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were averaged and treated as a single value for the experiment. The
ratios from the independent samples were log transformed, and then
the data for each individual spot were averaged between the replicate
experiments. We then calculated the geometric mean and standard
deviation of the entire population. Any spot that had a ratio that was
more than 2.5 standard deviations away from the mean was considered an
outlier. Outliers were then removed from the population, and the means
and standard deviations were recalculated. Once again, any spot more
than 2.5 standard deviations away from the mean was considered an
outlier. This process was repeated until few or no outliers were
detected. In these experiments generally three iterations were needed
to identify all outliers in the population.
Array data were also analyzed with the Rosetta Resolver application
Axon error model (Rosetta Biosoftware). The lists of outliers from the
two analysis methods were compared, and only those genes that were
considered significantly changed in both were considered further. The
range of ratios of the outliers was from a high of 12 to a low of 1.6.
HMM analysis.
The sigma-H promoter sequence was modeled by using the HMMER 2.1.1
suite of software packages to create a series of closely related HMMs
(http://hmmer.wustl.edu). Known sigma-H promoter sequences from
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structure factor amplitudes of solvent molecules in the crystal were
calculated using the bulk solvent correction routine in XPLOR ([70]19),
and thus the low resolution limit could be extended to 50.0 Ã
resolution. Crystallographic refinement including simulated annealing,
conjugate gradient minimization, and individual B-factor refinement was
then performed at the resolution between 50.0 and 2.5 Ã
. After the
first round of refinement, the quality of the structure was
dramatically improved with a working R factor of 27.4% and a freeR
factor of 30.1%. The F [o] âF [c] difference map showed continuous
density for CoA, verifying the correct molecular replacement solution.
Several iterations of model building in the program O ([71]17) and the
refinement in the program XPLOR ([72]19) further dropped both R
factors. The final refinement statistics are shown in Table [73]II.
Because of the slight difference between four subunits,
noncrystallographic symmetry restraints were applied to only 89% of
total residues of each subunit. In the final model, residues 1â5 in
subunit 1; residues 1â7 and 211â212 in subunit 2; residues 1â5 and
210â213 in subunit 3; and residues 1â7, 83â85, and 212â214 in subunit 4
are excluded because they are disordered in the crystal.
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