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Shackleford
Mar18-11, 08:54 PM
This looks to be a fairly straightforward problem. I'm not sure why I'm having trouble.

The radiant energy flux density is the energy emission per unit area. Why would I not simply multiply the solar constant of the Earth times the surface area of the Earth? Of course, it would be a plane area approximation. Then, whatever that energy emission value that is, set it equal to the Stefan-Boltzmann constant*(TE)4*4pi*(RE)2?

Is the radiant energy flux density multiplied by the area equal to the power?

http://i111.photobucket.com/albums/n149/camarolt4z28/IMG_20110318_204153.jpg?t=1300499036

AlexChandler
Mar19-11, 10:26 AM
The cross section of the earth you would use is not its surface area. It will be Pi*R^2. It is the area of the shadow that the earth would cast on a plane perpendicular to the sun's intensity vectors.

Shackleford
Mar19-11, 10:28 AM
The cross section of the earth you would use is not its surface area. It will be Pi*R^2. It is the area of the shadow that the earth would cast on a plane perpendicular to the sun's intensity vectors.

Sorry, I was ambiguous. I meant plane area approximation, not surface area.

How do you calculate the radiant energy flux density at the Earth in terms of the Sun's temperature?

Shackleford
Mar20-11, 10:07 AM
The manual has

JE = sigmaB*(TS)4*[(RS)/(DE)]2

I'm not quite sure why they multiplied it by the tangent squared.

Shackleford
Mar21-11, 09:32 PM
Why did they multiply it by [(RS)/(DE)]2?