High-resolution phosphorus nuclear magnetic resonance spectra of yeast phenylalanine transfer ribonucleic acid. Melting curves and relaxation effects
In a continuation of our studies on structural effects on the 31P chemical shifts of nucleic acids, we present 31P NMR spectra of yeast phenylalanine tRNA in the presence and absence of Mg2+. Superconducting field (146 MHz) and 32-MHz 31P NMR spectra reveal approximately 15 nonhelical diester signal...
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Veröffentlicht in: | Biochemistry (Easton) 1979-08, Vol.18 (17), p.3796-3804 |
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Sprache: | eng |
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Zusammenfassung: | In a continuation of our studies on structural effects on the 31P chemical shifts of nucleic acids, we present 31P NMR spectra of yeast phenylalanine tRNA in the presence and absence of Mg2+. Superconducting field (146 MHz) and 32-MHz 31P NMR spectra reveal approximately 15 nonhelical diester signals spread over approximately 7 ppm besides the downfield terminal 3'-phosphate monoester. In the presence of 10 mM Mg2+, most scattered and main cluster signals do not shift between 22--66 degrees C, thus supporting our earlier hypothesis that 31P chemical shifts are sensitive to phosphate ester torsional and bond angles. At 70 degrees C, all of the signals merge into a single random coil conformation signal. Similar effects are observed in the absence of Mg2+ except that the transition melting temperature is approximately 20 degrees C lower. Measured spin-lattice and spin-spin relaxation times reveal another lower temperature transition besides the thermal denaturation process. A number of the scattered peaks are shifted (0.2--1.7 ppm) and broadened between 22 and 66 degrees C in the presence of Mg2+ as a result of this conformational transition between two intact tertiary structures. The loss of the scattered peaks in the absence of Mg2+ occurs in the temperature range expected for melting of a tertiary structure. An attempt to simulate the 31P spectra of tRNA Phe based upon the X-ray crystallographically determined phosphate ester torsional agles supports the suggestion that the large shifts in the scattered peaks are due to bond angle distortions in the tertiary structure. |
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ISSN: | 0006-2960 1520-4995 |
DOI: | 10.1021/bi00584a024 |