Roger Penrose - Before the Big Bang

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Discussion Overview

The discussion centers around Roger Penrose's Weyl Curvature Hypothesis and its implications for the state of entropy at the beginning of the universe. Participants explore the relationship between thermal equilibrium, homogeneity, and entropy in the early universe, as well as the concept of gravitational entropy.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants express confusion regarding Penrose's assertion that entropy was low or zero at the beginning of the universe, despite evidence of thermal equilibrium and homogeneity suggesting high entropy.
  • One participant suggests that constraining the Weyl curvature to a specific value may imply a special state of low entropy, even in a thermal state.
  • Another participant notes that Penrose posits gravitational entropy is low for uniformly distributed matter and high for clumped matter, referencing established views on entropy increase due to clumping.
  • There is a challenge to the idea that clumping increases entropy, with one participant asserting that this is standard knowledge in the field.
  • Penrose's view is further elaborated, indicating that he associates gravitational entropy with the Weyl curvature tensor and suggests a complex relationship between thermodynamic entropy and gravitational changes during cosmic transitions.

Areas of Agreement / Disagreement

Participants express differing interpretations of Penrose's claims regarding entropy, with some agreeing on the standard view that clumping increases entropy while others challenge this notion based on Penrose's framework. The discussion remains unresolved regarding the implications of the Weyl Curvature Hypothesis on entropy.

Contextual Notes

Participants reference various interpretations of gravitational entropy and the implications of the Weyl curvature, indicating a need for clarity on definitions and assumptions related to entropy in cosmological contexts.

Sumo
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http://www.youtube.com/watch?v=fJ-D5AUGVcI&hl=de"
http://www.youtube.com/watch?v=inzgHjEVxAc&feature=channel"
http://www.youtube.com/watch?v=WD3BWt85bxA&feature=channel"
http://www.youtube.com/watch?v=YXDSCEX5wE8&feature=channel"
http://www.youtube.com/watch?v=YX30dxKdJkc&NR=1"
http://www.youtube.com/watch?v=aNS_8WTYVuM&NR=1"
http://www.youtube.com/watch?v=6mV6WnA52wQ&NR=1"
http://www.youtube.com/watch?v=LXYLLG7VkoI&NR=1"
http://www.youtube.com/watch?v=br1zHYH2hvA&NR=1"

This is an interesting video lecture by Roger Penrose talking about his Weyl Curvature Hypothesis. I found most of it fairly easy to understand. Maybe if someone can explain to me one thing: He talks about how entropy at the beginning of the universe was low or zero. But he also says (I think) that the background radiation shows thermal equilibrium, and that the early universe was almost perfectly homogeneous. Doesn't this mean that entropy was high?
 
Last edited by a moderator:
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Sumo said:
http://www.youtube.com/watch?v=fJ-D5AUGVcI&hl=de"
http://www.youtube.com/watch?v=inzgHjEVxAc&feature=channel"
http://www.youtube.com/watch?v=WD3BWt85bxA&feature=channel"
http://www.youtube.com/watch?v=YXDSCEX5wE8&feature=channel"
http://www.youtube.com/watch?v=YX30dxKdJkc&NR=1"
http://www.youtube.com/watch?v=aNS_8WTYVuM&NR=1"
http://www.youtube.com/watch?v=6mV6WnA52wQ&NR=1"
http://www.youtube.com/watch?v=LXYLLG7VkoI&NR=1"
http://www.youtube.com/watch?v=br1zHYH2hvA&NR=1"

This is an interesting video lecture by Roger Penrose talking about his Weyl Curvature Hypothesis. I found most of it fairly easy to understand. Maybe if someone can explain to me one thing: He talks about how entropy at the beginning of the universe was low or zero. But he also says (I think) that the background radiation shows thermal equilibrium, and that the early universe was almost perfectly homogeneous. Doesn't this mean that entropy was high?

I think the idea is that because one constrains the weyl cuvature to some value(zero?) this means that despite the universe being in a thermal state it still is in a very special state so the entropy is low. But it does seem confusing.
 
Last edited by a moderator:
Finbar said:
I think the idea is that because one constrains the weyl cuvature to some value(zero?) this means that despite the universe being in a thermal state it still is in a very special state so the entropy is low. But it does seem confusing.

Penrose thinks that gravitational entropy is low for uniformly distributed matter and high for clumped matter. See

https://www.physicsforums.com/showthread.php?p=1800223#post1800223
https://www.physicsforums.com/showthread.php?p=1577616#post1577616.
 
Maybe I'm confused.. Who disagrees with that? That clumping increases entropy has been standard lore and textbook for a long time now. In the cases we can actually calculate in, that's always been the case.
 
Haelfix said:
That clumping increases entropy has been standard lore and textbook for a long time now.
Penrose goes further than just that. He identifies the relevant degrees of freedom for gravitational entropy as the Weyl curvature tensor. As pointed out in the thread linked above by George, with a cyclic model for the Universe, he needs the entropy to be constant basically. So if I understand anything to his claim, the entropy flows to the gravitational field, and it takes an enormous change in thermodynamical entropy to make up a small change in the Weyl curvature so you get a very long process to transfer in this direction, while according to him when the Universe becomes conformal and undergoes a transition to the "next big bang", it takes literally no time since there is no reference for any kind of clock.
 
met a man from cambridge today, live in kansas city.
 

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