Real-time atomistic description of DNA unfolding.
Real-time atomistic description of DNA unfolding.
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DOI:
10.1002/anie.201000593
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发表时间:
2010-06
影响因子:
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通讯作者:
Alberto Pérez;M. Orozco
中科院分区:
文献类型:
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作者:
Alberto Pérez;M. Orozco
Despite recent efforts, the folding/unfolding of DNA (understood as a dramatic conformational change from the native conformation in a significantly large portion of the duplex) is still poorly described. A range of classical physical studies led to the assumption that the unfolding of short DNA fragments is reversible and follows a two-state mechanism, starting at d (A· T) pairs.[1–3] Nevertheless, this traditional view has been recently challenged [4–9] by ultrafast techniques, which suggested a more complex scenario where compact intermediates are detected during the microsecond-long unfolding process.[4] Unfortunately, these experiments were not able to provide atomistic-detailed information on the process, thus making necessary the use of simulation techniques (mainly molecular dynamics, MD) as complementary tools. For computational reasons MD simulations of unfolding have typically followed indirect approaches, such as the use of multiple short trajectories,[10, 11] replica exchange,[12, 13] or moderately large (100ns) simulations under nonphysical denaturing conditions (T= 400 K).[14, 15] These simulations provided clear evidence of the complexity of DNA unfolding but were unable to define a mechanistic view, which would require multiple very large unbiased trajectories. Herein, we present a full atomistic description [16] of the unfolding of a full turn of DNA under realistic denaturing conditions. The study, a real “tour de force” for MD, provides for the first time a detailed atomistic picture of DNA unfolding in the microsecond timescale.All simulations were performed using Dickerson s dodecamer [17](DDD; Protein Data Bank (PDB) code 1BNA), a well-studied model of a short nonhairpin duplex. To guarantee unfolding on the microsecond timescale,[10, 11] we simulated strong (but realistic) denaturing conditions by adding a high concentration of a chemical denaturant (pyridine; Pyr) and increasing the temperature to nearly the boiling point of water (these simulations are coded as PHT). Control simulations were performed that considered: 1) water at low temperature (WLT), where we expected no