I don't really care what you think is going on, but the surface of the photosphere is not a "black body".
Something on the sun sure as hell is, and whatever it is, it's above your solid surface. Unless you think your solid surface is at 6000 K. I've repeatedly stated that for the current argument, it makes no difference if it's the photosphere or not. Your repeated insistence that it's not the photosphere is a rather pathetic attempt to avoid addressing the fact that this 6000 K source will heat up your solid layer to at least as hot.
All you see is white light from a mostly NEON photosphere. That's all you see.
We see an entire 6000 K blackbody spectrum. I don't care where it comes from, but it's source is at 6000 K, and radiating as a blackbody.
No, but particles flow and carry heat with them.
Which is why I did those calculations. Calculations which you have yet to address. You claim I'm wrong, but you can't provide what you think are correct numbers for any of it.
So what? I'm sure the heat from a rock will travel in all direction in the stream. The water in the stream (in this case charged particles) will carry that heat downstream. If we measure the temperature of the water a mile upstream from my rock, it's not going to have the slightest effect on the temperature of the water upstream.
Provided we have enough water to do this. Which, again, was the point of my calculations: your mass flow cannot possibly do what you're claiming it does. There's just far too much heat involved.
You should care and you must care if you expect to comprehend the actual physics involved in this process.
Oh, but I'm not dealing with all the physics involved. I'm only dealing with the basic thermodynamics: are your proposed temperature differentials possible? And for that, many of the details (including the ones you keep trying to bring up) ARE irrelevant. Just like the atmospheric composition of the earth is irrelevant to its orbital trajectory around the sun.
Slapping math to an unrelated physical design is pointless.
Except that the math I've done is rather directly related to the physics in question. And you have been able to produce NO alternative numbers for any of the quantities involved. Why is that, Michael? Why have you wasted so much of your life on a "physics" theory that you can't quantify on even the most basic level? It's kind of sad, when you stop and think about it.
Sure, some heat will radiate inwards, but just like my water in the stream analogy, so what? The outbound particles will pick out that heat and transfer it to the heliosphere eventually.
Which is the model I did my calculations for. And what did I find? The numbers don't work out, not by many orders of magnitude. Which means that the outbound particles CANNOT do what you require them to do.
So what? That is the *AVERAGED* temperature that relates to many atmospheric layers all radiating at different temperatures as well as the heat contained in the outbound particle flow. It's not coming from ONE thing, or ONE place.
It doesn't matter if it's averaged or not, and it doesn't matter if it's coming from one layer or not. It's still what your solid surface will be subjected to. It's still the power that your solid surface will need to somehow remove in order to avoid heating up.
Yes you did. You tacked it to the photosphere. It has nothing (well little) to do with the surface of the photosphere.
No I didn't. I've repeatedly and explicitly stated that I don't care what layer you want to attribute it to. It's still there, and it will still act to heat up your solid layer.
You're missing the point. The particle flow is all *OUTBOUND*
I assumed that when I did my calculations.
Just like the water molecules pick up heat and carry it downstream, so too, the plasma particles moving in the outbound directly pick up heat and carry it away from the sun.
Won't stop heat transfer if there isn't enough water. And as my calculations demonstrate, there isn't.
BB theory is almost unrelated to solar theory. It's a handy oversimplification in some instances, but you can't use it to make your arguments, particularly in a Birkeland solar model.
Yes, I can. Why? Because the sun gives off a blackbody spectrum. If it gave off a highly non-blackbody spectrum, you might have a point. But it doesn't. Therefore, you don't.
If, and only if, there was no solar wind, your argument would in fact have merit.
I did my first calculation based on the premise that the solar wind WAS the driver for your model. Did you somehow
miss that? Because your response doesn't indicate that you actually understood any of my post.
Because the flow of particles is constant and outbound, your argument is moot.
The
entire point of those calculations was to see what would happen if a constant flow of particles was carrying away heat to keep your solid surface cool. And you've got... no answer. No alternative set of numbers. No different way of doing the calculation. Instead, you irrationally claim I'm wrong because I'm not considering the
exact thing those calculations were done to quantify.