A bit of context
In this exercise, we will see how to make a color plot of \(4\pi r^2\times G(r,t)\) data obtained from Molecular Dynamics simulations. These files can be downloaded here. These auto-correlators \(G(r,t)\) are obtained from MD trajectories of a fluid encapsulated in a porous medium by computing the probability that each molecule moves by a distance \(r\) over a time \(t\). The MD trajectories are performed with LAMMPS and the trajectories treated by a home-made C program producing these files.
In these simulations, we varied the depth of the interaction well. It is given in the name of the file such as Grt_xx.dat
, where xx = 0.01, 0.1, 0.2, 0.3, 0.5, 0.8, 1 corresponds to \(\varepsilon/k_BT\). \(\varepsilon/k_BT\) is the depth of the interaction well in units of temperature.
The Grt_xx.dat
files contain the \(4\pi r^2\times G(r,t)\) data under the form of a matrix, with \(r\) increasing with the rows and \(t\) with the columns. \(r\) goes from 0 to 20 Å and \(t\) goes from 0 to 200 ps.
Plotting data
We should have a Grt
dataset that looks like this:
## # A tibble: 2,815,407 x 4
## r.A t.ps r2Grt epskt
## <dbl> <dbl> <dbl> <dbl>
## 1 0 0 77.7 0.01
## 2 0 0.1 0.000512 0.01
## 3 0 0.2 0.000203 0.01
## 4 0 0.3 0.000148 0.01
## 5 0 0.4 0.0000979 0.01
## 6 0 0.5 0.0000817 0.01
## 7 0 0.6 0.0000714 0.01
## 8 0 0.7 0.0000683 0.01
## 9 0 0.8 0.0000687 0.01
## 10 0 0.9 0.0000552 0.01
## # … with 2,815,397 more rows
We will now plot this as a colored heatmap using geom_raster
from ggplot2
:
- We will first plot
Grt
only for times below 100 ps and \(\varepsilon/k_BT=0.5\), so recursively filter the data accordingly, then provide this to ggplot
- Use a nicer axis labels
- Do you see anything on the plot?
- In fact, we need to saturate values above a certain limit in order to see the fine evolution of the \(G(r,t)\) auto-correlator. Add a mutation of the tibble attributing the limit value to all points above this limit, and play with the limit value in order to have a nicer plot.
- Add a vertical dashed line in x=8.18Å marking the mean pore size for this structure.
- Use a nicer color scheme with more colors in order to better see the variations.
lim <- 0.1
nbreak <- 6
colors <- colorRampPalette(c("white","royalblue","seagreen","orange","red","brown"))(50)
Grt %>%
filter(t.ps<=100, epskt==0.5) %>%
mutate(r2Grt=ifelse(r2Grt>lim, lim, r2Grt)) %>%
ggplot(aes(x=r.A, y=t.ps, fill=r2Grt))+
geom_raster()+
geom_vline(aes(xintercept=8.18), lty=2)+
scale_fill_gradientn(
colors = colors,
name = '',
breaks = seq(0, lim, length=nbreak),
labels = c(seq(0, lim, length=nbreak)[1:(nbreak-1)], paste(">",lim))
) +
labs(x = "r [Å]", y="Time [ps]") +
scale_x_continuous(expand = c(0,0)) +
scale_y_continuous(expand = c(0,0))
Now we want to see the evolution of \(G(r,t)\) as a function of \(\varepsilon/k_BT\). Using the procedure above, plot \(G(r,t)\) for all \(\varepsilon/k_BT\) on a grid.
lim <- 0.1
nbreak <- 6
colors <- colorRampPalette(c("white","royalblue","seagreen","orange","red","brown"))(50)
Grt %>%
filter(t.ps<=100) %>%
mutate(r2Grt=ifelse(r2Grt>lim, lim, r2Grt)) %>%
ggplot(aes(x=r.A, y=t.ps, fill=r2Grt))+
geom_raster()+
geom_vline(aes(xintercept=8.18), lty=2)+
scale_fill_gradientn(
colors = colors,
name = '',
breaks = seq(0, lim, length=nbreak),
labels = c(seq(0, lim, length=nbreak)[1:(nbreak-1)], paste(">",lim))
) +
labs(x = "r [Å]", y="Time [ps]") +
scale_x_continuous(expand = c(0,0)) +
scale_y_continuous(expand = c(0,0)) +
facet_wrap(~epskt)
---
title : "R Exercises - G(r,t)"
date  : "2020-07-07"
output: 
    html_document:
        toc            : true
        toc_float      : true
        toc_depth      : 4
        highlight      : tango
        number_sections: true
        code_download  : true
params: 
    solution:
        value: true
---

```{r setup, include=FALSE, warning = FALSE, cache=FALSE}
library(plotly)
library(ggplot2)
library(tidyverse)
my_theme <- theme_bw()+
            theme(axis.text = element_text(size = 14,colour="black"),
                  text = element_text(size = 14),
                  axis.ticks = element_blank(),
                  plot.title = element_text(size=14),
                  legend.text = element_text(size = 14,colour="black"),
                  legend.title = element_text(size = 14,colour="black"),
                  panel.border = element_rect(colour = "black", fill=NA, size=1),
                  panel.grid.major = element_blank(),
                  panel.grid.minor = element_blank(),
                  legend.key.height=unit(1,"cm"),
                  legend.justification = "center",
                  strip.background = element_blank(),
                  strip.text=element_text(size = 14),
                  strip.text.y = element_text(angle=0),
                  panel.spacing = unit(1, "lines")
                  )
theme_set(my_theme)
```

# A bit of context

In this exercise, we will see how to make a color plot of $4\pi r^2\times G(r,t)$ data obtained from Molecular Dynamics simulations.
These files can be downloaded <a href="Data/Grt.zip" download target="_blank">here</a>.
These auto-correlators $G(r,t)$ are obtained from MD trajectories of a fluid encapsulated in a porous medium by computing the probability that each molecule moves by a distance $r$ over a time $t$. The MD trajectories are performed with [LAMMPS](https://lammps.sandia.gov/) and the trajectories treated by a home-made C program producing these files.

In these simulations, we varied the depth of the interaction well. It is given in the name of the file such as `Grt_xx.dat`, where xx = 0.01, 0.1, 0.2, 0.3, 0.5, 0.8, 1 corresponds to $\varepsilon/k_BT$. $\varepsilon/k_BT$ is the depth of the interaction well in units of temperature.

The `Grt_xx.dat` files contain the $4\pi r^2\times G(r,t)$ data under the form of a matrix, with $r$ increasing with the rows and $t$ with the columns. $r$ goes from 0 to 20 Å and $t$ goes from 0 to 200 ps.

# Reading and tidying the data

We want to read all data files and store them into a tidy tibble for ease of plotting.

- Load the `tidyverse` and `ggplot2` packages
- Find all files starting by "Grt" and store them in a vector `Grt_files`
- Initiate an empty tibble `Grt` that will store all data
- Using a `for` loop:
    - read the files
    - add columns names as the times values
    - add the `r.A` column containing the r values
    - and recursively (using the pipe `%>%`) 
        - pivot the table to make it tidy, with the columns `r.A`, `t.ps` and `r2Grt`
        - make sure that the times are read as numeric values
        - add the `epskt` column containing the $\varepsilon/k_BT$ value
    - store this in `Grt`


```{r include=params$solution, warning = FALSE, message=FALSE, cache=FALSE}
library(tidyverse)
library(ggplot2)
Grt_files <- list.files(pattern = "Grt_", path="Data")
Grt       <- tibble()
for(Grt_file in Grt_files){#Grt_file <- Grt_files[1]
    d <- read_table2(file.path("Data",Grt_file), col_names=FALSE)
    names(d) <- as.character(seq(0,200, length=ncol(d)))
    d$r.A    <- seq(0,20, length=nrow(d))
    eps <- gsub(".dat","",gsub("Grt_","",Grt_file))
    d <- d %>% 
        pivot_longer(cols=-r.A,
                     names_to="t.ps",
                     names_transform=list(t.ps = as.numeric),
                     values_to="r2Grt") %>% 
        mutate(epskt=as.numeric(eps))
    Grt <- bind_rows(Grt, d)
}
```

# Plotting data

We should have a `Grt` dataset that looks like this:

```{r include=TRUE, warning = FALSE, message=FALSE, cache=FALSE}
Grt
```

We will now plot this as a colored heatmap using `geom_raster` from `ggplot2`:

- We will first plot `Grt` only for times below 100 ps and $\varepsilon/k_BT=0.5$, so recursively filter the data accordingly, then provide this to `ggplot`
+ Use a nicer axis labels
+ Do you see anything on the plot?
+ In fact, we need to saturate values above a certain limit in order to see the fine evolution of the $G(r,t)$ auto-correlator. Add a mutation of the tibble attributing the limit value to all points above this limit, and play with the limit value in order to have a nicer plot.
- Add a vertical dashed line in x=8.18Å marking the mean pore size for this structure.
- Use a nicer color scheme with more colors in order to better see the variations.

```{r include=params$solution, warning = FALSE, message=FALSE, cache=FALSE}
lim    <- 0.1
nbreak <- 6
colors <- colorRampPalette(c("white","royalblue","seagreen","orange","red","brown"))(50)
Grt %>% 
    filter(t.ps<=100, epskt==0.5) %>% 
    mutate(r2Grt=ifelse(r2Grt>lim, lim, r2Grt)) %>% 
    ggplot(aes(x=r.A, y=t.ps, fill=r2Grt))+
        geom_raster()+
        geom_vline(aes(xintercept=8.18), lty=2)+
        scale_fill_gradientn(
            colors = colors, 
            name   = '',
            breaks = seq(0, lim, length=nbreak), 
            labels = c(seq(0, lim, length=nbreak)[1:(nbreak-1)], paste(">",lim)) 
        ) +
        labs(x = "r [Å]", y="Time [ps]") +
        scale_x_continuous(expand = c(0,0)) + 
        scale_y_continuous(expand = c(0,0))
```


Now we want to see the evolution of $G(r,t)$ as a function of $\varepsilon/k_BT$. Using the procedure above, plot $G(r,t)$ for all 
$\varepsilon/k_BT$ on a grid.

```{r include=params$solution, warning = FALSE, message=FALSE, cache=FALSE}
lim    <- 0.1
nbreak <- 6
colors <- colorRampPalette(c("white","royalblue","seagreen","orange","red","brown"))(50)
Grt %>% 
    filter(t.ps<=100) %>% 
    mutate(r2Grt=ifelse(r2Grt>lim, lim, r2Grt)) %>% 
    ggplot(aes(x=r.A, y=t.ps, fill=r2Grt))+
        geom_raster()+
        geom_vline(aes(xintercept=8.18), lty=2)+
        scale_fill_gradientn(
            colors = colors, 
            name   = '',
            breaks = seq(0, lim, length=nbreak), 
            labels = c(seq(0, lim, length=nbreak)[1:(nbreak-1)], paste(">",lim)) 
        ) +
        labs(x = "r [Å]", y="Time [ps]") +
        scale_x_continuous(expand = c(0,0)) + 
        scale_y_continuous(expand = c(0,0)) +
        facet_wrap(~epskt)
```

