ΔS = ΔQ / T
At very low temperatures, certain systems can exhibit a Bose-Einstein condensate, where a macroscopic fraction of particles occupies a single quantum state.
f(E) = 1 / (e^(E-μ)/kT - 1)
One of the most fundamental equations in thermodynamics is the ideal gas law, which relates the pressure, volume, and temperature of an ideal gas:
ΔS = nR ln(Vf / Vi)
The second law of thermodynamics states that the total entropy of a closed system always increases over time:
ΔS = ΔQ / T
At very low temperatures, certain systems can exhibit a Bose-Einstein condensate, where a macroscopic fraction of particles occupies a single quantum state. ΔS = ΔQ / T At very low
f(E) = 1 / (e^(E-μ)/kT - 1)
One of the most fundamental equations in thermodynamics is the ideal gas law, which relates the pressure, volume, and temperature of an ideal gas: which relates the pressure
ΔS = nR ln(Vf / Vi)
The second law of thermodynamics states that the total entropy of a closed system always increases over time: ΔS = ΔQ / T At very low
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