Publication date: Available online 31 October 2014 Source:Journal of Magnetic Resonance
Author(s): Yang Zhou , Daiwen Yang
Chemical Exchange Saturation Transfer (CEST) experiments have emerged as a powerful tool for characterizing dynamics and sparse populated conformers of protein in slow exchanging systems. We show that J couplings and ‘invisible’ minor states can cause systematic errors in kinetics parameters and chemical shifts extracted from CEST data. For weakly coupled spin systems, the J coupling effect can be removed using an approximation method. This method is warranted through detailed theoretical derivation, supported by results from simulations and experiments on an acyl carrier protein domain. Simulations demonstrate that the effect of ‘invisible’ minor states on the extracted kinetics parameters depends on the chemical shifts, populations, exchange rates of the ‘invisible’ states to the observed major or minor state and exchange models. Moreover, the chemical shifts of the observed minor state can also be influenced by the “invisible” minor states. The presence of an off-pathway folding intermediate in the acyl carrier protein domain explains why the exchange rates obtained with a two-state model from individual residues that displayed only two obvious dips varied significantly and the extracted exchange rates for 15N and 13CO spins located in the same peptide bond could be very different. The approximation method described here simplifies CEST data analysis in many situations where the coupling effect cannot be ignored and decoupling techniques are not desirable. In addition, this study also raises alerts for ‘invisible’ minor states which can cause errors in not only kinetics parameters but also chemical shifts of the observed minor state. Graphical abstract
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From Mendeley Biomolecular NMR group:
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[NMRpipe Yahoo group] Re: Phasing 1H-15N HSQC Kinetics data from Bruker Instrument
Re: Phasing 1H-15N HSQC Kinetics data from Bruker Instrument
De. DeRose, Thank you for directing me to the "macro edit" pull down in NMRDraw. This, in addition to your comment regarding dwell times, has seemed to solve
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[NMRpipe Yahoo group] Re: Phasing 1H-15N HSQC Kinetics data from Bruker Instrument
Re: Phasing 1H-15N HSQC Kinetics data from Bruker Instrument
Hi Nicole, If the first data point in the indirect dimension started at half the dwell time, the phase correction in the indirect dimension should be -p0 -90
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