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Mapping of spectral density functions using heteronuclear NMR relaxation measurements

dc.contributor.authorPeng, Jeffrey W.en_US
dc.contributor.authorWagner, Gerharden_US
dc.date.accessioned2006-04-10T15:25:34Z
dc.date.available2006-04-10T15:25:34Z
dc.date.issued1992-06-15en_US
dc.identifier.citationPeng, Jeffrey W., Wagner, Gerhard (1992/06/15)."Mapping of spectral density functions using heteronuclear NMR relaxation measurements." Journal of Magnetic Resonance (1969) 98(2): 308-332. <http://hdl.handle.net/2027.42/30338>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B7GXD-4CRG8NH-124/2/b50fdc7abd5997bb94e6f6bbe0def715en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/30338
dc.description.abstractA method is proposed for direct mapping of spectral density functions of the rotational motions of H-X bond vectors, such as 1H---15N, by measuring a set of NMR relaxation parameters. The well known and frequently measured relaxation parameters T1 and T2 probe the spectral density function J([omega]) at five frequencies: 0, [omega]N, [omega]H, [omega]H - [omega]N, and [omega]H + [omega]N. In this study, the longitudinal relaxation time T1(Nz), the transverse relaxation times of in-phase coherence, T2(Nx,y), and of antiphase coherence, T2(2HzNx,y), the relaxation time of longitudinal two-spin order, T1(2HzNz), and the heteronuclear cross-relaxation rate [sigma]HN are measured for the heteronucleus N. These five relaxation parameters sample the spectral density function J([omega]) at the same five points where each measurement samples a subset of these frequencies with different weights. The five measurements permit an analytical calculation of J([omega]) at these five frequencies. Since longitudinal proton relaxation plays a role in these relaxation parameters, a sixth measurement is necessary to determine this relaxation time. The theory and experimental techniques for measuring these relaxation parameters are discussed. Preliminary results of these techniques as applied to the 15N-enriched protein eglin c are described. The proposed approach has the advantage that it does not rely on any a priori model assumptions about the shape of J([omega]); i.e., measurement of J([omega]) and interpretation can be separated.en_US
dc.format.extent1731875 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleMapping of spectral density functions using heteronuclear NMR relaxation measurementsen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelElectrical Engineeringen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumBiophysics Research Division, University of Michigan, 2200 Bonisteel Boulevard, Ann Arbor, Michigan 48109, USA; Department of Biological Chemistry and Molecular Pharmacology, Harvard Medical School, 240 Longwood Avenue, Boston, Massachusetts 02115, USAen_US
dc.contributor.affiliationotherDepartment of Biological Chemistry and Molecular Pharmacology, Harvard Medical School, 240 Longwood Avenue, Boston, Massachusetts 02115, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/30338/1/0000740.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0022-2364(92)90135-Ten_US
dc.identifier.sourceJournal of Magnetic Resonanceen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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