The interaction cutoff contribution to the ruggedness of protein-protein energy landscape (the artificial ruggedness) is studied in terms of relative energy fluctuations for 1/r^n potentials based on a simplistic model of a protein complex. Contradicting the principle of minimal frustration, the artificial ruggedness exists for short cutoffs and gradually disappears with the cutoff increase. The critical values of the cutoff were calculated for each of eleven popular power-type potentials with n=0-9, 12 and for two thresholds of 5% and 10%. The artificial ruggedness decreases to tolerable thresholds for cutoffs longer than the critical ones. The results showed that for both thresholds the critical cutoff is a non-monotonic function of the potential power n. The functions reach the maximum at n=3-4 and then decrease with the increase of the potential power. The difference between two cutoffs for 5% and 10% artificial ruggedness becomes negligible for potentials decreasing faster than 1/r^12. The results suggest that cutoffs longer than critical ones can be recommended for protein-protein potentials.
Deep Dive into The ruggedness of protein-protein energy landscape and the cutoff for 1/r^n potentials.
The interaction cutoff contribution to the ruggedness of protein-protein energy landscape (the artificial ruggedness) is studied in terms of relative energy fluctuations for 1/r^n potentials based on a simplistic model of a protein complex. Contradicting the principle of minimal frustration, the artificial ruggedness exists for short cutoffs and gradually disappears with the cutoff increase. The critical values of the cutoff were calculated for each of eleven popular power-type potentials with n=0-9, 12 and for two thresholds of 5% and 10%. The artificial ruggedness decreases to tolerable thresholds for cutoffs longer than the critical ones. The results showed that for both thresholds the critical cutoff is a non-monotonic function of the potential power n. The functions reach the maximum at n=3-4 and then decrease with the increase of the potential power. The difference between two cutoffs for 5% and 10% artificial ruggedness becomes negligible for potentials decreasing faster than 1/
7/14/08
The ruggedness of protein-protein energy landscape and the
cutoff for 1/rn potentials
Anatoly M. Ruvinsky1 and Ilya A. Vakser2
1Anatoly M. Ruvinsky, Center for Bioinformatics, The University of Kansas, 2030 Becker
Drive, Lawrence, Kansas 66047; tel: (785) 864-1057, fax: (785) 864-5558, email:
ruvinsky@ku.edu
2Center for Bioinformatics and Department of Molecular Biosciences, The University of
Kansas, Lawrence, Kansas 66047; 2030 Becker Drive, Lawrence, Kansas 66047; tel:
(785) 864-1057, fax: (785) 864-5558, email: vakser@ku.edu
Keywords: docking, protein recognition, structure prediction, structural bioinformatics
ABSTRACT
The interaction cutoff contribution to the ruggedness of protein-protein energy
landscape (the artificial ruggedness) is studied in terms of relative energy fluctuations for
1/rn potentials based on a simplistic model of a protein complex. Contradicting the
principle of minimal frustration, the artificial ruggedness exists for short cutoffs and
gradually disappears with the cutoff increase. The critical values of the cutoff were
calculated for each of eleven popular power-type potentials with n=0÷9, 12 and for two
thresholds of 5% and 10%. The artificial ruggedness decreases to tolerable thresholds for
cutoffs longer than the critical ones. The results showed that for both thresholds the
critical cutoff is a non-monotonic function of the potential power n. The functions reach
the maximum at n=3÷4 and then decrease with the increase of the potential power. The
difference between two cutoffs for 5% and 10% artificial ruggedness becomes negligible
for potentials decreasing faster than1/
. The results suggest that cutoffs longer than
critical ones can be recommended for protein-protein potentials.
12
r
2
INTRODUCTION
Protein binding can be explained in terms of the funnel-based concept initially
developed to describe protein folding 1-10. The concept suggests that unbound proteins are
guided by the slope of the rugged energy landscape funnel into the bound state. The
nature of the ruggedness and related effects is a subject of active research 11-14. Highly
frustrated interactions are observed on the protein surface near the binding site 14.
Mechanical unfolding experiments to measure the scale of the landscape ruggedness of
proteins and RNAs have been suggested 15 and performed 16.
The amplitude of the of protein-protein energy landscape ruggedness has a
component associated with the range of the energy potentials 12. The range of non-bonded
inter-atomic interactions and related truncation methods are known to play an important
role in protein folding 17-22, protein-protein docking 4,12, and all atom molecular dynamics
and Monte-Carlo simulations of macromolecules and liquids 23-29. The cutoff is one of
only two parameters used in coarse-grained normal mode analysis and elastic networks of
proteins and their assemblies 30,31. The choice of the cutoff affects the functional form
and performance of knowledge-based potentials in small molecule docking 32. The
importance of long range interactions for protein stability 33, protein folding 34 and RNA
binding 35 has been revealed experimentally.
The interactions are usually truncated at specific cutoff distances to reduce a number
of interacting pairs of atoms or atomic groups in order to make feasible large scale
macromolecular calculations. Despite the considerable progress achieved in methodology
and computer power, the cutoff-related artifacts are still a bottleneck in macromolecular
modeling. In comparison with other modeling approaches, the protein docking
community has been less focused on the problem. Our attention to the cutoff problem is
3
motivated by observations that the choice of larger cutoffs results in the ruggedness
depression 12 and thus in smooth protein-protein energy landscapes 4,36, which according
with the principal of minimal frustration, 1,7,37 better approximate the actual binding
landscape. Similar effects of the energy landscape smoothing due to the cutoff extension
have been found in studies of liquids and atomic clusters 38-43, helix dimers 4,44,45 and
protein complexes 4,36,46.
We have recently demonstrated 12,47 that short cutoffs perturb protein-protein energy
landscape and thus lead to false minima, changed positions and altered shape of true
conformation-based minima. Such changes of the landscape impede the search for the
global minimum in protein docking 4 and introduce errors in calculations of binding free
energy 6,48-50. The false minima cause the artificial ruggedness of the energy landscape.
The fine structure of the funnel or conformational substates 51 can be blurred due to the
artificial ruggedness. The amplitude of the artificial ruggedness decreases with the
increase of the cutoff 12. Thus it is important to know the cutoffs for different potentials
that form a minimally frustrated funnel-like landscape, while al
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