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Gibbs Free Energy Gibbs free energy is a measure of chemical energy All chemical systems tend naturally toward states of minimum Gibbs free energy G =

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Presentation on theme: "Gibbs Free Energy Gibbs free energy is a measure of chemical energy All chemical systems tend naturally toward states of minimum Gibbs free energy G ="— Presentation transcript:

1 Gibbs Free Energy Gibbs free energy is a measure of chemical energy All chemical systems tend naturally toward states of minimum Gibbs free energy G = H - TS Where: G = Gibbs Free Energy H = Enthalpy (heat content) T = Temperature in Kelvins S = Entropy (can think of as randomness)

2 Products and reactants are in equilibrium when their Gibbs free energies are equal A chemical reaction will proceed in the direction of lower Gibbs free energy (i.e.,  G r < 0) …so the reaction won’t proceed if the reaction produces an increase in Gibbs free energy Gibbs Free Energy

3  G° r =  nG° f (products) -  nG° f (reactants)  G° r > 0, backwards reaction with deficient energy  G° r < 0, forwards reaction with excess energy  G° r = 0, reaction is in equilibrium  G° r is a measure of the driving force

4 Thermodynamics For a phase we can determine V, T, P, etc., but not G or H We can only determine changes in G or H as we change some other parameters of the system Example: measure  H for a reaction by calorimetry - the heat given off or absorbed as a reaction proceeds Arbitrary reference state and assign an equally arbitrary value of H to it: Choose 298.15 K/25°C and 0.1 MPa/1 atm/1 bar (lab conditions)...and assign H = 0 for pure elements (in their natural state - gas, liquid, solid) at that reference

5 Thermodynamics In our calorimeter we can then determine  H for the reaction: Si (metal) + O 2 (gas) = SiO 2  H = -910,648 J/mol = molar enthalpy of formation of quartz (at 25°C, 1 atm) It serves quite well for a standard value of H for the phase Entropy has a more universal reference state: entropy of every substance = 0 at 0K, so we use that (and adjust for temperature) Then we can use G = H - TS to determine G for quartz = -856,288 J/mol

6 Thermodynamics K=equilibrium constant at standard T T in kelvin 298.18K R=gas constant=1.987 cal/mol o

7 Example: What is the  G o R of calcite dissociation? Use data in appendix B for  G o f  G o R = [(-132.3)+(-126.17)] - [(-269.9)] = +11.43 kcal (+) means that the reaction goes from right to left so K must be small What is the value of K? K = 10 (-11.43/1.364) = 10 -8.3798 = 4.171 x 10 -9 CaCO 3 Ca 2+ + CO 3 2-

8 What if T  25 o C? Use the Van’t Hoff Equation Enthalpy of reaction R=1.987 cal/mol° T in Kelvin  G° r =  H° r -T  S° r and lnK T - lnK T° = (-  H° r /R)(1/T-1/T°) We can derive:

9 Example: What is K T of calcite dissociation at T=38°C? = [(-129.74)+(-161.8)] - [(-288.46)] = -3.08 When T increases, K decreases ( K T° = 4.171 x 10 -9 )

10 Thermodynamics Summary thus far: –G is a measure of relative chemical stability for a phase –We can determine G for any phase by measuring H and S for the reaction creating the phase from the elements –We can then determine G at any T and P mathematically Most accurate if know how V and S vary with P and T –dV/dP is the coefficient of isothermal compressibility –dS/dT is the heat capacity (Cp) If we know G for various phases, we can determine which is most stable Why is melt more stable than solids at high T? Is diamond or graphite stable at 150 km depth? What will be the effect of increased P on melting?


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