60 Neuhaus and Evans studies of protein-ligand complexes, for example, one can focus on the ligand (see Chapter 7). Thus, one can study ligands by hetero- nuclear NMR methods if they are labeled or, in the case of metal ions, if they can be substituted by ions, such as ’ 13Cd2+t,h at can be studied directly by NMR. For example, in studies of metallothionein, it was possible to determine which residues coordinate the metal ion by detect- ing coupling of cysteinyl CPH protons to li3Cd2+ (47). Alternatively, it may be possible to study the conformation of the bound ligand when it is in equilibrium with the free form (which may be in excess, so that its spectrum is readily observed) by the detection of transferred NOES (48). It may also be possible to use labeled ligands to obtain structural information about the residues of the protein itself, to which they are bound. NOES can also be detected between nuclei of the ligand and of the protein, potentially providing a very powerful specific probe of the binding site; however, the success of such experiments has so far proven to be limited m practice, principally because they do not over- come the problem of assigning the protein resonances concerned. NMR also has considerable potential as a technique for studying nonnative states of proteins. This is of considerable importance in protein folding studies, and even though the information available may be rather limited, it is, in most cases, virtually the only residue- specific structural information obtainable and therefore very valuable. The problem with partially unfolded states is that they tend to give very poorly resolved spectra, so that direct assignment and structural interpretation are very difficult. However, it may be possible to use the well resolved native state spectrum to obtain mformation indirectly about the nonnative one (8,49). For example, chemical shifts of indi- vidual protons in the partially folded state may be determined by mag- netization transfer from the corresponding native stater esonancesw here the two forms are interconverting. Hydrogen bonded structure in the partially folded form may be detectable by means of the protection it offers against exchange of NHs for deuterons when the protein is dissolved in D20. The pattern of labeling in the partially folded form can be determined by allowing the protein to fold and determining the extent of proton occupancy at individual sites m the well resolved spectrum of the native form. This idea has now been extended to the characterization of transient structural intermediates on refolding pathways (50,51). Proteins in Solution 61 7. Practical Considerations The feasibility of undertaking a detailed structural study of a protein by NMR depends, in part, on the intrinsic properties of the protein, as discussed in Section 2. A full 3D structure determination generally requires a level of assignment and analysis that is only currently attain- able forrelatively small proteins. Thus, the NMR spectroscopist’s first question about a protein is always said to be “how big is it?” As we pointed out before, there are no hard and fast rules; as a guideline, we would suggest that if the mol wt is cl0 kDa, it is a possibility well worth considering, although only preliminary studies to gage the qual- ity of the spectrum can really tell. For proteins between 10 and 15 kDa, it may still be possible, but the undertaking becomes increasingly onerous. A few spectra of proteins of this size have been assigned using only homonuclear ‘HNMR, although in these cases, other tricks were generally used to obtain “edited” spectra in order to resolve problems of resonance overcrowding- for example, differential sol- vent exchange rates of amide protons in the case of lysozyme (13) and the variable oxidation state of the prosthetic group in the case of flavo- doxin (I 7). In the caseo f proteins much larger than approx 15 kDa, 13C or 15Nl abeling to permit heteronuclear studies will undoubtedly become necessary to permit much progress with assignment to be made. The alternative with these and still larger proteins is to settle for seeking more limited structural information, as discussed in Section 6. The other major limitation of NMR is its Insensitivity. Obtaining a 1- mit4 solution, the minimum desirable for ‘H NMR, requires 5 mg of protein to be dissolved in a OS-mL sample, in the case of a protein of 10 kDa. The overall requirement, both in terms of the amount of pro- tein needing to be purified and its solubility, could therefore in some casesb e excessive. It is also important to note that the protein must not only be soluble at this concentration, but it must also not aggregate appreciably; otherwise, the effective mol wt will of course be greatly increased, and the spectrum will correspondingly tend to be poorer. It may be necessary to experiment with a variety of solution conditions m order to optimize the spectral quality obtainable. In preparing a sample for NMR studies, several factors unique to this technique need to be borne in mind. In particular, the solvent conditions may have to be adjusted. NMR studies require that the 62 Neuhaus and Evans solvent water be at least 10% deuteratedt o permit the field frequency lock to function; for some studies, it may be desirablet o work in virtually 100% D,O. Thus, some form of buffer exchange is generally necessary.S ince NMR samples are typically more concentratedt han those used for other studies, this is usually associatedw ith a concentration step. The simplest method is to freeze-dry the protein, in the absenceo f added buffer salts, and then redissolve the product in a buffer appropriate to NMR work. Some proteins cannot be freeze-dried, however, and m that case, it may be necessary to use some form of concentrator that employs a semi- permeable membrane to effect buffer exchange and concentration. A particular problem with protein samples is the presence of small molecule signals that can interfere with the spectrum. The most obvi- ous of these is water. Since it is in general necessary to work in H,O rather than D20 solution, in order to observe all of the exchangeable NH signals, considerable effort has been put mto developing methods for suppressing the water peak in protein spectra. This may be achieved either by selective saturation of the water or selective excitation of the remainder of the spectrum (52). Whatever technique is applied, the key to successi s excellent field homogeneity, since line-shaped istortions can lead to poor suppression of parts of the peak, resulting m serious baseline distortions in the protein spectra obtained. It must be remem- bered that any solute molecule contaimng protons will also give rise to signals in the ‘H spectrum and, therefore, that it is desirable to remove such species as far as possible. This can usually be achieved by dialy- sis or gel filtration, but it can present more of a problem in relation to the buffer requirements of the particular protein. The simplest solution is to use an inorganic buffer, such as phosphate, whose only protons are in fast exchange with the water and can readily be preexchanged for deuterons if need be simply by freeze-drying from D20 solution; alternatively, several common buffer salts are available asp erdeuterated derivatives-simple compounds, such as (d,)-acetic acid are indeed quite cheap to obtain. If it is necessary to use a protonated buffer, its concentration should be kept to an absolute minimum. It is desirable, as with all experiments, to minimize contaminants of any kind, but certain types present particular hazards to NMR samples, and it may be necessary to take special steps to avoid them. Paramag- netic impurities can cause broadening and shifting of resonances in protein spectra, and need to be excluded if they are found to be present Proteins in Solution 63 in a protein sample. To remove trace metal ions, it may be sufficient to add a low concentration of EDTA or EGTA to the solution, but it is probably preferable to remove them altogether by dialysis against one of these agents or passing the protein through a column of a metal ion sequestering resin, Of course, the problem may need more careful consideration in the case of a metalloprotein! It should be noted that molecular oxygen is itself aparamagnetic impurity, and some workers remove dissolved oxygen from NMR samples by freeze-thaw meth- ods. However, the effects are rather marginal in practice, and since the process is time-consuming and may have deleterious effects on some proteins, it is not very common today. Optimum linewidths in NMR spectra depend on a number of fac- tors. One is the condition of the sample, which should be free of extrane- ous matter. This can usually be achieved by centrifugation prior to placing the sample in the NMR tube. Most important of all is the homogeneity of the magnetic field, which must be optimized by “shim- ming.” This may be a very tedious process (although increasingly it is possible to get the instrument to do it, at least in part, automatically), but is absolutely necessary. Some workers fmd that it is best to shim using a sample of a small molecule first, where resolution of very fine couplmgs provides a very stringent test of homogeneity-it should then only be necessary to make small final adjustments on introducing the protein sample. Another factor that is a key to the success of 2D experiments is stability; this is to some extent dependento n the quality and situation of the instrument, but care should also be taken by the experi- menter to ensure, for example, that the probe temperature is fully equili- brated before commencing acquisition. Running the experiment without spinning the sample also improves stability substantially, without degrad- mg the resolution noticeably, provided the shimming is adequate. The discussion presented here can serve only to provide a brief introduction to the study of protein structure by NMR. Today NMR is becoming an increasingly accessible technique, no longer solely the preserve of specialist spectroscopists. Nonetheless, it should be clear that an NMR study, particularly at the level of detailed assignment and structural analysis, is still a major undertaking requiring a considerable input of time, far beyond that requiredj ust to acquire the spectra, and that a degree of acquired expertise is necessary to obtain useful spectra and interpret them correctly. Protein NMR is still far from being a routme 64 Neuhaus and Evans technique, but the opportunities are constantly increasing to take advan- tages of the unique structural information that it can generate. References 1. Wilthrrch, K. (1986) NMR of Proterns and Nucleic Aczds. Wiley, New York 2 Wuthrrch, K (1989) Protein structure determmatron m solution by nuclear magnetic resonance spectroscopy. Scrence 243,45-50 3. Wdthrich, K. (1989) The development of nuclear magnettc resonance spec- troscopy as a technique for protein structure determmatton Accounts Chem Res 22,36-44 4 Clore, G M and Gronenborn, A. M. (1990) Determination of three-drmen- sional structures of proteins and nucleic acids m solutton by nuclear magnetic resonance spectroscopy CRC Cnt. Rev Biochem 24,419-564 5 Griffey, R H. and Redfield, A. G. (1987) Proton-detected heteronuclear edited and correlated nuclear magnetic resonance and nuclear Overhauser effect m solution. Q. Rev. Biophys 19,51-82 6 McIntosh, L. P. and Dahlqurst, F W. (1990) Biosynthettc mcorporation of 15N and t3C for assignment and interpretation of NMR spectra of proteins. Q. Rev Biophys 23, l-38. 7 Perkins, S. J. (1982) Applications of rmg current calculations to the proton NMR of proteins and nucleic acids, in Blologzcal Magnetic Resonance, vol 4 (Berliner, L. J. and Reuben, J., eds ), pp 193-336 8. Baum, J., Dobson, C. M., Evans, P. A., and Hanley, C. (1989) Characterlsation of a partly folded protein by NMR methods. Studies on the molten globule state of a-lactalbumm. Biochemistry 28, 7-13. 9. Smith, S. 0 and Griffin, R G (1988) High resolution solid state NMR of proteins. Annu Rev. Phys Chem. 39,511-536. 10. Tappin, M. J., Pastore, A., Norton, R. S., Freer, J. H., and Campbell, I D (1988) High resolution NMR study of the solution structure of b-hemolysin Blochemcstry 27, 1643-l 647 11 Braun, W , Wider, G , Lee, K. H., and Wuthrrch, K (1983) Conformation of glucagon in a lipid-water interphase by ‘H nuclear magnetic resonance. J Mol Biol. 169,921-948. 12 Neuhaus, D , Nakaseko, Y , Nagar, K , and Klug, A (1990) Sequence-specdtc [‘H]NMR resonance assignments and secondary structure identiftcation for I- and 2-zinc finger constructs from SWIS; a hydrophobic core mvolvmg four invariant residues. FEBS Lett 262, 179-l 84 13. Redfield, C. and Dobson, C M. (1988) Sequential assignments and secondary structure of hen egg-white lysozyme m solution Blochemlstry 27, 122-I 36 14 Wagman, M. E , Dobson, C. M , and Karplus, M (1980) Proton NMR studres of the association and folding of glucagon in solution FEBS Lett 119,265-270 15. Bogusky, M., Dobson, C. M., and Smith, R. A G (1989) Reverstble indepen- dent unfolding of the domains of urokinase monitored by proton NMR Blo- chemrstry 28,6728-6735. Proteins in Solution 65 16 LeMaster, D. (1990) Deutermm labeling m NMR structural analysts of larger proteins Q. Rev. Biophys 23, 133-174. 17 van Mterlo, C P. 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(1985) Compartson and evaluatton of methods for two-dlmensronal NMR spectra with absorption-mode lineshapes J Magn Reson 63,454-472. 23 Williamson, M P (1987) Guidelines for the design of kinetic NOE expert- ments from computer simulation Magn Reson Chem 25, 356-36 1 24. Borgras, B. A and James, T. L. (1989) Two-dimensional nuclear Overhauser effect. complete relaxation matrix analysis Methods Enzymol 176, 169-l 83 25 Otting, G. and Wuthrich, K (1990) Heteronuclear filters in 2D [ lH, lH] NMR spectroscopy Combmed use with tsotoprc labelling for studies of macromolecu- lar conformatton and intermolecular mteractrons. Q. Rev Blophys. 23,39-96. 26 Grresinger, C , Sorensen, 0 W , and Ernst, R R. (1989) Novel three-dimen- sional NMR techniques for studies of peptides and brologtcal macromolecules .I. Am. Chem Sot 109,7227-7228. 27 Englander, S W. and Wand, A J. (1987) Main-chain-directed strategy for the assignment of ‘H NMR spectra of proteins. Biochemistry 26,5953-5958 28 Hyberts, S. 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Methods Enzymol. 176,64-77 CHAPTER3 Peptide Structure Determination by NMR Michael I? Williamson 1. Introduction The difference between peptides and proteins (the subject of Chapter 2) is that peptides are molecules too small to have a “globu- lar” structure. This means that the spectral assignment process is often much simpler for peptides than it is for proteins, because there are fewer signals present m peptide spectra; on the other hand, peptides seldom adopt a single, well defined structure in solution, which makes the interpretation of structural data more contentious for peptides than it is for proteins. The emphasis in this chapter is therefore different from that in Chapter 2. The acquisition of structurally relevant data is straightforward, given a familiarity with modern two-dimensional (2D) NMR techniques and is given less emphasis here, but the analysis of the data is seen as the key to obtaining a meaningful answer, and is the area where experience and expertise are most necessary. The difficulty in dealing with flexible structures by NMR derives from the fact that intramolecular motion (i.e., rotation about single bonds) causes most NMR parameters, such as NOE, coupling con- stant, and chemical shift, to be averaged, rather than giving a superpo- sition of values, as IS seen in many other branches of spectroscopy. This has a number of consequences. First, it is not at all obvious from inspection of a spectrum whether one conformation or many confor- From Methods m Molecular Biology, Vol 17 Spectroscop/c Methods and Analyses NMR, Mass Spectrometry, and Metalloprotem Techmques Edited by C Jones, B Mulloy, and A H Thomas CopyrIght 01993 Humana Press Inc , Totowa, NJ 69
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