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Published byMarshall Conley Modified over 9 years ago
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PROTEIN PHYSICS LECTURE 5
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Energy: E (enthalpy: H=E+PV) PV=Nk B T for gases, PV << Nk B T for solids & liquids Entropy: S = k B ln(#STATES) If AB=A+B E AB = E A +E B ; V AB = V A +V B ; S AB = S A +S B while # AB = # A # B while # AB = # A # B Free energy: G = H-TS F = E-TS ------- ------- G: used when P=const for solids & liquids Chemical potential: G (1) = G/N Probability ~ exp(-G/k B T) max G min G min
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G = H-TS; dG = (dH-TdS) - SdT At T=const (i.e., at dT=0): at equilibrium, G = min, i.e., dH-TdS=0. Thus: 1) T = dH/dS 2) S = -dG/dT 3) H = G+TS = G-T(dG/dT) Probability ~ exp(-G/k B T) k B = 2cal/(6 10 23 ) = 2cal/mol = R k B 300 o = R 300 o = 0.6 kcal/mol
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int : “Free energy of interactions” int : “Free energy of interactions” Chemical potential: Chemical potential: G (1) = G int - Tk B ln(V (1) ) G int + Tk B ln[C] EQUILIBRIUM for transition of molecule 1 from A to B: G A (1) = G B (1) chemical potentials in A and B are equal chemical potentials in A and B are equal G int A B = G int B – G int A G int A B = k B Tln([C inA ]/[C inB ]) ===================================================
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Experiment: G int A B = k B T ln([C 1 in A ]/[C 1 in B ]) S int A B = -d( G int A B )/dT H int A B = G int A B +T S int A B C 6 H 12 [C] of C 6 H 12 in H 2 O: 50 times less than in gas; 100000 times less than in liquid C 6 H 12 T=298 0 K=25 0 C
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-2/3 +1/3 Loss: S (usual case) (usual case)-2/3Loss: LARGE E (rare case) (rare case) H-bond: directed
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High heat capacity d( H)/dT: Melting of “iceberg”
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20-25 cal/mol per Å 2 of accessible non-polar surface
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______largeeffect _______ small small______ large large
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