Wherever there is matter in an ever-thinning universe, there might be an entire cosmologically-sized era dominated by an entirely different chemistry to what we have now.
Wherever there is matter in an ever-thinning universe, there might be an entire cosmologically-sized era dominated by an entirely different chemistry to what we have now.
I’m under the impression that if the proton does not decay - and there is still no evidence that it does - whatever matter is left in cold, dead stars that didn’t fall into a black hole, will slowly quantum tunnel their way into becoming spheres of iron.
Also, I thought that B-E Condensates have been created in the lab, by freezing lithium atoms to a fraction above 0K, their electrons slow down, to compensate and still satisfy the Uncertainty Principle, their orbitals swell and overlap, becoming the condensate. Then when they fire up the photon gun and shoot bosons at this gel or whatever it is, they’ve been able to slow them down, to freeze them inside the Condensate.
So fast forward to cold stars supposedly working their way through the quantum tunnel towards iron… won’t the orbitals of these atoms also swell, essentially turning the stellar remnant into a massive sphere of B-E Condensate?
If the answer is YES, there’s gotta be some emergent properties in systems such as this.
While I’m not an astrophysicist, I happen to be a theoretical chemist. While iron is the lowest energy state, you also have to account for entropy here, unless you’re at zero kelvin. Assuming our dead star is in an empty universe without any cosmic microwave background, it will eventually radiate out all heat and (asymptotically) approach zero kelvin, but in finite time you’ll always maintain a number of other elements due to entropy.
As long as there is background radiation, the star will never get colder than that radiation, and you will maintain some other elements.
What do you do in that role? Is it about finding new materials?
My background is in materials chemistry, but I’m currently doing research in thermodynamics. Specifically I work on developing predictive models for fluid behaviour. I’ve done some stuff on solids as well, but then mostly on solid-fluid interfaces. Let me know if you want more details :)
More details please.
I never would have made the connection between chemistry and fluid behaviour. Other than, y’know, this fluid dissolves that.
Hehe, I think a lot of people attribute to physics what I attribute to chemistry. Put simply, I (slightly jokingly) say that “chemistry is when there’s too many electrons for the physicists” ;)
I work in a junction of several fields: One side is in developing equations of state, which means we develop models that tell you everything from how compressible a fluid is, to how much heat it releases when condenses, to what the equilibrium state is (liquid, vapour, several immiscible liquids, etc.), or how the density changes with temperature and pressure, etc. These models primarily apply to bulk fluids at equilibrium. The primary framework we work in here is called “statistical associating fluid theory (SAFT)”.
Another side is what’s called “interfacial thermodynamics”, which involves looking at how liquid-liquid, liquid-vapour, and fluid-solid interfaces behave. Here we develop models for predicting how surface tension changes under different conditions, the nucleation energy of bubbles and droplets, and how various species “adsorb” on different surfaces/interfaces. The major framework we’re working in here is called “classical density functional theory”, which is quite similar to the more “commonly” known “quantum (or electron) density functional theory”.
Then there’s irreversible thermodynamics, which is a framework linking local thermodynamic properties (temperature, pressure, chemical potential, etc.) outside equilibrium to transport rates. This lets us model stuff like evaporation rates, ion transfer in batteries, and much more. Essentially, if you have transport processes with more than one driving force (e.g. a battery, where you have simultaneous gradients in temperature, electrical potential, and chemical potential), you need irreversible thermodynamics to make accurate transport models, because Fouriers law, Ficks law, Ohms law, etc. don’t really apply anymore.
Finally, I’ve done quite a bit of work on transport theory. Specifically, I’ve worked on developing predictive models for the transport properties (viscosity, thermal conductivity, diffusion coefficients, etc.) of fluids at moderate-high pressures. The major framework here is kinetic gas theory, more specifically revised Enskog theory.
This became quite a list, but yeah… that’s what I do :) let me know if you would like some follow-up reading recommendations or more details:)