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Question
Assuming the sun to have a spherical outer surface of radius r, radiating like a black body at temperature toC, the power received by a unit surface, (normal to the incident rays) at a distance R from the centre of the sun is
where $\sigma $ is the Stefan's constant.
${{{r^2}\sigma {{\left( {t + 273} \right)}^4}} \over {4\pi {R^2}}}$
${{16{\pi ^2}{r^2}\sigma {t^4}} \over {{R^2}}}$
${{{r^2}\sigma {{\left( {t + 273} \right)}^4}} \over {{R^2}}}$
${{4\pi {r^2}\sigma {t^4}} \over {{R^2}}}$

Solution

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