Abstract. The complexity of coupled transport of heat and moisture at the soil surface necessitates a combination of field and numerical experiments to evaluate the interactions between liquid and vapor phase flow. The near-surface moisture and temperature conditions of a bare soil were investigated experimentally and by using the SOIL model to assess the importance of water vapor flow. During a 1-month period in early fall, intensive measurements of water content, water tension, and temperature were made in a bare soil plot. Soil thermal conductivity, measured on soil cores extracted for laboratory analysis, was found to agree with estimates based on the Kersten equation. Simulated water content and soil temperature agreed well with observations. Modeled soil vapor flow was significant compared to liquid flow only during the initial dry days when the inclusion of vapor flow improved the predicted diurnal variation in water tension. Model predictions were sensitive to an accurate representation of the soil surface energy balance, including the consideration of steep gradients in tension near the soil surface, and to the enhancement of vapor flow.
IntroductionThe unsaturated soil layers near the surface play an important role in several environmental phenomena: The soil surface conditions control the partitioning of precipitation into surface runoff and infiltration and the partitioning of radiant energy into latent and sensible heat losses. Soil microbial activity, seed germination, and plant development depend on the moisture content and temperature of the topsoil.The moisture and energy balance at the surface are influenced by liquid as well as vapor phase flow, and both processes are important for an accurate representation of the surface energy balance. The model soil hydraulic properties can be specified using either the Brooks and Cer• [1964] expression or the van Genuchten [1980] expression. In our study we found that the soil properties were adequately described using the Brooks and Corey parameterization.
Field MeasurementsThe continuous field measurements were initiated on September 12 and continued until October 10, 1991. During this period, soil temperature, soil water tension, and soil water content were logged with a time resolution of 30 min.Soil temperature was measured using thermistor-based probes at the soil surface and at depths of 2.5, 5, 7.5, 10, 12.5, 15, 20, and 25 cm, with two replicates at the three uppermost depths.Soil water tension was measured at depths of 5, 10, 15, 20, and 25 cm, using small tensiometers (2100 F) and pressure transducers (5301) The model was initialized by specifying a uniform temperature (13øC) profile and a nonuniform water tension profile estimated from observations at the start of the experiment.Because of the diurnal heat flow in the soil, the simulated temperature profile rapidly changed from its initial uniform value to match the observed profile (see Figure 6).The saturated soil hydraulic conductivity, Ks, was initially estimated from laboratory measu...