1975
DOI: 10.1109/proc.1975.9712
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Geologic applications of thermal infrared images

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Cited by 143 publications
(72 citation statements)
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“…Manga (1998) and James et al (2000) propose calculating the thermal energy from the di¡erence in discharge and recharge temperatures (using isotopes to determine recharge elevation) and then go on to assign the source of the thermal energy to geothermal heating. However, the temperature of the ground surface is determined by a balance between incoming solar energy and the outgoing ground radiation (Watson, 1975). If these radiative £uxes are out of balance, heat £uxes comparable to typical geothermal values can go into the ground.…”
Section: Temperature Chemistry and Isotopes Of Springsmentioning
confidence: 99%
“…Manga (1998) and James et al (2000) propose calculating the thermal energy from the di¡erence in discharge and recharge temperatures (using isotopes to determine recharge elevation) and then go on to assign the source of the thermal energy to geothermal heating. However, the temperature of the ground surface is determined by a balance between incoming solar energy and the outgoing ground radiation (Watson, 1975). If these radiative £uxes are out of balance, heat £uxes comparable to typical geothermal values can go into the ground.…”
Section: Temperature Chemistry and Isotopes Of Springsmentioning
confidence: 99%
“…where the depth z is erroneously reported in Xue and Cracknell (1995) and Cai et al (2007) under the square root, whereas it is reported correctly in Watson (1975) and Sobrino et al (1998); -A c /B is also reported erroneously in Xue and Cracknell (1995) without the minus sign. In particular, within equation (8), the phase difference of the soil temperature for the n-order, δ n (equation (9)), is a function of the thermal inertia, P, and of the angular velocity of rotation of the Earth, ω, assuming a value of 7.27 × 10 -5 rad s -1 :…”
Section: The One-dimensional (1d) Thermal Diffusion Equationmentioning
confidence: 93%
“…To solve the diffusion equation, boundary conditions have to be imposed (Watson 1975). Firstly, the surface (z = 0) temperature fluctuation depends on the shortwave instantaneous irradiance, E Sun , entering the soil proportional to the shortwave co-albedo (1 -α SW ), after passing through the atmospheric transmittance, τ SW , plus the net longwave radiation, R nLW , minus sensible, H, and latent, λET, heat fluxes to the atmosphere through the dynamic energy balance equation:…”
Section: The One-dimensional (1d) Thermal Diffusion Equationmentioning
confidence: 99%
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“…On the other hand, the heat loss due to ground radiation is given by qsoil(t) = σ ε T soil 4 , where ε is the mean emissivity of the surface and Tsoil(t)= T(x,y,0,t) is the soil temperature at the soil-air interface. This boundary condition involves a non-linear function of T. Nevertheless, in the range of interest, this term can be linearized, [7]. To obtain a numerical solution of Eq.…”
Section: Thermal Model Of the Soilmentioning
confidence: 99%