| L1 |
²¤¶Introduction
²Îp¤O¾Çªº¥ØªºPurpose of Stat Mech
¾÷²vProbability |
«ü©w#1½m²ßÃD¶°Problem set #1 out |
| L2 |
¾÷²v(Äò)Probability (cont.) |
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| L3 |
¥¿Åª¬ºAEquilibrium States |
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| L4 |
¥¿Åª¬ºAEquilibrium States
ÂX´²¤§´¹®æ¼Ò«¬Lattice Model for Diffusion
¾ó½¦¼u©Ê¾ÇRubber Elasticity
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¥æ#1½m²ßÃD¶°¸ÑµªProblem set #1 due
«ü©w#2½m²ßÃD¶°Problem set #2 out |
| L5 |
²¤¶¼ö¤O¾Ç¦u«í©w«ß(²Ä¤@©w«ß¡A¶q¤Æ»P²Ä¤G©w«ß)Introduction to Conservation Laws (1st Law, Quantization, 2nd Law) |
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| L6 |
¥~©µ©Ê½è¡Gªi¯÷°Ò©w«ß»Pæi(entropy)Boltzmann's Law and Entropy as an Extensive Property
æi¼W¥[ªº©w«ßLaw of Increased Entropy |
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| L7 |
ªi¯÷°Ò©w«ß»P¥~©µ©Ê½èæi(entropy)More Boltzmann's Law
¤À°t¨ç¼ÆPartition Functions |
¥æ#2½m²ßÃD¶°¸ÑµªProblem set #2 due |
| L8 |
¼ÒÀÀpºâSimulations
»E¦X»Ã¯ÀÃìÂê¤ÏÀ³PCR |
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| E1 |
ÀH°ó´úÅç¤@Quiz I |
«ü©w#3½m²ßÃD¶°Problem set #3 out |
| L9 |
¼ö¤O¾Ç¨t²ÎThermodynamic Systems
¤º§t»P¥~©µ©Ê½èIntensive/Extensive Properties
¯à¶q»Pæi(Entropy)ªº°ò¥»¤èµ{¦¡ Fundamental Equations for Energy and Entropy
¼ö¤O¾ÇÅX°Ê¤O¤§©w¸q(²Ä¤@³¡¤À)Definitions of Thermodynamic Driving Forces (Part 1)
¼ö¤O¾Ç§@¥Î¤OThermodynamic Forces
Homogeneous Functions
¥¿Å¡A·Å«×»PÀ£¤Oªº©w¸qDefinition of Equilibrium, Temperature, Pressure
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| L10 |
²¤¶¤Æ¾Ç¦ì¯àIntroduction to Chemical Potential
¼ö´`ÀôThermo Cycles
¼ö¡A¥\»P¯à¶q¤§¶¡Ãö«Yªº²Ä¤@©w«ßFirst Law Relations between Heat, Work, Energy
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| L11 |
¥i°f»P¤£¥i°fµ{§ÇReversible and Irreversible Processes |
¥æ#3½m²ßÃD¶°¸ÑµªProblem set #3 due
«ü©w#4½m²ßÃD¶°Problem set #4 out |
| L12 |
²¤¶¦Û¥Ñ¯àIntroduction to Free Energy
»®©i²ü¯÷¦Û¥Ñ¯àHelmholtz Free energy |
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| L13 |
ÖUEnthalpy
¦N¥¬´µ¦Û¥Ñ¯àGibbs Free Energy |
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| L14 |
°ò¥»¤èµ{¦¡»P¨ä¦ÛµMÅܼÆFundamental Equations and their Natural Variables
¼ö®eHeat Capacities
¥¿Å·Å«× Equilibrium Temperature |
¥æ#4½m²ßÃD¶°¸ÑµªProblem set #4 due
«ü©w#5½m²ßÃD¶°Problem set #5 out |
| L15 |
¼ö¤O¾Ç´`ÀôThermodynamic Cycles
¥dY´`Àô»P¤£µ¥©Ê½èCarnot Cycle and Inequality
¼ö¤ÞÀºHeat Engines
¸ô®|¬Û¨Ì©ÊPath Dependence |
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| L16 |
²öº¸°¾·L©Ê½èPartial Molar Properties |
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| L17 |
³¡²öº¸°¾·L©Ê½èIIPartial Molar Properties II |
¥æ#5½m²ßÃD¶°¸ÑµªProblem set #5 due |
| L18 |
¹q¸£¼ÒÀÀSimulations
»X¦a¥dùªkMonte Carlo |
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| E2 |
ÀH°ó´úÅç¤GQuiz II |
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| L19 |
ªi¯÷°Ò¤À¥¬©w«ßBoltzmann Distribution Law |
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| L20 |
¤À°t¨ç¼ÆPartition Functions |
L20½Òµ{«e¤¤Ñ«ü©w#6½m²ßÃD¶°Problem set #6 out 5 days before L20 |
| L21 |
±q¤À°t¨ç¼Æ¹w´ú¼ö¤O¾Ç©Ê½èPrediction of Thermodynamic Properties from Partition Functions
¨t¶°Ensembles |
¥æ#6½m²ßÃD¶°¸ÑµªProblem set #6 due
«ü©w#7½m²ßÃD¶°Problem set #7 out |
| L22 |
¶q¤l¤À°t¨ç¼ÆQuantum Partition Function |
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| L23 |
§¡¤Àì²zEquipartition |
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| L24 |
§¡¤Àì²z (Äò)Equipartition (cont.) |
¥æ#7½m²ßÃD¶°¸ÑµªProblem set #7 due
«ü©w#8½m²ßÃD¶°Problem set #8 out |
| L25 |
¤Æ¾Ç¥¿ÅChemical Equlibria
¦C¨F¯S°Çì²z (Ex. 8, ³J¥Õ½èªºÀ³¤OÅÜ©Ê)Le Chatelier's Principle (Ex. 8, Pressure Denaturation of Proteins)
¤Z¯S¦ó¤Ò(van¡¦t Hoff)ì²zvan't Hoff |
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| L26 |
©T-²G-®ð¥¿ÅSolid-liquid-gas Equilibrium |
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| L27 |
·»²G»P²V¦Xª«Solutions and Mixtures
°ª¤À¤lPolymers |
¥æ#8½m²ßÃD¶°¸ÑµªProblem set #8 due |
| L28 |
·»¸Ñ²{¶H:º¯³zÀ£Solvation: Osmotic Pressure
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L28½Òµ{«e2¤Ñ«ü©w#9½m²ßÃD¶°Problem set #9 out two days before L28 |
| L29 |
·»¸Ñ²{¶H:³J¥Õ½è/¥¨¤À¤l¦b¤¶±ªº§lªþ²{¶HSolvation: Protein/Macromolecule Adsorption at Interfaces |
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| L30 |
°ª¤À¤lÃìPolymer Chain |
¥æ#9½m²ßÃD¶°¸ÑµªProblem set #9 due |
| E3 |
ÀH°ó´úÅç¤TQuiz III |
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| L31 |
°ª¤À¤lÃì IIPolymer Chain II |
«ü©w#10½m²ßÃD¶°Problem set #10 out |
| L32 |
°ª¤À¤lÃì IIIPolymer Chain III |
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| L33 |
¨ó¦P©ÊCooperativity |
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| L34 |
¨ó¦P©Ê (Äò)Cooperativity (cont.) |
¥æ#10½m²ßÃD¶°¸ÑµªProblem set #10 due |
| L35 |
³J¥Õ½èºPÅ|²{¶HProtein Folding |
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| L36 |
¦^ÅUReview |
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