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MD simulations were run with AMBER 14 (ref. 35, http://ambermd.org/) for another 80 ns using the NPT ensemble (1 atm, 303 K) with periodic boundary conditions and the Langevin thermostat.
Given that the total memory transfer took 320 ns, allowing for the 100 ns streaming overhead, the single stream time indicates calculation was achieved in 440 ns using the CUDA FFT algorithm, including conversion time.
Thereby, to predict the thermostabilities of AoXyn11AY13F and AoXyn11AG21I Y13F, the modeled 3-D structures of AoXyn11A, AoXyn11AY13F and AoXyn11AG21I Y13F were subjected to MD simulations, respectively, at 500 K for 7 ns using the GROMACS 4.5 package, followed by calculating their RMSD values using a g_rms software in the GROMACS 4.5.
The production simulations of the systems were performed for 25 ns using the methods as in the equilibration period.
The number of apoptotic cells was not significantly different when comparing ID vs. IS (p = ns using the Mann Whitney U test).
Molecular dynamics (MD) simulation was performed for 4 ns using the SANDER module of AMBER 9 program suite.
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Compute x p (n) using the proposed algorithm for other pixels.
Then we obtain for all N, M ∈ N with M < N using the factorization method (cf. [[23], Sect.
When the older man tried to exit, he asked to be excused to the younger, who looked at him and exclaimed "go on n" using the "N" word.
In contrast, ROM 784 could exert a force of 797 1127 N, using the specific tensions used by Carpenter et al. [19], and 571 N using a more realistic specific tension, creating an impact stress of 2900 5600 N/cm29 56–56 MPa).
The enriched fragments were reamplified with the primer MseI-N using the PCR conditions described above.
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