Helmholtz free energies of atom pair interactions in proteins

被引:84
作者
Sippl, MJ
Ortner, M
Jaritz, M
Lackner, P
Flockner, H
机构
[1] Center for Applied Molecular Engineering, Institute for Chemistry and Biochemistry, University of Salzburg, A-5020 Salzburg
来源
FOLDING & DESIGN | 1996年 / 1卷 / 04期
关键词
potential of mean force; protein folding; protein structure; radial distribution function; structure prediction;
D O I
10.1016/S1359-0278(96)00042-9
中图分类号
Q5 [生物化学]; Q7 [分子生物学];
学科分类号
071010 ; 081704 ;
摘要
Background: Proteins fold io unique three-dimensional structures, but how they achieve this transition and how they maintain their native folds is controversial, Information on the functional form of molecular interactions is required to address these issues, The basic building blocks are the free energies of atom pair interactions in dense protein solvent systems. In a dense medium, entropic effects often dominate over internal energies but free energy estimates are notoriously difficult to obtain, A prominent example is the peptide hydrogen bond (H-bond). It is still unclear to what extent H-bonds contribute to protein folding and stability of native structures. Results: Radial distribution functions of atom pair interactions are compiled from a database of known protein folds. The functions are transformed to Helmholtz free energies using a recipe from the statistical mechanics of dense interacting systems. In particular we concentrate on the features of the free energy functions of peptide H-bonds. Differences in Helmholtz free energies correspond to the reversible work required or gained when the distance between two particles is changed, Consequently, the functions directly display the energetic features of the respective thermodynamic process, such as H-bond formation or disruption. Conclusions: In the H-bond potential, a high barrier isolates a deep narrow minimum at H-bond contact from large distances, but the free energy difference between H-bond contact and large distances is close to zero. The energy barrier plays an intriguing role in H-bond formation and disruption: both processes require activation energy in the order of 2kT. H-bond formation opposes folding to compact states, but once formed, H-bonds act as molecular locks and a network of such bonds keeps polypeptide chains in a precise spatial configuration. On the other hand, peptide H-bonds do not contribute to the thermodynamic stability of native folds, because the energy balance of H-bond formation is close to zero. (C) Current Biology Ltd
引用
收藏
页码:289 / 298
页数:10
相关论文
共 25 条
[1]  
BALDWIN RL, 1993, OUTSTANDING PAPERS B, P1
[2]   PROTEIN DATA BANK - COMPUTER-BASED ARCHIVAL FILE FOR MACROMOLECULAR STRUCTURES [J].
BERNSTEIN, FC ;
KOETZLE, TF ;
WILLIAMS, GJB ;
MEYER, EF ;
BRICE, MD ;
RODGERS, JR ;
KENNARD, O ;
SHIMANOUCHI, T ;
TASUMI, M .
JOURNAL OF MOLECULAR BIOLOGY, 1977, 112 (03) :535-542
[3]  
BRAXENTHALER M, 1995, PROTEIN FOLDS, P80
[4]   STRUCTURE-DERIVED HYDROPHOBIC POTENTIAL - HYDROPHOBIC POTENTIAL DERIVED FROM X-RAY STRUCTURES OF GLOBULAR-PROTEINS IS ABLE TO IDENTIFY NATIVE FOLDS [J].
CASARI, G ;
SIPPL, MJ .
JOURNAL OF MOLECULAR BIOLOGY, 1992, 224 (03) :725-732
[5]  
FLOECKNER H, 1995, PROTEINS, V23, P376
[6]   The diffraction of x-rays by liquid elements [J].
Gingrich, NS .
REVIEWS OF MODERN PHYSICS, 1943, 15 (01) :0090-0110
[7]   IDENTIFICATION OF NATIVE PROTEIN FOLDS AMONGST A LARGE NUMBER OF INCORRECT MODELS - THE CALCULATION OF LOW-ENERGY CONFORMATIONS FROM POTENTIALS OF MEAN FORCE [J].
HENDLICH, M ;
LACKNER, P ;
WEITCKUS, S ;
FLOECKNER, H ;
FROSCHAUER, R ;
GOTTSBACHER, K ;
CASARI, G ;
SIPPL, MJ .
JOURNAL OF MOLECULAR BIOLOGY, 1990, 216 (01) :167-180
[8]   FREE-ENERGY BALANCE IN PROTEIN-FOLDING [J].
HONIG, B ;
YANG, AS .
ADVANCES IN PROTEIN CHEMISTRY, VOL 46: PROTEIN STABILITY, 1995, 46 :27-58
[9]   Adding backbone to protein folding: Why proteins are polypeptides [J].
Honig, B ;
Cohen, FE .
FOLDING & DESIGN, 1996, 1 (01) :R17-R20
[10]  
March N.H., 1991, Atomic Dynamics in Liquids