Formacetal-Modified Oligonucleotides
A R T I C L E S
concentrations were provided by Drs. Spink and Chaires. The slope
of the plot of reciprocal temperature (in K) of melting vs the
logarithm of water activity (lnaw) at different concentrations (0, 5,
10, 15, and 20%) of small cosolutes gave the value of d(Tm-1)/
d(lnaw). The final ∆nW were obtained by linear fitting using
KaleidaGraph software (Version 3.51) with a confidence level
usually better than 98%. The experimental uncertainties in the final
∆nW were calculated as previously described by us.13
Our studies also suggest that formacetal may be an interesting
modification to test in siRNAs, where the charge reduction may
help cellular uptake and biodistribution. However, the structural
consequences of extensive formacetal modification of RNA need
to be further investigated.
Experimental Section
Crystallization and Data Collection. Crystals of 5′-GCGT-
fAUMeACGC-3′ (UMe ) 2′-OMe-U) were grown by the hanging-
drop vapor diffusion technique using the Nucleic Acid Miniscreen
(Hampton Research, Aliso Viejo, CA).21 Droplets (2 µL) containing
oligonucleotide (0.6 mM), sodium cacodylate (20 mM, pH 6.0),
potassium chloride (40 mM), magnesium chloride (10 mM),
spermine tetrahydrochloride (6 mM), and 2-methyl-2,4-pentanediol
(MPD; 5% (v/v)) were equilibrated against a reservoir of MPD (1
mL, 35%). Crystals were mounted in nylon loops without further
cryo-protection and frozen in liquid nitrogen. Diffraction data were
collected on the undulator beamline X25 at the National Synchro-
tron Light Source (NSLS). Diffraction data were processed with
the program HKL2000.22 Selected crystal data and refinement
parameters are listed in Table 2.
Structure Refinement. The structure was determined by the
Molecular Replacement (MR) technique with the program MOL-
REP,23 using a single strand of an A-form DNA (PDB ID 411D)
as the search model. Initially the single strand was refined as an
all-DNA model and the refinement was carried out with the program
Refmac,24 randomly setting aside 8% of the reflections for
calculating the R-free.25 Water molecules were added into regions
of superimposed (2Fo - Fc) sum and (Fo - Fc) difference Fourier
electron density. The refinement was carried out in both space
groups P41 and P41212. However, refinement in the former space
group resulted in higher values for R-free and R-work (typically
around 3-4% difference), thereby indicating the higher symmetry
is correct. At a later stage refinement was continued and the
phosphorus and the two nonbridging oxygen atoms between the
T4 and A5 residues replaced by a carbon. The refinement of the
structure clearly reveals all the atoms of the formacetal linkage.
Data Deposition. Final coordinates and structure factors have
been deposited in the Protein Data Bank (http://www.rcsb.org): PDB
ID code 3HR3.
Synthesis of Formacetal Modified Oligonucleotides. Formac-
etal containing RNAs and DNAs were synthesized by following
and modifying the reported procedures.4,10 For details, see the
Supporting Information.
UV Thermal Melting and Osmotic Stress. Melting of each
oligonucleotide (2 µM) was done in 10 mM sodium cacodylate,
0.1 mM EDTA, and 300 mM NaCl in presence of 0, 5, 10, 15, and
20% weight/volume of each of the three osmolytes in Table 1.
Oligonucleotide concentration were calculated using extinction
coefficients obtained using the nearest-neighbor approximation.19
Absorbance vs temperature profiles were measured at 260 nm on
a Varian Bio 100 spectrometer equipped with a six-position Peltier
temperature controller. The temperature was increased at 0.5 °C
per minute. Five samples were measured concurrently in the double-
beam mode. At temperatures below 15 °C the sample compartment
was flushed with dry nitrogen gas.
The melting temperatures and thermodynamic parameters were
obtained using Varian Cary software (Version 02.00). The experi-
mental absorbance vs temperature curves were converted into a
fraction of strands remaining hybridized (R) vs temperature curves
by fitting the melting profile to a two-state transition model, with
linearly sloping lower and upper base lines. The melting temper-
atures (Tm) were obtained directly from the temperature at R )
0.5. The final Tm was an approximation of at least five to eight
measurements. The thermodynamic parameters were determined
using two different methods20 as described below:
(i) from the width at the half-height of differentiated melting
curve (Table 1, column 4). The fraction of strands remaining
hybridized (R) vs temperature curves were converted into dif-
ferentiated melting curves (δR/δ(Tm-1) vs Tm) using Varian Cary
software (Version 02.00). The width of the of the differentiated
melting curve at the half-height is inversely proportional to the van’t
Hoff transition enthalpy; for a bimolecular transition ∆H ) 10.14/
(T1-1-T2-1) where T1 is the lower temperature at one-half of (δR/
δ(Tm-1)) and T2 is the upper temperature at one-half of (δR/
δ(Tm-1)).20 The final -∆H is the average of at least 10 measurements.
Full experimental data are given in Supporting Information Tables
S2-S4 and in ref13 for OL1 and OL3.
(ii) from the van’t Hoff plot of ln K vs 1/Tm (Table 1, columns
6-7). For a bimolecular transition of self-complementary strands
the equilibrium constant K ) R/[2C(1 - R)2] where C is the total
strand concentration (C ) 2 × 10-6 M). The van’t Hoff plot (ln K
vs 1/Tm) is linear with -∆H/R as the slope and ∆S/R as the intercept
(R is the universal gas constant 1.986 cal/mol/K). All fitting and
calculation operations were done using Varian Cary software
(Version 02.00) using settings for a bimolecular transition of self-
complementary strands. The final -∆H and -∆S is the average of
at least 10 measurements. Full experimental data are given in
Supporting Information Tables S2-S4 and in ref13 for OL1 and
OL3.
Acknowledgment. We thank Binghamton University, NIH (R01
GM071461 to E.R. and R01 GM055237 to M.E.), and NSF-NATO
(fellowship DGE-0410935 to A.K.) for support of this research.
We also thank Dr. Annie He´roux for the X-ray data collection at
beamline X25 of the National Synchrotron Light Source (NSLS),
Brookhaven National Laboratory, New York. Financial support for
the beamline comes principally from the Offices of Biological and
Environmental Research and of Basic Energy Sciences of the US
Department of Energy, and from the National Center for Research
Resources of the National Institutes of Health.
Supporting Information Available: Experimental procedures,
details of thermal melting and osmotic stress experiments, and
copies of 1H and 13C NMR data. This material is available free
The changes in the number of water molecules associated with
the melting process ∆nW were determined as described previously
by Spink and Chaires14 and by us:13 ∆nW ) -∆H/R)[d(Tm-1)/
d(lnaw)], where -∆H is the enthalpy determined from the width at
the half-height of differentiated melting curve in pure buffer and R
is the universal gas constant (1.986 cal/mol/K). The experimentally
determined values of water activity (lnaw) at given cosolute
JA904926E
(21) Berger, I.; Kang, C. H.; Sinha, N.; Wolters, M.; Rich, A. Acta Cryst.
D 1996, 52, 465–468.
(22) Otwinowski, Z.; Minor, W. Methods Enzymol. 1997, 276, 307–326.
(23) Vagin, A. A.; Teplyakov, A. J. Appl. Crystallogr. 1997, 30, 1022–
1025. Collaborative Computational Project, Number 4, Acta Cryst. D
1994, 50, 760-763.
(24) Murshudov, G. N.; Vagin, A. A.; Dodson, E. J. Acta Cryst. D 1997,
53, 240–255.
(25) Bru¨nger, A. T. Nature 1992, 355, 472–475.
(19) Puglisi, J. D.; Tinoco, I., Jr. Methods Enzymol. 1989, 180, 304–324.
(20) Breslauer, K. J. Methods Enzymol. 1995, 259, 221–242.
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