Thermodynamics, gravity, entropy

Click For Summary
SUMMARY

The discussion centers on the relationship between thermodynamics, gravity, and entropy, specifically addressing the second law of thermodynamics and its applicability to cosmic structures. It asserts that while thermodynamics suggests matter should become evenly distributed over time, in reality, matter in the universe has clumped into structures like planets due to gravitational forces. The original thermodynamic model, designed for gases, fails to account for gravity, leading to a contradiction in its application on a cosmic scale. This topic is explored in depth by Ian Stewart, Jack Cohen, and Terry Pratchett in "The Science of Discworld II."

PREREQUISITES
  • Understanding of the second law of thermodynamics
  • Basic knowledge of gravitational forces and their effects on matter
  • Familiarity with entropy concepts in physics
  • Awareness of the limitations of thermodynamic models for gases
NEXT STEPS
  • Research the implications of gravity on thermodynamic systems
  • Study the concept of entropy in black holes and its significance
  • Explore the differences between classical thermodynamics and statistical mechanics
  • Investigate the role of convection and diffusion in stellar environments
USEFUL FOR

Physicists, cosmologists, students of thermodynamics, and anyone interested in the interplay between gravity and thermodynamic principles in the universe.

kernelpenguin
Messages
45
Reaction score
0
The laws of thermodynamics (the second one, if I'm not mistaken) basically say that if matter is in clumps, it will become equally distributed over time and not the other way around.

But if we look into space, we see that matter was (probably) equally distributed in the beginning and has now condensed into clumps. (Known as planets, even.)

The thermodynamic model was originally made to model the behaviour of gases. It does not take into account gravity at all. (From what I can tell.)

Therefore, thermodynamics does not apply on the bigger scale as matter tends to collect into clumps, not become equally distributed.

This was the point argued by Ian Stewart, Jack Cohen and Terry Pratchett in The Science of Discworld II. (They've been wrong in that book before -- wouldn't surprise me if they were wrong again.)

So which is the case?

Oh and I've heard that black holes have a very high entropy. How is that possible? Or was this added just so that the laws of thermodynamics would hold?
 
Science news on Phys.org
kernelpenguin said:
The thermodynamic model was originally made to model the behaviour of gases. It does not take into account gravity at all. (From what I can tell.)

Therefore, thermodynamics does not apply on the bigger scale as matter tends to collect into clumps, not become equally distributed.


Why not?. You only have to make \rho to take variations in the space. Surely the thermodynamic field inside a star suffers of convection and diffusion phenomena. That effects are mirrored by thermodynamics equations, and the principal cause of such mass movements are the spatial density differences.
 
The way my physics lecturer explained it (I'm majoring in compsci so it wasn't a very technical explanation) was that the probability of having an even distribution of matter is higher than having it all gather into a clump or clumps.

For example, if you have 4 indistinguishable particles of gas in a two-part container, then the probability of finding the particles in different parts is higher than finding them both in the left part or both in the right part.

From that, it's supposed to follow that the universe is more likely smoother than clumpier as the probability of many particles gathering into the same place is very very small.

However, the above gas model does not take into account attractive forces and as such can't be applied to the universe at large. Or so the story went in The Science of Discworld.
 
This seems to have two sides:
1. The matter of the universe becomes one piece and clumps together.
2. The matter of the universe is evenly distributed out, so that for any particle, attractive forces from every side cancel out each other's effects.
Both seem reasonable, but personally I think the first is more probable.
 

Similar threads

  • · Replies 33 ·
2
Replies
33
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
596
  • · Replies 3 ·
Replies
3
Views
2K
Replies
19
Views
8K
  • · Replies 7 ·
Replies
7
Views
4K
Replies
1
Views
3K
  • · Replies 33 ·
2
Replies
33
Views
2K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 152 ·
6
Replies
152
Views
11K