2023
DOI: 10.1029/2022gl101222
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A Dynamics of Surface Temperature Forced by Solar Radiation

Abstract: Surface temperature of the earth plays a uniquely important role in solar radiation energy entering the Earth system through the surface energy balance, that is, the partition of solar radiation into long-wave radiation and turbulent and conductive heat fluxes into the atmosphere and the earth. A fundamental physical principle governing the dynamics of surface temperature is the conservation of energy represented by the energy balance equation linking radiation and conductive/turbulent heat fluxes at the earth… Show more

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Cited by 4 publications
(4 citation statements)
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“…The vegetation is assumed as uniform layer of constant dielectric properties. The diffusivity of radiative transfer, a non‐gradient‐based radiative energy transfer process, is parameterized as an analogy of gradient‐based transport processes, such as conductive and turbulent heat transfer in soil and atmosphere (Jing & Wang, 2023), leftκw=ω0δw2κs=ω0δs2κv=ω0δv2 \begin{align*}{\kappa }_{w}={\omega }_{0}{\delta }_{w}^{2}\\ {\kappa }_{s}={\omega }_{0}{\delta }_{s}^{2}\\ {\kappa }_{v}={\omega }_{0}{\delta }_{v}^{2}\end{align*} where ω 0 is the characteristic (e.g., diurnal or seasonal) angular frequency (i.e., time scales of the thermal effect of the microwave radiation) and δ w , δ s , δ v are the wavelength‐dependent e ‐fold penetration depth of electromagnetic wave in dielectric media of liquid water, dry soil and dry vegetation, respectively. The penetration depth δ is a function of complex dielectric constant ε ′ – iε ″ (e.g., Ulaby et al., 1982, p. 847) leftδ=λ4π|Imε|Imε=ε2+ε214sin[]12tan1()εεε2ε0.25emfor0.25emεε \begin{align*}\delta =\frac{\lambda }{4\pi \vert \mathrm{Im}\sqrt{\varepsilon }\vert }\\ \mathrm{Im}\sqrt{\varepsilon }={\left({{\varepsilon }^{\prime }}^{2}+{{\varepsilon }^{{\prime\prime}}}^{2}\right)}^{\tfrac{1}{4}}\sin \left[\frac{1}{2}{\tan }^{-1}\left(\frac{{\varepsilon }^{{\prime\prime}}}{{\varepsilon }^{\prime }}\right)\right]\approx \frac{{\varepsilon }^{{\prime\prime}}}{2\sqrt{{\varepsilon }^{\prime }}}\,\text{for}\,{\varepsilon }^{\prime }\gg {\varepsilon }^{{\prime\prime}}\end{align*} where λ is the wavelength of microwave radiation (e.g., 21 cm at L‐band 1.4 GHz).…”
Section: Methodsmentioning
confidence: 99%
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“…The vegetation is assumed as uniform layer of constant dielectric properties. The diffusivity of radiative transfer, a non‐gradient‐based radiative energy transfer process, is parameterized as an analogy of gradient‐based transport processes, such as conductive and turbulent heat transfer in soil and atmosphere (Jing & Wang, 2023), leftκw=ω0δw2κs=ω0δs2κv=ω0δv2 \begin{align*}{\kappa }_{w}={\omega }_{0}{\delta }_{w}^{2}\\ {\kappa }_{s}={\omega }_{0}{\delta }_{s}^{2}\\ {\kappa }_{v}={\omega }_{0}{\delta }_{v}^{2}\end{align*} where ω 0 is the characteristic (e.g., diurnal or seasonal) angular frequency (i.e., time scales of the thermal effect of the microwave radiation) and δ w , δ s , δ v are the wavelength‐dependent e ‐fold penetration depth of electromagnetic wave in dielectric media of liquid water, dry soil and dry vegetation, respectively. The penetration depth δ is a function of complex dielectric constant ε ′ – iε ″ (e.g., Ulaby et al., 1982, p. 847) leftδ=λ4π|Imε|Imε=ε2+ε214sin[]12tan1()εεε2ε0.25emfor0.25emεε \begin{align*}\delta =\frac{\lambda }{4\pi \vert \mathrm{Im}\sqrt{\varepsilon }\vert }\\ \mathrm{Im}\sqrt{\varepsilon }={\left({{\varepsilon }^{\prime }}^{2}+{{\varepsilon }^{{\prime\prime}}}^{2}\right)}^{\tfrac{1}{4}}\sin \left[\frac{1}{2}{\tan }^{-1}\left(\frac{{\varepsilon }^{{\prime\prime}}}{{\varepsilon }^{\prime }}\right)\right]\approx \frac{{\varepsilon }^{{\prime\prime}}}{2\sqrt{{\varepsilon }^{\prime }}}\,\text{for}\,{\varepsilon }^{\prime }\gg {\varepsilon }^{{\prime\prime}}\end{align*} where λ is the wavelength of microwave radiation (e.g., 21 cm at L‐band 1.4 GHz).…”
Section: Methodsmentioning
confidence: 99%
“…This prototype of the MEP models paved the way for developing a non‐gradient model of latent, sensible and ground heat flux over the land surface (Wang & Bras, 2011), which has been extended to all surface types including water, snow, and ice (Wang et al., 2014). The MEP model has been extensively validated and widely applied (e.g., El Sharif et al., 2019; Hajji et al., 2018, 2021; Isabelle et al., 2021; Jia et al., 2023; Jing & Wang, 2023; Nearing et al., 2012; Shanafield et al., 2015; Tang et al., 2021; Wang et al., 2017; Wang, Liu, & Shen, 2023; Xu et al., 2019, 2023; Yang et al., 2022; Yang & Wang, 2014).…”
Section: Methodsmentioning
confidence: 99%
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“…During the winter period, when the Sun is at its lowest position above the horizon, areas situated on steep northwestern slopes receive relatively little solar radiation. As surface temperature and, consequently, the near-surface air layer temperature are linked to solar radiation [94], the maximum temperatures reached during daytime decrease, thus reducing their positive influence.…”
Section: Local Topography As An Equalizer Of the Dendroclimatic Responsementioning
confidence: 99%