Is there any example of a real-life system which violates the “third law” of thermodynamics while remaining at equilibrium?
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I assume the following statement for the "third law" of thermodynamics:
limN→∞limT→0SN=0(1)(1)limN→∞limT→0SN=0
That is to say, I am considering those systems with a sub-exponential ground state degeneracy to satisfy the third law (see this answer of mine for more details about what I mean).
My question is: is there any real-life system that does not satisfy 11, while also remaining at equilibrium as T→0T→0?
Of course, there are examples of systems which don't satisfy 11, but all the examples I know concern non-equilibrium systems, like glasses (see residual entropy). For these system, however, no definition of entropy is in principle available, since SS can only be defined at equilibrium∗∗. Therefore, we cannot reallysay that they don't satisfy 11.
Note: I am not interested in model systems, but in real life systems, that can be studied experimentally.
limN→∞limT→0SN=0(1)(1)limN→∞limT→0SN=0
That is to say, I am considering those systems with a sub-exponential ground state degeneracy to satisfy the third law (see this answer of mine for more details about what I mean).
My question is: is there any real-life system that does not satisfy 11, while also remaining at equilibrium as T→0T→0?
Of course, there are examples of systems which don't satisfy 11, but all the examples I know concern non-equilibrium systems, like glasses (see residual entropy). For these system, however, no definition of entropy is in principle available, since SS can only be defined at equilibrium∗∗. Therefore, we cannot reallysay that they don't satisfy 11.
Note: I am not interested in model systems, but in real life systems, that can be studied experimentally.
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❥ Yes ; there are example of a real-life system which violates the “third law” of thermodynamics while remaining at equilibrium.
❥ At absolute zero the internal energy of the system would be zero since temperature is proportional to internal energy.
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❥ This law states that the entropy of a crystal of a pure substance reaches zero as the temperature reaches zero.
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