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Fourier transform infrared spectroscopy for the characterization of a model peptide–DNA interaction

✍ Scribed by S. B. Dev; Lee Walters


Publisher
Wiley (John Wiley & Sons)
Year
1990
Tongue
English
Weight
819 KB
Volume
29
Category
Article
ISSN
0006-3525

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✦ Synopsis


To better understand the structural basis of protein-DNA interactions, the conformational changes that accompany these interactions need to be described. In order to develop a methodological approach to this problem, Fourier transform infrared spectroscopy (FTIR) with derivative resolution enhancement has been used to identify conformational changes that occur when a 29-residue synthetic peptide binds nonspecifically to heterogeneous cellular DNA in aqueous solution. The peptide sequence w a s chosen de novo, m order to rationally design a peptide model that would allow the relationship between DNA!binding and the stability of protein secondary structure to be studied. Peptide a t a concentration of 100-200 pM produces 50% saturation of heterogeneous phage DNA sequences as well as of short synthetic oligonucleotides. mIII spectra reveal significant changes in peptide and DKA upon binding. Second-derivative spectra resolve the amide I band of native peptide into components located a t 1627 (&strand), 1658 (a-helix), and 1681 (turn or /%strand) cm-', with a distinct shoulder a t 1647 cm ' (disordered structure). Assignment of the 1681 cm-' vibration to a turn conformation iS supported by uv CD studies, which indicate significant amounts of turn structure in unbound peptide. Ultraviolet CD also confirms the existence of disordered and B-strand regions in the free peptide. IJpon interacting with DNA the band at 1681 cm ' (turn) is no longer seen; a new band appears at 1675 cm-'; the 1627 cm-' band (&strand) is considerably reduced in intensity; the position of the a-helical (1658 cm-') component remains unchanged; the shoulder at 1647 cm-. ' (disorder) disappears. The new vibration at 1675 cm ' is characteristic of 8-strand structures. The asymmetric stretch ( V ,,~) . of the IINA phasphates shifts from 1223 (unbound) to 1229 c m -' (bound); the relative intensities of v-and the PO; symmetric stretch ( u s ) are altertd upon peptide binding. The data is consistent with the following conclusions: (a) DNA binding changes the secondary structure of the peptide, (b) disordered region(s) are only observed in free peptide, i.e.. DNA binding stabilizes and increases order in the peptide secondary structure, (c) turn@) change into B-strand and/or a-helical conformation(s) when peptide binds to DNA, (d) a 8-strand conformation that is characterized by a 1627 cm-' vibration is present in free and bound peptide, (e) there is a particular B-strand vibration/conformation that is only present in the bound peptide, ( f ) an a-helical region exists in both free and bound peptide, (g) DNA remains in a R-family conformation upon peptide bindmg, and (h) DNA phosphates participate in peptide binding and/or subtle changes occur in the DNA conformation upon complex formation.


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