heat Transport in Porous Aquifers With Nonlinear Velocity‐Dependent Thermal Dispersion

2025
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Overview
Accurate modeling of heat transport behavior near the test well is essential for the efficient operation and management of aquifer thermal energy storage (ATES) systems. Existing models typically assume a linear relationship between thermal dispersion and velocity, whereas previous controlled experiments have revealed that this relationship is nonlinear. We present a finite element model for thermal single‐well push‐pull (SWPP) tests in ATES systems, incorporating both nonlinear velocity‐dependent thermal dispersion and wellbore mixing effects. Morris global sensitivity analysis shows that heat transport is most affected by nonlinear velocity‐dependent thermal dispersion, followed by injection and extraction rates. A higher exponent of nonlinear velocity‐dependent thermal dispersion leads to a smaller thermal breakthrough curve at the wellbore and a shorter heat transport distance, while thermal dispersivity has the opposite effect. Also, neglecting nonlinear velocity‐dependent thermal dispersion significantly underestimates both effective thermal diffusivity and thermal recovery efficiency in the SWPP tests, where the former is potentially underestimated by four orders of magnitude in the thermal dispersivity range of 1.478–1,000 s. Moreover, the proposed model is used to analyze the relationship between thermal recovery efficiency and the injection‐extraction rate ratio, suggesting that keeping the ratio below one ensures that efficiency exceeds 60%. The capabilities of new model are further demonstrated through two in situ thermal SWPP tests on different time scales (1,000 min and 3 months), highlighting that incorporating nonlinear velocity‐dependent thermal dispersion into models significantly enhances their ability to interpret observations, and the thermal dispersion potentially connected to the test duration.