1980
DOI: 10.1007/bf01593046
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Vertical and off-diagonal eddy diffusivities in the Northern Hemispheric stratosphere and lower mesosphere

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1983
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Cited by 2 publications
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“…The thermal diffusivities (K yy ) in Table 1 (∼10 9 cm 2 s −1 for atmosphere above ocean, 40 times greater for atmosphere above land) might seem surprisingly large for Earth; in fact, however, they comport with what is expected when a process that involves large-scale advective motions is modeled as being purely diffusive (Kao & Kau 1980;Keeling & Heimann 1986). 13 Alternatively, we may write a fully nondimensional version of Equation (1) by mapping t → P orb t * , T → T 0 T * , I → I 0 I * , and S → I 0 S * , with I 0 ≡ σ T 0 4 (σ is the Stefan-Boltzmann constant).…”
Section: Dimensional Analysis Of Ebmmentioning
confidence: 96%
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“…The thermal diffusivities (K yy ) in Table 1 (∼10 9 cm 2 s −1 for atmosphere above ocean, 40 times greater for atmosphere above land) might seem surprisingly large for Earth; in fact, however, they comport with what is expected when a process that involves large-scale advective motions is modeled as being purely diffusive (Kao & Kau 1980;Keeling & Heimann 1986). 13 Alternatively, we may write a fully nondimensional version of Equation (1) by mapping t → P orb t * , T → T 0 T * , I → I 0 I * , and S → I 0 S * , with I 0 ≡ σ T 0 4 (σ is the Stefan-Boltzmann constant).…”
Section: Dimensional Analysis Of Ebmmentioning
confidence: 96%
“…We find that over land, thick ice, thin ice, and ocean, τ diff has the following respective values: ∼4 months, ∼7 months, ∼3 years, and ∼12 years. The thermal diffusivities (K yy ) in Table 1 (∼ 10 9 cm 2 s −1 for atmosphere above ocean, 40 times greater for atmosphere above land) might seem surprisingly large for Earth; in fact, however, they comport with what is expected when a process that involves large-scale advective motions is modeled as being purely diffusive (Kao & Kau 1980;Keeling & Heimann 1986). 5…”
Section: Dimensional Analysis Of Ebmmentioning
confidence: 97%