Experiment

The aim of the experiment is to determine the density of Sla1-EGFP patches in yeast mutants where the central region of Ede1 protein (amino acids 366-900, PQ-rich and coiled-coil domains) was replaced by a heterologous protein domain, one of:

  • yeast Snf5 prion-like IDR
  • yeast Sup35 prion-like IDR
  • mCherry (monomeric fluorescent protein)
  • dTomato (dimeric fluorescent protein)
  • kinesin-1 coiled-coil from Drosophila melanogaster (dimeric)
  • kinesin-5 coiled-coil from Homo sapiens (tetrameric)

Imaging

I acquired all data on the Olympus IX81 equipped with a 100x/1.49 objective, using the X-Cite 120PC lamp at 50% intensity and 400 ms exposure for illumination. Light was filtered through a U-MGFPHQ filter cube. I acquired stacks of 26 planes with a step size of 0.2 microns.

Image processing

Individual non-budding cells were cropped from fields of view. Patch numbers were extracted using Python function count_patches from my personal package mkimage containing a set of wrappers for scikit-image functions. Briefly, the images were median-filtered with a 5 px disk brush, and the filtered images were subtracted from the originals to subtract local background. The background-subtracted images were thresholded using the Yen method. The thresholded images were eroded using the number of non-zero neighbouring pixels in 3D as the erosion criterion. The spots were counted using skimage.measure.label() function with 2-connectivity.

Cross-section area was obtained by median-filtering of the stack with 10px disk brush, calculating the maximum projection image, thresholding using Otsu’s algorithm, and using skimage.measure.regionprops() to measure area. Note that these are pixel counts of cross-section area. To determine the total surface area, I assumed that an unbudded cell is spherical (suface area is four times the cross-section area).

This call to site_counter was used to process all datasets:

process_folder(path, median_radius = 5, erosion_n = 1, con = 2,
                   method = Yen, mask = False, loop = False, save_images = True)

Another notebook was used to gather all output into tidy data frames available here, with no further modifications.

Strain list

strain ede1
MKY0140 EDE1
MKY3782 ∆PQCC
MKY0654 ede1∆
MKY4617 mCherry
MKY4576 dTom
MKY4578 Khc
MKY4580 Eg5
MKY4291 Snf5
MKY4282 Sup35

Per-dataset summary

Patch number and area

ede1 dataset n patches_mean patches_sd patches_se area_mean area_sd area_se
EDE1 1 63 27.73016 6.715909 0.8461250 51.94079 10.645161 1.3411642
EDE1 2 58 29.12069 5.846209 0.7676449 56.44771 11.552946 1.5169761
EDE1 3 64 29.32812 6.519944 0.8149930 49.56184 7.991786 0.9989733
∆PQCC 1 73 16.41096 4.954896 0.5799267 52.33093 11.200530 1.3109229
∆PQCC 2 74 18.44595 5.698214 0.6624039 54.32342 10.600985 1.2323395
∆PQCC 3 58 18.29310 6.833890 0.8973338 54.40918 11.287895 1.4821732
ede1∆ 1 61 14.98361 4.801013 0.6147067 52.08469 7.516644 0.9624076
ede1∆ 2 65 15.98462 5.704966 0.7076139 56.48160 10.966704 1.3602522
ede1∆ 3 60 14.61667 5.249993 0.6777712 48.98833 8.084606 1.0437182
mCherry 4 54 17.70370 5.638913 0.7673589 59.99512 15.108871 2.0560569
mCherry 5 70 18.48571 4.760169 0.5689491 50.13624 7.121412 0.8511715
mCherry 6 78 14.21795 4.874123 0.5518858 49.94668 9.651742 1.0928446
dTom 4 68 15.82353 5.268723 0.6389265 48.63283 7.470632 0.9059472
dTom 5 59 15.71186 5.378921 0.7002758 53.89653 9.640562 1.2550942
dTom 6 42 18.92857 5.654236 0.8724675 55.65860 10.453794 1.6130555
Khc 4 61 13.62295 5.612973 0.7186675 47.46450 6.633740 0.8493634
Khc 5 64 14.31250 4.189462 0.5236827 49.50749 8.223165 1.0278956
Khc 6 54 16.62963 5.003004 0.6808226 53.91222 8.693893 1.1830890
Eg5 4 60 18.81667 5.776902 0.7457949 50.86488 6.825151 0.8811232
Eg5 5 78 16.06410 5.112602 0.5788881 50.41711 10.283088 1.1643305
Eg5 6 60 16.26667 5.868233 0.7575856 51.62094 11.500195 1.4846688
Snf5 1 90 19.34444 6.182907 0.6517356 45.21896 7.520545 0.7927350
Snf5 2 79 20.75949 5.137133 0.5779726 56.24489 10.959846 1.2330790
Snf5 3 62 18.59677 8.177257 1.0385127 48.89502 11.491233 1.4593880
Sup35 1 77 22.02597 5.155411 0.5875136 51.53718 8.410510 0.9584666
Sup35 2 61 21.21311 7.071338 0.9053921 55.34524 9.881855 1.2652419
Sup35 3 54 22.11111 5.967417 0.8120626 52.71252 10.581480 1.4399571

Sla1 density

We can combine the patch number and area into \(density = \frac{patches}{area}\), calculated individually for each cell. We can summarise the data for each Ede1 mutant in each dataset:

ede1 dataset n density_mean density_sd density_se density_median density_mad
EDE1 1 63 0.5481701 0.1446301 0.0182217 0.5645806 0.1440384
EDE1 2 58 0.5277718 0.1198626 0.0157387 0.5120066 0.1172980
EDE1 3 64 0.5948730 0.1110449 0.0138806 0.5869729 0.1016109
∆PQCC 1 73 0.3178281 0.0936706 0.0109633 0.3144940 0.0989302
∆PQCC 2 74 0.3463387 0.1057420 0.0122923 0.3237286 0.0907352
∆PQCC 3 58 0.3343710 0.1086607 0.0142679 0.3384717 0.0852853
ede1∆ 1 61 0.2905893 0.0926398 0.0118613 0.2893412 0.0784925
ede1∆ 2 65 0.2812039 0.0815060 0.0101096 0.2864278 0.0766339
ede1∆ 3 60 0.2988538 0.1021170 0.0131832 0.3085457 0.1075222
mCherry 4 54 0.2960346 0.0649451 0.0088379 0.2913582 0.0658805
mCherry 5 70 0.3720760 0.0922860 0.0110303 0.3616950 0.0877807
mCherry 6 78 0.2871355 0.0912629 0.0103335 0.3002458 0.0946702
dTom 4 68 0.3240302 0.0977476 0.0118536 0.3172533 0.0954928
dTom 5 59 0.2908285 0.0862263 0.0112257 0.2827884 0.0858295
dTom 6 42 0.3464929 0.1032743 0.0159356 0.3458182 0.0946929
Khc 4 61 0.2850212 0.1032656 0.0132218 0.2863498 0.1103514
Khc 5 64 0.2929173 0.0839598 0.0104950 0.2984537 0.0814191
Khc 6 54 0.3084453 0.0835851 0.0113745 0.2990882 0.0817657
Eg5 4 60 0.3698412 0.1012370 0.0130696 0.3727275 0.1171072
Eg5 5 78 0.3236706 0.0976318 0.0110546 0.3266622 0.0931995
Eg5 6 60 0.3182508 0.1076020 0.0138914 0.3163651 0.1029646
Snf5 1 90 0.4276246 0.1221145 0.0128720 0.4228668 0.1211030
Snf5 2 79 0.3760389 0.0943727 0.0106178 0.3684693 0.1011870
Snf5 3 62 0.3725138 0.1277070 0.0162188 0.3669131 0.1374652
Sup35 1 77 0.4362761 0.1133273 0.0129148 0.4255176 0.1124559
Sup35 2 61 0.3870802 0.1225512 0.0156911 0.3899448 0.1170396
Sup35 3 54 0.4281938 0.1241646 0.0168967 0.4192432 0.1205993

Plots

SuperPlots

I have chosen to show this data using the SuperPlot style. Each point shows density of Sla1-EGFP patches in an individual cell.

Big colour points show mean measurements from three independent repeats.

Range is mean +/- SD, calculated based on the three independent repeat means.

Beeswarm

Violin

With significance

There are 9 levels of Ede1, resulting in 36 possible pairwise comparisons. This is too unwieldy for any plot, at least a plot intended to also show the data.

As such, I propose to not even attempt this kind of illustration. An alternative is a compact letter display. In this view, groups sharing at least one letter are not significantly different at a chosen \(\alpha\) (here, 5%).

Pros:

  • less cluttered and simpler to read
  • focus away from p-values; provide a binary decision on the null hypothesis

Cons:

  • cannot distinguish different confidence levels
  • can get complicated just as well
  • focuses on non-findings rather than findings.

As this is also complicated, I propose a final solution: indicate that all groups are significantly different from wild-type in the text, and mark those with a significant improvement from ede1∆PQCC with a star, all while providing a table of p-values for each pairwise comparison in the supplement.

Pooled box plot

This might be useful in situations where this much data is too much data.

Modeling

We want to consider:

  1. What are the Sla1 densities in different Ede1 backgrounds?
  2. Are the differences between strains statistically significant?

The design is not ideal here:

  • we want to compare all mutants against each other
  • we want to block for nuisance factors, which might come from co-culturing the cells or things related to the microscope such as lamp power hence the independently repeated experiments
  • half the experiment was added after the reviewers request, so the design is disconnected. Datasets 1-3 have both controls and IDRs, datasets 4-6 have the globular / coiled-coil replacements. Finally, the mCherry strain was added after all of the others on separate dates.

Bad design cannot be solved in statistical analysis, but on the bright side, the data is nice and there is no reason for a systematic error to be associated with any particular dataset. Since we are measuring an absolute property (number of sites), and not something directly proportional to exposure settings like intensity, the influence of lamp power etc. should be limited

If the experiment was not disconnected, we could try to see if the effects of date / dataset can be modeled.

Because it is disconnected, it’s a bit more tricky. For example we cannot really get useful information from trying to model date as a fixed effect after ede1. What we could do for starters is to make a model which disregards the dataset information, and look if the residuals are clustered by date or dataset, informing us about whether this actually matters.

pooled_lm <- lm(density ~ ede1, data = sla1_density)
plot(as.factor(sla1_density$date), resid(pooled_lm),
     xlab = '', ylab = 'Residuals', las = 2,
     main = 'Univariate model residuals by date')

These seem to be very well distributed around zero. The exception is the single mCherry acquisition on 10/02/2022, which, to be honest, does seem like an outlier.

So what to do? The decision seems fairly arbitrary. I do not necessarily think that the univariate model on all cells would be wrong, but it does seem like a controversial issue. A model of replicate means (means-pooled analysis) will be conservative and lose power, but it seems appropriate for once, considering the segregated design.

Means-pooled linear model ANOVA

We will test the null hypothesis that mean Sla1 density is the same across different Ede1 strains. We will use repeat-level data for the tests to account for experimental variability.

We can use ANOVA and a post-hoc test to find out how likely this data is to occur under the null hypothesis.

More importantly, we will try to find the effect sizes of different contrasts.

We start by making a model of density_mean ~ ede1:

## 
## Call:
## lm(formula = density_mean ~ ede1, data = sla1_density_stats)
## 
## Residuals:
##       Min        1Q    Median        3Q       Max 
## -0.031280 -0.017512 -0.002544  0.013238  0.053661 
## 
## Coefficients:
##             Estimate Std. Error t value Pr(>|t|)    
## (Intercept)  0.55694    0.01613  34.531  < 2e-16 ***
## ede1∆PQCC   -0.22409    0.02281  -9.825 1.17e-08 ***
## ede1ede1∆   -0.26672    0.02281 -11.694 7.64e-10 ***
## ede1mCherry -0.23852    0.02281 -10.457 4.47e-09 ***
## ede1dTom    -0.23649    0.02281 -10.368 5.11e-09 ***
## ede1Khc     -0.26148    0.02281 -11.464 1.05e-09 ***
## ede1Eg5     -0.21968    0.02281  -9.631 1.59e-08 ***
## ede1Snf5    -0.16488    0.02281  -7.229 1.01e-06 ***
## ede1Sup35   -0.13975    0.02281  -6.127 8.70e-06 ***
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Residual standard error: 0.02794 on 18 degrees of freedom
## Multiple R-squared:  0.9236, Adjusted R-squared:  0.8897 
## F-statistic: 27.21 on 8 and 18 DF,  p-value: 1.573e-08
## Analysis of Variance Table
## 
## Response: density_mean
##           Df   Sum Sq   Mean Sq F value    Pr(>F)    
## ede1       8 0.169852 0.0212316  27.207 1.573e-08 ***
## Residuals 18 0.014047 0.0007804                      
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1

One-way ANOVA on means-pooled data rejects the null with \(p = 1.5 \times 10^{-8}\).

Diagnostic plots

This is one problem with the small N of replicate means: there are definitely differences in variance for different levels, but we cannot tell whether they reflect a difference in populations or just noise. But it’s probably the lattter; if we go back to the cell-level observations modeled by pooled_lm we can see that the residuals are fine there, too:

Estimated group means

The following are the model estimates of mean densities associates with each Ede1 level:

##  ede1    emmean     SE df lower.CL upper.CL
##  EDE1     0.557 0.0161 18    0.523    0.591
##  ∆PQCC    0.333 0.0161 18    0.299    0.367
##  ede1∆    0.290 0.0161 18    0.256    0.324
##  mCherry  0.318 0.0161 18    0.285    0.352
##  dTom     0.320 0.0161 18    0.287    0.354
##  Khc      0.295 0.0161 18    0.262    0.329
##  Eg5      0.337 0.0161 18    0.303    0.371
##  Snf5     0.392 0.0161 18    0.358    0.426
##  Sup35    0.417 0.0161 18    0.383    0.451
## 
## Confidence level used: 0.95

Post-hoc test (Tukey)

We are not necessarily interested in every possible comparison, but we do want to obtain all the p-values at least against ∆PQCC (is there a rescue?) and wild-type (is it complete?). Tukey’s test for contrasts of all 9 estimates:

##  contrast        estimate     SE df t.ratio p.value
##  EDE1 - ∆PQCC     0.22409 0.0228 18   9.825  <.0001
##  EDE1 - ede1∆     0.26672 0.0228 18  11.694  <.0001
##  EDE1 - mCherry   0.23852 0.0228 18  10.457  <.0001
##  EDE1 - dTom      0.23649 0.0228 18  10.368  <.0001
##  EDE1 - Khc       0.26148 0.0228 18  11.464  <.0001
##  EDE1 - Eg5       0.21968 0.0228 18   9.631  <.0001
##  EDE1 - Snf5      0.16488 0.0228 18   7.229  <.0001
##  EDE1 - Sup35     0.13975 0.0228 18   6.127  0.0002
##  ∆PQCC - ede1∆    0.04263 0.0228 18   1.869  0.6407
##  ∆PQCC - mCherry  0.01443 0.0228 18   0.633  0.9991
##  ∆PQCC - dTom     0.01240 0.0228 18   0.543  0.9997
##  ∆PQCC - Khc      0.03738 0.0228 18   1.639  0.7727
##  ∆PQCC - Eg5     -0.00441 0.0228 18  -0.193  1.0000
##  ∆PQCC - Snf5    -0.05921 0.0228 18  -2.596  0.2537
##  ∆PQCC - Sup35   -0.08434 0.0228 18  -3.698  0.0341
##  ede1∆ - mCherry -0.02820 0.0228 18  -1.236  0.9371
##  ede1∆ - dTom    -0.03023 0.0228 18  -1.326  0.9105
##  ede1∆ - Khc     -0.00525 0.0228 18  -0.230  1.0000
##  ede1∆ - Eg5     -0.04704 0.0228 18  -2.062  0.5245
##  ede1∆ - Snf5    -0.10184 0.0228 18  -4.465  0.0071
##  ede1∆ - Sup35   -0.12697 0.0228 18  -5.567  0.0007
##  mCherry - dTom  -0.00204 0.0228 18  -0.089  1.0000
##  mCherry - Khc    0.02295 0.0228 18   1.006  0.9803
##  mCherry - Eg5   -0.01884 0.0228 18  -0.826  0.9943
##  mCherry - Snf5  -0.07364 0.0228 18  -3.229  0.0847
##  mCherry - Sup35 -0.09877 0.0228 18  -4.330  0.0094
##  dTom - Khc       0.02499 0.0228 18   1.096  0.9675
##  dTom - Eg5      -0.01680 0.0228 18  -0.737  0.9974
##  dTom - Snf5     -0.07161 0.0228 18  -3.139  0.1000
##  dTom - Sup35    -0.09673 0.0228 18  -4.241  0.0113
##  Khc - Eg5       -0.04179 0.0228 18  -1.832  0.6627
##  Khc - Snf5      -0.09660 0.0228 18  -4.235  0.0114
##  Khc - Sup35     -0.12172 0.0228 18  -5.337  0.0012
##  Eg5 - Snf5      -0.05480 0.0228 18  -2.403  0.3387
##  Eg5 - Sup35     -0.07993 0.0228 18  -3.504  0.0500
##  Snf5 - Sup35    -0.02512 0.0228 18  -1.102  0.9665
## 
## P value adjustment: tukey method for comparing a family of 9 estimates

This is a lot; perhaps we can put it in a graphical matrix.

p-value matrix

The bottom line

  • every mutant is significantly different from wild-type at \(\alpha = 0.05\)
  • only Sup35 replacement is a significant improvement over ∆PQCC

Effect sizes

Effect sizes are perhaps more important than the p-values. Here I will calculate the classical Cohen’s d, defined as the mean differences over population standard deviation. Despite using means-pooled model to estimate contrast p-values and population means, I am confident that it is more appropriate to take the pooled observation-level SD for calculating the effect size.

Therefore \(\sigma\) will be a mean of SD for each Ede1 level, weighed by \(n-1\) (departing from emmeans default suggestion of residual SD). I am not quite sure what the appropriate degrees of freedom are, I used sample size minus Ede1 level count. In any case, it affects the 95% CI’s of effect size estimate, but not the estimate itself.

Below are effect sizes calculated for comparisons against wild-type and against ∆PQCC.

##  contrast       effect.size    SE df lower.CL upper.CL
##  ∆PQCC - EDE1         -2.11 0.217 18    -2.56   -1.651
##  ede1∆ - EDE1         -2.51 0.219 18    -2.97   -2.049
##  mCherry - EDE1       -2.24 0.218 18    -2.70   -1.786
##  dTom - EDE1          -2.22 0.218 18    -2.68   -1.767
##  Khc - EDE1           -2.46 0.219 18    -2.92   -2.000
##  Eg5 - EDE1           -2.07 0.217 18    -2.52   -1.609
##  Snf5 - EDE1          -1.55 0.216 18    -2.00   -1.097
##  Sup35 - EDE1         -1.31 0.216 18    -1.77   -0.861
## 
## sigma used for effect sizes: 0.1063 
## Confidence level used: 0.95
##  contrast        effect.size    SE df lower.CL upper.CL
##  EDE1 - ∆PQCC         2.1076 0.217 18    1.651   2.5645
##  ede1∆ - ∆PQCC       -0.4009 0.215 18   -0.852   0.0500
##  mCherry - ∆PQCC     -0.1357 0.215 18   -0.586   0.3150
##  dTom - ∆PQCC        -0.1166 0.215 18   -0.567   0.3341
##  Khc - ∆PQCC         -0.3516 0.215 18   -0.802   0.0993
##  Eg5 - ∆PQCC          0.0415 0.215 18   -0.409   0.4921
##  Snf5 - ∆PQCC         0.5569 0.215 18    0.106   1.0080
##  Sup35 - ∆PQCC        0.7932 0.215 18    0.342   1.2448
## 
## sigma used for effect sizes: 0.1063 
## Confidence level used: 0.95

Addendum: mixed model analysis

The p-values for different contrasts above are a result of a quite conservative model, which itself is a result of suboptimal design. In a pooled observation model, for example, we would find a couple more significant effects due to larger sample size:

##            EDE1   ∆PQCC   ede1∆ mCherry    dTom     Khc     Eg5    Snf5   Sup35
## EDE1    [0.558]  <.0001  <.0001  <.0001  <.0001  <.0001  <.0001  <.0001  <.0001
## ∆PQCC           [0.333]  0.0024  0.9274  0.9199  0.0149  1.0000  <.0001  <.0001
## ede1∆                   [0.290]  0.1551  0.2413  1.0000  0.0008  <.0001  <.0001
## mCherry                         [0.319]  1.0000  0.4044  0.8021  <.0001  <.0001
## dTom                                    [0.318]  0.5249  0.7960  <.0001  <.0001
## Khc                                             [0.295]  0.0057  <.0001  <.0001
## Eg5                                                     [0.336]  <.0001  <.0001
## Snf5                                                            [0.395]  0.3849
## Sup35                                                                   [0.418]
## 
## Row and column labels: ede1
## Upper triangle: P values   adjust = "tukey"
## Diagonal: [Estimates] (emmean)

Here we get low p-values for the differences between Snf5 and everything else, as well as ∆PQCC and actually less dense Khc/ede1∆.

This model would generate group means and effect sizes pretty much the same as the means-pooled model, but drastically different p-values. This serves to underscore that p-values should be treated with healthy skepticism, and play a minor role in the interpretation of the results.

Some would say that this model is an example of pseudoreplication, but this is a bit of a grey area. Yeast cells from different datasets grow in the same medium, incubator and so on, but they are individual organisms. Even if a ‘date effect’ exists beyond a simple sampling variation, there is no reason to think that the effect is consistent across mutants: after all, each mutant grows in a separate tube. If we try to look at an interaction plot, we cannot see a consistent date effect:

Of course this is undermined by the disconnect in date / mutant combinations.

Can we generate a linear mixed model for this, using date as a random effect? Because there does not seem to be any consistent effect of date in itself, let’s add an interaction term.

date_lmm1 <- lmer(density ~ ede1 + (1|date), data = sla1_density)
date_lmm2 <- lmer(density ~ ede1 + (1|ede1:date), data = sla1_density)
date_lmm3 <- lmer(density ~ ede1 + (1|date) + (1|ede1:date), data = sla1_density)
## Data: sla1_density
## Models:
## date_lmm1: density ~ ede1 + (1 | date)
## date_lmm2: density ~ ede1 + (1 | ede1:date)
## date_lmm3: density ~ ede1 + (1 | date) + (1 | ede1:date)
##           npar     AIC     BIC logLik deviance  Chisq Df Pr(>Chisq)
## date_lmm1   11 -2879.1 -2818.9 1450.5  -2901.1                     
## date_lmm2   11 -2887.4 -2827.2 1454.7  -2909.4 8.2988  0           
## date_lmm3   12 -2885.4 -2819.8 1454.7  -2909.4 0.0017  1      0.967

Using the anova table for mixed models from lmerTest we actually find the interaction-only model date_lmm2 has the lowest AIC.

Single-term deletions of effects from the main + interaction model date_lmm3 suggest that the interaction model is significant and the main date effect is not.

## ANOVA-like table for random-effects: Single term deletions
## 
## Model:
## density ~ ede1 + (1 | date) + (1 | ede1:date)
##                 npar logLik     AIC     LRT Df Pr(>Chisq)    
## <none>            12 1424.9 -2825.8                          
## (1 | date)        11 1424.9 -2827.8  0.0007  1  0.9796497    
## (1 | ede1:date)   11 1417.8 -2813.6 14.1967  1  0.0001647 ***
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1

What does this mean? I am getting out of my depth here, but I think that we simply cannot assign a meaningful change of intercept based on date because the effect is different for every Ede1 level (hence the interaction). Again, this makes sense because while theoretically there could be some issues affecting all strains on a given day (say, incubator failure), this just did not happen and so it’s not reflected in the data beyond a simple sampling error and that is going to be unique to each sample.

Note that this is very unlike the dataset in Figure 3, where any change in the microscope will affect intensity readings.

Let’s look at what the interaction-only model says about ede1 effects on density. First, how do model residuals look? Pretty good, but it’s not like the pooled observation-only model had any problems.

Even if we accept the interaction-only model, the random factor does not explain much of the variance anyway:

## Linear mixed model fit by REML. t-tests use Satterthwaite's method [
## lmerModLmerTest]
## Formula: density ~ ede1 + (1 | ede1:date)
##    Data: sla1_density
## 
## REML criterion at convergence: -2849.8
## 
## Scaled residuals: 
##     Min      1Q  Median      3Q     Max 
## -3.6089 -0.6576 -0.0241  0.6473  3.8921 
## 
## Random effects:
##  Groups    Name        Variance  Std.Dev.
##  ede1:date (Intercept) 0.0006184 0.02487 
##  Residual              0.0108813 0.10431 
## Number of obs: 1747, groups:  ede1:date, 27
## 
## Fixed effects:
##             Estimate Std. Error       df t value Pr(>|t|)    
## (Intercept)  0.55716    0.01628 18.50247  34.224  < 2e-16 ***
## ede1∆PQCC   -0.22433    0.02291 18.12580  -9.793 1.15e-08 ***
## ede1ede1∆   -0.26700    0.02302 18.47895 -11.601 6.37e-10 ***
## ede1mCherry -0.23854    0.02294 18.20417 -10.401 4.33e-09 ***
## ede1dTom    -0.23743    0.02318 18.98038 -10.241 3.62e-09 ***
## ede1Khc     -0.26183    0.02307 18.64776 -11.350 8.20e-10 ***
## ede1Eg5     -0.22015    0.02295 18.26477  -9.592 1.48e-08 ***
## ede1Snf5    -0.16452    0.02279 17.73636  -7.220 1.12e-06 ***
## ede1Sup35   -0.13977    0.02300 18.39854  -6.078 8.74e-06 ***
## ---
## Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
## 
## Correlation of Fixed Effects:
##             (Intr) e1∆PQC ed1d1∆ ed1mCh ed1dTm ed1Khc ed1Eg5 ed1Sn5
## ede1∆PQCC   -0.711                                                 
## ede1ede1∆   -0.707  0.503                                          
## ede1mCherry -0.710  0.504  0.502                                   
## ede1dTom    -0.702  0.499  0.497  0.498                            
## ede1Khc     -0.706  0.502  0.499  0.501  0.496                     
## ede1Eg5     -0.709  0.504  0.502  0.503  0.498  0.501              
## ede1Snf5    -0.714  0.508  0.505  0.507  0.502  0.504  0.507       
## ede1Sup35   -0.708  0.503  0.501  0.503  0.497  0.500  0.502  0.506

We have 5% of variance explained by the 1|ede1:date term in the model.

Let’s quickly generate group means (diagonal) and p-values for contrasts, with Tukey adjustment:

##            EDE1   ∆PQCC   ede1∆ mCherry    dTom     Khc     Eg5    Snf5   Sup35
## EDE1    [0.557]  <.0001  <.0001  <.0001  <.0001  <.0001  <.0001  <.0001  0.0003
## ∆PQCC           [0.333]  0.6443  0.9992  0.9996  0.7755  1.0000  0.2402  0.0347
## ede1∆                   [0.290]  0.9359  0.9265  1.0000  0.5368  0.0070  0.0008
## mCherry                         [0.319]  1.0000  0.9795  0.9952  0.0820  0.0099
## dTom                                    [0.320]  0.9748  0.9971  0.0935  0.0113
## Khc                                             [0.295]  0.6746  0.0112  0.0012
## Eg5                                                     [0.337]  0.3189  0.0500
## Snf5                                                            [0.393]  0.9687
## Sup35                                                                   [0.417]
## 
## Row and column labels: ede1
## Upper triangle: P values   adjust = "tukey"
## Diagonal: [Estimates] (emmean)

The values are strikingly similar to what we saw with the means-pooled model. Why? I suspect that these are actually equivalent because the mixed model we ended up with creates 27 unique groups with no shared information by ede1 / date combination just as we have 27 ede1 / dataset unique group means in the replicate_lm model.

Conclusions

Actual conclusions

  1. All mutations cause a significant reduction in patch density from wild type
  2. While Ede1∆PQCC is not significantly different from ede1∆, it has to be noted that the estimate is higher (~40% reduction instead of ~50%).
  3. Snf5 and Sup35 substitutions have significantly higher Sla1 densities than ede1∆; Sup35 is also significantly different from ∆PQCC.
  4. All the other mutants are similar across the board.
  5. Stepping away from p-values: IDRs rescue Sla1 density only somewhat, the others not at all. That is the take-home message.

Final estimates

Final estimates with lower / upper 95% confidence intervals, and a common-sense comparison to wild type (in %). half_ci is half of the confidence interval, for writing CI ranges in the format mean +/- error.

ede1 mean lower upper proc_wt half_ci
EDE1 0.557 0.471 0.642 100 0.085
∆PQCC 0.333 0.297 0.368 60 0.036
ede1∆ 0.290 0.268 0.312 52 0.022
mCherry 0.318 0.202 0.434 57 0.116
dTom 0.320 0.251 0.390 58 0.070
Khc 0.295 0.266 0.325 53 0.030
Eg5 0.337 0.267 0.408 61 0.070
Snf5 0.392 0.315 0.469 70 0.077
Sup35 0.417 0.352 0.483 75 0.066

Session info

## R version 4.1.0 (2021-05-18)
## Platform: x86_64-apple-darwin17.0 (64-bit)
## Running under: macOS Big Sur 10.16
## 
## Matrix products: default
## BLAS:   /Library/Frameworks/R.framework/Versions/4.1/Resources/lib/libRblas.dylib
## LAPACK: /Library/Frameworks/R.framework/Versions/4.1/Resources/lib/libRlapack.dylib
## 
## locale:
## [1] en_US.UTF-8/en_US.UTF-8/en_US.UTF-8/C/en_US.UTF-8/en_US.UTF-8
## 
## attached base packages:
## [1] stats     graphics  grDevices utils     datasets  methods   base     
## 
## other attached packages:
##  [1] emmeans_1.7.2      lmerTest_3.1-3     lme4_1.1-27.1      Matrix_1.3-3      
##  [5] multcompView_0.1-8 ggsignif_0.6.2     ggbeeswarm_0.6.0   knitr_1.36        
##  [9] broom_0.7.9        forcats_0.5.1      stringr_1.4.0      dplyr_1.0.7       
## [13] purrr_0.3.4        readr_2.0.1        tidyr_1.1.3        tibble_3.1.3      
## [17] ggplot2_3.3.5      tidyverse_1.3.1   
## 
## loaded via a namespace (and not attached):
##  [1] TH.data_1.1-0       minqa_1.2.4         colorspace_2.0-2   
##  [4] ellipsis_0.3.2      estimability_1.3    htmlTable_2.2.1    
##  [7] base64enc_0.1-3     fs_1.5.0            rstudioapi_0.13    
## [10] farver_2.1.0        fansi_0.5.0         mvtnorm_1.1-3      
## [13] lubridate_1.7.10    xml2_1.3.2          codetools_0.2-18   
## [16] splines_4.1.0       Formula_1.2-4       jsonlite_1.7.2     
## [19] nloptr_1.2.2.2      pbkrtest_0.5.1      cluster_2.1.2      
## [22] dbplyr_2.1.1        png_0.1-7           compiler_4.1.0     
## [25] httr_1.4.2          backports_1.2.1     assertthat_0.2.1   
## [28] cli_3.1.0           htmltools_0.5.1.1   tools_4.1.0        
## [31] gtable_0.3.0        glue_1.4.2          Rcpp_1.0.7         
## [34] cellranger_1.1.0    jquerylib_0.1.4     vctrs_0.3.8        
## [37] nlme_3.1-152        xfun_0.25           rvest_1.0.1        
## [40] mime_0.11           lifecycle_1.0.0     MASS_7.3-54        
## [43] zoo_1.8-9           scales_1.1.1        hms_1.1.0          
## [46] parallel_4.1.0      sandwich_3.0-1      RColorBrewer_1.1-2 
## [49] yaml_2.2.1          gridExtra_2.3       rpart_4.1-15       
## [52] latticeExtra_0.6-29 stringi_1.7.3       highr_0.9          
## [55] checkmate_2.0.0     boot_1.3-28         rlang_0.4.11       
## [58] pkgconfig_2.0.3     evaluate_0.14       lattice_0.20-44    
## [61] htmlwidgets_1.5.3   labeling_0.4.2      tidyselect_1.1.1   
## [64] magrittr_2.0.1      R6_2.5.1            generics_0.1.0     
## [67] Hmisc_4.5-0         multcomp_1.4-18     DBI_1.1.1          
## [70] pillar_1.6.2        haven_2.4.3         foreign_0.8-81     
## [73] withr_2.4.2         survival_3.2-11     nnet_7.3-16        
## [76] modelr_0.1.8        crayon_1.4.1        utf8_1.2.2         
## [79] tzdb_0.1.2          rmarkdown_2.11      jpeg_0.1-9         
## [82] grid_4.1.0          readxl_1.3.1        data.table_1.14.0  
## [85] reprex_2.0.1        digest_0.6.27       xtable_1.8-4       
## [88] numDeriv_2016.8-1.1 munsell_0.5.0       beeswarm_0.4.0     
## [91] vipor_0.4.5

WIP

---
title: "Sla1 patch density in Ede1 internal replacement mutants"
date: "Last compiled on `r format(Sys.time(), '%B %d, %Y')`"
output:
  html_document:
    code_download: true
---

```{r setup, include=FALSE}
knitr::opts_chunk$set(echo = FALSE, message=FALSE, warning=FALSE,
                      dpi = 96, fig.width = 6, fig.height = 4)
```

```{r libs}
# tidy stuff
library(tidyverse) 
library(broom) 
library(knitr)

# ggplot2 + extras
library(ggbeeswarm)
library(ggsignif)

# Extra tests and pairwise comparisons
library(multcompView)

# Mixed models and estimated marginal means
library(lmerTest)
library(emmeans)
```

```{r load}
# Load data generated by cleanup notebook
rm(list = ls())
load('data/idr_replacement_sla1.RData')
```

```{r theme}
# Custom ggplot2 theme
# --------------------

# minimal theme with border
# based on theme_linedraw without the grid lines
# also trying to remove all backgrounds and margins
# the aim is to make it as easy as possible to edit in illustrator

theme_clean <- function(base_size = 11, base_family = "",
                        base_line_size = base_size / 22,
                        base_rect_size = base_size / 22) {
  theme_linedraw(
    base_size = base_size,
    base_family = base_family,
    base_line_size = base_line_size,
    base_rect_size = base_rect_size
  ) %+replace%
    theme(
      # no grid and no backgrounds if I can help it
      legend.background =  element_blank(),
      panel.background = element_blank(),
      panel.grid = element_blank(),
      plot.background = element_blank(),
      plot.margin = margin(0, 0, 0, 0),
      complete = TRUE
    )
}

# Set default theme
# -----------------
theme_set(theme_clean(base_size = 14, base_family = "Myriad Pro"))

# Create a ggsave wrapper
# -----------------------

# This way we can set a default size and device for all plots
my_ggsave <- function(filename, plot = last_plot(),
                      device = cairo_pdf, units = "mm",
                      width = 100, height = 80, ...){
  ggsave(filename = filename, plot = plot,
         device = device, units = units,
         height = height, width = width,  ...)
  }
```

```{r functions}
# couple of small functions for extracting comparisons
# into a format understandable by ggplot

#' Add letter group labels generated by Tukey's HSD
#'
#' This function performs ANOVA and Tukey's HSD,
#' extracts the letter labels and attaches them
#' to the original data.
#'
#' @param x: df or tibble, the data (long format!)
#' @param yvar: chr, name of the dependent variable
#' @param xvar: chr, name of the independent variable
#' @param alpha: dbl, confidence level passed on to Tukey's test
#'
add_tukey_labels <- function(x, yvar, xvar, alpha = 0.95){
  aov_form <- formula(paste(yvar, '~', xvar))
  anova <- aov(formula = aov_form, data = x)
  tukey <- TukeyHSD(anova, which = xvar, conf.level = alpha)
  # Extract labels and factor levels from Tukey post-hoc 
  x_labels <- as_tibble(
    multcompLetters4(anova, tukey)[[xvar]]$Letters,
    rownames = xvar
    )
  
  if (is.factor(x[[xvar]])) {
    x_labels[[xvar]] <- factor(
      x_labels[[xvar]], levels = levels(x[[xvar]])
    )
  }
  
  x_labels <- rename(x_labels, tukey_group = value)
  x <- left_join(x, x_labels, by = xvar)
  
  return(x)
  }


#' Extract comparisons from rstatix tidy tests
#' 
#' This function subsets the selected comparisons in a Tukey,
#' Dunn or similar test done by rstatix.
#' It converts groups to a list of vectors that can be passed to geom_signif
#'
#'
#' @param x: df or tibble, the comparison results
#' @param rows: integer vector, the rows with desired comparisons
extract_comparisons <- function(x, rows){
  x_subset <- x[rows,] %>%
    .[nrow(.):1,]
  
  x_comparisons <- x_subset %>%
    select(group1, group2) %>%
    t() %>%
    as.data.frame() %>%
    as.list
  x_annotations <- x_subset$p.adj.signif %>%
    as.vector()
  
  significance <- list(
    comparisons = x_comparisons,
    annotations = x_annotations
  )
  
  return(significance)
}
```

# {.tabset .tabset-pills}

## Experiment

The aim of the experiment is to determine the density of Sla1-EGFP patches
in yeast mutants where the central region of Ede1 protein
(amino acids 366-900, PQ-rich and coiled-coil domains) 
was replaced by a heterologous protein domain, one of:
 
 - yeast Snf5 prion-like IDR
 - yeast Sup35 prion-like IDR
 - mCherry (monomeric fluorescent protein)
 - dTomato (dimeric fluorescent protein)
 - kinesin-1 coiled-coil from *Drosophila melanogaster* (dimeric)
 - kinesin-5 coiled-coil from *Homo sapiens* (tetrameric)

### Imaging

I acquired all data on the Olympus IX81
equipped with a 100x/1.49 objective,
using the X-Cite 120PC lamp at 50% intensity
and 400 ms exposure for illumination.
Light was filtered through a U-MGFPHQ filter cube.
I acquired stacks of 26 planes 
with a step size of 0.2 microns.

### Image processing

Individual non-budding cells were cropped from fields of view.
Patch numbers were extracted using Python function `count_patches`
from my personal package `mkimage`
containing a set of wrappers for `scikit-image` functions.
Briefly, the images were median-filtered with a 5 px disk brush,
and the filtered images were subtracted from the originals
to subtract local background.
The background-subtracted images were thresholded using the Yen method.
The thresholded images were eroded using the number of non-zero
neighbouring pixels in 3D as the erosion criterion.
The spots were counted using skimage.measure.label() function with 2-connectivity.

Cross-section area was obtained by 
median-filtering of the stack with 10px disk brush, 
calculating the maximum projection image, 
thresholding using Otsu's algorithm,
and using skimage.measure.regionprops() to measure area.
Note that these are pixel counts of *cross-section* area. 
To determine the total surface area, 
I assumed that an unbudded cell is spherical
(suface area is four times the cross-section area).

This call to `site_counter` was used to process all datasets:

```
process_folder(path, median_radius = 5, erosion_n = 1, con = 2,
                   method = Yen, mask = False, loop = False, save_images = True)
```

Another notebook was used to gather all output into tidy data frames
available here, with no further modifications.

### Strain list

```{r}
kable(strains)
```

## Per-dataset summary {.tabset}

### Patch number and area

```{r nums_dataset}
# means and SDs of number of patches and area
sla1_density %>%
  group_by(ede1, dataset) %>%
  summarise(n = n(),
            across(c(patches, area), list(mean = mean, sd = sd,
                                          se = ~sd(.x) / sqrt(n())))) %>%
  kable()
```

### Sla1 density

We can combine the patch number and area into
$density = \frac{patches}{area}$,
calculated individually for each cell.
We can summarise the data 
for each Ede1 mutant in each dataset:

```{r density}
sla1_density_stats <- sla1_density %>%
  group_by(ede1, dataset) %>%
  summarise(n = n(),
            across(density,
                   list(mean = mean, sd = sd, 
                        se = ~ sd(.x) / sqrt(n),
                        median = median, mad = mad)),
            .groups = 'drop')

sla1_density_stats %>% kable()
```

## Plots {.tabset}

```{r density.scatter}
plot_blank <- ggplot(sla1_density_stats,
                     aes(x = ede1, y = density_mean)) +
                         #shape = dataset, fill = dataset))+
  labs(title = NULL, x = 'Ede1', y = expression( "Sla1 patches/µm"^2)) +
  scale_y_continuous(breaks = seq(0.0, 1.0, 0.1)) +
  scale_shape_manual(values = c(21:25, 8)) +
  scale_color_brewer(palette = 'Set2') +
  scale_fill_brewer(palette = 'Set2')

plot_scatter <- plot_blank +
  geom_quasirandom(inherit.aes = F, data = sla1_density,
                   aes(x = ede1, y = density,
                       shape = dataset,# colour = dataset
                       ),
                   colour = 'grey75',# shape = 1,
                   show.legend = F, size = 0.8
                   )

plot_violin <- plot_blank + 
  geom_violin(inherit.aes = F,
              data = sla1_density, aes(x = ede1, y = density),
              colour = 'grey75', fill = 'transparent'
              )
```

### SuperPlots

I have chosen to show this data using the 
[SuperPlot](https://doi.org/10.1083/jcb.202001064) style.
Each point shows density of Sla1-EGFP patches in an individual cell.

Big colour points show mean measurements from three independent repeats.

Range is mean +/- SD, calculated based on the three independent repeat means.

#### Beeswarm

```{r}
plot_super <- plot_scatter +
  geom_quasirandom(aes(shape = dataset, fill = dataset),
                   show.legend = F,
                   width = 0.3, size = 2)+
  stat_summary(fun = mean, geom = 'crossbar',
               width = 0.5, fatten = 1)+
  stat_summary(fun.data = 'mean_sdl',
               fun.args = list(mult = 1), 
               geom = 'errorbar', width = 0.2)+
  guides(x = guide_axis(angle = -45))
  
print(plot_super)
my_ggsave('figures/density_super.pdf')

plot_super_flip <- plot_super +
  coord_flip()+
  scale_x_discrete(limits = rev(levels(sla1_density$ede1)))+
  theme(panel.border = element_blank(),
        axis.line.y = element_blank(),
        axis.ticks.y = element_blank(),
        axis.line.x = element_line())

my_ggsave('figures/density_super_flip.pdf', plot_super_flip,
          height = 100, width = 80)
```

#### Violin

```{r}
plot_super_violin <- plot_violin +
  geom_quasirandom(aes(shape = dataset, fill = dataset),
                   show.legend = F,
                   width = 0.3, size = 2)+
  stat_summary(fun = mean, geom = 'crossbar',
               width = 0.5, fatten = 1)+
  stat_summary(fun.data = 'mean_sdl',
               fun.args = list(mult = 1),
               geom = 'errorbar', width = 0.2)

print(plot_super_violin)
my_ggsave('figures/density_super_violin.pdf')
```

### With significance

There are 9 levels of Ede1,
resulting in 36 possible pairwise comparisons.
This is too unwieldy for any plot,
at least a plot intended to also show the data.

As such, I propose to not even attempt
this kind of illustration.
An alternative is a compact letter display.
In this view, groups sharing at least one letter 
are not significantly different
at a chosen $\alpha$ (here, 5%).

Pros:

  * less cluttered and simpler to read
  * focus away from p-values; provide a binary decision on the null hypothesis
  
Cons:

  * cannot distinguish different confidence levels
  * can get complicated just as well
  * focuses on non-findings rather than findings.

```{r}
sla1_density_stats <- sla1_density_stats %>%
  add_tukey_labels('density_mean', 'ede1')
```

```{r}
plot_super_letters <- plot_super +
  geom_text(data = sla1_density_stats,
            aes(label = tukey_group), y = Inf, vjust = 1.2)
  #stat_summary(aes(label = tukey_group),
  #             fun.y = Inf,
  #             geom = 'text', na.rm = T, vjust = -0.5,
  #             #fun.args = list(err = errors, mult = error_range)
  #             )
print(plot_super_letters)
my_ggsave('figures/density_super_letters.pdf', width = 150)
```

As this is also complicated,
I propose a final solution:
indicate that all groups are significantly different
from wild-type in the text,
and mark those with a significant improvement from 
ede1∆PQCC with a star,
all while providing a table of p-values
for each pairwise comparison in the supplement.

### Pooled box plot

This might be useful in situations
where this much data is too much data.

```{r}
plot_box <- plot_blank + 
  geom_boxplot(inherit.aes = F, data = sla1_density,
               aes(x = ede1, y = density),
               outlier.shape = 21, width = 0.5, notch = T)+
  guides(x = guide_axis(angle = -45))

print(plot_box)
```

## Modeling

We want to consider:

  1. What are the Sla1 densities in different Ede1 backgrounds?
  2. Are the differences between strains statistically significant?

The design is not ideal here:

  - we want to compare all mutants against each other
  - we want to block for nuisance factors,
  which might come from co-culturing the cells
  or things related to the microscope such as lamp power
  hence the independently repeated experiments
  - half the experiment
  was added *after* the reviewers request,
  so the design is disconnected. 
  Datasets 1-3 have both controls and IDRs,
  datasets 4-6 have the globular / coiled-coil replacements.
  Finally, the mCherry strain was added 
  after all of the others on separate dates.
  
Bad design cannot be solved
in statistical analysis,
but on the bright side, the data is nice
and there is no reason for a systematic error to be
associated with any particular dataset.
Since we are measuring an absolute property (number of sites),
and not something directly proportional
to exposure settings like intensity,
the influence of lamp power etc. should be limited

If the experiment was not disconnected,
we could try to see if the effects of date / dataset
can be modeled.

Because it *is* disconnected, it's a bit more tricky.
For example we cannot really get useful information
from trying to model `date` as a fixed effect after `ede1`.
What we could do for starters is to make a model
which disregards the dataset information, 
and look if the residuals are clustered by date or dataset,
informing us about whether this actually matters.

```{r echo = TRUE}
pooled_lm <- lm(density ~ ede1, data = sla1_density)
plot(as.factor(sla1_density$date), resid(pooled_lm),
     xlab = '', ylab = 'Residuals', las = 2,
     main = 'Univariate model residuals by date')
```

These seem to be very well distributed around zero.
The exception is the single mCherry acquisition
on 10/02/2022, which, to be honest,
does seem like an outlier.

So what to do? The decision seems fairly arbitrary.
I do not necessarily think that the univariate
model on all cells would be *wrong*,
but it does seem like a controversial issue.
A model of replicate means (*means-pooled analysis*)
will be conservative and lose power,
but it seems appropriate for once, 
considering the segregated design.

### Means-pooled linear model ANOVA

We will test the null hypothesis 
that mean Sla1 density is the same
across different Ede1 strains.
We will use repeat-level data for the tests
to account for experimental variability.

We can use ANOVA and a post-hoc test 
to find out how likely this data is to occur
under the null hypothesis.

More importantly,
we will try to find the effect sizes
of different contrasts.

We start by making a model
of `density_mean ~ ede1`:

```{r}
replicate_lm <- lm(density_mean ~ ede1, data = sla1_density_stats)
summary(replicate_lm)
anova(replicate_lm)
```

One-way ANOVA on means-pooled data 
rejects the null with $p = 1.5 \times 10^{-8}$.

#### Diagnostic plots

```{r}
plot(replicate_lm)
```

This is one problem with the small N of replicate means:
there are definitely differences in variance
for different levels, but we cannot tell
whether they reflect a difference in populations
or just noise. But it's probably the lattter;
if we go back to the cell-level observations
modeled by `pooled_lm` we can see that the residuals
are fine there, too:

```{r}
plot(pooled_lm)
```

### Estimated group means

The following are the model estimates 
of mean densities associates with each Ede1 level:

```{r}
replicate_emm <- emmeans(replicate_lm, spec = 'ede1')
summary(replicate_emm)
```

### Post-hoc test (Tukey)

We are not necessarily interested in every possible comparison,
but we do want to obtain all the p-values 
at least against ∆PQCC (is there a rescue?) and wild-type (is it complete?).
Tukey's test for contrasts of all 9 estimates:

```{r}
contrast(replicate_emm, method = 'pairwise')
```

This is a lot; perhaps we can put it in a graphical matrix.

#### p-value matrix

```{r fig.width=8}
p_matrix <- tidy(contrast(replicate_emm, method = 'pairwise'))%>%
  separate(contrast, c('gr1', 'gr2'), ' - ') %>%
  select(gr1, gr2, adj.p.value) %>%
  mutate(gr1 = fct_infreq(gr1), gr2 = fct_infreq(gr2))

p_matrix_plot <- ggplot(p_matrix, aes(gr1, gr2))+
  geom_tile(aes(fill = adj.p.value < 0.05), show.legend = F)+
  geom_text(aes(label = if_else(adj.p.value < 0.001,
                                '<0.001',
                                as.character(round(adj.p.value, 3)))))+
  labs(x = NULL, y = NULL)+
  #theme_clean()+
  theme(panel.border = element_blank(),
        axis.ticks = element_blank(),
        legend.title = element_text(face = 'bold'))+
  scale_fill_brewer()
print(p_matrix_plot)
my_ggsave('figures/p_matrix_plot.pdf', width = 150)
```

#### The bottom line

* every mutant is significantly different from wild-type at $\alpha = 0.05$
* only Sup35 replacement is a significant improvement over ∆PQCC

### Effect sizes

Effect sizes are perhaps more important than the p-values.
Here I will calculate the classical Cohen's d,
defined as the mean differences over population standard deviation.
Despite using means-pooled model
to estimate contrast p-values and population means,
I am confident that it is more appropriate
to take the pooled observation-level SD
for calculating the effect size.

Therefore $\sigma$ will be a mean of SD for each Ede1 level,
weighed by $n-1$ 
(departing from `emmeans` default suggestion of residual SD).
I am not quite sure what the appropriate degrees of freedom are,
I used sample size minus Ede1 level count. 
In any case, it affects the 95% CI's of effect size estimate,
but not the estimate itself.

Below are effect sizes calculated for comparisons against wild-type
and against ∆PQCC.

```{r}
pooled_var <- with(sla1_density,
     sqrt(weighted.mean(tapply(density, ede1, var),
                        tapply(density, ede1, length) - 1)))

eff_size(replicate_emm, sigma = pooled_var,
         edf = length(sla1_density$density) - length(levels(sla1_density$ede1)),
         method = 'trt.vs.ctrl', ref = 1)

eff_size(replicate_emm, sigma = pooled_var,
         edf = length(sla1_density$density) - length(levels(sla1_density$ede1)),
         method = 'trt.vs.ctrl', ref = 2)
```


### Addendum: mixed model analysis

The p-values for different contrasts above
are a result of a quite conservative model,
which itself is a result of suboptimal design. 
In a pooled observation model, for example, we would find 
a couple more significant effects due to larger sample size:

```{r}
pwpm(emmeans(pooled_lm, 'ede1'), diffs = F)
```

Here we get low p-values for the differences between Snf5 and everything else,
as well as ∆PQCC and actually *less* dense Khc/ede1∆.

This model would generate group means 
and effect sizes pretty much the same as the means-pooled model,
but drastically different p-values.
This serves to underscore that p-values 
should be treated with healthy skepticism,
and play a minor role in the interpretation of the results.

Some would say that this model is an example of *pseudoreplication*,
but this is a bit of a grey area.
Yeast cells from different datasets
grow in the same medium, incubator and so on,
but they are individual organisms.
Even if a 'date effect' exists beyond a simple sampling variation,
there is no reason to think that the effect is consistent
across mutants: after all, each mutant grows in a separate tube.
If we try to look at an interaction plot,
we cannot see a consistent date effect:

```{r}
ggplot(sla1_density, aes(x = as_factor(date), y = density, group = ede1, col = ede1)) + 
  #scale_color_brewer(palette = "Set2")+
  stat_summary(fun = mean, geom = "line")+
  stat_summary(fun = mean, geom = "point")+
  guides(x = guide_axis(angle = -45))+
  labs(x = 'Date', y = 'Sla1 density')
```

Of course this is undermined
by the disconnect in date / mutant combinations.

Can we generate a linear mixed model for this,
using `date` as a random effect? 
Because there does not seem to be any consistent effect of date in itself,
let's add an interaction term.

```{r echo = TRUE}
date_lmm1 <- lmer(density ~ ede1 + (1|date), data = sla1_density)
date_lmm2 <- lmer(density ~ ede1 + (1|ede1:date), data = sla1_density)
date_lmm3 <- lmer(density ~ ede1 + (1|date) + (1|ede1:date), data = sla1_density)
```

```{r}
anova(date_lmm1, date_lmm2, date_lmm3)
```

Using the `anova` table for mixed models from `lmerTest`
we actually find the interaction-only model `date_lmm2` has the lowest AIC.

Single-term deletions of effects from the main + interaction model
`date_lmm3` suggest that the interaction model is significant
and the main date effect is not.

```{r}
ranova(date_lmm3)
```

What does this mean? I am getting out of my depth here,
but I think that we simply cannot assign
a meaningful change of intercept based on `date`
because the effect is different for every Ede1 level (hence the interaction).
Again, this makes sense because while theoretically there could be some issues
affecting all strains on a given day (say, incubator failure),
this just did not happen and so it's not reflected in the data
beyond a simple sampling error and that is going to be unique to each sample.

Note that this is very unlike the dataset in Figure 3,
where any change in the microscope 
will affect intensity readings.

Let's look at what the interaction-only model
says about `ede1` effects on `density`.
First, how do model residuals look?
Pretty good, but it's not like the pooled
observation-only model had any problems.

```{r}
plot(date_lmm2)

par(mfrow = c(1, 2))

qqnorm(ranef(date_lmm2)$"ede1:date"[, 1], 
       main = "Random effects of interaction")
qqnorm(resid(date_lmm2), main = "Residuals")
```

Even if we accept the interaction-only model,
the random factor does not explain much of the variance anyway:

```{r}
summary(date_lmm2)
```

We have `r round(100 * 0.0006184 / (0.0006184 + 0.0108813))`% of variance 
explained by the `1|ede1:date` term in the model.

Let's quickly generate group means (diagonal)
and p-values for contrasts, with Tukey adjustment:

```{r}
pwpm(emmeans(date_lmm2, 'ede1'), diffs = F)
```

The values are strikingly similar
to what we saw with the means-pooled model.
Why? I suspect that these are actually equivalent
because the mixed model we ended up with
creates 27 unique groups with no shared information
by `ede1` / `date` combination
just as we have 27 `ede1` / `dataset` unique group means
in the `replicate_lm` model.

## Conclusions

### Actual conclusions

1. All mutations cause a significant reduction in patch density from wild type
2. While Ede1∆PQCC is not *significantly* different from ede1∆, 
  it has to be noted that the estimate is higher
  (~40% reduction instead of ~50%).
3. Snf5 and Sup35 substitutions have significantly higher Sla1 densities than ede1∆;
  Sup35 is also significantly different from ∆PQCC.
4. All the other mutants are similar across the board.
5. Stepping away from p-values: IDRs rescue Sla1 density only somewhat, 
  the others not at all. That is the take-home message.

### Final estimates

Final estimates with lower / upper 95% confidence intervals,
and a common-sense comparison to wild type (in %). 
`half_ci` is half of the confidence interval,
for writing CI ranges in the format mean +/- error.

```{r}
wt_mean <- sla1_density_stats %>%
  filter(ede1 == 'EDE1') %>%
  pull(density_mean) %>%
  mean()

density_ci <- sla1_density_stats %>%
  group_by(ede1)%>%
  summarise(mean_cl_normal(density_mean)) %>%
  rename(mean = y, lower = ymin, upper = ymax) %>%
  mutate(proc_wt = round(100 * mean / wt_mean),
         half_ci = (upper - lower) / 2) 

kable(density_ci, digits = 3)
```

## Source data

### .csv

```{r echo=FALSE}
xfun::embed_file('data/idr_replacement_sla1.csv')
```

### .RData

```{r echo=FALSE}
xfun::embed_file('data/idr_replacement_sla1.RData')
```

## Session info

```{r session, message=TRUE}
sessionInfo()
```

## WIP

```{r}
with(sla1_density, interaction.plot(x.factor = as.factor(date), trace.factor = ede1, 
                               response = density, las = 2, type = 'b'))
```
