# Modeling pandemics (1)

**R-english – Freakonometrics**, and kindly contributed to R-bloggers]. (You can report issue about the content on this page here)

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The most popular model to model epidemics is the so-called SIR model – or Kermack-McKendrick. Consider a population of size \(N\), and assume that \(S\) is the number of susceptible, \(I\) the number of infectious, and \(R\) for the number recovered (or immune) individuals, \(\displaystyle {\begin{aligned}&{\frac {dS}{dt}}=-{\frac {\beta IS}{N}},\\[6pt]&{\frac {dI}{dt}}={\frac {\beta IS}{N}}-\gamma I,\\[6pt]&{\frac {dR}{dt}}=\gamma I,\end{aligned}}\)so that \(\displaystyle{{\frac{dS}{dt}}+{\frac {dI}{dt}}+{\frac {dR}{dt}}=0}\)which implies that \(S+I+R=N\). In order to be more realistic, consider some (constant) birth rate \(\mu\), so that the model becomes\(\displaystyle {\begin{aligned}&{\frac {dS}{dt}}=\mu(N-S)-{\frac {\beta IS}{N}},\\[6pt]&{\frac {dI}{dt}}={\frac {\beta IS}{N}}-(\gamma+\mu) I,\\[6pt]&{\frac {dR}{dt}}=\gamma I-\mu R,\end{aligned}}\)Note, in this model, that people get sick (infected) but they do not die, they recover. So here, we can model chickenpox, for instance, not SARS.

The dynamics of the infectious class depends on the following ratio:\(\displaystyle{R_{0}={\frac {\beta }{\gamma +\mu}}}\) which is the so-called basic reproduction number (or reproductive ratio). The effective reproductive ratio is \(R_0S/N\), and the turnover of the epidemic happens exactly when \(R_0S/N=1\), or when the fraction of remaining susceptibles is \(R_0^{-1}\). As shown in Directly transmitted infectious diseases:Control by vaccination, if \(S/N

Want to see it ? Start with

mu = 0 beta = 2 gamma = 1/2

for the parameters. Here, [latex]R_0=4\). We also need starting values

epsilon = .001 N = 1 S = 1-epsilon I = epsilon R = 0

Then use the ordinary differential equation solver, in R. The idea is to say that \(\boldsymbol{Z}=(S,I,R)\) and we have the gradient \(\frac{\partial \boldsymbol{Z}}{\partial t} = SIR(\boldsymbol{Z})\)where \(SIR\) is function of the various parameters. Hence, set

p = c(mu = 0, N = 1, beta = 2, gamma = 1/2) start_SIR = c(S = 1-epsilon, I = epsilon, R = 0)

The we must define the time, and the function that returns the gradient,

times = seq(0, 10, by = .1) SIR = function(t,Z,p){ S=Z[1]; I=Z[2]; R=Z[3]; N=S+I+R mu=p["mu"]; beta=p["beta"]; gamma=p["gamma"] dS=mu*(N-S)-beta*S*I/N dI=beta*S*I/N-(mu+gamma)*I dR=gamma*I-mu*R dZ=c(dS,dI,dR) return(dZ)}

To solve this problem use

library(deSolve) resol = ode(y=start_SIR, times=times, func=SIR, parms=p)

We can visualize the dynamics below

par(mfrow=c(1,2)) t=resol[,"time"] plot(t,resol[,"S"],type="l",xlab="time",ylab="") lines(t,resol[,"I"],col="red") lines(t,resol[,"R"],col="blue") plot(t,t*0+1,type="l",xlab="time",ylab="",ylim=0:1) polygon(c(t,rev(t)),c(resol[,"R"],rep(0,nrow(resol))),col="blue") polygon(c(t,rev(t)),c(resol[,"R"]+resol[,"I"],rev(resol[,"R"])),col="red")

We can actually also visualize the effective reproductive number is \(R_0S/N\), where

R0=p["beta"]/(p["gamma"]+p["mu"])

The effective reproductive number is on the left, and as we mentioned above, when we reach 1, we actually reach the maximum of the infected,

plot(t,resol[,"S"]*R0,type="l",xlab="time",ylab="") abline(h=1,lty=2,col="red") abline(v=max(t[resol[,"S"]*R0>=1]),col="darkgreen") points(max(t[resol[,"S"]*R0>=1]),1,pch=19) plot(t,resol[,"S"],type="l",xlab="time",ylab="",col="grey") lines(t,resol[,"I"],col="red",lwd=3) lines(t,resol[,"R"],col="light blue") abline(v=max(t[resol[,"S"]*R0>=1]),col="darkgreen") points(max(t[resol[,"S"]*R0>=1]),max(resol[,"I"]),pch=19)

And when adding a \(\mu\) parameter, we can obtain some interesting dynamics on the number of infected,

times = seq(0, 100, by=.1) p = c(mu = 1/100, N = 1, beta = 50, gamma = 10) start_SIR = c(S=0.19, I=0.01, R = 0.8) resol = ode(y=start_SIR, t=times, func=SIR, p=p) plot(resol[,"time"],resol[,"I"],type="l",xlab="time",ylab="")

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