Why can you see stars (1/r or 1/r^2 dropoff of power)?

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The discussion centers on the relationship between the intensity of light from stars and the distance from the observer, specifically addressing the 1/r and 1/r^2 drop-off. It is clarified that while electromagnetic waves may drop off by 1/r, the intensity, which is proportional to the square of the electric field, actually decreases by 1/r^2. This is consistent with Gauss' law, as the light spreads over an expanding sphere, leading to a decrease in intensity with distance. The power required to activate the receptors in the eye is indeed dependent on this intensity drop-off. Understanding this relationship is crucial for comprehending how we perceive distant stars.
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I read somewhere that people can see stars because an electromagnetic wave drops off by 1/r, therefore the power delivered by the electromagnetic wave stays strong enough to activate the receptors in your eye. I believe, this 1/r relation was realized by Maxwell when he was analyzing and combining the Maxwell equations. But, even still, the intensity or flux of light waves should be dropping off by 1/r^2 because (according to Gauss' law) the light from that distant star all passes through a notional sphere that gets bigger and bigger the farther one gets away from that distant star. The sphere expands by r^2 for an increase of distance r. So why doesn't the intensity of the light drop off by 1/r^2 or does it? Even though the light itself decreases by 1/r, the intensity still has to follow this 1/r^2 relation.

Your eye being triggered depends on the power delivered by that electromagnetic radiation right? If this is true, what would be the equation for this? Dependent on 1/r or 1/r^2?

If someone could just generally shed some illumination on this overall situation and what is going on here with 1/r versus 1/r^2 and when one or the other matters, I would greatly appreciate it. Thanks! -xerxes73
 
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xerxes73 said:
I read somewhere that people can see stars because an electromagnetic wave drops off by 1/r, therefore the power delivered by the electromagnetic wave stays strong enough to activate the receptors in your eye. I believe, this 1/r relation was realized by Maxwell when he was analyzing and combining the Maxwell equations. But, even still, the intensity or flux of light waves should be dropping off by 1/r^2 because (according to Gauss' law) the light from that distant star all passes through a notional sphere that gets bigger and bigger the farther one gets away from that distant star. The sphere expands by r^2 for an increase of distance r. So why doesn't the intensity of the light drop off by 1/r^2 or does it? Even though the light itself decreases by 1/r, the intensity still has to follow this 1/r^2 relation.

Your eye being triggered depends on the power delivered by that electromagnetic radiation right? If this is true, what would be the equation for this? Dependent on 1/r or 1/r^2?

If someone could just generally shed some illumination on this overall situation and what is going on here with 1/r versus 1/r^2 and when one or the other matters, I would greatly appreciate it. Thanks! -xerxes73

The intensity is the square of the field. So if the field goes like 1/r the intensity goes like 1/r^2.

This is the case for light radiating from a localized source (like a star); the electric and magnetic fields both depend on the distance from the star as
<br /> E\sim\frac{1}{r}e^{ikr}\;,<br />
where ck is the angular frequency of the light.

As for the intensity:
<br /> I\sim |E|^2\sim \frac{1}{r^2}\;.<br />
 
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