Preparing the data
For simplicity the code used for fetching the cases_dataset is not printed, but is available in the embedded code.
First we will filter the data so we start modelling from the first recovered case.
N <- 10260893 # Portugal population, estimative for 2020
start <- min(which(cases_dataset$recuperados > 0))
end <- nrow(cases_dataset)
data <- cases_dataset[start:end, ]
data <- data %>%
mutate(
time = seq_len(end - start + 1) - 1, S = as.numeric(N - (casos_confirmados + recuperados + n_obitos)),
I = as.numeric(casos_confirmados), R = as.numeric(recuperados + n_obitos)
) %>%
select(time, S, I, R)
Initial SIR Model
Next, we compute the initial beta and gamma for the SIR Model.
S0 <- data$S[1]
I0 <- data$I[1]
R0 <- data$R[1]
S1 <- data$S[2]
I1 <- data$I[2]
R1 <- data$R[2]
S0_ <- S1 - S0
# S0_ = -beta*I0*S0/N
beta0 <- -(S0_ * N) / (I0 * S0)
I0_ <- I1 - I0
# I0_ = beta*I0*S0/N-gamma*I0
# gamma0 = (beta0*(I0*S0)/N -I0_)/I0
### OR
R0_ <- R1 - R0
# R0_ = gamma*I0
gamma0 <- R0_ / I0
beta0
[1] 0.4556289
[1] 0.00591716
This SIR function is a set of three differential equations that relates the S, I and R variables in respect with time:
\(\frac{dS}{dt} = - \frac{\beta I S}{N}\)
\(\frac{dI}{dt} = \frac{\beta I S}{N}- \gamma I\)
\(\frac{dR}{dt} = \gamma I\)
and for that we will use the ode() solver from package deSolve.
####### SIR Model #######
SIR <- function(time, state, pars) { # returns rate of change
with(as.list(c(state, pars)), {
dS <- -beta * S * I / N
dI <- beta * S * I / N - gamma * I
dR <- gamma * I
return(list(c(dS, dI, dR)))
})
}
##### Initial Parameters ########
state <- c(S = S0, I = I0, R = R0)
pars <- list(beta = beta0, gamma = gamma0)
time <- seq(0, 200, by = 1)
###### differential equations ########
out <- ode(y = state, times = time, func = SIR, parms = pars)
###### Initial Plot #############
oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
matplot(out[, 1], out[, -1],
type = "l", lty = 1:3, lwd = 2,
col = 1:3, xlab = "time, days", ylab = ""
)
legend("topright", c("S", "I", "R"),
lty = 1:3, lwd = 2, col = 1:4
)
minor.tick(2, 2, 0.7)
minor.tick(10, 10, 0.5)

Incremental SIR Model
Now we create a function that will fit the model to the available data using modFit() from package FME.
sir_step <- function(data, beta, gamma) {
state <- c(S = data$S[1], I = data$I[1], R = data$R[1])
time <- seq(0, 200, by = 1) ## output times
Objective <- function(x, parset = names(x)) {
pars[parset] <- x
out <- ode(y = state, times = time, func = SIR, parms = pars, method = method)
## Model cost
return(modCost(out, data))
}
Fit <- modFit(Objective, c(beta = beta0, gamma = gamma0))
Fit$par
R_0 <- Fit$par[1] / Fit$par[2]
R_0
out2 <- ode(y = state, times = time, func = SIR, parms = Fit$par, method = method)
return(list(beta = Fit$par[1], gamma = Fit$par[2], re = R_0, forecast = out2))
}
Here we simulate as if we get new data, and change de model accordingly.
res <- list(beta = beta0, gamma = gamma0)
invisible(saveGIF( # save all graphics in an animated gif
for (i in seq(2, nrow(data), by = 1)) {
be <- res$beta
ga <- res$gamma
slice <- 1:i
data_slice <- data[slice,]
res <- sir_step(data_slice, 0.5, 0.5)
if(i == 2) {
out <- res$forecast[1:150, ]
} else {
out[min(slice):150, ] <- res$forecast[min(slice):150, ]
}
oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
matplot(out[, 1], out[, -1],
type = "l", lty = 1:3, lwd = 2,
main = "Animated SIR",
col = 1:3, xlab = paste0("Time\n",
sprintf("R %6.2f, beta %.3f, gamma %.3f", res$re, res$beta, res$gamma)), ylab = ""
)
legend("topright", c("S", "I", "R"),
lty = 1:3, lwd = 2, col = 1:4
)
minor.tick(2, 2, 0.7)
minor.tick(10, 10, 0.5)
points(data_slice$R, pch = 16, col = "green")
points(data_slice$I, pch = 16, col = "red")
points(data_slice$S, pch = 16, col = "black")
par(oldpar)
},
"ani_sir.gif",
interval = 0.5, autobrowse = FALSE, ani.res = 96, ani.height = 500, ani.width = 800
))

For better view, here is a zoomed plot
res <- list(beta = beta0, gamma = gamma0)
invisible(saveGIF( # save all graphics in an animated gif
for (i in seq(2, nrow(data), by = 1)) {
be <- res$beta
ga <- res$gamma
slice <- 1:i
data_slice <- data[slice,]
res <- sir_step(data_slice, 0.5, 0.5)
if(i == 2) {
out <- res$forecast[1:150, ]
} else {
out[min(slice):150, ] <- res$forecast[min(slice):150, ]
}
oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
matplot(out[, 1], out[, -1],
type = "l", lty = 1:3, lwd = 2,
main = "Animated SIR Zoom",
col = 1:3, xlab = paste0("Time\n",
sprintf("R %6.2f, beta %.3f, gamma %.3f", res$re, res$beta, res$gamma)), ylab = "",
ylim = c(0, max(data$I)*1.1), xlim = c(0, nrow(data)*1.1)
)
legend("topright", c("S", "I", "R"),
lty = 1:3, lwd = 2, col = 1:4
)
minor.tick(2, 2, 0.7)
minor.tick(10, 10, 0.5)
points(data_slice$R, pch = 16, col = "green")
points(data_slice$I, pch = 16, col = "red")
points(data_slice$S, pch = 16, col = "black")
par(oldpar)
},
"ani_sir_zoom.gif",
interval = 0.5, autobrowse = FALSE, ani.res = 96, ani.height = 500, ani.width = 800
))

---
title: "HEADS - HIDA - COMPSTAT: Assignment 3"
output: 
  html_notebook: 
    fig_height: 8
    fig_width: 10
    highlight: pygments
    theme: united
    toc: yes
author: Francisco Bischoff
---

## Instructions

Consider the SIR model discussed in class. Using and adapting the code provided, deliver a report on different scenarios simulated using parameters that could be estimated from:

a) Portuguese data (all)

b) Other countries' data (all)

c) Selected periods of data (e.g. using landmark windows or sliding windows in data used to fit beta and gamma)

Submitted a PDF file with the report, explaining and interpreting the simulated scenario(s).


```{r setup, message=FALSE, warning=FALSE, include=FALSE}
knitr::opts_chunk$set(tidy.opts = list(width.cutoff = 60), tidy = TRUE)
library(deSolve)
library(lubridate)
library(Hmisc)
library(FME)
library(jsonlite)
library(dplyr)
library(animation) # animated gifs!
```

```{r load dataset, include=FALSE}
# Get data from DGS if the cache file is absent
if (!file.exists("./data/dgs.rda")) {
  dgs_cases_url <- "https://services.arcgis.com/CCZiGSEQbAxxFVh3/arcgis/rest/services/COVID19Portugal_view/FeatureServer/0/query?f=json&where=1=1&returnGeometry=false&spatialRel=esriSpatialRelIntersects&outFields=*&orderByFields=datarelatorio asc&resultOffset=0&resultRecordCount=1000"

  dgs_cases <- fromJSON(URLencode(dgs_cases_url))

  # save cache file
  save(dgs_cases, file = "./data/dgs.rda")
} else {
  # load cache file
  load("./data/dgs.rda")
}


cases_dataset <- dgs_cases[["features"]][["attributes"]]
colnames <- c(
  "id_objeto", "id_global", "data_relatorio", "casos_confirmados",
  "n_obitos", "recuperados", "casos_suspeitos", "casos_masculinos",
  "casos_femininos", "gr_etario_0_9", "gr_etario_10_19", "gr_etario_20_29",
  "gr_etario_30_39", "gr_etario_40_49", "gr_etario_50_59", "gr_etario_60_69",
  "gr_etario_70_79", "gr_etario_80_89", "gr_etario_90_99", "casos_importados",
  "casos_contacto", "sintoma_febre", "sintoma_tosse", "sintoma_dores",
  "sintoma_cefaleia", "sintoma_fraqueza", "creation_date", "creator", "edit_date",
  "editor", "casos_novos", "sintoma_difrespiratoria", "ultimo_registo",
  "estrangeiro", "casos_ativos", "aguarda_resultado", "contatos_vigilancia",
  "cadeias_transmissao", "casos_internados", "casos_internados_uci"
)
names(cases_dataset) <- colnames
cases_dataset$data_relatorio <- as.Date(as.POSIXct(cases_dataset$data_relatorio / 1000, origin = "1970-01-01"))
cases_dataset$edit_date <- as.POSIXct(cases_dataset$edit_date / 1000, origin = "1970-01-01")
cases_dataset$creation_date <- as.POSIXct(cases_dataset$creation_date / 1000, origin = "1970-01-01")

# remove rows that have all NA in a selection of columns
cases_dataset <- cases_dataset %>% filter_at(vars(casos_confirmados:sintoma_fraqueza), any_vars(!is.na(.)))

cases_dataset <- cases_dataset %>%
  select(
    id_objeto, data_relatorio, casos_confirmados, casos_novos,
    casos_suspeitos, recuperados, n_obitos, casos_masculinos, casos_femininos,
    casos_importados, casos_contacto, estrangeiro, casos_ativos, aguarda_resultado,
    gr_etario_0_9, gr_etario_10_19, gr_etario_20_29, gr_etario_30_39,
    gr_etario_40_49, gr_etario_50_59, gr_etario_60_69, gr_etario_70_79,
    gr_etario_80_89, gr_etario_90_99, contatos_vigilancia,
    casos_internados, casos_internados_uci, sintoma_febre, sintoma_tosse,
    sintoma_dores, sintoma_cefaleia, sintoma_fraqueza, sintoma_difrespiratoria
  ) %>%
  arrange(data_relatorio) %>%
  distinct_at(vars(data_relatorio:sintoma_difrespiratoria), .keep_all = TRUE) %>%
  mutate(id_objeto = 1:n())
```

## Preparing the data

For simplicity the code used for fetching the `cases_dataset` is not printed, but is available in the embedded code.

First we will filter the data so we start modelling from the first recovered case.

```{r data sir}
N <- 10260893 # Portugal population, estimative for 2020

start <- min(which(cases_dataset$recuperados > 0))
end <- nrow(cases_dataset)

data <- cases_dataset[start:end, ]
data <- data %>%
  mutate(
    time = seq_len(end - start + 1) - 1, S = as.numeric(N - (casos_confirmados + recuperados + n_obitos)),
    I = as.numeric(casos_confirmados), R = as.numeric(recuperados + n_obitos)
  ) %>%
  select(time, S, I, R)
```

## Initial SIR Model

Next, we compute the initial beta and gamma for the SIR Model.

```{r}
S0 <- data$S[1]
I0 <- data$I[1]
R0 <- data$R[1]

S1 <- data$S[2]
I1 <- data$I[2]
R1 <- data$R[2]

S0_ <- S1 - S0
# S0_ = -beta*I0*S0/N
beta0 <- -(S0_ * N) / (I0 * S0)


I0_ <- I1 - I0
# I0_ = beta*I0*S0/N-gamma*I0
# gamma0 = (beta0*(I0*S0)/N -I0_)/I0

### OR

R0_ <- R1 - R0
# R0_  = gamma*I0
gamma0 <- R0_ / I0

beta0
gamma0
```

This SIR function is a set of three differential equations that relates the S, I and R variables in respect with time:

$\frac{dS}{dt} = - \frac{\beta I S}{N}$

$\frac{dI}{dt} = \frac{\beta I S}{N}- \gamma I$

$\frac{dR}{dt} = \gamma I$

and for that we will use the `ode()` solver from package `deSolve`.

```{r first model, fig.height=7, fig.width=10}
####### SIR Model #######
SIR <- function(time, state, pars) { # returns rate of change
  with(as.list(c(state, pars)), {
    dS <- -beta * S * I / N
    dI <- beta * S * I / N - gamma * I
    dR <- gamma * I
    return(list(c(dS, dI, dR)))
  })
}

##### Initial Parameters ########
state <- c(S = S0, I = I0, R = R0)
pars <- list(beta = beta0, gamma = gamma0)
time <- seq(0, 200, by = 1)

###### differential equations ########
out <- ode(y = state, times = time, func = SIR, parms = pars)

###### Initial Plot #############
oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
matplot(out[, 1], out[, -1],
  type = "l", lty = 1:3, lwd = 2,
  col = 1:3, xlab = "time, days", ylab = ""
)
legend("topright", c("S", "I", "R"),
  lty = 1:3, lwd = 2, col = 1:4
)
minor.tick(2, 2, 0.7)
minor.tick(10, 10, 0.5)
par(oldpar)
```

## Incremental SIR Model

Now we create a function that will fit the model to the available data using `modFit()` from package `FME`.

```{r sir_step function}
sir_step <- function(data, beta, gamma) {

  state <- c(S = data$S[1], I = data$I[1], R = data$R[1])

  time <- seq(0, 200, by = 1) ## output times
    
  Objective <- function(x, parset = names(x)) {
    pars[parset] <- x
    out <- ode(y = state, times = time, func = SIR, parms = pars, method = method)
    ## Model cost
    return(modCost(out, data))
  }
  
  Fit <- modFit(Objective, c(beta = beta0, gamma = gamma0))
  
  Fit$par
  R_0 <- Fit$par[1] / Fit$par[2]
  R_0
  
  out2 <- ode(y = state, times = time, func = SIR, parms = Fit$par, method = method)

  return(list(beta = Fit$par[1], gamma = Fit$par[2], re = R_0, forecast = out2))
}

```

Here we simulate as if we get new data, and change de model accordingly.

```{r animated sir, fig.height=7, fig.width=10}

res <- list(beta = beta0, gamma = gamma0)

invisible(saveGIF( # save all graphics in an animated gif
  for (i in seq(2, nrow(data), by = 1)) {
    be <- res$beta
    ga <- res$gamma
    
    slice <- 1:i
    
    data_slice <- data[slice,]

    res <- sir_step(data_slice, 0.5, 0.5)
    
    if(i == 2) {
      out <- res$forecast[1:150, ]
    } else {
      out[min(slice):150, ] <- res$forecast[min(slice):150, ]
    }
    
    oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
    matplot(out[, 1], out[, -1],
      type = "l", lty = 1:3, lwd = 2,
      main = "Animated SIR",
      col = 1:3, xlab = paste0("Time\n", 
                               sprintf("R %6.2f, beta %.3f, gamma %.3f", res$re, res$beta, res$gamma)), ylab = ""
    )
    legend("topright", c("S", "I", "R"),
      lty = 1:3, lwd = 2, col = 1:4
    )
    minor.tick(2, 2, 0.7)
    minor.tick(10, 10, 0.5)
    
    points(data_slice$R, pch = 16, col = "green")
    points(data_slice$I, pch = 16, col = "red")
    points(data_slice$S, pch = 16, col = "black")
    
    par(oldpar)
  },
  "ani_sir.gif",
  interval = 0.5, autobrowse = FALSE, ani.res = 96, ani.height = 500, ani.width = 800
))
```

![](ani_sir.gif)

For better view, here is a zoomed plot

```{r animated sir zoom, fig.height=7, fig.width=10}

res <- list(beta = beta0, gamma = gamma0)

invisible(saveGIF( # save all graphics in an animated gif
  for (i in seq(2, nrow(data), by = 1)) {
    be <- res$beta
    ga <- res$gamma
    
    slice <- 1:i
    
    data_slice <- data[slice,]

    res <- sir_step(data_slice, 0.5, 0.5)
    
    if(i == 2) {
      out <- res$forecast[1:150, ]
    } else {
      out[min(slice):150, ] <- res$forecast[min(slice):150, ]
    }
    
    oldpar <- par(las = 1, tcl = 0.5, mgp = c(3, 0.8, 0), bty = "l")
    matplot(out[, 1], out[, -1],
      type = "l", lty = 1:3, lwd = 2,
      main = "Animated SIR Zoom",
      col = 1:3, xlab = paste0("Time\n", 
                               sprintf("R %6.2f, beta %.3f, gamma %.3f", res$re, res$beta, res$gamma)), ylab = "",
      ylim = c(0, max(data$I)*1.1), xlim = c(0, nrow(data)*1.1)
    )
    legend("topright", c("S", "I", "R"),
      lty = 1:3, lwd = 2, col = 1:4
    )
    minor.tick(2, 2, 0.7)
    minor.tick(10, 10, 0.5)
    
    points(data_slice$R, pch = 16, col = "green")
    points(data_slice$I, pch = 16, col = "red")
    points(data_slice$S, pch = 16, col = "black")
    
    par(oldpar)
  },
  "ani_sir_zoom.gif",
  interval = 0.5, autobrowse = FALSE, ani.res = 96, ani.height = 500, ani.width = 800
))
```

![](ani_sir_zoom.gif)
