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Biochemistry

BioTutorial 253

Biochemistry

September 18, 2000

Lecture 9: Biochemical Energetics 1

Assigned reading in Campbell: Chapter 11.1-11.5.

Key Terms:
Spontaneous
Endergonic
Exergonic
Equilibrium constant (DG° = -RTln Keq)
Free energy (DG = DH - TDS)
Enthalpy (DH)
Entropy (DS)
dlnK/dT = DH/RT2
Conformational entropy (S = R ln W)
 

Take the Review Quiz on Lecture 9 concepts.


11.1 Energy and Change
We want to relate the measured equilibrium constants of spontaneous reactions to the thermodynamic features of those reactions.

11.2 The Criterion for Spontaneity

DG < 0   Spontaneous, exergonic.
DG = 0   Equilibrium.
DG > 0   Nonspontaneous, endergonic.
(typo in Campbell, here)

11.3 Standard States and the Standard Free Energy Change

Standard states are arbitrary, but are agreed upon to allow easy comparisons between experimental results. Chemists and biochemists have agreed to use these standard states:
Concentration: 1.0 M
Water: 1.0
Pressure: 1.0 atm
Free energy changes under these standard state conditions are designated as DG°.

Relationship between free energy (DG) and the equilibrium constant:

DG = DG° + RT ln [Products]/[Reactants]

At equilibrium, DG = 0, and
0 = DG° + RT ln [Products]/[Reactants]; therefore,
DG° = -RT ln [Products]/[Reactants]
Since these are equilibrium concentrations of products and reactants, we can write,
DG = DG° + RT ln Keq. Rewriting this equation, we have:

DG° = -RT ln Keq

Thus, Keq and DG° are both measures of how favorable a reaction will be.

Some frequently used numbers at 300K (27°C):
RT = 0.60 kcal/mol = 2.50 kJ/mol
RTln10 = 2.303log10 = 1.38 kcal/mol = 5.76 kJ/mol

11.4 A Modified Standard State for Biochemical Applications

To the list of standard conditions above, biochemists add another, namely:
[H+] = 10-7 M, i.e. pH 7.0.
The use of this standard state is indicated by DG°'.
If H+ is neither a reactant nor a product, DG°' = DG°.

See the example of ATP hydrolysis in Campbell, p. 398.
Consider another example:
  pKa Ka (M-1) DG° (kJ/mol) DG°' (kJ/mol)
Acetic acid 4.76 10-4.76 27.4 -12.9
Alanine 2.34 10-2.34 13.5 -26.8
Difference
{or ratio}
2.42
 
{102.42}
 
13.9
 
13.9
 

For the comparison between the acid dissociation constants (Ka) of acetic acid and alanine, we see that both DG° and DG°' give identical values (as they must). This comparison also leads to the question, Why does alanine lose its H+ at a much lower pH than does acetic acid?

  1. Qualitatively, the positively charged -NH3+ group, on the Ca of alanine facilitates proton dissociation from the adjacent carboxyl group.
  2. We can add to the above (correct) description by calculating how much the -NH3+ group facilitates carboxyl dissociation:
    1. The answer shown in the table is that dissociation from alanine is favored by 13.9 kJ/mol.
    2. You should convince yourself that the following simple expression applies to comparisons of pKa's:
      DDG = 2.303*RTDpKa

      where,
      DDG is the difference in DG between the two ionizations (acetic acid - alanine, above), and
      DpKa is the difference between the respective pKa values (second column, above).


11.5 Thermodynamics and Life

The free energy is also related to changes in the enthalpy (heat) and entropy (disorder) of the system:

DG = DH - TDS

  • DG, DH, DS refer to differences between the two states.
  • DG, DH, DS are thermodynamic values which depend only on the initial and final state
  • DH is the amount of heat generated/consumed by the reaction
  • DS is the change in entropy or disorder of the system
  • For a spontaneous reaction: DG<0
  • For a non-spontaneous reaction: DG>0

If DS = 0, then DG = DH, and all reactions that give off heat are spontaneous (DH<0 therefore DG<0).

If DH = 0, then DG = -TDS, and all reactions that increase entropy (DS>0) are spontaneous.

The entropy (DS) is related to the number of possible configurations (W) of the system:

S = R ln W

Consider the following simple example of vaporization of a gas. Two molecules of methane which are restricted to three of the nine possible compartments of a flask. The number of ways that the molecules can arrange themselves is (3*2)/2! =3. If the two molecules, in the vapor phase can occupy any of the nine cells then the number of possible arrangements are (9*8/2!)=36. The entropy difference between these two states is: DS=Sg-Sl=R (ln 36 ñ ln 3) = 4.92 cal/mol-deg. The total free energy available for this reaction is: DG=-TDS=1.5 kcal/mol at 300K.

The thermodynamics of methane transfer from an inert liquid to either the vapor phase or to liquid water has been measured:


First consider the process of going from the inert liquid (benzene) to the gas:
DG=-3.5 kcal/mol
DH= 0.5 kcal/mol
DS=+14 kcal/mol-deg
The reaction is favorable because of the large change in entropy. There is actually a loss of enthalpy because the methane molecules no longer interact in the gas phase.
Next consider the transfer of methane from an inert liquid to liquid water:
DG= +2.8 kcal/mol
DH= -3.2 kcal/mol
DS= -32.0 kcal/mol-deg
This reaction is unfavorable (hydrocarbons are hydrophobic). The large unfavorable entropy observed here is due to the ordering of water around the dissolved methane molecules. Since this restricts the possible positions of the water molecules the entropy of the system decreases. Note that the loss of free energy due to the entropic term is partially offset by a gain in enthalpy due to the newly created water-water hydrogen bonds. Thus the burial of hydrophobic amino acids during folding is favorable.

Temperature Dependence of the Equilibrium Constant:

The temperature dependence of the equilibrium constant can be obtained by equating our two equations for DG:


  • Exothermic Reaction (DH<0, reaction produces heat)
  • Endothermic Reaction (DH>0, reaction consumes heat)

The above is another example of Le Chatelier's principle. Note that the enthalpy of a reaction can be obtained from a plot of lnK versus 1/T.


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