Revisiting the standard for modeling the spread of infectious diseases

The COVID-19 epidemic brought to the forefront the value of mathematical modelling for infectious diseases as a guide to help manage a formidable challenge for human health. A standard dynamic model widely used for a spreading epidemic separates a population into compartments—each comprising individuals at a similar stage before, during, or after infection—and keeps track of the population fraction in each compartment over time, by balancing compartment loading, discharge, and accumulation rates. The standard model provides valuable insight into when an epidemic spreads or what fraction of a population will have been infected by the epidemic’s end. A subtle issue, however, with that model, is that it may misrepresent the peak of the infectious fraction of a population, the time to reach that peak, or the rate at which an epidemic spreads. This may compromise the model’s usability for tasks such as “Flattening the Curve” or other interventions for epidemic management. Here we develop an extension of the standard model’s structure, which retains the simplicity and insights of the standard model while avoiding the misrepresentation issues mentioned above. The proposed model relies on replacing a module of the standard model by a module resulting from Padé approximation in the Laplace domain. The Padé-approximation module would also be suitable for incorporation in the wide array of standard model variants used in epidemiology. This warrants a re-examination of the subject and could potentially impact model-based management of epidemics, development of software tools for practicing epidemiologists, and related educational resources.

The global epidemic of COVID-19 has brought to the forefront the importance of mathematical modelling in the development of strategies for managing the spread of infectious diseases [1][2][3][4][5][6][7] . Terms such as flattening the curve, R 0 , or herd immunity, which entered public discourse 8 emerge from mathematical models that purport to provide useful predictions and thus to help guide effective management strategies 9 . A basic class of such models separates a population into various compartments-each comprising individuals at a similar stage before, during, or after infection-and keeps track of the population fraction in each compartment over time, by balancing loading, discharge, and accumulation rates. The archetype for this modelling approach is the celebrated SIR model structure [10][11][12][13][14][15][16][17] which splits a population into three compartments: susceptible (S) to the infection, infectious (I), and the rest (R) being immune or removed from infectious by recovery or death. The dynamics of how individuals move from S to I to R was developed almost a century ago in a mathematical modelling tour-deforce by Kermack and McKendrick 18 who derived a general, if elaborate model structure in Eqs. (11)-(15) of their landmark paper. In the same publication (Eq. (29) ibid.) these authors also presented a well characterized special case in the form of the following three simple ordinary differential equations (ODEs) comprising the widely used standard SIR model: where s, i, r are the susceptible, infectious, and removed fractions of a fixed-size population, respectively; β, γ are infectivity and discharge constants, respectively; and each of the Eqs. (1)-(3) can be derived from the remaining two using the compatibility condition (1) s ′ (t) = −βs(t)i(t) (2) i ′ (t) = βs(t)i(t) − γ i(t)  15,18 . In fact, it immediately follows from stability analysis of Eqs. (1) and (2) that the threshold value for s implied by the SIR model is where R 0 (introduced as such later 15,19,20 ) is the basic reproductive ratio, widely considered "one of the most critical epidemiological parameters" 11,21 . It also follows 18 from Eqs. (1)-(3) that the total fraction of individuals infected throughout an epidemic, r(∞) , is the real solution of the transcendental algebraic equation as depicted in Fig. 1. That figure shows the rapid escalation of r(∞) as R 0 rises above 1, given an initially susceptible population (In fact, making time dimensionless as η def = γ t , immediately transforms Eqs. (1) and (2) to s ′ (η) = R 0 s(η)i(η), i ′ (η) = (R 0 s(η) − 1)i(η) , whose only parameter is R 0 ).
The above two quantitative predictions by Eqs. (5) and (6) lend exceptional value to the SIR model, both conceptually and computationally. For instance, they can be used to assess herd immunity 11 for a population, corresponding to an estimated value of R 0 achieved by non-pharmaceutical or pharmaceutical interventions 22 . Or, conversely, for an epidemic that ran its course or in development, data can be used to gauge an overall or temporary value of R 0 21 .
However, as we will substantiate in the next section, there are another two important quantitative predictions of the standard SIR model that, we argue, can be problematic (see Fig. 1 for visualization): The above two shortcomings are not confined to the standard SIR model but, as we elaborate in the next section, are far more pervasive and reach a wide area in compartment-based epidemiology modeling spanned by SIR variants.
To start with, good prediction of both the infectious peak, i * , and the time to that peak, t * , is of paramount importance when considering management strategies for an epidemic. This is because i * and t * significantly affect the resources needed for care of infectious patients. To wit, calls for Flattening the Curve 22 during the COVID-19 epidemic aimed precisely at lowering i * and thus averting the overwhelming of medical care resources 23 .
In addition, good estimates of R 0 from data of exponential growth during the spread of an epidemic are critical for assessing the situation and for designing effective interventions 9,21 .
Furthermore, and more importantly, to the extent that predictions of the infectious peak and time-to-peak by the standard SIR model may be problematic, the problem is not confined to the I compartment of the standard SIR model. Rather, it may be endemic (no pun intended) in the numerous possible variants of compartmentbased epidemiology models with loading and discharge terms. Such variants include a variety of compartments with corresponding arrangements and interactions (e.g., SEIR, SI, SIS, or similar 24 ), multiple subpopulations (e.g., of different age and/or social contact structure 11,16,17,25 ), spatial variation in addition to temporal (entailing partial differential equations 11 ), and any combinations thereof, which collectively lead to diverse stratification patterns 26 . In the voluminous literature dealing with such models, the discharge rate from a compartment is virtually always represented by a term similar to the term −γ i(t) of Eq. (2) 27 . In fact, this practice is so widespread in the entire literature of epidemiology 11,15,[28][29][30] that it is selected, perhaps uncritically, even in advanced modeling efforts which employ sophisticated tools (e.g., automated algorithmic discovery 31 ) in attempts to uncover more realistic expressions for infection dynamics. It is plausible, therefore, to claim that peak and time-to-peak predictions for a related compartment in any of these models may be as problematic as the corresponding predictions of the simple SIR model, with similarly adverse consequences.
Of course, for more accurate predictions, one could forego the simplifying assumptions leading to Eqs. (1)-(3) and its variants, in favor of the general time-varying integrodifferential equation patterns introduced by Kermack and McKendrick 12,29,32 . This, however, would significantly increase complexity of analysis and use 32 , which partly explains the popularity and underscores the importance of simplified models such as SIR.
Consequently, a natural question arises: Given the aforementioned shortcomings of the standard SIR model, is there a mathematical model of comparable simplicity to Eqs. (1)-(3) that retains the two sound conclusions about the epidemic threshold (Eq. (5)) and long-term epidemic course (Eq. (6)) while avoiding the two issues mentioned above, namely misrepresentation of the infectious peak, i * , and time to that peak, t * ?
Here, we constructively answer this question in the positive. Using a combination of Laplace transforms and Padé approximations to describe compartment discharge dynamics, we develop in the "The Padé SIR model structure" section (Eqs. (12) and (13)) of similar simplicity to SIR. The Padé SIR structure produces the exact same threshold and long-term values (Eqs. (5) and (6)) as Eqs. (1)-(3), while predicting more realistic infectious peak and time to peak for a wide range of practically significant cases. More importantly, because the proposed structure relies on replacement of the discharge term −γ i(t) in the I module of the SIR Eq. (2) without increasing complexity, it can be used widely in the large array of compartment-based epidemiology models to realistically represent the dynamics of compartment discharge. This immediately prompts a re-evaluation and possible revision of the wide literature on compartment-based modeling in epidemiology inspired by the SIR model. It is emphasized that the preceding prompt is not motivated by a mere intent for higher accuracy; rather, the aim is to offer higher utility, in the spirit of George Box's dictum "all models are wrong, but some are useful" 33 .
In the rest of the paper, we first present the significant merits and subtle issues of the SIR structure. Subsequently, we offer a remedy to these shortcomings, in the form of a new class of SIR variants (the Padé SIR model structure) whose properties and implications we explore for epidemiology modeling and epidemic management. Discussion and extensions follow, pointing to the usability of the proposed modeling approach and its applicability to the wide class of compartment-based epidemiology models.

Methods
To provide context and intuition for the developments that follow, we will rely on the basic schematic of Fig. 2. Directly inspired by the original Kermack-McKendrick ideas, Fig. 2 shows how the stacked fractions s, i, r of a fixed-size population change during an epidemic, as individuals move from compartment S to I to R over time. Infectious individuals in the I compartment are discharged (to enter the R compartment) at times T ≥ 0 after becoming infectious, where the infectious period T follows a cumulative distribution and corresponding density 18,29 defined in the standard way as F (θ) def = P[T ≤ θ] and {(θ ) = F ′ (θ). Simple balances around the boxed areas in Fig. 2 for a time-invariant cumulative distribution F (θ) (APPEN-DIX A) yield the equation www.nature.com/scientificreports/ which, combined with the infectivity Eq. (1) and the consistency Eq. (4) forms a general representation of the SIR system dynamics 29,32 . Selecting F in Eq. (7) to be the cumulative density function of the exponential distribution , one immediately gets the SIR model, Eqs. (1)-(3) (APPENDIX A). For that model, the parameter γ is the inverse of the average infectious period … estimated relatively precisely from epidemiological data 11 .
As will be detailed in what follows, it is at this point where issues with peak and time-to-peak misrepresentations by the SIR model may originate: Schematic of time-varying susceptible ( s, green), infectious ( i, orange), and removed ( r, blue) fractions of a fixed-size population after an initial infection, i 0 , at discretized time t 0 . Each new part of the infectious fraction i (thick-framed orange rectangles) moves to the removed fraction, r (thick-framed blue rectangles) piecewise in a number of time steps following a certain distribution. The population eventually reaches a steady state at s ∞ , r ∞ = 1 − s ∞ , and i ∞ = 0 . The pattern analogy with the stacked chart in Fig. 1  www.nature.com/scientificreports/ Heeding the above suggestion to use epidemiological data for direct estimation of the average, 1/γ , of the infectious period, T , is indeed sensible (in fact, necessary for a reasonable estimate). However, the associated distribution of T is typically far from exponential (because an exponential distribution would suggest, inter alia, that most infectious individuals leave the I compartment in zero time, an untenable assumption). Rather, T follows distributions with peak not near zero 34 as shown in Fig. 3 by the curves indexed by n ≫ 1 . The exact shape of these curves is not important; rather, these curves serve as examples of distributions f (γ θ) with peak not near 0.
The assumption of exponential distribution for the infectious period "has appeared in many epidemic models but has seldom been questioned" 27 yet would be conveniently acceptable, if it did not lead to inadvertent outcomes. Unfortunately it does, in the following subtle yet important way: While the same threshold and long-term values (Eqs. (5) and (6), respectively) would result from Eqs. (1), (7), and (4), and for practically any reasonable distribution of T with the same average, D def = 1/γ , (an insight already provided by Kermack and McKendrick 18 ) the estimated infectious peak and time to peak would be significantly affected by the kind of distribution considered, in an interesting fashion, as demonstrated in Fig. 4. This figure shows the profiles of the infectious fraction, i(t) , for the infectious period distributions in Fig. 3, with time in both dimensional and dimensionless form. The latter is in terms of dimensionless time t/D , because this simple transformation trivially makes the dynamics of all considered models dependent on R 0 alone and allows for meaningful comparisons without loss of generality. The dimensional time is in days, to provide some context for epidemics such as COVID-19 with related values [34][35][36] What is remarkable in Fig. 4 is that while different distributions of T sharing the same average, D def = 1/γ , expectedly yield different profiles of i(t) 27 these profiles quickly approach the profile corresponding to the unitimpulse distribution shown in Fig. 3. For that distribution of T , it immediately follows from Eqs. (1), (7), and (4) (APPENDIX A) that the resulting dynamic model, which we will term dSIR, comprises the delay differential equation (DDE) and the delay algebraic equations with D def = 1 γ . Therefore, the dSIR model of Eqs. (9)-(11) constitutes a more realistic representation of spreading epidemic dynamics than the standard SIR model.
Delay differential equations (DDEs) such as the above have been a classic subject of study in biology 37,38 ). DDEs are generally perceived as more difficult to analyze than ODEs 32, p. 5 perhaps because of infinite spectra (for linear DDEs) or discontinuities in the derivatives of DDE solutions-albeit the corresponding theory for DDEs such as the above "does not present substantial additional difficulties" compared to ODEs 39, p]. 6 . Nevertheless, even though Eqs. (9)-(11) have long been known 29 they are typically bypassed in favor of their ODE counterparts, Eqs. (1)-(3), along with their misrepresentations of the infectious peak and time to peak already discussed.
To address this issue, in the next section we derive novel approximations of the dSIR Eqs. (9)- (11) in the form of the Padé SIR ODEs, which have a number of advantages: While the Padé SIR model structure is as simple as that of the standard SIR model, Eqs. (1)-(3), and produces the same threshold and long-term values captured All distributions are shown in terms of the dimensionless variable γ θ and have the same average equal to 1.  (5) and (6), it produces more realistic representations for the infectious peak and time to peak than the standard SIR ODEs. As such, the Padé SIR model structure not only creates an alternative to the standard SIR model but also provides a general module that can be immediately incorporated in the wide variety of compartmentbased models used in epidemiology.

Main results
The Padé SIR model structure. Combining Laplace transforms with first-order Padé approximation (a popular approach for approximating transcendental transfer functions by polynomial rational fractions in automatic control 40,41 ) one can show (APPENDIX C) that Eqs. (9)-(11) of the dSIR model can be approximated by the first-order Padé SIR model, comprising Eqs. (1), (4), and the novel ODE  (7), for distributions shown in Fig. 3. Note that the distribution for n = 4 is closer to the exponential distribution (n = 1) than to the impulse distribution (n = ∞) in Fig. 3, yet the response of i(t) for n = 4 is a lot closer to the response for n = ∞ rather than to that for n = 1. Why Padé SIR? A basic merit of the Padé SIR model is illustrated in Fig. 5, which shows that the profiles of i(t) obtained by numerically integrating the (first-or second-order) Padé SIR models are close to that produced Figure 5. www.nature.com/scientificreports/ by the dSIR model for a range of values of R 0 , but far from the corresponding profile produced by the standard SIR model. Note that the approximation in Fig. 5 depends on R 0 def = βD and deteriorates as R 0 takes values farther away from 1, as expected by the properties of Padé approximants. In fact, the first-order Padé SIR model should be used with caution for R 0 ≥ 2 , because it would yield negative early values of r(t) , as can be immediately deduced by linear analysis of the corresponding third ODE, r ; and the same model, for larger R 0 ≥ 2 , would produce peak values of i(t) > 1 , which is clearly meaningless. However, as shown in Fig. 5, the predictions of i * by the first-order Padé SIR remain remarkably close to those of the dSIR model, even for fairly large R 0 well above 2. This behavior of approximation accentuates the value of the Padé SIR model, as values of R 0 close to (or lower than) 1 would be far more desirable than values well above 1 (Fig. 1). Of course, one could easily extend the Padé SIR model to yield r(t) values in the interval [0, 1] through the simple modification r ′ (t) = max − R 0 D s(t)i(t) + 2 D i(t), 0 , as indicated for R 0 = 5, 6 in Fig. 5. Figure 5 also shows profiles of i(t) by the second-order Padé SIR model, and indicates that Padé approximations of third or higher order could be used in an similar way, but the point of diminishing returns would be quickly reached, as model complexity would increase a lot more quickly than quality of approximation.
Before discussing the important consequences implied by the Padé SIR model, relevant properties of that model are briefly summarized next, to better support the consequences established thereafter.
Comparative summary of important properties of the Padé SIR models. The models considered can be analyzed using standard ODE or DDE theory, as already mentioned. Therefore, only aspects that bear insight or novelty will be discussed and corresponding comparisons will be made.    (18) the rates p 0 depend on R 0 s alone, as is anticipated by the corresponding dSIR, Padé SIR, and SIR models, for which introduction of the dimensionless time η = γ t def = t/D leaves R 0 as the only remaining parameter in the corresponding equations. Therefore, the above exponential rates p 0 are shown as functions of sR 0 in Fig. 6. Note that s = 1 for an epidemic without prior immunity in the population.
It is evident in Fig. 6 that the rates (or doubling periods) corresponding to the Padé SIR and dSIR models differ from their SIR counterparts by a factor of about 2, for sR 0 not much higher than 1. This agrees well with the more rapid early rise of i(t) from numerical integration of the dSIR and Padé SIR models compared to that of the SIR model, as shown in Fig. 5. Note again that despite these rate differences shown in Fig. 6, all four models considered eventually reach the same steady-state values, as captured by Eq. (14).
The importance of these discrepancies for estimation of R 0 from early epidemic data will made clear shortly.
Peak of infectious fraction. While an analytical solution for i * according to the dSIR model is not obvious to the author, a good approximation can be easily obtained (APPENDIX G) through the first-order Padé SIR model, following the same approach taken for the SIR model, to get The above i * , for the same R 0 , is exactly double the i * of the standard SIR model, which is known to be (APPENDIX G). This discrepancy accounts for the differences observed in Fig. 5 between the i * produced by the SIR and by the other three models considered. Obviously, this approximation breaks down for values of R 0 that yield i * Padé−1SIR > 1 , a situation that would be expected for large values of R 0 , as illustrated in the last plot (R 0 = 6) of Fig. 5.
The discrepancy between the SIR and Padé SIR models also manifests itself in using them for model-based predictions that depend on parameter estimates driven by epidemiological data, as discussed in the next section.

Discussion and extensions
Model-based predictions form fitting epidemiological data. An immediate and important discrepancy for the models discussed is in the estimation of R 0 from epidemiological data on daily new cases during exponential growth, i.e. from i(t) or i ′ (t) , and from the average infectious period, D def = 1/γ . Figure 6 captures the relationship between the exponential growth rate p 0 given a corresponding sR 0 . Therefore, for s(t) ≈ s = 1 , it is standard to use a simple log-plot of daily new cases vs. time to estimate the slope p 0 = ln(2)D/t d of exp p 0 t/D (where t d is the doubling period) and from that the resulting R 0 . Following this procedure for s = 1 (no prior immunity) the two Padé SIR models, Eqs. (15) and (16), yield the novel R 0 estimates the dSIR model yields Figure 6. Dimensionless exponential rate,p 0 , or doubling period, t d /D (with respect to dimensionless time, η = γ t def = t/D ) for the dSIR, Padé SIR, and SIR models, by Eqs. (17), (15), (16), and (18), respectively. The first three rates approach each other as sR 0 approaches 1, whereas the SIR rate remains about half of the other two. The dashed portion of the Padé-1 SIR line is included only to indicate the trend, as the corresponding model would not be used in that range. Recall that p 0 = ln(2)D/t d and that s = 1 for an epidemic with no prior immunity. The above Eqs. and that R 0,dSIR ≈ R 0,Padé−1SIR for small p 0 .
The important message of Fig. 6 is that systematic error may arise in the estimation of R 0 when using the standard SIR model. For example, taking D = 8.4days (Eq. (8) for COVID-19) and t d = 2.3 days (corresponding to early COVID-19 spread in the US 45 ) yields R 0,dSIR ≈ R 0,Pade−2SIR = 3.2 vs. R 0,SIR = 4 for t d D = 0.23 in Fig. 6. As t d increases, the discrepancy between R 0,dSIR or R 0,Pade−2SIR on one hand and R 0,SIR on the other becomes more pronounced.
Systematic errors in estimates of R 0 have important implications. For example, the conceptual anticipation of total infected through the pandemic, as shown in Fig. 1, following Eq. (14), is going to be significantly affected. In addition, the infectious peak is also going to be affected in a non-trivial way, as shown in Fig. 7. In that figure, profiles of i * are plotted as functions of the exponential growth rate, p 0 , through the following procedure: Given p 0 , the corresponding values of R 0 are computed according to the dSIR, Padé-1 SIR, Padé-2 SIR, and SIR models (Eqs. (21)- (24)) and, subsequently, values of i * are computed using Eq. (19) (Padé-1 SIR model) for the first three R 0 values and Eq. (20) for the fourth value of R 0 . For calibration, the dots in Fig. 7 represent calculation of i * through direct numerical integration of the dSIR Eqs. (9)-(11) for values of R 0 computed using Eq. (23). There is remarkable closeness of i * values produced by the Padé SIR models to the ideal values produced by the dSIR model, contrasted to the distance of i * values produced by the standard SIR model.
The message from this exercise is that although adjusting the parameter R 0 of the standard SIR model can fit data from exponential epidemic growth well, there will remain two significant problems, namely neither the estimated R 0 nor the predicted i * will be represented well. The proposed model structures offer a better representation.  25) and (26), with corresponding definitions, are shown in Fig. 8. It is evident that the Padé SIR model places twice as tight a restriction on (R 0 − 1) as the standard SIR model, if i is not to exceed the specified i * value. The implications of this result for tasks such as Flattening the Curve through interventions that adjust R 0 are clear.

How does the Padé SIR model work?
Underlying the Padé SIR model are constructs for approximating the unit-step cumulative distribution of the infectious time period, T , shown in Fig. 3 (n = ∞) , as explained in APPENDIX C. Graphs of these approximations and their corresponding formulas are presented in Fig. 9, along with the exponential and unit-step distributions for comparison. Note that the two Padé SIR distributions in Fig. 9 might appear absurd, as they involve negative values. However, this pattern turns out to yield acceptable values for the fractions s, i, r.
It should also be noted that Eq. (12) of the first-order Padé SIR suggests that the infectious loading rate remains   The assumption about constant φ is plausible, as it refers to the rate of spread of the epidemic (cf. Eq. (1)). While that parameter might change over time as a result of interventions taken to curb an epidemic, such changes could easily be reflected in the SIR model by a timevarying φ (cf. β in Eqs. (1) and (2)). The assumption about constant ψ, however, as widely as it may have been used, is chosen for mathematical convenience rather than for reasonableness of representation: If ψ θ denotes the rate of removal, …, then the number who are removed from each θ group at the end of the interval t is ψ θ v t,θ , (ibid., p. 703).
where v t,θ shall denote the number of individuals in unit area at the time t who have been infected for θ intervals (ibid., p. 702).  Figure 1). The horizontal slices of equal length D shown in the orange area for i(t) are the continuous counterparts of the same area in the discretized plot of Fig. 2 Indeed, all four models considered in this study (dSIR, 1-/2-Padé SIR, and SIR) fit well the data mentioned. Yet, were these models to be used for fitting the early exponential spread of the epidemic, their projections would be quite different, as already elaborated on.
Extensions. As already mentioned, the proposed approach to compartment-based epidemiological modeling is applicable to model structures with a variety of compartments and flows among them. For these structures, the corresponding ODE models resulting from compartment discharge rates proportional to the load of each corresponding compartment 14 can be immediately translated (a) from ODEs to DDEs with each compartment delay equal to the average residence time of that compartment, and (b) from DDEs to (first-or secondorder) Padé approximations, which retain an ODE structure.
To substantiate these claims by an example, we briefly discuss next an extension of the ideas developed for the SIR structure to the SPIR variant that includes a compartment P between S and I (APPENDIX H). Individuals in the P compartment (equivalent to the E compartment in the standard SEIR structure 10,11,46,47 ) are asymptomatic infectious, that is they can transmit the disease before they enter the I compartment as symptomatic infectious 48 a trait observed in several occasions, notably in the current COVID-19 epidemic 23,49,50 . Corresponding equations are shown in Table 1. Figure 11 presents a comparison of profiles of i(t) which result from numerical solution of the dSPIR, Padé SPIR, and SPIR models. The values relevant to COVID-19 35,36 are used in all simulations with R 0 def = β i D i − D p + β p D p . Additional properties of the proposed SPIR models can be established in a similar manner 51 and will be explored in more detail elsewhere.
Finally, in situations where there are data to warrant it, one can relax the basic premise of the preceding discussion, namely that the dynamics of a system with S, I, R compartments will likely be close to the dynamics of a system with a step function as cumulative distribution F of infectious period (Figs. 3 and 4). In such situations (e.g. models by Anderson et al. 52 ) a corresponding SIR-like model structure can be developed that employs the ODE i ′ (t) = α D (R 0 s(t) − 1)i(t) in place of Eq. (12), where the parameter α ( 1 ≤ α ≤ 2) is associated with the sigmoidicity of F . A full development of that case is presented in a separate publication 53 .  s ′ (t) = −β i s(t)i(t) − β p s(t)p(t) p ′ (t) = β i s(t)i(t) + β p s(t)p(t) − αp(t) i ′ (t) = αp(t) − γ i(t) r ′ (t) = γ i(t) s ′ (t) = −β i s(t)i(t) − β p s(t)p(t) p(t) = s t−D p − s(t) i(t) = s(t−D i ) − s t−D p = = s(t−D i ) − s(t) − p(t) r(t) = 1 − s(t−D i ) s ′ (t) = −β i s(t)i(t) − β p s(t)p(t) p ′ (t) = 2 β i s(t)i(t) + β p s(t)p(t) − p(t) Dp

Conclusion
We have made a case for revisiting the standard SIR model that describes the spread of infectious disease epidemics. While that model features valuable insights, it also has fundamental shortcomings related to quantifying the spread of an epidemic, as detailed in the main text. Therefore, use of that model to manage an epidemic could have adverse consequences. A remedy to this problem is proposed in the form of the Padé SIR model structure, which retains all qualitative features of the standard SIR structure as well as its simplicity, yet mitigates its systematic errors. It is also noted that the remedy proposed is not confined to the standard SIR model, but is applicable to the numerous compartment-based epidemiological models that constitute SIR variants, a re-examination of which would be warranted. The tools developed here can be easily and transparently incorporated in related software for practitioners or researchers 44,54,55 . Related formulas, derived in the main text, can be used both for epidemiological data processing to guide decision making as well as for theoretical analysis to advance the mathematical theory of epidemics.
Received: 7 January 2021; Accepted: 30 March 2022 Figure 11. Comparison of the infectious fraction, i, produced by the dSPIR, Padé-1 SPIR, Padé-2 SPIR, and SPIR models for a number of values of R 0 (cf. Figure 5). Note that the total infected fraction at any moment would comprise the sum of p and i fractions.