I don't really understand how this is supposed to work, on any level. Why doesn't the heat radiate out like it normally would?Somewhere in this hypothetical universe is a galaxy made not naturally but through artificial means, with a diameter of 16 million parsecs. This "Z-Kardashev Galaxy" is comprised solely of copies of one same solar system: a single Kardashev-type star with a diameter of 1,860,000 miles and a temperature of 72,000,000,000,000 degrees Fahrenheit, which results in a luminosity of 2,657,599,202,344,462,135,749,473,441,629,625,102,087,912,417 times brighter than the sun. In spite of its massively hyper-high heat, the Kardashev-type star is actually inactive, meaning the heat is trapped within it and can't escape.
That temperature is equivalent to 4.0 * 10^13 K. At that temperature, hadrons separate out into individual quarks and matter stops acting normal. I don't really understand quantum chromodynamics very well, but my instinct is that if a star gets that hot, it's going to stop being a star. I think this star has more heat than its relativistic mass-energy equivalent, which is hard to wrap my head around. While I will continue to use this value for temperature and the other values you've provided, I would suggest that you decrease the temperature by a large amount, so that you're not causing the laws of physics to break down.Theoretically, it will expand the giant star's lifespan to 100 billion billion years (no, this is not a typo.)
With that luminosity, I think that this star would be brighter than our entire observable universe. That diameter is a little over twice the Sun's. This type of star is physically impossible and its existence would break the universe in a lot of ways. The peak wavelength for electromagnetic radiation from a black body at this temperature is almost at very-high-energy gamma ray levels, and it's well into the spectrum for gamma radiation, at 7 * 10^-17 m.
Based on a simple inverse square law calculation, to receive as much insolation from this star as Earth receives from the sun, the distance from would need to be roughly 8.8 * 10^6 times the current diameter of the observable universe.
I'll take your word for it on the lifespan; assuming you mean 10^9 when you say billion, that would be 10^20 years.
Even just one star like this is enough to vaporize the entire universe. If you want a theoretical maximum, I don't really know how to estimate that. This galaxy is around 500 times the diameter of the Milky Way.In turn, orbiting it from within its habitable zone are co-orbital binaries of one same star type: K5, 74% as wide, 69% as massive and only 16% as bright as our sun. Orbiting each of the binaries P-style, in turn, are co-orbits of Earth- to Venus-sized rocky planets.
With the specifics now in place, questions ensue:
- How many Kardashev-type stars can fit within the 16-million-parsec parameters of the Z-Kardashev Galaxy?
The habitable zone will be at around 1.7 * 10^7 Hubble lengths, or nearly a quintillion light-years, based on a naïve inverse square law calculation.
- How far and how wide is the Kardashev-type star's habitable zone?
What do you mean? How many systems could realistically form within this time? No K5V star is going to last 10^20 years.
- How many K5 binaries can co-orbit each other within the 100-billion-billion-year timespan?
What is the mass of the Kardashev-type star? You gave its radius and temperature, but not mass. This information is necessary to determine the size of the hill sphere of the binaries.
- How many of the K5 binary co-orbitals can fit inside the Kardashev-type star's habitable zone?
About 60 AU is the minimum distance from the binary star for a planet's tidal locking time to be less that 10^20 years, based on Wikipedia's formula. However, since none of these stars will last that long anyway, the planet only needs to avoid tidal locking for the lifetime of the star (~25 Gyr), which gives us a much more manageable ~1.5 AU minimum distance to avoid tidal locking.
- How many Earth- or Venus-sized planets can fit within each K5 binary's gravitational pull within the 100-billion-billion-year timespan and not get themselves tidally locked?
Out of curiosity, why are you calling it Kardashev? Does it have to do with the Kardashev scale, or is it something else?