Download presentation
Presentation is loading. Please wait.
Published byAlexandrina Shaw Modified over 8 years ago
1
Thermodynamics Brown, LeMay Ch 19 AP Chemistry Monta Vista High School To properly view this presentation on the web, use the navigation arrows below and left-click on each page to view any animations.
2
2 Review 1 st Law of Thermodynamics In any process energy is neither created nor destroyed. When a system changes from one state to another ( E = q + w), it 1.Gains heat (+ q) or loses heat (- q) and/or 2.Does work (- w) or has work done on it (+ w) T and internal energy, E, are state functions (depend only on initial and final states of system and not path taken between them). q and w are not state functions. But why does a reaction occur in a particular direction?
3
3 Reversible reaction: can proceed forward and backward along same path (equilibrium is possible) Ex: H 2 O freezing & melting at 0ºC Irreversible reaction: cannot proceed forward and backward along same path Ex: ice melting at room temperature Spontaneous reaction: an irreversible reaction that occurs without outside intervention Ex: Gases expand to fill a container, ice melts at room temperature (even though endothermic), salts dissolve in water 19.1: Spontaneous Processes
4
4 19.2: Molecules & Probability Spontaneity of a reaction is related to the number of possible states a system can have. Ex: 2 gas molecules are placed in a two-chambered container, yielding 4 possible states: There is a ½ probability that one molecule will be in each chamber, and a ¼, or (1/2) 2, probability that both will be in the right-side chamber.
5
5 With 3 molecules: There is a ¾ probability that one molecule will be in one chamber and two in the other, and only a 1/8, or (1/2) 3, probability that all 3 molecules will be in the right-side chamber. All on left Evenly distributed All on right Frequency
6
6 All on left Evenly distributed All on right Frequency As the number of molecules increases to 100, a bell- shaped distribution of probable states, called a Gaussian distribution, is observed. # molecules = 100 Carl Gauss (1777-1855)
7
7 All on left Evenly distributed All on right Frequency # molecules = 10 23 Expanding this to 1 mole of molecules, there is only a (1/2) 10^23 probability that every molecule will be in the right-side chamber. The Gaussian distribution is so narrow that we often forget that it is a distribution at all, thinking of the most probable state as a necessity.
8
8 This demonstrates that: The most probable arrangements are those in which the molecules are evenly distributed. Processes in which the disorder of the system increases tend to occur spontaneously. spontaneousnon-spontaneous
9
9 These probability distributions apply to the motion and energy of molecules, and thus can predict the most probable flow of heat. We call a process spontaneous if it produces a more probable outcome, and non-spontaneous if it produces a less likely one. spontaneousnon-spontaneous high K.E. low K.E. evenly distributed K.E.
10
10 Entropy Entropy (S): a measure of molecular randomness or disorder S is a state function: S = S final - S initial + S = more randomness - S = less randomness For a reversible process that occurs at constant T: Units: J/K
11
11 2 nd Law of Thermodynamics The entropy of the universe increases in a spontaneous process and remains unchanged in a reversible (equilibrium) process. S is not conserved; it is either increasing or constant Reversible reaction: S UNIVERSE = S SYS + S SURR = 0 or S SYS = - S SURR Irreversible reaction: S UNIV = S SYS + S SURR > 0
12
12 Examples of spontaneous reactions: Gases expand to fill a container: Ice melts at room temperature: Salts dissolve in water: Particles are more evenly distributed Particles are no longer in an ordered crystal lattice Ions are not locked in crystal lattice
13
13 19.3: 3 rd Law of Thermodynamics The entropy of a crystalline solid at 0 K is 0. How to predict S: S gas > S liquid > S solid S more gas molecules > S fewer gas molecules S high T > S low T Ex: Predict the sign of S for the following: 1.CaCO 3 (s) → CaO (s) + CO 2 (g) 2.N 2 (g) + 3 H 2 (g) → 2 NH 3 (g) 3.N 2 (g) + O 2 (g) → 2 NO (g) +, solid to gas -, fewer moles produced ?
14
14 19.4: Standard Molar Entropy, Sº Standard state (º): 298 K and 1 atm Units = J/mol·K Hº f of all elements = 0 J/mol However, S° of all elements ≠ 0 J/mol·K See Appendix C for list of values. Where n and m are coefficients in the balanced chemical equation.
15
15 19.5: Gibbs free energy, G Represents combination of two forces that drive a reaction: H (enthalpy) and S (disorder) Units: kJ/mol G = H - T S G° = H° - T S° (absolute T) Called “free energy” because G represents maximum useful work that can be done by the system on its surroundings in a spontaneous reaction. (See p. 708 for more details.) Josiah Willard Gibbs (1839-1903)
16
16 Determining Spontaneity of a Reaction If G is: Negative (the free energy of system decreases) The reaction is spontaneous (proceeds in the forward direction) Positive Forward reaction is non-spontaneous; the reverse reaction is spontaneous ZeroThe system is at equilibrium
17
17 19.6: Free Energy & Temperature G depends on enthalpy, entropy, and temperature: G = H - T S H S G and reaction outcome -+Always (-); spontaneous at all T 2 O 3 (g) → 3 O 2 (g) +-Always +; non-spontaneous at all T 3 O 2 (g) → 2 O 3 (g) --Spontaneous at low T; non-spontaneous at high T H 2 O (l) → H 2 O (s) ++Spontaneous only at high T ; non-spontaneous at low T H 2 O (s) → H 2 O (l)
18
18 19.7: Free Energy & Equilibria The value of G determines where the system stands with respect to equilibrium. G = G° + RT ln Q where R = 8.314 J/Kmol or G° = - RT ln K eq or
19
19 19.7: Free Energy & Equilibria G ° Reaction outcome NegativeSpontaneous forward rxn, K > 1 PositiveNon-spontaneous forward rxn, K < 1 ZeroSystem is at equilibrium, K = 1
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.