Compartmental models in epidemiology

Compartmental models are a very general modelling technique. They are often applied to the mathematical modelling of infectious diseases. The population is assigned to compartments with labels – for example, S, I, or R, (Susceptible, Infectious, or Recovered). People may progress between compartments. The order of the labels usually shows the flow patterns between the compartments; for example SEIS means susceptible, exposed, infectious, then susceptible again.

The origin of such models is the early 20th century, with important works being that of Ross^[1] in 1916, Ross and Hudson in 1917,^[2][3] Kermack and McKendrick in 1927,^[4] and Kendall in 1956.^[5] The Reed–Frost model was also a significant and widely overlooked ancestor of modern epidemiological modelling approaches.^[6]

The models are most often run with ordinary differential equations (which are deterministic), but can also be used with a stochastic (random) framework, which is more realistic but much more complicated to analyze.

These models are used to analyze the disease dynamics and to estimate the total number of infected people, the total number of recovered people, and to estimate epidemiological parameters such as the basic reproduction number or effective reproduction number. Such models can show how different public health interventions may affect the outcome of the epidemic.

The SIR model^{[7][8][9][10]} is one of the simplest compartmental models, and many models are derivatives of this basic form. The model consists of three compartments:

S: The number of susceptible individuals. When a susceptible and an infectious individual come into "infectious contact", the susceptible individual contracts the disease and transitions to the infectious compartment.

I: The number of infectious individuals. These are individuals who have been infected and are capable of infecting susceptible individuals.

R for the number of removed (and immune) or deceased individuals. These are individuals who have been infected and have either recovered from the disease and entered the removed compartment, or died. It is assumed that the number of deaths is negligible with respect to the total population. This compartment may also be called "recovered" or "resistant".

This model is reasonably predictive^[11] for infectious diseases that are transmitted from human to human, and where recovery confers lasting resistance, such as measles, mumps, and rubella.

These variables (S, I, and R) represent the number of people in each compartment at a particular time. To represent that the number of susceptible, infectious, and removed individuals may vary over time (even if the total population size remains constant), we make the precise numbers a function of t (time): S(t), I(t), and R(t). For a specific disease in a specific population, these functions may be worked out in order to predict possible outbreaks and bring them under control.^[11] Note that in the SIR model, ${\displaystyle R(0)}$ and ${\displaystyle R_{0}}$ are different quantities – the former describes the number of recovered at t = 0 whereas the latter describes the ratio between the frequency of contacts to the frequency of recovery.

As implied by the variable function of t, the model is dynamic in that the numbers in each compartment may fluctuate over time. The importance of this dynamic aspect is most obvious in an endemic disease with a short infectious period, such as measles in the UK prior to the introduction of a vaccine in 1968. Such diseases tend to occur in cycles of outbreaks due to the variation in number of susceptibles (S(t)) over time. During an epidemic, the number of susceptible individuals falls rapidly as more of them are infected and thus enter the infectious and removed compartments. The disease cannot break out again until the number of susceptibles has built back up, e.g. as a result of offspring being born into the susceptible compartment.^{[citation needed]}

Each member of the population typically progresses from susceptible to infectious to recovered. This can be shown as a flow diagram in which the boxes represent the different compartments and the arrows the transition between compartments (see diagram).

For the full specification of the model, the arrows should be labeled with the transition rates between compartments. Between S and I, the transition rate is assumed to be ${\displaystyle d(S/N)/dt=-\beta SI/N^{2}}$, where ${\displaystyle N}$ is the total population, ${\displaystyle \beta }$ is the average number of contacts per person per time, multiplied by the probability of disease transmission in a contact between a susceptible and an infectious subject, and ${\displaystyle SI/N^{2}}$ is the fraction of all possible contacts that involves an infectious and susceptible individual. (This is mathematically similar to the law of mass action in chemistry in which random collisions between molecules result in a chemical reaction and the fractional rate is proportional to the concentration of the two reactants.^[12])

Between I and R, the transition rate is assumed to be proportional to the number of infectious individuals which is ${\displaystyle \gamma I}$. If an individual is infectious for an average time period ${\displaystyle D}$, then ${\displaystyle \gamma =1/D}$. This is also equivalent to the assumption that the length of time spent by an individual in the infectious state is a random variable with an exponential distribution. The "classical" SIR model may be modified by using more complex and realistic distributions for the I-R transition rate (e.g. the Erlang distribution).^[13]

For the special case in which there is no removal from the infectious compartment (${\displaystyle \gamma =0}$), the SIR model reduces to a very simple SI model, which has a logistic solution, in which every individual eventually becomes infected.

The dynamics of an epidemic, for example, the flu, are often much faster than the dynamics of birth and death, therefore, birth and death are often omitted in simple compartmental models. The SIR system without so-called vital dynamics (birth and death, sometimes called demography) described above can be expressed by the following system of ordinary differential equations:^[8][14]

${\displaystyle \left\{{\begin{aligned}&{\frac {dS}{dt}}=-\beta IS,\\[6pt]&{\frac {dI}{dt}}=\beta IS-\gamma I,\\[6pt]&{\frac {dR}{dt}}=\gamma I,\end{aligned}}\right.}$

where ${\displaystyle S}$ is the stock of susceptible population, ${\displaystyle I}$ is the stock of infected, ${\displaystyle R}$ is the stock of removed population (either by death or recovery), and ${\displaystyle N}$ is the sum of these three.

This model was for the first time proposed by William Ogilvy Kermack and Anderson Gray McKendrick as a special case of what we now call Kermack–McKendrick theory, and followed work McKendrick had done with Ronald Ross.^{[citation needed]}

This system is non-linear, however it is possible to derive its analytic solution in implicit form.^[7] Firstly note that from:

${\displaystyle {\frac {dS}{dt}}+{\frac {dI}{dt}}+{\frac {dR}{dt}}=0,}$

it follows that:

${\displaystyle S(t)+I(t)+R(t)={\text{constant}}=N,}$

expressing in mathematical terms the constancy of population ${\displaystyle N}$. Note that the above relationship implies that one need only study the equation for two of the three variables.

Secondly, we note that the dynamics of the infectious class depends on the following ratio:

${\displaystyle R_{0}={\frac {\beta }{\gamma }},}$

the so-called basic reproduction number (also called basic reproduction ratio). This ratio is derived as the expected number of new infections (these new infections are sometimes called secondary infections) from a single infection in a population where all subjects are susceptible.^[15][16] This idea can probably be more readily seen if we say that the typical time between contacts is ${\displaystyle T_{c}=\beta ^{-1}}$, and the typical time until removal is ${\displaystyle T_{r}=\gamma ^{-1}}$. From here it follows that, on average, the number of contacts by an infectious individual with others before the infectious has been removed is: ${\displaystyle T_{r}/T_{c}.}$

By dividing the first differential equation by the third, separating the variables and integrating we get

${\displaystyle S(t)=S(0)e^{-R_{0}(R(t)-R(0))/N},}$

where ${\displaystyle S(0)}$ and ${\displaystyle R(0)}$ are the initial numbers of, respectively, susceptible and removed subjects. Writing ${\displaystyle s_{0}=S(0)/N}$ for the initial proportion of susceptible individuals, and ${\displaystyle s_{\infty }=S(\infty )/N}$ and ${\displaystyle r_{\infty }=R(\infty )/N}$ for the proportion of susceptible and removed individuals respectively in the limit ${\displaystyle t\to \infty ,}$ one has

${\displaystyle s_{\infty }=1-r_{\infty }=s_{0}e^{-R_{0}(r_{\infty }-r_{0})}}$

(note that the infectious compartment empties in this limit). This transcendental equation has a solution in terms of the Lambert W function,^[17] namely

${\displaystyle s_{\infty }=1-r_{\infty }=-R_{0}^{-1}\,W(-s_{0}R_{0}e^{-R_{0}(1-r_{0})}).}$

This shows that at the end of an epidemic that conforms to the simple assumptions of the SIR model, unless ${\displaystyle s_{0}=0}$, not all individuals of the population have been removed, so some must remain susceptible. A driving force leading to the end of an epidemic is a decline in the number of infectious individuals. The epidemic does not typically end because of a complete lack of susceptible individuals.

The role of both the basic reproduction number and the initial susceptibility are extremely important. In fact, upon rewriting the equation for infectious individuals as follows:

${\displaystyle {\frac {dI}{dt}}=\left(R_{0}{\frac {S}{N}}-1\right)\gamma I,}$

it yields that if:

${\displaystyle R_{0}\cdot S(0)>N,}$

then:

${\displaystyle {\frac {dI}{dt}}(0)>0,}$

i.e., there will be a proper epidemic outbreak with an increase of the number of the infectious (which can reach a considerable fraction of the population). On the contrary, if

${\displaystyle R_{0}\cdot S(0)<N,}$

then

${\displaystyle {\frac {dI}{dt}}(0)<0,}$

i.e., independently from the initial size of the susceptible population the disease can never cause a proper epidemic outbreak. As a consequence, it is clear that both the basic reproduction number and the initial susceptibility are extremely important.

Note that in the above model the function:

${\displaystyle F=\beta I,}$

models the transition rate from the compartment of susceptible individuals to the compartment of infectious individuals, so that it is called the force of infection. However, for large classes of communicable diseases it is more realistic to consider a force of infection that does not depend on the absolute number of infectious subjects, but on their fraction (with respect to the total constant population ${\displaystyle N}$):

${\displaystyle F=\beta {\frac {I}{N}}.}$

Capasso^[18] and, afterwards, other authors have proposed nonlinear forces of infection to model more realistically the contagion process.

In 2014, Harko and coauthors derived an exact so-called analytical solution (involving an integral that can only be calculated numerically) to the SIR model.^[7] In the case without vital dynamics setup, for ${\displaystyle {\mathcal {S}}(u)=S(t)}$, etc., it corresponds to the following time parametrization

${\displaystyle {\mathcal {S}}(u)=S(0)u}$

${\displaystyle {\mathcal {I}}(u)=N-{\mathcal {R}}(u)-{\mathcal {S}}(u)}$

${\displaystyle {\mathcal {R}}(u)=R(0)-\rho \ln(u)}$

for

${\displaystyle t={\frac {N}{\beta }}\int _{u}^{1}{\frac {du^{*}}{u^{*}{\mathcal {I}}(u^{*})}},\quad \rho ={\frac {\gamma N}{\beta }},}$

with initial conditions

${\displaystyle ({\mathcal {S}}(1),{\mathcal {I}}(1),{\mathcal {R}}(1))=(S(0),N-R(0)-S(0),R(0)),\quad u_{T}<u<1,}$

where ${\displaystyle u_{T}}$ satisfies ${\displaystyle {\mathcal {I}}(u_{T})=0}$. By the transcendental equation for ${\displaystyle R_{\infty }}$ above, it follows that ${\displaystyle u_{T}=e^{-(R_{\infty }-R(0))/\rho }(=S_{\infty }/S(0)}$, if ${\displaystyle S(0)\neq 0)}$ and ${\displaystyle I_{\infty }=0}$.

An equivalent so-called analytical solution (involving an integral that can only be calculated numerically) found by Miller^[19][20] yields

${\displaystyle {\begin{aligned}S(t)&=S(0)e^{-\xi (t)}\\[8pt]I(t)&=N-S(t)-R(t)\\[8pt]R(t)&=R(0)+\rho \xi (t)\\[8pt]\xi (t)&={\frac {\beta }{N}}\int _{0}^{t}I(t^{*})\,dt^{*}\end{aligned}}}$

Here ${\displaystyle \xi (t)}$ can be interpreted as the expected number of transmissions an individual has received by time ${\displaystyle t}$. The two solutions are related by ${\displaystyle e^{-\xi (t)}=u}$.

Effectively the same result can be found in the original work by Kermack and McKendrick.^[4]

These solutions may be easily understood by noting that all of the terms on the right-hand sides of the original differential equations are proportional to ${\displaystyle I}$. The equations may thus be divided through by ${\displaystyle I}$, and the time rescaled so that the differential operator on the left-hand side becomes simply ${\displaystyle d/d\tau }$, where ${\displaystyle d\tau =Idt}$, i.e. ${\displaystyle \tau =\int Idt}$. The differential equations are now all linear, and the third equation, of the form ${\displaystyle dR/d\tau =}$ const., shows that ${\displaystyle \tau }$ and ${\displaystyle R}$ (and ${\displaystyle \xi }$ above) are simply linearly related.

A highly accurate analytic approximant of the SIR model as well as exact analytic expressions for the final values ${\displaystyle S_{\infty }}$, ${\displaystyle I_{\infty }}$, and ${\displaystyle R_{\infty }}$ were provided by Kröger and Schlickeiser,^[9] so that there is no need to perform a numerical integration to solve the SIR model (a simplified example practice on COVID-19 numerical simulation using Microsoft Excel can be found here ^[21]), to obtain its parameters from existing data, or to predict the future dynamics of an epidemics modeled by the SIR model. The approximant involves the Lambert W function which is part of all basic data visualization software such as Microsoft Excel, MATLAB, and Mathematica.

While Kendall^[5] considered the so-called all-time SIR model where the initial conditions ${\displaystyle S(0)}$, ${\displaystyle I(0)}$, and ${\displaystyle R(0)}$ are coupled through the above relations, Kermack and McKendrick^[4] proposed to study the more general semi-time case, for which ${\displaystyle S(0)}$ and ${\displaystyle I(0)}$ are both arbitrary. This latter version, denoted as semi-time SIR model,^[9] makes predictions only for future times ${\displaystyle t>0}$. An analytic approximant and exact expressions for the final values are available for the semi-time SIR model as well.^[10]

Numerical solutions to the SIR model can be found in the literature. An example is using the model to analyze COVID-19 spreading data.^[21][22] Three reproduction numbers can be pulled out from the data analyzed with numerical approximation,

the basic reproduction number:

${\displaystyle R_{0}={\frac {\beta _{0}}{\gamma _{0}}}}$

the real-time reproduction number:

${\displaystyle R_{t}={\frac {\beta _{t}}{\gamma _{t}}}}$

and the real-time effective reproduction number:

${\displaystyle R_{e}={\frac {\beta _{t}S}{\gamma _{t}N}}}$

${\displaystyle R_{0}}$ represents the speed of reproduction rate at the beginning of the spreading when all populations are assumed susceptible, e.g. if ${\displaystyle \beta _{0}=0.4day^{-1}}$ and ${\displaystyle \gamma _{0}=0.2day^{-1}}$ meaning one infectious person on average infects 0.4 susceptible people per day and recovers in 1/0.2=5 days. Thus when this person recovered, there are two people still infectious directly got from this person and ${\displaystyle R_{0}=2}$, i.e. the number of infectious people doubled in one cycle of 5 days. The data simulated by the model with ${\displaystyle R_{0}=2}$ or real data fitted will yield a doubling of the number of infectious people faster than 5 days because the two infected people are infecting people. From the SIR model, we can tell that ${\displaystyle \beta }$ is determined by the nature of the disease and also a function of the interactive frequency between the infectious person ${\displaystyle I}$ with the susceptible people ${\displaystyle S}$ and also the intensity/duration of the interaction like how close they interact for how long and whether or not they both wear masks, thus, it changes over time when the average behavior of the carriers and susceptible people changes. The model use ${\displaystyle SI}$ to represent these factors but it indeed is referenced to the initial stage when no action is taken to prevent the spread and all population is susceptible, thus all changes are absorbed by the change of ${\displaystyle \beta }$.

${\displaystyle \gamma }$ is usually more stable over time assuming when the infectious person shows symptoms, she/he will seek medical attention or be self-isolated. So if we find ${\displaystyle R_{t}}$ changes, most probably the behaviors of people in the community have changed from their normal patterns before the outbreak, or the disease has mutated to a new form. Costive massive detection and isolation of susceptible close contacts have effects on reducing ${\displaystyle 1/\gamma }$ but whose efficiencies are under debate. This debate is largely on the uncertainty of the number of days reduced from after infectious or detectable whichever comes first to before a symptom shows up for an infected susceptible person. If the person is infectious after symptoms show up, or detection only works for a person with symptoms, then these prevention methods are not necessary, and self-isolation and/or medical attention is the best way to cut the ${\displaystyle 1/\gamma }$ values. The typical onset of the COVID-19 infectious period is in the order of one day from the symptoms showing up, making massive detection with typical frequency in a few days useless.

${\displaystyle R_{t}}$ does not tell us whether or not the spreading will speed up or slow down in the latter stages when the fraction of susceptible people in the community has dropped significantly after recovery or vaccination. ${\displaystyle R_{e}}$ corrects this dilution effect by multiplying the fraction of the susceptible population over the total population. It corrects the effective/transmissible interaction between an infectious person and the rest of the community when many of the interaction is immune in the middle to late stages of the disease spreading. Thus, when ${\displaystyle R_{e}>1}$, we will see an exponential-like outbreak; when ${\displaystyle R_{e}=1}$, a steady state reached and no number of infectious people changes over time; and when ${\displaystyle R_{e}<1}$, the disease decays and fades away over time.

Using the differential equations of the SIR model and converting them to numerical discrete forms, one can set up the recursive equations and calculate the S, I, and R populations with any given initial conditions but accumulate errors over a long calculation time from the reference point. Sometimes a convergence test is needed to estimate the errors. Given a set of initial conditions and the disease-spreading data, one can also fit the data with the SIR model and pull out the three reproduction numbers when the errors are usually negligible due to the short time step from the reference point.^[21][22] Any point of the time can be used as the initial condition to predict the future after it using this numerical model with assumption of time-evolved parameters such as population, ${\displaystyle R_{t}}$, and ${\displaystyle \gamma }$. However, away from this reference point, errors will accumulate over time thus convergence test is needed to find an optimal time step for more accurate results.

Among these three reproduction numbers, ${\displaystyle R_{0}}$ is very useful to judge the control pressure, e.g., a large value meaning the disease will spread very fast and is very difficult to control. ${\displaystyle R_{t}}$ is most useful in predicting future trends, for example, if we know the social interactions have reduced 50% frequently from that before the outbreak and the interaction intensities among people are the same, then we can set ${\displaystyle R_{t}=0.5R_{0}}$. If social distancing and masks add another 50% cut in infection efficiency, we can set ${\displaystyle R_{t}=0.25R_{0}}$. ${\displaystyle R_{e}}$ will perfectly correlate with the waves of the spreading and whenever ${\displaystyle R_{e}>1}$, the spreading accelerates, and when ${\displaystyle R_{e}<1}$, the spreading slows down thus useful to set a prediction on the short-term trends. Also, it can be used to directly calculate the threshold population of vaccination/immunization for the herd immunity stage by setting ${\displaystyle R_{t}=R_{0}}$, and ${\displaystyle R_{E}=1}$, i.e. ${\displaystyle S=N/R_{0}}$.

Consider a population characterized by a death rate ${\displaystyle \mu }$ and birth rate ${\displaystyle \Lambda }$, and where a communicable disease is spreading.^[8] The model with mass-action transmission is:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\Lambda -\mu S-{\frac {\beta IS}{N}}\\[8pt]{\frac {dI}{dt}}&={\frac {\beta IS}{N}}-\gamma I-\mu I\\[8pt]{\frac {dR}{dt}}&=\gamma I-\mu R\end{aligned}}}$

for which the disease-free equilibrium (DFE) is:

${\displaystyle \left(S(t),I(t),R(t)\right)=\left({\frac {\Lambda }{\mu }},0,0\right).}$

In this case, we can derive a basic reproduction number:

${\displaystyle R_{0}={\frac {\beta }{\mu +\gamma }},}$

which has threshold properties. In fact, independently from biologically meaningful initial values, one can show that:

${\displaystyle R_{0}\leq 1\Rightarrow \lim _{t\to \infty }(S(t),I(t),R(t))={\textrm {DFE}}=\left({\frac {\Lambda }{\mu }},0,0\right)}$

${\displaystyle R_{0}>1,I(0)>0\Rightarrow \lim _{t\to \infty }(S(t),I(t),R(t))={\textrm {EE}}=\left({\frac {\gamma +\mu }{\beta }},{\frac {\mu }{\beta }}\left(R_{0}-1\right),{\frac {\gamma }{\beta }}\left(R_{0}-1\right)\right).}$

The point EE is called the Endemic Equilibrium (the disease is not totally eradicated and remains in the population). With heuristic arguments, one may show that ${\displaystyle R_{0}}$ may be read as the average number of infections caused by a single infectious subject in a wholly susceptible population, the above relationship biologically means that if this number is less than or equal to one the disease goes extinct, whereas if this number is greater than one the disease will remain permanently endemic in the population.

In 1927, W. O. Kermack and A. G. McKendrick created a model in which they considered a fixed population with only three compartments: susceptible, ${\displaystyle S(t)}$; infected, ${\displaystyle I(t)}$; and recovered, ${\displaystyle R(t)}$. The compartments used for this model consist of three classes:^[4]

• ${\displaystyle S(t)}$ is used to represent the individuals not yet infected with the disease at time t, or those susceptible to the disease of the population.
• ${\displaystyle I(t)}$ denotes the individuals of the population who have been infected with the disease and are capable of spreading the disease to those in the susceptible category.
• ${\displaystyle R(t)}$ is the compartment used for the individuals of the population who have been infected and then removed from the disease, either due to immunization or due to death. Those in this category are not able to be infected again or to transmit the infection to others.

The flow of this model may be considered as follows:

${\displaystyle {\color {blue}{{\mathcal {S}}\rightarrow {\mathcal {I}}\rightarrow {\mathcal {R}}}}}$

Using a fixed population, ${\displaystyle N=S(t)+I(t)+R(t)}$ in the three functions resolves that the value ${\displaystyle N}$ should remain constant within the simulation, if a simulation is used to solve the SIR model. Alternatively, the analytic approximant^[9] can be used without performing a simulation. The model is started with values of ${\displaystyle S(t=0)}$, ${\displaystyle I(t=0)}$ and ${\displaystyle R(t=0)}$. These are the number of people in the susceptible, infected and removed categories at time equals zero. If the SIR model is assumed to hold at all times, these initial conditions are not independent.^[9] Subsequently, the flow model updates the three variables for every time point with set values for ${\displaystyle \beta }$ and ${\displaystyle \gamma }$. The simulation first updates the infected from the susceptible and then the removed category is updated from the infected category for the next time point (t=1). This describes the flow persons between the three categories. During an epidemic the susceptible category is not shifted with this model, ${\displaystyle \beta }$ changes over the course of the epidemic and so does ${\displaystyle \gamma }$. These variables determine the length of the epidemic and would have to be updated with each cycle.

${\displaystyle {\frac {dS}{dt}}=-\beta SI}$

${\displaystyle {\frac {dI}{dt}}=\beta SI-\gamma I}$

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

Several assumptions were made in the formulation of these equations: First, an individual in the population must be considered as having an equal probability as every other individual of contracting the disease with a rate of ${\displaystyle a}$ and an equal fraction ${\displaystyle b}$ of people that an individual makes contact with per unit time. Then, let ${\displaystyle \beta }$ be the multiplication of ${\displaystyle a}$ and ${\displaystyle b}$. This is the transmission probability times the contact rate. Besides, an infected individual makes contact with ${\displaystyle b}$ persons per unit time whereas only a fraction, ${\displaystyle S/N}$ of them are susceptible. Thus, we have every infective can infect ${\displaystyle abS=\beta S}$ susceptible persons, and therefore, the whole number of susceptibles infected by infectives per unit time is ${\displaystyle \beta SI}$. For the second and third equations, consider the population leaving the susceptible class as equal to the number entering the infected class. However, a number equal to the fraction ${\displaystyle \gamma }$ (which represents the mean recovery/death rate, or ${\displaystyle 1/\gamma }$ the mean infective period) of infectives are leaving this class per unit time to enter the removed class. These processes which occur simultaneously are referred to as the Law of Mass Action, a widely accepted idea that the rate of contact between two groups in a population is proportional to the size of each of the groups concerned. Finally, it is assumed that the rate of infection and recovery is much faster than the time scale of births and deaths and therefore, these factors are ignored in this model.^[23]

The only steady state solution to the classic SIR model as defined by the differential equations above is I=0, S and R can then take any values. The model can be changed while retaining three compartments to give a steady-state endemic solution by adding some input to the S compartment.

For example, one may postulate that the expected duration of susceptibility will be ${\displaystyle \operatorname {E} [\min(T_{L}\mid T_{S})]}$ where ${\displaystyle T_{L}}$ reflects the time alive (life expectancy) and ${\displaystyle T_{S}}$ reflects the time in the susceptible state before becoming infected, which can be simplified^[24] to:

${\displaystyle \operatorname {E} [\min(T_{L}\mid T_{S})]=\int _{0}^{\infty }e^{-(\mu +\delta )x}\,dx={\frac {1}{\mu +\delta }},}$

such that the number of susceptible persons is the number entering the susceptible compartment ${\displaystyle \mu N}$ times the duration of susceptibility:

${\displaystyle S={\frac {\mu N}{\mu +\lambda }}.}$

Analogously, the steady-state number of infected persons is the number entering the infected state from the susceptible state (number susceptible, times rate of infection) ${\displaystyle \lambda ={\tfrac {\beta I}{N}},}$ times the duration of infectiousness ${\displaystyle {\tfrac {1}{\mu +v}}}$:

${\displaystyle I={\frac {\mu N}{\mu +\lambda }}\lambda {\frac {1}{\mu +v}}.}$

There are many modifications of the SIR model, including those that include births and deaths, where upon recovery there is no immunity (SIS model), where immunity lasts only for a short period of time (SIRS), where there is a latent period of the disease where the person is not infectious (SEIS and SEIR), and where infants can be born with immunity (MSIR). Compartmental models can also be used to model multiple risk groups, and even the interaction of multiple pathogens.^[25]

Some infections, for example, those from the common cold and influenza, do not confer any long-lasting immunity. Such infections may give temporary resistance but do not give long-term immunity upon recovery from infection, and individuals become susceptible again.

We have the model:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=-{\frac {\beta SI}{N}}+\gamma I\\[6pt]{\frac {dI}{dt}}&={\frac {\beta SI}{N}}-\gamma I\end{aligned}}}$

Note that denoting with N the total population it holds that:

${\displaystyle {\frac {dS}{dt}}+{\frac {dI}{dt}}=0\Rightarrow S(t)+I(t)=N}$.

It follows that:

${\displaystyle {\frac {dI}{dt}}=(\beta -\gamma )I-{\frac {\beta }{N}}I^{2}}$,

i.e. the dynamics of infectious is ruled by a logistic function, so that ${\displaystyle \forall I(0)>0}$:

${\displaystyle {\begin{aligned}&{\frac {\beta }{\gamma }}\leq 1\Rightarrow \lim _{t\to +\infty }I(t)=0,\\[6pt]&{\frac {\beta }{\gamma }}>1\Rightarrow \lim _{t\to +\infty }I(t)=\left(1-{\frac {\gamma }{\beta }}\right)N.\end{aligned}}}$

It is possible to find an analytical solution to this model (by making a transformation of variables: ${\displaystyle I=y^{-1}}$ and substituting this into the mean-field equations),^[26] such that the basic reproduction rate is greater than unity. The solution is given as

${\displaystyle I(t)={\frac {I_{\infty }}{1+Ve^{-\chi t}}}}$.

where ${\displaystyle I_{\infty }=(1-\gamma /\beta )N}$ is the endemic infectious population, ${\displaystyle \chi =\beta -\gamma }$, and ${\displaystyle V=I_{\infty }/I_{0}-1}$. As the system is assumed to be closed, the susceptible population is then ${\displaystyle S(t)=N-I(t)}$.

Whenever the integer nature of the number of agents is evident (populations with fewer than tens of thousands of individuals), inherent fluctuations in the disease spreading process caused by discrete agents result in uncertainties.^[27] In this scenario, the evolution of the disease predicted by compartmental equations deviates significantly from the observed results. These uncertainties may even cause the epidemic to end earlier than predicted by the compartmental equations.

As a special case, one obtains the usual logistic function by assuming ${\displaystyle \gamma =0}$. This can be also considered in the SIR model with ${\displaystyle R=0}$, i.e. no removal will take place. That is the SI model.^[28] The differential equation system using ${\displaystyle S=N-I}$ thus reduces to:

${\displaystyle {\frac {dI}{dt}}\propto I\cdot (N-I).}$

In the long run, in the SI model, all individuals will become infected.

The Susceptible-Infectious-Recovered-Deceased model differentiates between Recovered (meaning specifically individuals having survived the disease and now immune) and Deceased.^[15] The SIRD model has semi analytical solutions based on the four parts method.^[29] This model uses the following system of differential equations:

${\displaystyle {\begin{aligned}&{\frac {dS}{dt}}=-{\frac {\beta IS}{N}},\\[6pt]&{\frac {dI}{dt}}={\frac {\beta IS}{N}}-\gamma I-\mu I,\\[6pt]&{\frac {dR}{dt}}=\gamma I,\\[6pt]&{\frac {dD}{dt}}=\mu I,\end{aligned}}}$

where ${\displaystyle \beta ,\gamma ,\mu }$ are the rates of infection, recovery, and mortality, respectively.^[30]

The Susceptible-Infectious-Recovered-Vaccinated model is an extended SIR model that accounts for vaccination of the susceptible population.^[31] This model uses the following system of differential equations:

${\displaystyle {\begin{aligned}&{\frac {dS}{dt}}=-{\frac {\beta (t)IS}{N}}-v(t)S,\\[6pt]&{\frac {dI}{dt}}={\frac {\beta (t)IS}{N}}-\gamma (t)I,\\[6pt]&{\frac {dR}{dt}}=\gamma (t)I,\\[6pt]&{\frac {dV}{dt}}=v(t)S,\end{aligned}}}$

where ${\displaystyle \beta ,\gamma ,v}$ are the rates of infection, recovery, and vaccination, respectively. For the semi-time initial conditions ${\displaystyle S(0)=(1-\eta )N}$, ${\displaystyle I(0)=\eta N}$, ${\displaystyle R(0)=V(0)=0}$ and constant ratios ${\displaystyle k=\gamma (t)/\beta (t)}$ and ${\displaystyle b=v(t)/\beta (t)}$ the model had been solved approximately.^[31] The occurrence of a pandemic outburst requires ${\displaystyle k+b<1-2\eta }$ and there is a critical reduced vaccination rate ${\displaystyle b_{c}}$ beyond which the steady-state size ${\displaystyle S_{\infty }}$of the susceptible compartment remains relatively close to ${\displaystyle S(0)}$. Arbitrary initial conditions satisfying ${\displaystyle S(0)+I(0)+R(0)+V(0)=N}$ can be mapped to the solved special case with ${\displaystyle R(0)=V(0)=0}$.^[31]

The numerical solution of this model to calculate the real-time reproduction number ${\displaystyle R_{t}}$ of COVID-19 can be practiced based on information from the different populations in a community.^[22] Numerical solution is a commonly used method to analyze complicated kinetic networks when the analytical solution is difficult to obtain or limited by requirements such as boundary conditions or special parameters. It uses recursive equations to calculate the next step by converting the numerical integration into Riemann sum of discrete time steps e.g., use yesterday's principal and interest rate to calculate today's interest which assumes the interest rate is fixed during the day. The calculation contains projected errors if the analytical corrections on the numerical step size are not included, e.g. when the interest rate of annual collection is simplified to 12 times the monthly rate, a projected error is introduced. Thus the calculated results will carry accumulative errors when the time step is far away from the reference point and a convergence test is needed to estimate the error. However, this error is usually acceptable for data fitting. When fitting a set of data with a close time step, the error is relatively small because the reference point is nearby compared to when predicting a long period of time after a reference point. Once the real-time ${\displaystyle R_{t}}$ is pulled out, one can compare it to the basic reproduction number ${\displaystyle R_{0}}$. Before the vaccination, ${\displaystyle R_{t}}$ gives the policy maker and general public a measure of the efficiency of social mitigation activities such as social distancing and face masking simply by dividing ${\displaystyle {\frac {R_{t}}{R_{0}}}}$. Under massive vaccination, the goal of disease control is to reduce the effective reproduction number ${\displaystyle R_{e}={\frac {R_{t}S}{N}}<1}$, where ${\displaystyle S}$ is the number of susceptible population at the time and ${\displaystyle N}$ is the total population. When ${\displaystyle R_{e}<1}$, the spreading decays and daily infected cases go down.

The susceptible-infected-recovered-vaccinated-deceased (SIRVD) epidemic compartment model extends the SIR model to include the effects of vaccination campaigns and time-dependent fatality rates on epidemic outbreaks. It encompasses the SIR, SIRV, SIRD, and SI models as special cases, with individual time-dependent rates governing transitions between different fractions.^[32] This model uses the following system of differential equations for the population fractions ${\displaystyle S,I,R,V,D}$:

${\displaystyle {\begin{aligned}&{\frac {dS}{dt}}=-a(t)SI-v(t)S,\\[6pt]&{\frac {dI}{dt}}=a(t)SI-\mu (t)I-\psi (t)I,\\[6pt]&{\frac {dR}{dt}}=\mu (t)I,\\[6pt]&{\frac {dV}{dt}}=v(t)S,\\[6pt]&{\frac {dD}{dt}}=\psi (t)I\end{aligned}}}$

where ${\displaystyle a(t),v(t),\mu (t),\psi (t)}$ are the infection, vaccination, recovery, and fatality rates, respectively. For the semi-time initial conditions ${\displaystyle S(0)=1-\eta }$, ${\displaystyle I(0)=\eta }$, ${\displaystyle R(0)=V(0)=D(0)=0}$ and constant ratios ${\displaystyle k=\mu (t)/a(t)}$, ${\displaystyle b=v(t)/a(t)}$, and ${\displaystyle q=\psi (t)/a(t)}$ the model had been solved approximately, and exactly for some special cases, irrespective of the functional form of ${\displaystyle a(t)}$.^[32] This is achieved upon rewriting the above SIRVD model equations in equivalent, but reduced form

${\displaystyle {\begin{aligned}&{\frac {dS}{d\tau }}=-SI-b(\tau )S,\\[6pt]&{\frac {dI}{d\tau }}=SI-[k(\tau )+q(\tau )]I,\\[6pt]&{\frac {dR}{d\tau }}=k(\tau )I,\\[6pt]&{\frac {dV}{d\tau }}=b(\tau )S,\\[6pt]&{\frac {dD}{d\tau }}=q(\tau )S\end{aligned}}}$

where

${\displaystyle \tau (t)=\int _{0}^{t}a(\xi )d\xi }$

is a reduced, dimensionless time. The temporal dependence of the infected fraction ${\displaystyle I(\tau )}$ and the rate of new infections ${\displaystyle j(\tau )=S(\tau )I(\tau )}$ differs when considering the effects of vaccinations and when the real-time dependence of fatality and recovery rates diverge. These differences have been highlighted for stationary ratios and gradually decreasing fatality rates.^[32] The case of stationary ratios allows one to construct a diagnostics method to extract analytically all SIRVD model parameters from measured COVID-19 data of a completed pandemic wave.^[32]

For many infections, including measles, babies are not born into the susceptible compartment but are immune to the disease for the first few months of life due to protection from maternal antibodies (passed across the placenta and additionally through colostrum). This is called passive immunity. This added detail can be shown by including an M class (for maternally derived immunity) at the beginning of the model.

To indicate this mathematically, an additional compartment is added, M(t). This results in the following differential equations:

${\displaystyle {\begin{aligned}{\frac {dM}{dt}}&=\Lambda -\delta M-\mu M\\[8pt]{\frac {dS}{dt}}&=\delta M-{\frac {\beta SI}{N}}-\mu S\\[8pt]{\frac {dI}{dt}}&={\frac {\beta SI}{N}}-\gamma I-\mu I\\[8pt]{\frac {dR}{dt}}&=\gamma I-\mu R\end{aligned}}}$

Some people who have had an infectious disease such as tuberculosis never completely recover and continue to carry the infection, whilst not suffering the disease themselves. They may then move back into the infectious compartment and suffer symptoms (as in tuberculosis) or they may continue to infect others in their carrier state, while not suffering symptoms. The most famous example of this is probably Mary Mallon, who infected 22 people with typhoid fever. The carrier compartment is labelled C.

For many important infections, there is a significant latency period during which individuals have been infected but are not yet infectious themselves. During this period the individual is in compartment E (for exposed).

Assuming that the latency period is a random variable with exponential distribution with parameter ${\displaystyle a}$ (i.e. the average latency period is ${\displaystyle a^{-1}}$), and also assuming the presence of vital dynamics with birth rate ${\displaystyle \Lambda }$ equal to death rate ${\displaystyle N\mu }$ (so that the total number ${\displaystyle N}$ is constant), we have the model:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\mu N-\mu S-{\frac {\beta IS}{N}}\\[8pt]{\frac {dE}{dt}}&={\frac {\beta IS}{N}}-(\mu +a)E\\[8pt]{\frac {dI}{dt}}&=aE-(\gamma +\mu )I\\[8pt]{\frac {dR}{dt}}&=\gamma I-\mu R.\end{aligned}}}$

We have ${\displaystyle S+E+I+R=N,}$ but this is only constant because of the simplifying assumption that birth and death rates are equal; in general ${\displaystyle N}$ is a variable.

For this model, the basic reproduction number is:

${\displaystyle R_{0}={\frac {a}{\mu +a}}{\frac {\beta }{\mu +\gamma }}.}$

Similarly to the SIR model, also, in this case, we have a Disease-Free-Equilibrium (N,0,0,0) and an Endemic Equilibrium EE, and one can show that, independently from biologically meaningful initial conditions

${\displaystyle \left(S(0),E(0),I(0),R(0)\right)\in \left\{(S,E,I,R)\in [0,N]^{4}:S\geq 0,E\geq 0,I\geq 0,R\geq 0,S+E+I+R=N\right\}}$

it holds that:

${\displaystyle R_{0}\leq 1\Rightarrow \lim _{t\to +\infty }\left(S(t),E(t),I(t),R(t)\right)=DFE=(N,0,0,0),}$

${\displaystyle R_{0}>1,I(0)>0\Rightarrow \lim _{t\to +\infty }\left(S(t),E(t),I(t),R(t)\right)=EE.}$

In case of periodically varying contact rate ${\displaystyle \beta (t)}$ the condition for the global attractiveness of DFE is that the following linear system with periodic coefficients:

${\displaystyle {\begin{aligned}{\frac {dE_{1}}{dt}}&=\beta (t)I_{1}-(\gamma +a)E_{1}\\[8pt]{\frac {dI_{1}}{dt}}&=aE_{1}-(\gamma +\mu )I_{1}\end{aligned}}}$

is stable (i.e. it has its Floquet's eigenvalues inside the unit circle in the complex plane).

The SEIS model is like the SEIR model (above) except that no immunity is acquired at the end.

${\displaystyle {\color {blue}{{\mathcal {S}}\to {\mathcal {E}}\to {\mathcal {I}}\to {\mathcal {S}}}}}$

In this model an infection does not leave any immunity thus individuals that have recovered return to being susceptible, moving back into the S(t) compartment. The following differential equations describe this model:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\Lambda -{\frac {\beta SI}{N}}-\mu S+\gamma I\\[6pt]{\frac {dE}{dt}}&={\frac {\beta SI}{N}}-(\epsilon +\mu )E\\[6pt]{\frac {dI}{dt}}&=\varepsilon E-(\gamma +\mu )I\end{aligned}}}$

For the case of a disease, with the factors of passive immunity, and a latency period there is the MSEIR model.

${\displaystyle \color {blue}{{\mathcal {M}}\to {\mathcal {S}}\to {\mathcal {E}}\to {\mathcal {I}}\to {\mathcal {R}}}}$

${\displaystyle {\begin{aligned}{\frac {dM}{dt}}&=\Lambda -\delta M-\mu M\\[6pt]{\frac {dS}{dt}}&=\delta M-{\frac {\beta SI}{N}}-\mu S\\[6pt]{\frac {dE}{dt}}&={\frac {\beta SI}{N}}-(\varepsilon +\mu )E\\[6pt]{\frac {dI}{dt}}&=\varepsilon E-(\gamma +\mu )I\\[6pt]{\frac {dR}{dt}}&=\gamma I-\mu R\end{aligned}}}$

An MSEIRS model is similar to the MSEIR, but the immunity in the R class would be temporary, so that individuals would regain their susceptibility when the temporary immunity ended.

${\displaystyle {\color {blue}{{\mathcal {M}}\to {\mathcal {S}}\to {\mathcal {E}}\to {\mathcal {I}}\to {\mathcal {R}}\to {\mathcal {S}}}}}$

It is well known that the probability of getting a disease is not constant in time. As a pandemic progresses, reactions to the pandemic may change the contact rates which are assumed constant in the simpler models. Counter-measures such as masks, social distancing, and lockdown will alter the contact rate in a way to reduce the speed of the pandemic.

In addition, Some diseases are seasonal, such as the common cold viruses, which are more prevalent during winter. With childhood diseases, such as measles, mumps, and rubella, there is a strong correlation with the school calendar, so that during the school holidays the probability of getting such a disease dramatically decreases. As a consequence, for many classes of diseases, one should consider a force of infection with periodically ('seasonal') varying contact rate

${\displaystyle F=\beta (t){\frac {I}{N}},\quad \beta (t+T)=\beta (t)}$

with period T equal to one year.

Thus, our model becomes

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\mu N-\mu S-\beta (t){\frac {I}{N}}S\\[8pt]{\frac {dI}{dt}}&=\beta (t){\frac {I}{N}}S-(\gamma +\mu )I\end{aligned}}}$

(the dynamics of recovered easily follows from ${\displaystyle R=N-S-I}$), i.e. a nonlinear set of differential equations with periodically varying parameters. It is well known that this class of dynamical systems may undergo very interesting and complex phenomena of nonlinear parametric resonance. It is easy to see that if:

${\displaystyle {\frac {1}{T}}\int _{0}^{T}{\frac {\beta (t)}{\mu +\gamma }}\,dt<1\Rightarrow \lim _{t\to +\infty }(S(t),I(t))=DFE=(N,0),}$

whereas if the integral is greater than one the disease will not die out and there may be such resonances. For example, considering the periodically varying contact rate as the 'input' of the system one has that the output is a periodic function whose period is a multiple of the period of the input. This allowed to give a contribution to explain the poly-annual (typically biennial) epidemic outbreaks of some infectious diseases as interplay between the period of the contact rate oscillations and the pseudo-period of the damped oscillations near the endemic equilibrium. Remarkably, in some cases, the behavior may also be quasi-periodic or even chaotic.

Spatiotemporal compartmental models describe not the total number, but the density of susceptible/infective/recovered persons. Consequently, they also allow to model the distribution of infected persons in space. In most cases, this is done by combining the SIR model with a diffusion equation

${\displaystyle {\begin{aligned}&\partial _{t}S=D_{S}\nabla ^{2}S-{\frac {\beta IS}{N}},\\[6pt]&\partial _{t}I=D_{I}\nabla ^{2}I+{\frac {\beta IS}{N}}-\gamma I,\\[6pt]&\partial _{t}R=D_{R}\nabla ^{2}R+\gamma I,\end{aligned}}}$^[33]

where ${\displaystyle D_{S}}$, ${\displaystyle D_{I}}$ and ${\displaystyle D_{R}}$ are diffusion constants. Thereby, one obtains a reaction-diffusion equation. (Note that, for dimensional reasons, the parameter ${\displaystyle \beta }$ has to be changed compared to the simple SIR model.) Early models of this type have been used to model the spread of the black death in Europe.^[34] Extensions of this model have been used to incorporate, e.g., effects of nonpharmaceutical interventions such as social distancing.^[35]

As social contacts, disease severity and lethality, as well as the efficacy of prophylactic measures may differ substantially between interacting subpopulations, e.g., the elderly versus the young, separate SEIR models for each subgroup may be used that are mutually connected through interaction links.^[33] Such Interacting Subpopulation SEIR models have been used for modeling the COVID-19 pandemic at continent scale to develop personalized, accelerated, subpopulation-targeted vaccination strategies^[36] that promise a shortening of the pandemic and a reduction of case and death counts in the setting of limited access to vaccines during a wave of virus Variants of Concern.

The SIR model has been studied on networks of various kinds in order to model a more realistic form of connection than the homogeneous mixing condition which is usually required. A simple model for epidemics on networks in which an individual has a probability p of being infected by each of his infected neighbors in a given time step leads to results similar to giant component formation on Erdos Renyi random graphs.^[37] A stochastic compartment model with a transmission pathway via vectors has been developed recently in which a multiple random walkers approach is implemented to investigate the spreading dynamics in random graphs of the Watts-Strogatz and the Barabási-Albert type to mimic human mobility patterns in complex real world environments such as cities, streets, and transportation networks. This model captures the class of vector transmitted infectious diseases such as Dengue, Malaria (transmission by mosquitoes), pestilence (transmission by fleas), and others.

Dynamics of epidemics depend on how people's behavior changes in time. For example, at the beginning of the epidemic, people are ignorant and careless, then, after the outbreak of epidemics and alarm, they begin to comply with the various restrictions and the spreading of epidemics may decline. Over time, some people get tired/frustrated by the restrictions and stop following them (exhaustion), especially if the number of new cases drops down. After resting for some time, they can follow the restrictions again. But during this pause the second wave can come and become even stronger than the first one. Social dynamics should be considered. The social physics models of social stress complement the classical epidemics models.^[38]

The simplest SIR-social stress (SIR_SS) model is organised as follows. The susceptible individuals (S) can be split in three subgroups by the types of behavior: ignorant or unaware of the epidemic (S_ign), rationally resistant (S_res), and exhausted (S_exh) that do not react on the external stimuli (this is a sort of refractory period). In other words: S(t) = S_ign(t) + S_res(t) + S_exh(t). Symbolically, the social stress model can be presented by the "reaction scheme" (where I denotes the infected individuals):

• ${\displaystyle {\color {blue}{{\mathcal {S_{ign}}}+2{\mathcal {I}}\to {\mathcal {S_{res}}}+2{\mathcal {I}}}}}$ – mobilization reaction (the autocatalytic form here means that the transition rate is proportional to the square of the infected fraction I);
• ${\displaystyle {\color {blue}{{\mathcal {S_{res}}}\to {\mathcal {S_{exh}}}}}}$ – exhaustion process due to fatigue from anti-epidemic restrictions;
• ${\displaystyle {\color {blue}{{\mathcal {S_{exh}}}\to {\mathcal {S_{ign}}}}}}$ – slow relaxation to the initial state (end of the refractory period).

The main SIR epidemic reaction

• ${\displaystyle {\color {blue}{{\mathcal {S_{...}}}+{\mathcal {I}}\to {\mathcal {2I}}}}}$

has different reaction rate constants ${\displaystyle \beta }$ for S_ign, S_res, and S_exh. Presumably, for S_res, ${\displaystyle \beta }$ is lower than for S_ign and S_ign.

The differences between countries are concentrated in two kinetic constants: the rate of mobilization and the rate of exhaustion calculated for COVID-19 epidemic in 13 countries.^[38] These constants for this epidemic in all countries can be extracted by the fitting of the SIR_SS model to publicly available data ^[39]

Based on the classical SIR model, a Korteweg-de Vries (KdV)–SIR equation and its analytical solution have been proposed to illustrate the fundamental dynamics of an epidemic wave, the dependence of solutions on parameters, and the dependence of predictability horizons on various types of solutions.^[40] The KdV-SIR equation is written as follows:

${\displaystyle {\frac {d^{2}I}{dt}}-\sigma _{o}^{2}I+{\frac {3}{2}}{\frac {\sigma _{o}^{2}}{I_{max}}}I^{2}=0}$.

Here,

${\displaystyle \sigma _{o}=\gamma (R_{o}-1)}$,

${\displaystyle R_{o}={\frac {\beta }{\gamma }}{\frac {S_{o}}{N}}}$,

and

${\displaystyle I_{max}={\frac {S_{o}}{2}}{\frac {(R_{o}-1)^{2}}{R_{o}^{2}}}}$.

${\displaystyle S_{o}}$ indicates the initial value of the state variable ${\displaystyle S}$. Parameters ${\displaystyle \sigma _{o}}$(σ-naught) and ${\displaystyle R_{o}}$ (R-naught) are the time-independent relative growth rate and basic reproduction number, respectively. ${\displaystyle I_{max}}$presents the maximum of the state variables ${\displaystyle I}$(for the number of infected persons). An analytical solution to the KdV-SIR equation is written as follows:

${\displaystyle I=I_{max}sech^{2}\left({\frac {\sigma _{o}}{2}}t\right)}$,

which represents a solitary wave solution.

Modeling a full population of possibly millions people using two constants ${\displaystyle \beta }$ and ${\displaystyle \gamma }$ seem far fetched; each individual has personal characteristics that influence the propagation : immunity status, contact habits and so on. So it is interesting to know what happens if, for instance, ${\displaystyle \beta }$ and ${\displaystyle \gamma }$ are not two constants but some random variables (a pair for each individual). This procedure has several names : "heterogeneous model", "structuration" (see also below for age structured models) or "Bayesian" view.^[41][42][43] Surprising results emerge, for instance it was proved in^[41] that the number of infected at the peak of a heterogeneous epidemic is smaller than the deterministic epidemic having same average ${\displaystyle \beta }$; the same holds true for the total epidemic size ${\displaystyle S(0)-S(\infty )}$ and other models, e.g. SEIR.^[41]

The SIR model can be modified to model vaccination.^[44] Typically these introduce an additional compartment to the SIR model, ${\displaystyle V}$, for vaccinated individuals. Below are some examples.

In presence of a communicable diseases, one of the main tasks is that of eradicating it via prevention measures and, if possible, via the establishment of a mass vaccination program. Consider a disease for which the newborn are vaccinated (with a vaccine giving lifelong immunity) at a rate ${\displaystyle P\in (0,1)}$:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\nu N(1-P)-\mu S-\beta {\frac {I}{N}}S\\[8pt]{\frac {dI}{dt}}&=\beta {\frac {I}{N}}S-(\mu +\gamma )I\\[8pt]{\frac {dV}{dt}}&=\nu NP-\mu V\end{aligned}}}$

where ${\displaystyle V}$ is the class of vaccinated subjects. It is immediate to show that:

${\displaystyle \lim _{t\to +\infty }V(t)=NP,}$

thus we shall deal with the long term behavior of ${\displaystyle S}$ and ${\displaystyle I}$, for which it holds that:

${\displaystyle R_{0}(1-P)\leq 1\Rightarrow \lim _{t\to +\infty }\left(S(t),I(t)\right)=DFE=\left(N\left(1-P\right),0\right)}$

${\displaystyle R_{0}(1-P)>1,\quad I(0)>0\Rightarrow \lim _{t\to +\infty }\left(S(t),I(t)\right)=EE=\left({\frac {N}{R_{0}(1-P)}},N\left(R_{0}(1-P)-1\right)\right).}$

In other words, if

${\displaystyle P<P^{*}=1-{\frac {1}{R_{0}}}}$

the vaccination program is not successful in eradicating the disease, on the contrary, it will remain endemic, although at lower levels than the case of absence of vaccinations. This means that the mathematical model suggests that for a disease whose basic reproduction number may be as high as 18 one should vaccinate at least 94.4% of newborns in order to eradicate the disease.

Modern societies are facing the challenge of "rational" exemption, i.e. the family's decision to not vaccinate children as a consequence of a "rational" comparison between the perceived risk from infection and that from getting damages from the vaccine. In order to assess whether this behavior is really rational, i.e. if it can equally lead to the eradication of the disease, one may simply assume that the vaccination rate is an increasing function of the number of infectious subjects:

${\displaystyle P=P(I),\quad P'(I)>0.}$

In such a case the eradication condition becomes:

${\displaystyle P(0)\geq P^{*},}$

i.e. the baseline vaccination rate should be greater than the "mandatory vaccination" threshold, which, in case of exemption, cannot hold. Thus, "rational" exemption might be myopic since it is based only on the current low incidence due to high vaccine coverage, instead taking into account future resurgence of infection due to coverage decline.

In case there also are vaccinations of non newborns at a rate ρ the equation for the susceptible and vaccinated subject has to be modified as follows:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\mu N(1-P)-\mu S-\rho S-\beta {\frac {I}{N}}S\\[8pt]{\frac {dV}{dt}}&=\mu NP+\rho S-\mu V\end{aligned}}}$

leading to the following eradication condition:

${\displaystyle P\geq 1-\left(1+{\frac {\rho }{\mu }}\right){\frac {1}{R_{0}}}}$

This strategy repeatedly vaccinates a defined age-cohort (such as young children or the elderly) in a susceptible population over time. Using this strategy, the block of susceptible individuals is then immediately removed, making it possible to eliminate an infectious disease, (such as measles), from the entire population. Every T time units a constant fraction p of susceptible subjects is vaccinated in a relatively short (with respect to the dynamics of the disease) time. This leads to the following impulsive differential equations for the susceptible and vaccinated subjects:

${\displaystyle {\begin{aligned}{\frac {dS}{dt}}&=\mu N-\mu S-\beta {\frac {I}{N}}S,\quad S(nT^{+})=(1-p)S(nT^{-}),&&n=0,1,2,\ldots \\[8pt]{\frac {dV}{dt}}&=-\mu V,\quad V(nT^{+})=V(nT^{-})+pS(nT^{-}),&&n=0,1,2,\ldots \end{aligned}}}$

It is easy to see that by setting I = 0 one obtains that the dynamics of the susceptible subjects is given by:

${\displaystyle S^{*}(t)=1-{\frac {p}{1-(1-p)E^{-\mu T}}}E^{-\mu MOD(t,T)}}$

and that the eradication condition is:

${\displaystyle R_{0}\int _{0}^{T}S^{*}(t)\,dt<1}$

A huge literature recognizes that the vaccination can be seen as a game: in a population where everybody is vaccinated any epidemic will die off immediately so an additional person will have no interest to vaccinate at all. On the contrary, a person arriving in a population where nobody is vaccinated will have all incentives to vaccinate (the epidemic will break loose in such a population). So, it seems that the individual has interest to do the opposite of the population as a whole. But the population is the sum of all individuals, and the previous affirmation should be false. So, in fact, a Nash equilibrium is reached.^{[45][46][47][48][49]} Technical tools to treat such situations involve game theory or modern tools such as Mean-field game theory.^[49][50]

Age has a deep influence on the disease spread rate in a population, especially the contact rate. This rate summarizes the effectiveness of contacts between susceptible and infectious subjects. Taking into account the ages of the epidemic classes ${\displaystyle s(t,a),i(t,a),r(t,a)}$ (to limit ourselves to the susceptible-infectious-removed scheme) such that:

${\displaystyle S(t)=\int _{0}^{a_{M}}s(t,a)\,da}$

${\displaystyle I(t)=\int _{0}^{a_{M}}i(t,a)\,da}$

${\displaystyle R(t)=\int _{0}^{a_{M}}r(t,a)\,da}$

(where ${\displaystyle a_{M}\leq +\infty }$ is the maximum admissible age) and their dynamics is not described, as one might think, by "simple" partial differential equations, but by integro-differential equations:

${\displaystyle \partial _{t}s(t,a)+\partial _{a}s(t,a)=-\mu (a)s(a,t)-s(a,t)\int _{0}^{a_{M}}k(a,a_{1};t)i(a_{1},t)\,da_{1}}$

${\displaystyle \partial _{t}i(t,a)+\partial _{a}i(t,a)=s(a,t)\int _{0}^{a_{M}}{k(a,a_{1};t)i(a_{1},t)da_{1}}-\mu (a)i(a,t)-\gamma (a)i(a,t)}$

${\displaystyle \partial _{t}r(t,a)+\partial _{a}r(t,a)=-\mu (a)r(a,t)+\gamma (a)i(a,t)}$

where:

${\displaystyle F(a,t,i(\cdot ,\cdot ))=\int _{0}^{a_{M}}k(a,a_{1};t)i(a_{1},t)\,da_{1}}$

is the force of infection, which, of course, will depend, though the contact kernel ${\displaystyle k(a,a_{1};t)}$ on the interactions between the ages.

Complexity is added by the initial conditions for newborns (i.e. for a=0), that are straightforward for infectious and removed:

${\displaystyle i(t,0)=r(t,0)=0}$

but that are nonlocal for the density of susceptible newborns:

${\displaystyle s(t,0)=\int _{0}^{a_{M}}\left(\varphi _{s}(a)s(a,t)+\varphi _{i}(a)i(a,t)+\varphi _{r}(a)r(a,t)\right)\,da}$

where ${\displaystyle \varphi _{j}(a),j=s,i,r}$ are the fertilities of the adults.

Moreover, defining now the density of the total population ${\displaystyle n(t,a)=s(t,a)+i(t,a)+r(t,a)}$ one obtains:

${\displaystyle \partial _{t}n(t,a)+\partial _{a}n(t,a)=-\mu (a)n(a,t)}$

In the simplest case of equal fertilities in the three epidemic classes, we have that in order to have demographic equilibrium the following necessary and sufficient condition linking the fertility ${\displaystyle \varphi (.)}$ with the mortality ${\displaystyle \mu (a)}$ must hold:

${\displaystyle 1=\int _{0}^{a_{M}}\varphi (a)\exp \left(-\int _{0}^{a}{\mu (q)dq}\right)\,da}$

and the demographic equilibrium is

${\displaystyle n^{*}(a)=C\exp \left(-\int _{0}^{a}\mu (q)\,dq\right),}$

automatically ensuring the existence of the disease-free solution:

${\displaystyle DFS(a)=(n^{*}(a),0,0).}$

A basic reproduction number can be calculated as the spectral radius of an appropriate functional operator.

One way to calculate ${\displaystyle R_{0}}$ is to average the expected number of new infections over all possible infected types. The next-generation method is a general method of deriving ${\displaystyle R_{0}}$ when more than one class of infectives is involved. This method, originally introduced by Diekmann et al. (1990),^[51] can be used for models with underlying age structure or spatial structure, among other possibilities.^[52] In this picture, the spectral radius of the next-generation matrix ${\displaystyle G}$ gives the basic reproduction number, ${\displaystyle R_{0}=\rho (G).}$^[53]

Consider a sexually transmitted disease. In a naive population where almost everyone is susceptible, but the infection seed, if the expected number of gender 1 is ${\displaystyle f}$ and the expected number of infected gender 2 is ${\displaystyle m}$, we can know how many would be infected in the next-generation. Such that the next-generation matrix