O. D. Schꢁrer, C. Simmerling et al.
duplex, no significant amounts of the slower migrating spe-
cies were observed, further demonstrating the specificity of
ICL formation (Figure 1, lanes 1 and 5).
twist[11] of the two crosslinked base pairs (Table S1 and Fig-
ure S2 for sequence, in the Supporting Information). Since
molecular mechanics force fields have limited accuracy, it is
more important to note the trends rather than the specific
values. It is well accepted that differences are more reliable
in simulations than absolute values, due to cancellation of
systematic error. The crosslinked guanine 16 that neighbors
the large purine ring of adenine (residue 17) accommodates
the crosslink by buckling of the 7:16 base pair (C: À3.5Æ
0.28, 1: À13.2Æ0.18, and 2: À21.8Æ0.68). The crosslinked
guanine 5 that neighbors the small pyrimidine ring of thy-
mine 6 has more room to move and accommodates the ICL
by an increased propeller twist of the 5:18 base pair (C:
À13.2Æ0.18, 1: À22.3Æ0.28, and 2: À26.9Æ0.88). The addi-
tion of a covalent bridge between both strands of DNA
nearly doubles residue to residue correlation in the central
region of the duplex. Residues 5 and 16 have a correlation
coefficient (r) of 0.29Æ0.04, 0.62Æ0.01, and 0.58Æ0.02 for
C, 1, and 2 respectively (Figure S2 in the Supporting Infor-
mation). ICLs 1 and 2 have a substantial decrease in flexibil-
ity (Figure 2, top) when compared to the uncrosslinked ref-
erence CNT, resulting in the formation of a slight kink in
the duplex of both 1 and 2 to accommodate the ICL
(Figure 2, bottom).
Molecular modeling was used to validate ICL 2 as a
model for NM 1 and to compare the structural consequen-
ces of the two ICLs with the uncrosslinked control (C) in
identical 11-mer sequences. We used the Amber simulation
package with atomic detail and explicit water (see Support-
ing Information) to validate that 2 gives similar amounts of
distortion when compared to the NM ICL 1 and consistent
differences when both are compared to C.[9] Two indepen-
ACHTUNGTRENNUNGdent simulations of 50 ns were run for each of the 1, 2, and
C systems. The duplex was stable throughout all six simula-
tions.
The N7 to N7 distances of the NM ICL 1 overlapped well
with the C7 to C7 distances of 2; both are restricted as com-
pared to C, which samples a broader range (Figure 2, top).
The decreased distance between the two crosslinked bases
has a direct effect on the local distortion around the ICL,
and is also influenced by the sequence (Figure 2 bottom,
and Table S1 in the Supporting Information). One measure
of distortion is to examine the buckling and propeller
To test for local duplex bending at the crosslink site we
measured an angle that would encompass the tightening of
the 7- to 7-position of residues 5 and 16 (Figure 2, top). The
smaller angles sampled by 1 and 2 suggest that the analogue
slightly bends the duplex outside the crosslink in the same
manner that the NM ICL simulations do (Figure 2, bottom).
The slight bending of the central region of the ICL simula-
tions of 1 and 2 compared to C is qualitatively similar to
past experimental work.[7]
Circular dichroism (CD) spectra were recorded to gain
experimental insight into to what extent the NM ICLs con-
taining oligonucleotide 2 deviates from B-form DNA. The
CD spectra of 2 and an unmodified duplex of the same se-
quence displayed the characteristic features of B-form DNA
(Figure S4 in the Supporting Information), consistent with
our molecular dynamics simulations, indicating the NM ICL
induces only a minor bend in the DNA. It has been shown
that only more dramatic distortions, such as the ones in-
duced by cisplatin ICL result in significant changes in CD
spectra.[2j,12]
In summary, we describe the synthesis of the stable NM
ICL analogue 2 by post-synthetic double reductive amina-
tion. Although this ICL has three atoms substituted with re-
spect to the NM ICL 1 (the two N at the 7-positions of dG
by C and one C by N in the hydrazine-formed bridge), our
molecular dynamics simulations show that the two ICLs
affect DNA structure and motion in equivalent ways. The
availability of stable, site-specific NM ICLs will enable stud-
ies of the structural consequences and biological responses
induced by NM ICLs,[13] more than sixty years after NMs
were the first agents to be used in cancer chemotherapy.[14]
Such studies will provide new insights into how tumors
become resistant to treatment by crosslinking agents.
Figure 2. Data from MD simulations of 2 (black), 1 (blue) and C (red).
Top: Distance measurement marked in pink, C/N7 to C/N7 atoms be-
tween residues 5 and 16. Bottom: Center of mass angle measurement, in
which each point is defined by the heavy atoms of the base pair (high-
lighted in blue in inset picture): point 1 represents 4A and 19T, point 2
represents 6T and 17A and point 3 represents 8A and 15T.[10]
12102
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Chem. Eur. J. 2010, 16, 12100 – 12103