The term is a mass-action incidence rate: each infective individual makes potentially transmitting contacts with susceptible individuals, and the total rate is proportional to the product of the two compartment sizes. An infection transfers one animal from to , accounting for opposite signs in their equations. The per-capita mortality rate of an infective individual is , giving transfer from to .
There are no births, recoveries or additional deaths in this model. Adding the three equations gives , so the total initial biological population is conserved when the dead compartment is included. Before quarantine, decreases whenever ; after effective isolation no further transmission is permitted.
Write and . Until quarantine and while , division of the equations gives
Integration from the initial state yields the first integral
Let be the susceptible count at the first time . It is the root of an equation reached on the decreasing- outbreak trajectory of
For a strictly rising threshold crossing this is the larger admissible root of an equation, with ; if the threshold equals the peak, . The assumption that quarantine is reached selects the physically relevant branch and excludes a merely hypothetical declining-branch crossing after an earlier one.
Since there is no incubation period here, all removals from have already become infection cases by quarantine. No further susceptible individuals are infected after isolation. The requested number among the initially susceptible individuals is therefore
The delayed influx represents animals exposed one incubation period earlier who enter the infective individual compartment now. They die at the instantaneous rate once in that compartment. The displayed bookkeeping removes an animal from at the same delayed time that it enters , preserving .
For this bookkeeping, must include the exposed animals which have not yet completed incubation period. If were instead defined as strictly unexposed susceptible individuals, its loss term would be the current exposure rate and a separate latent compartment would be needed. The calculations here follow the printed delay differential equation. A full initial-value problem for a delay differential equation also needs a history on ; the following small-delay expansion of an epidemic transfer rate concerns a smooth compatible history and the regular regime assumed by the question.
In the first-order Taylor expansion correction it suffices to use the zeroth-order derivatives. They give
The delayed product is consequently
Multiplying by and substituting into the two transfer equations produces
The opposite signs of and are also required by conservation law of : this correction changes the timing of the transfer between and , while leaving the instantaneous death term unchanged.
At the retained order define . Neglecting terms of order in the incidence correction gives
Dividing and expanding consistently,
Thus the susceptible count at the first threshold crossing obeys the same retained-order equation as before:
It is important to distinguish completed case transfers at quarantine from all infections already initiated. Let the quarantine time be . Isolation prevents exposures after , but animals exposed during still finish their incubation period during . Their number, in the printed bookkeeping, is
The infection cases transferred by time among the initial class number . Adding those pending infection cases gives the eventual number who catch the infectious disease:
This adds only infections caused by exposures before isolation; it does not allow secondary transmission after quarantine. If one asks instead only for the transfers completed by the instant of quarantine, the answer is . The distinction is necessary because the model keeps incubating animals in its compartment.

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