Department of Chemistry, Indiana UniVersity Bloomington, Indiana 47405 ReceiVed March 3, 1997 Interest in producing gas-phase nucleic acid ions1a-g has been stimulated by recent mass spectrometry (MS) based sequencing strategies for biomolecules.2a-h Recently mass spectra for plasmid and linear DNAs having molecular weights of 106108 daltons have been recorded.3a-c In contrast to the wealth of structural data for nucleic acids in solution, there is no information about conformations of the gas-phase ions. The conformations of protein ions can influence fragment formation;4 thus, the issue of conformation is important for sequencing nucleic acids by MS. Here, we report the first study of the conformations of a deprotonated DNA oligomer in the gas phase: oligothymidine comprised of ten thymine nucleotides. Using electrospray ionization5 and ion mobility techniques,6 we have measured collision cross sections for the -2 to -6 states, (T10-nH), where n is the deprotonation state, and deprotonated states of oligothymidine with sodium ions attached (NaT10nH)(n-1)-, where n ) 5-7. A sharp structural transition is observed when four or more protons are removed; lower charge states favor compact globular conformers and higher ones favor elongated forms. Addition of a single sodium ion to deprotonated states stabilizes more compact conformers. Conformations that were derived using molecular modeling techniques provide complementary information that allows many important structural features to be delineated. Our experimental apparatus and procedures have been described previously.6 Negatively-charged (deprotonated) oligothymidine ions were formed by electrospraying a ∼3 × 10-5 M oligothymidine7 solution in 49.9:49.9:0.2 water:acetonitrile: ammonium hydroxide. Sodium adducts are readily formed, although no sodium was added. Ions were extracted into a highvacuum region and 30 microsecond pulses were injected into a drift tube containing ∼3.0 Torr of helium in order to record ion mobility distributions. The drift times depend on the ions’ conformations; compact conformers drift through faster than extended forms. Ions that exit the drift tube are focussed into a quadrupole mass spectrometer that transmits only the ion of interest. As ions enter the drift tube they are heated by collisions with the buffer gas. Further collisions cool the ions to the buffer gas temperature. Ion mobility distributions at varying injection energies (∼150-450 eV) yield identical drift times; thus, we expect these data correspond to relatively stable conformations. Figure 1 shows charge normalized ion mobility distributions for the -2 to -6 charge states of (T10-nH). Each distribution shows a single peak. The -2 and -3 states have similar normalized drift times, ∼5.2 ms, suggesting similar conformations. A shift to 6.2 ms is observed for the -4 charge state. The -5 and -6 ions have drift times of 7.2 and 7.4 ms, respectively. These ions favor more open conformations. Ion mobility distributions for oligothymidine ions containing sodium, (NaT10-5H), (NaT10-6H), and (NaT10-7H), are also shown in Figure 1. The average drift time of (NaT10-7H) is similar to that for (T10-6H). The (NaT10-5H) and (NaT106H)5ions have higher mobilities than the pure DNA ions of the same charge. Binding sodium leads to more compact conformations of these high charge states. Drift times can be converted into experimental collision cross sections as described previously6 and are shown in Figure 2. Additional insight was gained by comparing calculated cross sections for an array of conformers generated by molecular modeling techniques to the experimental data.8 Trial conformers were obtained using the Insight II molecular modeling software with the CVFF forcefield.9 The forcefield used a dielectric constant of 1.0 for the surrounding media; thus, these are in Vacuo conformations. For each charge state, 100 different trial conformers were generated by simulated annealing. The temperature was increased to 1000 K over 2 ps, equilibrated for 2 ps, and then cooled over 1 ps to 300 K. The structures obtained were energy minimized, and the atomic coordinates of conformations that fell within 30 kcal/mol of the lowest energy model conformer were used to calculate average cross (1) (a) Hunt, D. F.; Hignite, C. E.; Biemann, K. Biochem. Biophys. Res. Commun. 1968, 33, 378. (b) McNeal, C. J.; Ogilvie, K. K.; Theriault, N. Y.; Nemer, M. J. J. Am. Chem. Soc. 1982, 104, 976. (c) Grotjahn, L.; Frank, R.; Blocker, H. Nucleic Acids Res. 1982, 10, 4671. (d) Cerney, R. L.; Gross M. L.; Grotjahn, L. C. Anal. Biochem. 1986, 156, 424. (e) Covey, T. R.; Bonner, R. F.; Shushan, B. I.; Henion, J. D. Rapid Commun. Mass Spectrom. 1988, 2, 249. (f) Hillenkamp, F.; Karas, M.; Ingendoh, A.; Stahal, B. In Biological Mass Spectrometry; Burlingame, A. L., McCloskey, J. A., Eds.; Elsevier: Amsterdam, 1990. (g) Spengler, B.; Pan, Y.; Cotter, R. Rapid Commun. Mass Spectrom. 1990, 4, 99. (2) (a) Crain, P. F. Mass Spectrom. ReV. 1990, 9, 505. (b) McLuckey, S. A.; Van Berkel, G. J.; Glish, G. L. J. Am. Soc. Mass Spectrom. 1992, 3, 60. (c) McLuckey, S. A.; Habibi-Goudzrzi, S. J. Am. Chem. Soc. 1993 115, 12085. (d) Little, D. P.; Speir, J. P.; Senko, M. W.; O’Connor, P. B.; McLafferty, F. W. Anal. Chem. 1994, 66, 2809. (e) Little, D. P.; Chorush, R. A.; Speir, J. P.; Senko, M. W.; Kelleher, N. L.; McLafferty, F. W. J. Am. Chem. Soc. 1994, 116, 4893. (f) Little, D. P.; McLafferty, F. W. J. Am. Chem. Soc. 1995, 117, 6783. (g) Christian, N. P.; Colby, S. M.; Giver, L.; Houston, C. T.; Arnold, R. J.; Ellington, A. D.; Reilly, J. P. Rapid Commun. Mass Spectrom. 1995, 9, 1061. (h) Ni, J.; Pomerantz, S. C.; Rozenski, J.; Zhang, Y.; McCloskey, J. A. Anal. Chem. 1996, 68, 1989. (3) (a) Fuerstenau, S. D.; Benner, W. H. Rapid Commun. Mass Spectrom. 1995, 9, 1528. (b) Chen, R.; Cheng, X.; Mitchell, D. W.; Hofstadler, S. A.; Wu, Q.; Rockwood, A. S.; Sherman, M. G.; Smith, R. D. Anal. Chem. 1995, 67, 1159. (c) Cheng, X.; Camp II, D. G.; Wu, Q.; Bakhtiarl, R.; Springer, D. L.; Morris, B. J.; Bruce, J. E.; Anderson, G. A.; Edmonds, C. G.; Smith, R. D. Nucleic Acids Res. 1996, 24, 2183. (4) Loo, J. A.; Edmonds, C. G.; Smith, R. D. Science 1990, 248, 201. (5) Fenn, J. B.; Mann, M.; Meng, C. K.; Wong, S. F.; Whitehous, C. M. Science 1989, 246, 64. (6) For a recent review, see: Clemmer, D. E.; Jarrold, M. F. J. Mass. Spectrom. 1997, 32, 577 and references therein. (7) Oligothymidine used was synthesized using an Applied Biosystems 391 DNA synthesizer utilizing the phosphoramidite method. The ions studied here are dephosphorylated at the 5′ end. (8) This approach is similar to a method discussed by Wyttenbach, T.; von Helden, G.; Bowers, M. T. J. Am. Chem. Soc. 1996, 118, 8355. (9) Insight II; BIOSYM/MSI: San Diego, CA, 1995. Figure 1. Ion mobility distributions for deprotonated (T10-nH) (solid lines) and (NaT10-nH) (dotted lines) ions formed by electrospray ionization. The distributions are shown on a modified time scale t*z which normalizes for differences in effective drift fields. 9051 J. Am. Chem. Soc. 1997, 119, 9051-9052