Chapter 4
Soil Temperature Model
4.0 Introduction
The soil temperature at the current time step is a function of the past soil temperature, soil
moisture state, and the surface forcing. The latter depends on the time of day, wind,
relative humidity, precipitation, air temperature, and presence of clouds.
4.1 Soil Thermal Model
The temperature gradient in a non-uniform soil layer can be described by the one-
dimensional heat flow equation:
c ∂T l fus ρi ∂θi
∂T ∂ ⎛ ∂T ⎞
- v p,w
= ⎜ kth
+
⎟
c p ∂z c p ρw ∂t
∂t ∂z ⎝ ∂z ⎠
(4.1)
c p,w ∂T l fus ρi ∂θi
∂k ∂T
∂T
2
= th
+ kth 2 - v
+
c p ∂z c p ρw ∂t
∂z ∂z
∂z
where T is the temperature (K), t is time (s), kth is the thermal diffusivity (m2/s), cp,w is the
specific heat of water (J/kg⋅K), cp is the specific heat of the soil (J/kg⋅K), v is the vertical
rate of water flow (m/s), lfus is the latent heat of fusion (J/kg), θi is the volumetric ice
content (cm3/cm3), ρi is the density of ice (kg/m3), ρw is the density of water (kg/m3), and z
is depth (m) measured positive downward from the surface. Further discussions on the
water flow rate and the change in ice content are found in Chapter 5 and Chapter 6,
respectively. The temperature is subject to the following boundary condition:
F (T ) = (1 - α ) I s ↓ +Ιi↓r - Ι↑r + H + L - P +
i
ρ ∂θi
(4.2)
∂T
κ
+ l fus i
∆z - vc pT = 0
@ z = 0m
ρw ∂t
∂z
where α is the surface albedo, I s ↓ is the total solar radiation (W/m2) impinging on the
surface, Ii↓ is the incoming longwave radiation (W/m2), Ii↑ is the outgoing longwave
r
r
radiation (W/m ) both reflected and emitted, H is the sensible heat (W/m2), L is the latent
2
heat (W/m2), P is the heat due to precipitation (W/m2), and κ is the surface thermal
conductivity (W/mK). In Equation (4.2), heat that is transferred to the surface is
considered positive, as is shown in Figure 4.1. Energy that can be transferred either
to/from the surface depending on the gradient is shown as double-headed arrows.
The first term in Equation (4.2) represents the amount of solar, or shortwave radiation,
absorbed by the surface. The second term is the incoming longwave radiation while the
third term is the outgoing longwave radiation, which is composed of radiation emitted
from the surface and incoming radiation reflected from the surface. The sensible and
latent heat fluxes together are called the turbulent heat fluxes and have non-zero values in
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