The measurement of anisotropic spin interactions, such as residual dipolar couplings, in partially ordered solutions can provide valuable information on biomolecular structure. While the information can be used to refine local structure, it can make a unique contribution in determining the relative orientation of remote parts of molecules, which are locally well structured, but poorly connected based on NOE data. Analysis of dipolar couplings in terms of Saupe order matrices provides a concise description of both orientation and motional properties of locally structured fragments in these cases. This paper demonstrates that by using singular value decomposition as a method for calculating the order matrices, principal frames and order parameters can be determined efficiently, even when a very limited set of experimental data is available. Analysis of 1H-15N dipolar couplings, measured in a two-domain fragment of the barley lectin protein, is used to illustrate the computational method.

The data most commonly available for the determination of macromolecular structures in solution are NOE based distance estimates and spin-spin coupling constant based dihedral angle estimates. This information is, unfortunately, inherently short-range in nature. Thus, for many multidomain proteins, little information is available to accurately position weakly interacting domains with respect to each other. Recent studies of proteins aligned in dilute liquid crystalline solvents have shown the utility of measuring anisotropic spin interactions, such as residual dipolar couplings, to obtain unique long-range structural information. In this work, the latter approach is taken to explore the relative domain orientation in a two-domain fragment from the protein barley lectin. An approach based on singular value decomposition as opposed to simulated annealing is used to directly determine order tensors for each domain from residual (15)N-(1)H dipolar couplings, and the limitations of the two approaches are discussed. Comparison of the order tensor principal axis frames as separately determined for each domain indicates that the two domains are not oriented as in the crystal structure of wheat germ agglutinin, a highly homologous protein ( approximately 95% sequence identical). Furthermore, differences in the order tensor values suggest that the two domains are not statically positioned but are experiencing different reorientational dynamics and, to a large degree, may be considered to reorient independently. Data are also presented that suggest that a specific association occurs between one domain and the lipid bicelles comprising the liquid crystal solvent.

Dissolving biological macromolecules in dilute bicelle solutions, which form oriented liquid crystals in the presence of a magnetic field, permits measurement of anisotropic spin interactions such as dipolar couplings [Tjandra, N. and Bax, A., Science, 278, 1111-1114]. However, the lifetimes and temperature ranges of orientation for these samples are critically dependent on sample composition and experimental conditions. This paper demonstrates that doping dilute bicelle solutions with small amounts of charged amphiphiles substantially improves the stability and degree of alignment, as well as extends the temperature range of orientation for these systems. An explanation of the dependence of bicelle aggregation on sample composition is proposed based on the DLVO theory of colloids.

The Bcl-2 family of proteins play a pivotal role in the regulation of programmed cell death. One of the postulated mechanisms for the function of these proteins involves the formation of ion channels in membranes. As a first step to structurally characterize these proteins in a membrane environment, we investigated the structure of a Bcl-x(L) mutant protein when incorporated into small detergent micelles. This form of Bcl-x(L) lacks the loop (residues 49-88) between helix 1 and helix 2 and the putative C-terminal transmembrane helix (residues 214-237). Below the critical micelle concentration (CMC), Bcl-x(L) binds detergents in the hydrophobic groove that binds to pro-apoptotic proteins. However, above the CMC, Bcl-x(L) undergoes a dramatic conformational change. Using NMR methods, we characterized the secondary structure of Bcl-x(L) in the micelle-bound form. Like Bcl-x(L) in aqueous solution, the structure of the protein when dissolved in dodecylphosphocholine (DPC) micelles consists of several alpha-helices separated by loops. However, the length and position of the individual helices of Bcl-x(L) in micelles differ from those in aqueous solution. The location of Bcl-x(L) within the micelle was examined from the analysis of protein-detergent NOEs and limited proteolysis. In addition, the mobility of the micelle-bound form of Bcl-x(L) was investigated from NMR relaxation measurements. On the basis of these studies, a model is proposed for the structure, dynamics, and location of Bcl-x(L) in micelles. In this model, Bcl-x(L) has a loosely packed, dynamic structure in micelles, with helices 1 and 6 and possibly helix 5 partially buried in the hydrophobic interior of the micelle. Other parts of the protein are located near the surface or on the outside of the micelle.