 |
PDBsum entry 1q4c
|
|
|
|
 |
|
|
|
|
|
|
|
|
|
|
|
 |
|
|
|
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
 |
|
|
|
|
|
|
|
|
|
|
Luminescent protein
|
PDB id
|
|
|
|
1q4c
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
 |
Contents |
 |
|
|
|
|
|
|
|
|
|
* Residue conservation analysis
|
|
|
|
|
References listed in PDB file
|
 |
|
Key reference
|
 |
|
Title
|
 |
Local complexity of amino acid interactions in a protein core.
|
 |
|
Authors
|
 |
R.K.Jain,
R.Ranganathan.
|
 |
|
Ref.
|
 |
Proc Natl Acad Sci U S A, 2004,
101,
111-116.
[DOI no: ]
|
 |
|
PubMed id
|
 |
|
 |
 |
|
Abstract
|
 |
|
Atomic resolution structures of proteins indicate that the core is typically
well packed, suggesting a densely connected network of interactions between
amino acid residues. The combinatorial complexity of energetic interactions in
such a network could be enormous, a problem that limits our ability to relate
structure and function. Here, we report a case study of the complexity of amino
acid interactions in a localized region within the core of the GFP, a
particularly stable and tightly packed molecule. Mutations at three sites within
the chromophore-binding pocket display an overlapping pattern of conformational
change and are thermodynamically coupled, seemingly consistent with the dense
network model. However, crystallographic and energetic analyses of coupling
between mutations paint a different picture; pairs of mutations couple through
independent "hotspots" in the region of structural overlap. The data
indicate that, even in highly stable proteins, the core contains sufficient
plasticity in packing to uncouple high-order energetic interactions of residues,
a property that is likely general in proteins.
|
 |
 |
 |
|
 |
|
 |
Figure 1.
Fig. 1. Energetic characterization of the GFP
chromophore-binding pocket. (a) Stereoview of the binding pocket
viewed down the -barrel axis showing
sites included in the mutagenic scan. The
p-hydroxybenzylideneimidazolin-one chromophore is shown in
green. (b) Mutagenic scan of the chromophore environment
including the perturbation of pH shift from 8.5 to 5.5 ( pH). The
energetic effect of each mutation is measured as change in
chromophore absorbance maximum, a property that derives from
changes to the ground state structure of GFP (24). Mutation of
some sites has no significant energetic effect despite direct
interaction with the chromophore (H148C), whereas the largest
effect is seen for Q183, which only indirectly contacts the
chromophore. This and subsequent figures were prepared by using
GL-RENDER (L. Esser, personal communication), POVRAY (34), and
RASTER3D (35).
|
 |
Figure 4.
Fig. 4. Structure cycle analysis shows independent
interaction mechanisms for the two-way thermodynamic couplings.
Bar graphs (a and c) and colorimetric representations (b and d)
of the magnitude of structural coupling (  r[norm]) for each atom
in the T203C- pH (a and b) and
Y145C-T203C (c and d) cycles. The values report the degree to
which each atom feels the effect of one mutation differently
when in the background of another mutation and is the structural
analog of the double mutant cycle. Despite two-way thermodynamic
coupling (Fig. 3) and overlapping structural change (Fig. 2) of
the single mutants, the structural cycle analysis predicts that
T203C and pH interact through a
distinct mechanism from that of the T203C-Y145C pair.
|
 |
|
 |
 |
|
|
|
|
 |