Is Spontaneous Symmetry Breaking Truly Random?

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Discussion Overview

The discussion revolves around the concept of spontaneous symmetry breaking (SSB), particularly using the analogy of a pencil balanced on its tip. Participants explore the implications of symmetry and randomness in this context, questioning the nature of equilibrium and the factors that lead to symmetry breaking in various systems.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions whether the randomness of the pencil falling indicates that it was never truly symmetrical to begin with, expressing confusion about the concept of equilibrium.
  • Another participant suggests that the term "spontaneous" may depend on external factors, proposing that thermal motion could cause the pencil to tip over.
  • A different participant argues that internal forces in a system cannot change the position of its center of mass, implying that the pencil's fall is not influenced by temperature.
  • One participant challenges the idea that a slight imbalance in particle distribution would cause the pencil to fall without external forces, emphasizing the importance of the center of mass in determining equilibrium.
  • Another participant reiterates that the condition of equilibrium is based on the center of mass position, asserting that the pencil would not fall under ideal conditions without external influences.
  • One participant acknowledges that external thermal energy, such as from the air, could affect the pencil, but not the thermal energy of the pencil itself.
  • A participant introduces a broader perspective on SSB, indicating that it is a fundamental concept in physics that arises from unstable states, using the example of water convection patterns as a manifestation of symmetry breaking.
  • Another participant provides a reference to a philosophical encyclopedia to further explain the concept of SSB.

Areas of Agreement / Disagreement

Participants express differing views on the nature of symmetry breaking, the role of internal versus external forces, and the implications of equilibrium. There is no consensus on the interpretations of these concepts, and the discussion remains unresolved.

Contextual Notes

Participants highlight various assumptions regarding equilibrium, the influence of thermal motion, and the definitions of symmetry and stability, which may affect their arguments. These assumptions are not fully resolved within the discussion.

skywolf
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whats the deal with spontaneus symetry breaking?
i mean

the analogy they use is where a pencil is standing on its tip, and therefore symetrical, and then it falls in a random direction.

now, if it falls in a random direction, wouldn't it mean it wasnt symetrical to begin with?

i mean, as far as i am aware an object at rest tends to stay at rest.

so confused,
sw
 
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I would expect that it depends upon what is meant by 'spontaneous'. Something has to act upon it to upset the balance. In the case of a pencil on it's point, I figure that just the random thermal motion of its own molecules would be enough to tip it, even without air currents or surface vibrations. I'm not sure about that, though.
 
The internal forces of a system of particle (e.g. a pen) cannot change the position of its center of mass. So the moment a pen in unstable equilibrium falls is not a function of its temperature. :)
 
quasar987 said:
The internal forces of a system of particle (e.g. a pen) cannot change the position of its center of mass. So the moment a pen in unstable equilibrium falls is not a function of its temperature. :)

if for casuality, 49,999999% of particles would be in one side of the pencil, and 50,000001% in the other side, i don't see reasons why it should not fall without help of external forces.
 
Last edited:
The condition of equilibrium is not a matter of how many particles are on each side, but of the position of the center of mass (CM). The particles can take any position they want, as long as the line joining the CM and the tip of the pencil remain perpendicular to the surface.

To put the pencil in equilibrium, it was necessary that the CM be so located. Then we let go of the pencil and if all external forces and external torques are nul, the CM will remain there. For the proof of that theorem, grab any classical mechanics textbook.

In lights of this theorem, it is evident that the situation you suggest willl never happen, because the line joining the CM of this system with the tip of the pencil would not be perpendicular to the surface. Hence, the CM would have move since the moment the pencil was in equilibrium. This is impossible according to the theorem.
 
Of course, the thermal energy of the air may knock the pencil over... but not the thermal energy of the pencil itself
 
I think there's a misunderstanding here on the meaning of "spontaneous symmetry breaking (SSB)", and in what systems are these things manifested. I'm probably one of the last people to cite a "philosophy" encyclopedia to describe what SSB is, but this is actually a good description of it.

http://plato.stanford.edu/entries/symmetry-breaking/#4.2

And note that this is another example of something that came out of condensed matter physics and is now a fundamental part of all of physics.

Zz.
 
the matter of the pencil is an example, but the central point in symmetry breaking is that the state which has all the symmetry of the system in consideration is unstable, and therefore hardly observable, and will relax to something more stable which has but part of the original symmetry. In the pencil example, the standing over the type state is always unstable, but let us take ,for example, a recipient of water. if you ignore the boundaries, the surface is homogeneous, if you take any point in the surface, everything looks the same in any direction, provided you are far from the borders. it is rotational and translational invariant. Now, if you heat that below, there's a point where that uniform state becomes unstable, and convection starts to make patterns in the surface of the fluid, thus BREAKING the original symmetry. In a well controlled experiment, you could see that first patterns to form are hexagonal, which have as symmetry a subset of the original one
 

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