knitr::opts_chunk$set(fig.width=8, fig.height=8, echo=FALSE, warning=FALSE, message=TRUE)
\newpage
library(knitr) library(dplyr) library(tidyr) library(ggplot2) library(bfabricShiny) knitr::kable(rawfileQC.parameter$data.Info)
\newpage
The Total Ion Chromatogram (TIC) as well as the Base Peak plot should present a quick overview about the signal distribution over the LC-MS run. It should help to descide if the proper amount of sample was loaded and give insights about the complexity of the sample.
try(QC <- bfabricShiny:::.calc.master.scan(rawfileQC.parameter$data.QC)) try(QC <- bfabricShiny:::.calc.transient(QC))
try(bfabricShiny:::.TIC.BasePeak(QC))
\newpage
The cycle time plot should help to descide if the current instrument method is suited for the LC gradient. A too long cycle time will result in to few points over the chromatographic peaks. This is especially problematic for a quantitative experiment. A estimation of the number of Ms data points over three fixed assumed peak widths (10 sec, 20 sec, 30 sec).
try(bfabricShiny:::.cycle.time(QC))
\newpage
try(bfabricShiny:::.mz.dist(QC))
\newpage
try(bfabricShiny:::.mz.frequency(QC))
\newpage
try(bfabricShiny:::.charge.states(QC))
\newpage
try(bfabricShiny:::.charge.states.quantiles(QC))
\newpage
For HF instruments currently the scan to scan time difference is calculated. For Fusion data the "Elapsed Scan Time" value is plotted
try(bfabricShiny:::.scan.times(QC))
\newpage
try(bfabricShiny:::.injection.times(QC))
\newpage
try(bfabricShiny:::.ms2.vs.RT(QC))
\newpage
try(bfabricShiny:::.ms2.frequency(QC))
\newpage
try(bfabricShiny:::.lm.correction(QC))
\newpage
try(bfabricShiny:::.ms.data.points(QC))
\newpage
This report was compiled by using bfabricShiny version r packageVersion('bfabricShiny')
and r R.version.string
.
New RawFileReader from Thermo Fisher Scientific planetorbitrap, 2017
https://github.com/cpanse/bfabricShiny
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