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From these simulations, we calculated the global average completeness.
Using Monte Carlo radiation transport simulations, we calculated the total CR yield inside a tumor volume during EBRT compared to that of the radionuclides.
From the set of simulations, we calculated the proportion of the cohort of birds present on 1 January 2005 that had not yet died from lead poisoning on each successive day until the end of 2007.
To quantify the headpiece opening that occurred during MD simulations, we calculated the y-component of the distance d between a portion of the β-propeller domain (residues α250 438) and a portion of the hybrid domain (residues β55 106 and β356 434, Fig. 2A B).
For 200 repeated simulations, we calculated the average number of true and false positives for this method.
After MD simulations, we calculated RMSDs between Cα trajectory of h20S and Cα of its modelled structure recorded every 1 ps.
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By comparing with simulations, we calculate T base=14°C.
Using powertrain simulations we calculate hybridization ratio and tank size.
Using atomistic simulations, we calculate the effect of SAM and magnesium ions on the folding free energy landscape of the SAM-I riboswitch.
By the average results in the 10 random topologies of 50 simulations, we calculate the success probability and the average energy consumption of successfully transmitting one packet, which are shown in Figure 12.
Using the FDTD simulations, we calculate LEE of nanorod deep UV LED structures for both TE and TM polarization modes and investigate the dependence of LEE on structural parameters to find optimized nanorod structures for high LEE.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com