Title : Comparison between the fAcs settings used for Werner in 2017 with the ones I am using currently.
Contents
56. Title : Comparison between the fAcs settings used for Werner in 2017 with the ones I am using currently.#
56.1. Date#
13022020-14022020
56.2. Objective#
To understand what happen to the output fluorescence signal if the settings are slightly changed, and perhaps we can understand why in 2017 when he measured with Marit they measured 6-7 fold between 0-2% gal while I am only measuring 1.5-2.5 fold change, when taking the geometric means of the histograms.
{#fig:marit-data width=50%}
{#fig:leila-data width=50%}
From @fig:marit-data we can observe that already the sugar source it was used is different than mine experiments. The used glucose as a second sugar source for the galactose promoter , and all the reamining controls are in incbated in glucose. The cells here were incubated in 30C and I incubated them in 36C (as Ilse measured in the bulk growth). I used raffinose as a second sugar source , and also for the controls without galactose promoter, as Ilse used in her bulk growth experiments.
From the histograms, we can see that @fig:marit-data have a long tail for 2% gal (gray curve), going until 25000.
The 2% Raff in my case(@fig:leila-data) is more spread than the 2% glu for @fig:marit-data. maybe because Raffinose has some galactose???
Looking from peak to peak in @fig:leila-data, we can see that the fold change is around 8, from 1000 to 8000.
56.3. Method#
I am going to use only the following strains:
ywkd024 : RWS119 Wedlich-Söldner Lab collection a W303 can 1 1-100 his3 11,15 Galpr-myc-GFP-CDC42 YipLac204-MET-CLN2 cln1\(\Delta\)::HisG, cln2\(\Delta\), cln3\(\Delta\)::HisG (strain to compare with ywkd065(sfGFP))
ywkd038: RWS1421 Wedlich-Söldner Lab collection a W303 can1 1-100 his3 11,15 CDC42pr-myc-GFP-CDC42 YipLac204-MET-CLN2 cln1\(\Delta\)::HisG, cln2\(\Delta\), cln3\(\Delta\)::HisG (Reference for the native CDC42 expression)
ywkd001: \(\alpha\) W303 can 1 1-100 his3 11,15 leu2 3,112 S288C ,yLL3a -Laan Lab collection (Reference for the background fluorescence)
The incubation is going to be for 15 hours from glycerol stock to the measurement point, in 0% and 2% Gal.
Incubation started at 8:50 am on 13022020
56.3.1. Different setting used for Werner (2017) and for me (2020)#
Equipment-Model: BDFACSCelesta
Lasers-488nm: 375V (Werner) // 495V (Leila)
FSC threshold: 50000 (Werner) // 20000 (Leila)
FSC voltage: 375V (Werner) // 407V (Leila)
SSC volatge: 233V (Werner) // 275V (Leila)
56.4. Results#
56.4.1. Doublet correction#
From this website
Notice the differences between the doublet pulse and the single particle pulse: both the area and the width of the doublet pulse are larger than the single cell’s (because two cells spend longer passing through a laser beam than one cell) but the heights of the two pulses are very close, if not identical. We can take advantage of these observations to parse out which pulses belong to doublets and which belong to true single events in the data set.
The magnitude of difference in any pulse parameter between a doublet and single event is not large, and the resolution of linear scale is necessary to be able to accurately identify doublets to exclude. This requirement precludes most fluorescent parameters, which are typically scaled logarithmically, leaving forward and side scatter (which are coincidentally also nice and bright signals) as the best choices.
One important tip: if you are using BD “digital” FACSDiva instrumentation, the pulse width parameter is not really measured, but is calculated from the pulse area. Therefore, in order to ensure an accurate doublet exclusion gate, be sure to calibrate the Area Scaling Factor associated with the doublet discrimination parameter if you intend to use the width pulse parameter for doublet exclusion.
So, what we shuld plot is FSC-H vs FSC-A and the same for SSC-H vs SSC-A. In our case this corresponds to:
{#fig:024-doublet width=80%}
{#fig:038-doublet width=80%}
{#fig:001-doublet width=80%}
56.4.2. Histograms#
{#fig:hist width=80%}
{#fig:hist-gated width=80%}
56.4.3. Beads profile#
{#fig:beads-profile width=80%}
56.4.4. Fold change after autofluorescence removal with/without doublet correction#
{#fig:mean-gated-leila width=50%}
{#fig:mean-leila width=50%}
{#fig:mean-gated-werner width=50%}
{#fig:mean-werner width=50%}
56.5. Conclusion#
The settings of Werner , what does is to shift the signal to the left including the signal from the beads.
After the analysis of the height and the area output from the GFP output pulse , we can say that we can see 7 fold variation among the means of intensities when taking the height measure as the intensity signal.
The doublet correction could help us to more accurately estimate the expression from single cells.
To avoid clumps of cells we should keep th edensity low and sonicate the cells!!
Still there are some unclear points:
In order to take into account the height as the most informative parameter for the fluorescence of each cell, we should be able to see the 3 peaks of the calibration beads in the height channel!! Which we dont see with these settings, only in the area channel is where we see the three peaks.
However, still the height channel looks more promesing than the area channel because the shape of the distributions look more log-normal distributed ,as we expect for genetic expression distributions.