2020
DOI: 10.1007/s10858-020-00348-4
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A suite of 19F based relaxation dispersion experiments to assess biomolecular motions

Abstract: Proteins and nucleic acids are highly dynamic bio-molecules that can populate a variety of conformational states. NMR relaxation dispersion (RD) methods are uniquely suited to quantify the associated kinetic and thermodynamic parameters. Here, we present a consistent suite of 19F-based CPMG, on-resonance R1ρ and off-resonance R1ρ RD experiments. We validate these experiments by studying the unfolding transition of a 7.5 kDa cold shock protein. Furthermore we show that the 19F RD experiments are applicable to v… Show more

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Cited by 27 publications
(40 citation statements)
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“…The comparison of transverse relaxation at two different effective B 1 fields revealed the presence of motions occurring at the microsecond to millisecond timescales. It should be noted that the presence of many 1 H-19 F couplings within the FPro spin system implies that recently developed 19 F relaxation dispersion experiments cannot be applied (Overbeck et al, 2020). The dispersion of proton frequencies in the fluorinated prolines enable their selective excitation, a feature that was exploited for the selective Hγ -Fγ NOE and can be further used to develop sequences adapted to FPro spin systems.…”
Section: Discussionmentioning
confidence: 99%
“…The comparison of transverse relaxation at two different effective B 1 fields revealed the presence of motions occurring at the microsecond to millisecond timescales. It should be noted that the presence of many 1 H-19 F couplings within the FPro spin system implies that recently developed 19 F relaxation dispersion experiments cannot be applied (Overbeck et al, 2020). The dispersion of proton frequencies in the fluorinated prolines enable their selective excitation, a feature that was exploited for the selective Hγ -Fγ NOE and can be further used to develop sequences adapted to FPro spin systems.…”
Section: Discussionmentioning
confidence: 99%
“…The comparison of transverse relaxation at two different effective B 1 fields revealed the presence of motions occurring at the µs to ms time-scale. It should be noted that the presence of many 1 H-19 F couplings within the FPro spin system implies that recently developed 19 F relaxation dispersion experiments cannot be applied (Overbeck et al, 2020). The dispersion of proton 420 frequencies in the fluorinated prolines enable their selective excitation, a feature that was exploited for the selective Hγ-Fγ NOE and can be further used to develop sequences adapted to FPro spin systems.…”
Section: Discussionmentioning
confidence: 99%
“…The 2D 1 H, 15 N-SOFAST HMQC experiments 46 were recorded with acquisition times of 50.4 and 29.5 ms in the direct and indirect dimensions, respectively, and a recycle delay of 100 ms. The 19 F CEST measurements 36 47 were recorded using different spin-lock times with a spin-lock field of 7,500 Hz and the 19 F frequency carrier centred at −62.6 ppm (isolated) or −62.2 ppm (RNC).…”
Section: Methodsmentioning
confidence: 99%
“…2D 1 H, 15 N-SOFAST HMQC experiments 46 were recorded with acquisition times of 50.4 and 29.5 ms in the direct and indirect dimensions respectively, and a recycle delay of 100 ms. 19 F CEST measurements 36 were recorded with an acquisition time of 200 ms and a recycle delay of 30 ms, weak B 1 field of 15 Hz applied for a saturation time of 800 ms at saturation frequencies of either -40, -61.2 and -61.3 ppm, or -40, -62.2, -61.8 and -62.6 ppm. 19 F on-resonance R 1ρ measurements 47 were recorded using different spin-lock times with a spin-lock field of 7500 Hz, and the 19 F frequency carrier centred at -62.6 (isolated) or -62.2 ppm (RNC).…”
Section: Methodsmentioning
confidence: 99%