Bioenergetics and high-energy compounds Tomáš Kučera
[email protected] Department of Medical Chemistry and Clinical Biochemistry 2nd Faculty of Medicine, Charles University in Prague and Motol University Hospital 2017 Bioenergetics how organisms gain, convert, store and utilize energy Gibbs free energy G = H − TS ) ∆G = ∆H − T∆S = Qp − T∆S G decrease in a biological process represents its maximum recoverable work. equilibrium: ∆G = 0 spontaneous (exergonic) process: ∆G < 0 (it can do work) endergonic process: ∆G > 0 Gibbs free energy one of the thermodynamic potentials no information on the rate – it is given by the mechanism (im-)possibility of a process given only by the initial and final states a catalyst (enzyme) can accelerate equilibrium aainment, not change its state ) possibility of coupling = ∆H depends on temperature: equilibrium: T ∆S ∆H ∆S ∆G = ∆H − T∆S − + Both enthalpically favored (exothermic) and entropically favored. Spontaneous (exergonic) at all temperatures. − − Enthalpically favored but entropically opposed. Sponta- = ∆H neous only at temperatures below T ∆S . + + Enthalpically opposed (endothermic) but entropically fa- = ∆H vored. Spontaneous only at temperatures above T ∆S . + − Both enthalpically and entropically opposed. Unspontaneous (endergonic) at all temperatures. Rewrien from Voet, D., Voet, J. G.: Biochemistry, John Wiley & Sons, Inc., 2011 (4th edition) Chemical equilibria Reaction a A + b B c C + d D [C]c[D]d ∆G =∆ G0 + RT ln [A]a[B]b (∆G0 = standard G change of the reaction) constant term —