Chemistry 163B Thermodynamics Winter 2013
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1 Chemistry 163B Thermodynamics Winter 013 Thermodynamics is a really beautiful scientific story!! 1 rules of science Observations (QM vs Thermo) observations Thermodynamics is very working class in its origins: guiding principles predictions and applications based on principles quantum mechanics Effete spectra H = E thermodynamics canons Blue Collar S universe > observations: thermo heat observations: mechanical efficiency of steam engine Count Rumford, 1799 observed water turning into steam when canon barrel was bored work heat Sadi Carnot, 184 efficiency of engines 5 6 1
2 guiding principles Applications U,H,S,G Conservation of heat and work (Joule, 1845) 1st LAW OF THERMODYNAMICS How does knowledge about efficiencies of steam engines, mechanical systems, etc, relate to processes in chemical, biological, and geological systems? Clausius, 1860 Entropy nd LAW OF THERMODYNAMICS ANSWERED BY: Boltzmann, late 19 th century, molecular picture of entropy Clausius the thermodynamic functions U, H, and S (1 st and nd laws) Boltzmann 7 J. W. Gibbs- arguably the frist great American scientist who combined the concepts of heat and entropy and proposed [Gibbs] Free Energy, G, a thermodynamic state function that leads to a whole spectrum of applications 8 from: Einstein s Autobiographical Notes types of problems that thermodynamics addresses (reactions) might 1. Under what conditions will a reaction occur? C (graphite) C (diamond) 30,000 00,000 atm 1000 K 3000 K 1 st artificially produced diamonds, 1954 at General Electric Labs 9 10 types of problems that thermodynamics addresses (equilibria) types of problems that thermodynamics addresses (biology). How far will a reaction proceed (given enough time)? How do the thermal and entropic properties determine EQUILIBRIUM? How do the EQUILIBRIUM conditions depend on T,P? N (g) + 3H (g) NH 3 (g) what are best T,P for NH 3 products? The Haber Process 3. Chemical and physical changes in biological systems [K + ] inside cell [K+] outside what difference in [K + ] out vs [K + ] in can be tolerated before cell wall bursts or collapses? SiO + CaCO 3 CaO SiO + CO (g) quartz calcite wollastonite geologic thermometer: The fraction of wollastonite in a rock sample can be used to estimate the temperature at which the rock metamorphosis occurred [the T at which the equilibrium was rapidly frozen] 11 low extracellular salt hypotonic (rupture) normal isotonic extracellular salt high hypertonic (collapse) 1
3 types of problems that thermodynamics addresses (biology) types of problems that thermodynamics addresses (ecology) 4. Why does an egg hard boil? (protein conformation) 5. Membrane potentials and ion concentrations in neurons. (electrochemistry and thermodynamics) 6. Thermodynamic feasibility of SO removal SO (g) S(s) + O (g) what thermodynamics can t answer aims of class 1. How fast a reaction proceeds (kinetics, catalysts, enzymes; in chem 103, BMB 100, chem 163C). Macroscopic thermodynamics does not prove or require hypotheses about molecular structure; however we will use our knowledge of molecular structure to get an atomic picture of thermodynamic processes. The quantitative connection is made by statistical thermodynamics: chem 163A chem 163B chem 163C 3. Although in chemistry 163B we will study how thermodynamics put limits on processes at equilibrium, there exists a whole other field of non-equilibrium thermodynamics. 1. Clear conceptual picture of thermodynamics. Ability to relate and apply thermodynamics to chemical and biological systems 3. PROBLEM SOLING: Chemistry + Logic + Mathematics 4. How to do independent and advanced reading/research in areas that utilize thermodynamics. 5. THE GRAND PICTURE of how thermodynamics and quantum mechanics fit into our picture of nature. 6. Advanced mathematical techniques class administration Learn Thermodynamics course pages Chemistry 163B lectures: A MUST homework: A MUST Lectures Sections (start TODAY Mon, Jan 7; HW#1 Probs 1-) Tutorial Event (starts NEXT Tues, Jan 15) Office hours (start TODAY Mon, Jan 7) LSS Tutor sections: required (A MUST) tutorial EENT & Office Hours & LSS (for YOU!) midterms: 1 st February 1 st March final: 0 th March, 4:00-7:00 PM (last class 18 th March)
4 Sections week of 7 th January ariables of state:, T, P (careful definitions) OLUME: MEASURED WITH A RULER TEMPERATURE: SEE IDEAL GAS THERMOMETER HANDOUT PRESSURE: FORCE/AREA EQUATION of STATE: RELATES P,, T (more later) 19 0 P lim 0 vs T handout and pp. 4-5 [sec 1.3] nd empirical TEMPERATURE: universal behavior of gas Tboiling RT boiling P T eq =boiling water at 1atm T eq =ice at 1atm P lim RTice 0 T ice 1 Choose R so that T boiling -T ice =100 1 [n.b. curves for various gasses are cartoons but actual data would converge to limit] P nrt P P RT n P P RT 1 Pressure, Kinetic Energy, and Temperature SEE HANDOUT P=nRT n=moles, R= gas constant P=n*kT n*=molecules, k=boltzmann's constant R k=, N=Avogadro's number N Fundamental and Defined Constants Engel & Reid [front cover, Table 1.1 (p8 ), Table 1. (p9 )] [7] [8] nd nd R= J mol K = L bar mol K = L atm mol K atm = 1 bar = 10 5 kg m s 10 5 Pa (pascal) L=1 dm =10 m 3 Game Plan Handout #6 [E&R pp -4] 3rd only of E=E(T) for ideal gas [U=U(T)] for monatomic ideal gas from P=n*kT and P=F/A use physics to relate pressure energy of gas 3 3 show E= n* kt (n* atoms gas) or E= nrt (n moles gas) and thus for monatomic ideal gas E depends only on T!!! [in thermodynamic notation E U (internal energy)] 3 4 4
5 1. molecules all with same v x (all same v x is heuristic ). elastic collision with wall mass velocity goes v x ö-v x 3. from physics F P= P=pressure A dp 4. from physics F= p=mv, momentum; t=time dt 5. dp º Dp = m v x per collision (m is mass of particle) total Dp in given time Dt, p dp t dt would depend on number of collisions in that interval, after some algebra and equating F n* kt P A n* 8. - is density of molecules, Av x Dt is volume of rectangular box, 1n* Av is number of molecules colliding with area A x t 9. total 1 n* n* p= mv Av t = mv A t x x x n* n* P= mv x = kt mv x =kt 1. in 3D with v x = v y = v z KE= mv x+ mv y+ mvz n* kt nrt 7 8 TAKE HOME MESSAGES Good warm up of physics and equation derivation For a molecule with only kinetic energy (e.g. monatomic species), and ideal gas (no intermolecular forces) 3 3 E= kt per molecule or E= RT per mole For monatomic ideal gas, E is function of only T; End of Lecture 1 T constant î E constant
6 various equations of state (Raff Table 1.) van der Waals equation a P brt 31 3 van der Waals equation The Haber Process (thermodynamics and kinetics)? size a P brt polarizability polarity Previously the problem had been that N is a very stable molecule, and so most attempts to convert it to less stable molecules, such as NH 3, failed because of thermodynamic or entropy problems. The secret to the Haber-Bosch process proved to be a catalyst of iron with a small amount of aluminium added (aluminium was at the time an exotic and expensive metal that probably attracted Haber's attention as a novelty). The Haber- Bosch process operates at high pressure so as to shift the equilibrium to the right, and high temperature to increase the rates of the reaction. Of course, operating at high temperature actually shifted the reaction to the left, but the trade-off for faster rates was accepted. By removing the ammonia as liquid ammonia, the equilibrium is continuously shifted to the right heuristic heu ris tic [hyoo-ris-tik or, often, yoo-] adjective 1. serving to indicate or point out; stimulating interest as a means of furthering investigation. 35 6
Chemistry 163B Thermodynamics Winter 2013
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