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So we know from the first law of thermodynamics:

$$ dU = dQ + dW $$

where $U$ is internal energy, $Q$ is heat and $W$ is work done. From Noether's theorem we also know that conservation of internal energy relates to time translational invariance

$$ dU = 0 \implies \text{Time Translational Invariance}$$

I haven't seen this done yet but what invariance does one gain when

$$dQ = 0 \implies ?$$

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I shall be providing a partial answer. We will restrict ourselves to the reversible case:

$$ Q = TdS$$

But, we also know from Gibbs entropy formula:

$$S = -k_B\sum_i p_i \ln p_i$$

Thus, $dS = 0$ implies,

$$ 0 = \sum_i (\ln p_i + 1 ) dp_i$$ Using $\sum_i p_i = 1$ $$ 0= \sum_i \ln p_i dp_i $$

Since $p_i \leq 1$ implies,

Either all the energy is in a particular energy state or there there is there is an invariance of thermodynamic probabilities.

Note: This derivation does not does apply in the irreversible case.