Protein Science (2001), 10:1260-1263.
Copyright © 2001 The Protein Society
FOR THE RECORD
Overcoming the problems associated with poor spectra quality of the protein kinase Byr2 using residual dipolar couplings
Wolfram Gronwald1,
Eike Brunner1,
Fritz Huber1,
Michael Wenzler1,
Christian Herrmann2 and
Hans Robert Kalbitzer1
1 Institut für Biophysik und physikalische Biochemie, Universität Regensburg, Postfach, D-93040 Regensburg, Federal Republic of Germany
2 Max-Planck-Institut für molekulare Physiologie, Otto-Hahn-Strasse 11, D-44227 Dortmund, Federal Republic of Germany
Reprint requests to: Professor Dr. Dr. Hans Robert Kalbitzer, Institut für Biophysik und Physikalische Biochemie, Universität Regensburg, Postfach, D-93040 Regensburg, Federal Republic of Germany; e-mail: Hans-Robert.Kalbitzer{at}biologie.uni-regensburg.de; fax: 49-941-943-2479.
(RECEIVED October 10, 2000;
FINAL REVISION March 8, 2001;
ACCEPTED March 9, 2001)
Article and publication are at www.proteinscience.org/cgi/doi/10.1110/ps.43201.
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Abstract
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For the Ras-binding domain of the protein kinase Byr2, only a limited number of NOE contacts could be initially assigned unambiguously, as the quality of the NOESY spectra was too poor. However, the use of residual 1H15N dipolar couplings in the beginning of the structure determination process allows to overcome this problem. We used a three-step recipe for this procedure. A previously unknown structure could be calculated reasonably well with only a limited number of unambiguously assigned NOE contacts.
Keywords: Byr2; residual dipolar couplings; structure calculation; NMR
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Introduction
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Small GTPases like Ras exhibit a central role in cellular signal transduction. A high percentage of human tumors are linked to mutations in the Ras gene (Barbacid 1987). In the GTP-bound form, Ras can interact with various effector molecules. It is, therefore, important to learn more about Ras/effector interactions. Known effectors are, for example, the serine/threonine kinase c-Raf1 and the Ral guanine-nucleotide exchange factors RalGDS, Rgl, and Rlf. An important step toward the understanding of the Ras/effector interactions is detailed knowledge about the structures of these molecules. Solution structures are known for the Ras-binding domains (RBDs) of c-Raf1 (Terada et al. 1999), Rgl (Kigawa et al. 1998), Rlf (Esser et al. 1998), and RalGDS (Geyer et al. 1997). The structure of the Ras-binding domain of the protein kinase Byr2 (Byr2-RBD) from Schizosaccharomyces pombe, a homolog to the Raf kinase of higher eukaryotes, is still unknown. Byr2-RBD was identified as a fragment of 116 residues in the amino-terminal part of the molecule and is only weakly related in primary sequence to other known effectors. A multiple sequence alignment of the Ras-binding domains of Byr2, Rgl, RalGDS, c-Raf1, and Rlf was performed using the program XALIGN (Wishart et al. 1994). For Byr2, the sequence identity with, for example, RalGDS and c-Raf1, amounts to only 15% and 14%, respectively.
One major obstacle in structure determination of the protein was the low stability, as well as the poor spectral quality caused by protein aggregation. To keep the protein in solution and stabilize the monomeric state, 200 mM of deuterated glycine was added to the protein solution. This, in turn, considerably increased the line width of the nuclear magnetic resonance (NMR) spectra to
17 Hz by increasing the viscosity of the solution. Further problems are related to the fact that
30% of the molecule is disordered. Despite the resulting signal overlap, almost complete resonance assignments could be obtained by heteronuclear methods (Huber et al. 2000). The quality of the NOESY spectra, however, did not allow to extract a sufficient number of unambiguous distance constraints to calculate a three-dimensional structure. On the other hand, Clore et al. (1999) have shown for proteins of known structure that the three-dimensional structure can still be determined by using residual dipolar couplings even if the majority of NOE contacts has been omitted. Here, we describe the use of residual dipolar couplings at a very early stage of structure determination of Byr2 when only a limited set of NOE contacts was available.
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Results and Discussion
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The preparation of Byr2 and sequential assignment of the NMR signals of Byr2 have been described elsewhere (Huber et al. 2000). Residual dipolar couplings are induced by the addition of phospholipid bicelles to the protein solution (Tjandra and Bax 1997). Solutions containing a bicelle-forming phospholipid mixture of dimyristoylphosphatidylcholine (DMPC) and dihexanoylphosphatidylcholine (DHPC) were prepared following the procedure described by Losonczi and Prestegard (1998) in 50 mM phosphate buffer at pH 6.2. The measurements were carried out at a total phospholipid concentration of 5 wt%. The presence and long-term stability of magnetically oriented bicelles were detected by 2H NMR spectroscopy (i.e., by the observation of the characteristic doublet splitting of the signal of 2H2O) (see, e.g., Ottiger and Bax 1998). One-bond 1H-15N residual dipolar couplings could be measured for 28 of the 116 amino acid residues by a heteronuclear single quantum coherence (HSQC) experiment without 1H decoupling during the 15N evolution period (t1). The above described overlap problems are responsible for the relatively small number of measured residual dipolar couplings. From the distribution function of the observed residual dipolar couplings one can estimate (Clore et al. 1998) the anisotropy of 15 Hz and the rhombicity of 0.3 of the molecular alignment tensor of Byr2. The following three-step "recipe" was used to overcome these problems (Fig. 1
). In the first step 61, 339, and 160 NOE contacts were identified from the homonuclear two-dimensional, heteronuclear three-dimensional 15N and 13C separated NOESY spectra, respectively. However, only 103 of them were long-range contacts and a considerable number of these were ambiguous. Because of the relatively low number of identified long-range contacts, 19 ambiguous contacts had to be included where one assignment seemed to be more likely than the other possibilities. Twelve hydrogen bond restraints were identified from an analysis of the slowly exchanging amide protons. Structure calculations were started with this relatively small number of distance restraints without using residual dipolar couplings. Because of the relatively small number of restraints, the resulting structures only showed the rough general fold of the molecule in which the orientation of the various secondary structure elements relative to each other was poorly defined. Therefore, on the basis of these structures it was impossible to unambiguously identify more NOE contacts or to verify the ambiguous NOE contacts. It is demonstrated in Figure 1
how the orientation of the secondary structure elements relative to each other changes during the three steps of structure calculation. As an example, the two
-helices of Byr2 (H1: residues 2232, H2: 5963) are shown. In step 1 the two helices are almost parallel (Fig. 1a,b
, step 1). In the second step, 28 residual dipolar couplings were included in addition to the distance restraints of step 1. The residual dipolar couplings were particularly helpful for defining the general arrangement of the various secondary structure elements (i.e., to determine their relative orientation). The axes of the two
-helices in Figure 1b
are now almost perpendicular relative to each other. However,
-helix H1 predicted by these calculations exhibits an unrealistic deformation (Fig. 1a,b
, step 2). The second turn is twisted by
180°. For each step of the structure determination process, the 10 structures of lowest total energy were superimposed and average rmsd values were calculated. To show the influence of the inclusion of residual dipolar couplings, Table 1
summarizes the results of steps 1 and 2 obtained with and without residual dipolar couplings, respectively. Identical sets of NOE contacts were used in steps 1 and 2. Note that the inclusion of residual dipolar couplings (step 2) only results in a small decrease of the rmsd value calculated for the C
atoms, whereas the other rmsd values remain constant or increase significantly. This behavior indicates the presence of misassigned NOE contacts. From the 19 ambiguous long-range contacts so far included into the structure calculations, 8 could be confirmed or unambiguously reassigned using the improved backbone structure (Fig. 1b
). The above-mentioned deformation of H1 was caused by the erroneous assignment of two of these ambiguous NOE contacts. Eleven contacts remained ambiguous and were excluded from the following structure calculations. In addition, using back-calculated NOESY spectra (Görler and Kalbitzer 1997) it was possible to identify 43 new unambiguous long-range contacts and two additional hydrogen bonds. In the third stage, new structures were calculated using the residual dipolar couplings and the improved set of distance restraints (Fig. 1a,b
, step 3). The rmsd value calculated for the C
atoms of the 10 best structures obtained in step 3 amounts to 3.52 Å. A generally accepted measure for the quality of a structure is the rmsd value. Comparing the rmsd values for the C
atoms of the selected structures for step 1 (5.47 Å), step 2 (5.17 Å), and step 3 (3.52 Å), it becomes clear that the quality of the obtained structures improves after the addition of the residual dipolar couplings and the correction of the ambiguous NOEs incorrectly assigned at the beginning. From the backbone structures obtained in step 3 (Fig. 1c
) it can be seen that Byr2 exhibits an ubiquitin-like fold similar to other Ras-binding domains (e.g., RalGDS).

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Fig. 1. Application of residual dipolar couplings for protein structure determination with a limited number of unambigously assignable NOEs. Strategy for residual dipolar coupling aided NOE cross-peak assignment and structure calculation (a). The structure and relative orientation of the two -helices H1 and H2 are displayed (b). The complete backbone of Byr2 is shown (c) in green, the helices H1 and H2 are colored in blue. One structure was selected from the ensemble obtained in step 3. For comparison, the backbone of human ubiquitin is shown in red (Cornilescu et al. 1998). Structures for Byr2 were obtained using the CNS 1.0 package (Brünger et al. 1998) and the standard dynamical annealing protocol delivered with CNS.
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Table 1. Comparison of rmsd values obtained for Byr2 structures calculated in step 1 and step 2 of the protocol described in Fig. 1
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Work is in progress to identify unambiguously more NOE contacts based on the structures of step 3 and to measure other residual dipolar couplings (1H13C, 13C15N, 13C
13C`) to obtain a highly resolved three-dimensional structure of Byr2.
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Acknowledgments
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This work was supported by the Deutsche Forschungsgemeinschaft and the Fonds der chemischen Industrie.
The publication costs of this article were defrayed in part by payment of page charges. This article must therefore be hereby marked "advertisement" in accordance with 18 USC section 1734 solely to indicate this fact.
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