| Literature DB >> 24981969 |
Dmitry N Ivankov1, Alexei V Finkelstein2, Fyodor A Kondrashov3.
Abstract
The study of molecular evolution is important because it reveals how protein functions emerge and evolve. Recently, several types of studies indicated that substitutions in molecular evolution occur in a compensatory manner, whereby the occurrence of a substitution depends on the amino acid residues at other sites. However, a molecular or structural basis behind the compensation often remains obscure. Here, we review studies on the interface of structural biology and molecular evolution that revealed novel aspects of compensatory evolution. In many cases structural studies benefit from evolutionary data while structural data often add a functional dimension to the study of molecular evolution.Entities:
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Year: 2014 PMID: 24981969 PMCID: PMC4141909 DOI: 10.1016/j.sbi.2014.05.004
Source DB: PubMed Journal: Curr Opin Struct Biol ISSN: 0959-440X Impact factor: 6.809
Typical physical interactions stabilizing protein structures.a
| Type | Covalent/noncovalent | Occurrence | Abundance of interactions | Stabilizing free energy, kcal/M | Specificity | Comments |
|---|---|---|---|---|---|---|
| Van der Waals interactions | Noncovalent | All proteins | Numerous | For methyl | Nonspecific | Electrons oscillate around positively charged nucleus making atom an oscillating dipole. In two interacting atoms these oscillations are correlated and the atoms attract each other with energy proportional to |
| Hydrophobic interactions | Noncovalent | All proteins | Numerous | For methyl | Less specific | The origin is that water molecules are partly constrained to minimize their interaction with hydrophobic (non-polar) groups in order to save hydrogen bonds. |
| Hydrogen bonds | Noncovalent | All proteins | Moderate | In water: ∼−1.5 | More specific | Electrostatic interactions between directed H-containing dipoles (–O−–H+ or –N−–H+ groups) and partially negatively charged O− or N− atoms. |
| Interaction of charged with uncharged groups | Noncovalent | All proteins | Moderate | Unit charge interacting with methyl group | Less specific | Electrostatic repulsion of charged Lys+, Arg+, His+, Asp−, Glu− from weakly polarizable protein medium to more polarizable water, and attraction of these groups to weakly polarizable protein medium from non-polarizable vacuum |
| Salt bridges | Noncovalent | Most proteins | Few | At the protein/water interface: ∼−2 | Specific | Electrostatic interaction between positively charged Lys+, Arg+ or His+ and negatively charged Asp− or Glu−. |
| Coordinate bonds | Covalent | Metal-binding proteins | Very few | In water: ∼−6 and higher | Highly specific | One metal cation is coordinated by several (e.g. six) O and/or N atoms in the protein (or balanced by interacting H2O molecules in water). |
| Disulfide bonds | Covalent | Mostly secreted proteins | Very few | Inside the cell: ∼0 | Highly specific | Inside the cell a special enzyme and glutathiones make the formation of disulfide bonds reversible. Outside the cell disulfide bonds are fixed. |
Data were compiled from or calculated after [8,70–73]. Covalent bonds (except for coordinate bonds and disulfides) are not included since they are the same in the native and unfolded protein structure and are canceled out. The strength of residue–residue and atom–atom contacts depends on the defined distance cutoff between interacting atoms. Usually, for VdW, hydrophobic interactions and interactions between charged and uncharged atoms the cutoff is defined as ≈4–8 Å (e.g. see [45,74]), ≈5 Å for salt bridges, ≈4 Å for H-bonds, ≈2.5 Å for coordinate and disulfide bonds. For in-vacuum interactions the stabilizing effect is energetic in nature, while for the in-water interactions the stabilizing free energy (i.e. mean force potentials) is mainly connected with entropy. Water is considered implicitly, as a medium rather than as particles.
Van der Waals interactions are the London dispersion forces, present in both the folded and unfolded state of the protein. In the folded state many interactions are between amino acid residues (and with water molecules at the surface). In the unfolded state the interactions are mostly between amino acid residues and the surrounding water molecules.
Van der Waals interactions are ‘sometimes used loosely for the totality of nonspecific attractive or repulsive intermolecular forces’ [72].
For aromatic rings, the strength of interaction is approximately twofold larger.
The stabilizing effect in water is mostly entropic in nature [8], which means that when a protein is folded, the entropy of water molecules increases stabilizing the folded protein structure. At the same time the enthalpy of the ‘protein-water’ system remains relatively unchanged. The formation of disulfide bonds inside the cell is assisted by thiol-disulfide exchange, which increases entropy of glutathione molecules and preserves enthalpy of S–S bonds.
The free energy of hydrophobic interaction of nonpolar atoms with water was estimated as 45 cal/M for Å2 of the molecular surface (i.e. 20–25 cal/M for Å2 of the water-accessible surface area) [71]. An isolated methyl group (approximated by a sphere with a radius of ∼2 Å) can contact about twelve neighboring groups of the same dimensions and, thus, has about −0.3 kcal/M per contact as the cost of exclusion of water from the contact.
Figure 1Thermostability compensation in mammalian mitochondrial tRNAs. (a) The secondary structure of the human mt-tRNATrp with the known pathogenic mutations from Mitomap [68] shown in red. All instances when the disease mutation is found to be compensated in another species, as judged by a secondary structure-based alignment [69] are shown in orange. (b) An example of two direct WC compensations in the secondary structure of the Philippine tarsier mt-tRNATrp. (c) An example of an allosteric compensation in the anticodon stem of the sei whale mt-tRNATrp.