Abstract
Amide solvent exchange rates are regarded as a valuable source of information on structure/dynamics of unfolded (disordered) proteins. Proton-based saturation transfer experiments, normally used to measure solvent exchange, are known to meet some serious difficulties. The problems mainly arise from the need to (1) manipulate water magnetization and (2) discriminate between multiple magnetization transfer pathways that occur within the proton pool. Some of these issues are specific to unfolded proteins. For example, the compensation scheme used to cancel the Overhauser effect in the popular CLEANEX experiment is not designed for use with unfolded proteins. In this report we describe an alternative experimental strategy, where amide 15N is used as a probe of solvent exchange. The experiment is performed in 50% H2O–50% D2O solvent and is based on the (HACACO)NH pulse sequence. The resulting spectral map is fully equivalent to the conventional HSQC. To fulfill its purpose, the experiment monitors the conversion of deuterated species, 15ND, into protonated species, 15NH, as effected by the solvent exchange. Conceptually, this experiment is similar to EXSY which prompted the name of 15NH/D-SOLEXSY (SOLvent EXchange SpectroscopY). Of note, our experimental scheme, which relies on nitrogen rather than proton to monitor solvent exchange, is free of the complications described above. The developed pulse sequence was used to measure solvent exchange rates in the chemically denatured state of the drkN SH3 domain. The results were found to correlate well with the CLEANEX-PM data, r = 0.97, thus providing a measure of validation for both techniques. When the experimentally measured exchange rates are converted into protection factors, most of the values fall in the range 0.5–2, consistent with random-coil behavior. However, elevated values, ca. 5, are obtained for residues R38 and A39, as well as the side-chain indole of W36. This is surprising, given that high protection factors imply hydrogen bonding or hydrophobic burial not expected to occur in a chemically denatured state of a protein. We, therefore, hypothesized that elevated protection factors are an artefact arising from the calculation of the reference (random-coil) exchange rates. To confirm this hypothesis, we prepared samples of several short peptides derived from the sequence of the drkN SH3 domain; these samples were used to directly measure the reference exchange rates. The revised protection factors obtained in this manner proved to be close to 1.0. These results also have implications for the more compact unfolded state of drkN SH3, which appears to be fully permeable to water as well, with no manifestations of hydrophobic burial.







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Generally speaking, our experiment can be described as an EXSY-style counterpart to the lineshape analyses by Hawkes et al. and spin echo experiments by Kateb et al., extending the observation window toward the slower exchange rates. At the same time, there is clearly a parallel with 15N zz-exchange experiment by Kay and co-workers (Farrow et al. 1994).
Our scheme is, therefore, well suited for measurements at or near physiological pH, but cannot be used with acid-denatured samples at pH ~2 where exchange rates are too slow.
The convergence of the fitting procedure generally presents no problem; for several residues it is recommendable to first fit the data with \( (0 , N_{z}^{D} (0)) \) initial conditions and then use the results as a starting point for the optimization involving \( (\varepsilon_{H} , N_{z}^{D} (0)) \).
In principle, such an experiment providing a full complement of two ‘axial peaks’ and two ‘cross-peaks’ can be designed using a HA(CACO)N-type sequence, although the detection of 1H resonances near the residual water line presents some practical difficulty.
There is another slowly exchanging residue, I27, which yields an exchange rate 0.34 ± 0.20 s−1 in our experiment, but cannot be detected in the CLEANEX spectra.
It can be pointed out that the e-PHOGSY scheme does not protect against the Overhauser transfer. This, however, is also true for CLEANEX outside the macromolecular limit. Given our successful validation of CLEANEX in this work, this does not appear to be a significant problem.
In addition, we have determined the protection factor for the W36 indole in the salt-stabilized F exch state, PF = 1.9. This result is in line with expectations since the tryptophan side chain is fully exposed to solvent in the folded protein. It is also consistent with the previous observations that W36 has the same (high) degree of solvent exposure in the F exch and U exch states (Evanics et al. 2006 Biochemistry 45:14120–1412). Note that in this study the exchange of W36 Hε1 proton with solvent, as quantified by e-PHOGSY, was mistakenly described as water NOE.
In applications involving unfolded proteins, the 1HN,15N spectral map generally offers better resolution than other 2D spectra. However, even in the case of small proteins, such as drkN SH3, there is a significant number of peak overlaps. In principle, this problem can be overcome with the help of reduced dimensionality schemes utilizing 13C′ and 13Cα chemical shifts (Brutscher et al. (1994) J. Magn. Reson. Ser. B 105:77–82; Tugarinov et al. (2004) J. Biomol. NMR 30:347–352).
Note that, in principle, heating effects can be compensated for (Wang and Bax 1993 J. Biomol. NMR 3:715–720).
Note that this constant refers to the deuterium-to-proton exchange catalyzed by \( {\text{OH}}^{-} \). In the context of our measurement, one is interested in deuterium-to-proton exchange catalyzed by both \( {\text{OH}}^{-} \) and \( {\text{OD}}^{-} \). The difference, however, appears to be subtle.
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Acknowledgments
We are thankful to Joseph Marsh for helpful discussions. The research has been funded through the NSF grants MCB-044563 and CHE-0723718 to N.R.S.
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Chevelkov, V., Xue, Y., Krishna Rao, D. et al. 15NH/D-SOLEXSY experiment for accurate measurement of amide solvent exchange rates: application to denatured drkN SH3. J Biomol NMR 46, 227–244 (2010). https://doi.org/10.1007/s10858-010-9398-8
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DOI: https://doi.org/10.1007/s10858-010-9398-8


