The Third Law of Thermodynamics

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The Third Law of Thermodynamics “If the entropy of every element in its stable state at T = 0 is taken as zero, every substance has a _______ entropy which at T = 0 may become zero, and does become zero for all perfect _______ substances, including compounds.” _______ Heat Theorem “The entropy change accompanying transformation between condensed phases in equilibrium, including chemical _______ , approaches zero as T  0. Practical consequence: Set S(0) = 0 for _______ by convention. Apply Nernst to determine S(0) for all else. “It is impossible to reach absolute zero in a _______ number of steps.” The 1st Law says U cannot be _______ or _______ . The 2nd Law says S cannot _______ . The 3rd Law says zero _______ cannot be reached. Modified by Jed Macosko 11/8/2018

The _______ Inequality Given and Substitute into the 1st Law: __________ Equation of Thermodynamics All _______ differentials, so path independent. But In general, i.e. any path  Pex dV P Clausius Inequality Equal for _______ change Even more generally, Conditions for: _________ equilibrium ____________ equilibrium Modified by Jed Macosko 11/8/2018

The Fundamental ______ of Thermodynamics Combine with Reversible change but true for all paths since dV exact  or This fundamental equation generates many more _________. Example 1: Comparison with  Example 2: Consider that dU is exact and cross __________. use this relation here which is a _______ relation Example 3: cyclic rule… …again… …and again! Modified by Jed Macosko 11/8/2018

How Entropy Depends on T and V  Compare with 0 for ideal gases For _____substance, assuming CV is T ___________ For _______ gases, (eqs 3.7.4, 6.1.6) Modified by Jed Macosko 11/8/2018

Entropy Depends on T and P (not in text) First problem: replace _____ ; second problem: replace _____. Use and both are solved!  But  Compare with 0 for ideal gases Modified by Jed Macosko 11/8/2018

Entropy Changes in __________ Processes Entropy is a __________ function, so DS(sys) = S2 – S1 __________ of path This can be used to calculate DS for an irreversible process. Consider isothermal expansion of a gas from V1 to V2: reversible and irreversible cases For the reversible case For the irreversible case e.g. for __________ expansion, w = 0  Consider freezing of __________ water at T < 273 K water, 0°C ice, 0°C reversible water, T ice, T irreversible rev. Modified by Jed Macosko 11/8/2018

Modified by Jed Macosko Entropy of __________ Consider the mixing of two ideal gases : P, T, V1 n1 P, T, V2 n2 P, ___ , V1+V2 n1+ ___ In general This expression applies to the arrangement of objects (__________ ) just as well as __________ (gases and liquids). For example, arrange N identical atoms in N sites in a crystal: Compare with the arrangement of two types of atoms, A and B. Application of ________ approximation: leads to do the math! Modified by Jed Macosko 11/8/2018

Using Entropy to Achieve Low T if CP is  constant To achieve lower temperatures, S must be reduced. Choose some property X that varies with S, i.e. S = f(X,T). This could be the pressure of a gas or, for example, the magnetic moment of a paramagnetic salt (whose energy varies with magnetic field). Alter X isothermally. Entropy changes. Restore X by a reversible adiabatic process. Repeat cycle. T S X1 T1 X2 curves coincide at 0 K, a consequence of the Nernst Heat Theorem Modified by Jed Macosko 11/8/2018