In defense of my original answer:
Quote:
Symmetry in physics
In mathematics, the language of physics, symmetry has a more precise meaning. Livio defines it as an immunity to change. “Namely you do a certain operation and something does not change, you call that a symmetry,” he told LiveScience.
This definition takes into account bilateral symmetry but it also includes other symmetries as well:
* Time translation symmetry: Physical laws do not change with time.
* Translational symmetry: The laws of physics are the same whether they are acting in our solar system or at the far end of the universe.
* Rotational symmetry: The laws of physics don’t change if we turn around.
These symmetries are crucial for understanding science, especially physics. If the laws of nature were not symmetrical, there would be no hope of ever discovering them. In a universe where the natural laws were not symmetrical, experimental results might change depending on where and when and in what direction an experiment was performed.
Here’s an example of the importance of all this: One way astronomers are able to determine the material composition of stars that are millions of light-years away is to examine the chemical signatures encoded in the light they emit. In order for the astronomer’s conclusions to be of any value, the atoms in those stars must obey the same laws that govern our corner of the universe.
Symmetry is so integral to the way the universe works that Albert Einstein used it as a guiding principle when he devised his General Theory of Relativity.
Einstein firmly believed that the laws of physics should be the same for all observers, regardless of how they were moving. Through various thought experiments, Einstein discovered another fundamental symmetry in nature, called general covariance. Under this symmetry, physical laws act the same regardless of whether an object is accelerating or at rest. In other words, the force of gravity and the force resulting from acceleration are two facets of the same force—that is, they are symmetrical.
Scientists have glimpsed other symmetries in nature as well.
A positron, for example, can be thought of as a mirror image of an electron. And James Clerk Maxwell, a 19th century mathematical physicist, demonstrated symmetry between electric and magnetic fields. Through a series of equations, Maxwell demonstrated that electricity and magnetism are actually two complementary aspects of a more fundamental force, called electromagnetism.
Many scientists suspect that there may be more natural symmetries waiting to be discovered. Some think that the so-far elusive “Theory of Everything,” which physicists have spent decades searching for, will contain some type of universal symmetry that fully explains and knits all the known laws of physics together.
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