Paper 1
Paper 1
                                          Abstract: It is a known fact that there are a particular set of people who are at higher risk of
                                          getting COVID-19 infection. Typically, these high-risk individuals are recommended to take more
                                          preventive measures. The use of non-pharmaceutical interventions (NPIs) and the vaccine are playing
                                          a major role in the dynamics of the transmission of COVID-19. We propose a COVID-19 model
                                          with high-risk and low-risk susceptible individuals and their respective intervention strategies.
                                          We find two equilibrium solutions and we investigate the basic reproduction number. We also
                                          carry out the stability analysis of the equilibria. Further, this model is extended by considering the
                                          vaccination of some non-vaccinated individuals in the high-risk population. Sensitivity analyses
                                          and numerical simulations are carried out. From the results, we are able to obtain disease-free and
Citation: Ibrahim, A.; Humphries,         endemic equilibrium solutions by solving the system of equations in the model and show their global
U.W.; Khan, A.; Iliyasu Bala, S.; Baba,   stabilities using the Lyapunov function technique. The results obtained from the sensitivity analysis
I.A.; Rihan, F.A. COVID-19 Model          shows that reducing the hospitals’ imperfect efficacy can have a positive impact on the control of
with High- and Low-Risk Susceptible       COVID-19. Finally, simulations of the extended model demonstrate that vaccination could adequately
Population Incorporating the Effect of    control or eliminate COVID-19.
Vaccines. Vaccines 2022, 1, 0.
https://doi.org/
                                          Keywords: equilibrium solutions; stability analysis; COVID-19; global stability; sensitivity; vaccine
Academic Editor: Giuseppe La Torre
                            Although COVID-19 vaccines are readily available, there is no antiviral treatment that
                      has been recommended at this time for any of the COVID-19 variants [9]. Several clinical
                      trials are being conducted to evaluate the effectiveness of potential treatments. Despite
                      this, there are treatments available that can help relieve symptoms and help shorten the
                      length of the illness as well [10,11]. There are a few treatments that are aimed at relieving
                      symptoms, as well as supporting the respiratory system. Hospitalization may be necessary
                      for some people, especially if they have an underlying medical condition that requires
                      treatment [12].
                            There are more than 30 COVID-19 vaccines approved by National regulatory authori-
                      ties around the world in which most of them are proven to be effective [13]. Additionally,
                      more than half of the world’s population received at least one dose of the vaccine [14].
                      Many people refused to take the optimal dosage of the vaccine due to various reasons,
                      including due to fake information related to its safety and long-term effects. Whatever
                      the reason, there are significant consequences when individuals opt out of vaccines [15].
                      Outbreaks of COVID-19 are more likely to occur in communities where vaccination rates
                      are low. This not only puts unvaccinated individuals at risk but also increases the chances
                      that these diseases will spread to other people, including low-risk individuals.
                            The COVID-19 vaccines are the subject of extensive debate on the ideal dosage that
                      would offer the greatest degree of protection. It has been claimed by several researchers
                      that taking the booster dose is crucial for managing the condition and preventing major
                      illness or even death induced by this disease. As an interim measure, the most effective
                      way to curb the spread of this disease is through vaccination on a regular basis and in
                      accordance with the recommended schedule [16].
                            There has been numerous studies conducted to better understand how the virus
                      spreads from one person to another. The use of mathematical models to predict disease
                      transmission is beneficial for analysis and prediction, especially when tested against acces-
                      sible disease data. The initial models generally consist of deterministic ordinary differential
                      equations of the SEIR form which are rigorously analyzed by different authors taking differ-
                      ent stages into account. See, for instance, Swati et al. in [17] analyze the COVID-19 model
                      considering hospitalized individuals, and home-quarantined, or home-treated individuals.
                      According to Iboi [18], a mathematical model was developed for evaluating the influence of
                      the NPIs on the transmission pattern of the COVID-19 pandemic, as well as investigating
                      the impact of the early removal of social distancing and community lockdown measures.
                      Their work was extended by Riyapan et al. in [19], in which he added a compartment.
                            Tylicki et al. in [20] shows that the susceptible class is divided into two: the high
                      risk and the low risk. They indicated that the elderly, males, hypertensive, and patients
                      with comorbidities, constitute the most well-characterized high-risk group for severe
                      manifestations of COVID-19. None of the research mentioned above considered this
                      division in detail mathematically.
                            Understanding the dynamics of the interactions between those at low risk and those
                      at high risk is crucial to the control and prevention of COVID-19. This requires some
                      mathematical models, which have the potential to enhance our understanding of the
                      parameters associated with the increase in infection rates. Hence, our aim in this paper is
                      to examine the dynamics of COVID-19 transmission in two susceptible populations setting
                      (low- and high-risk individuals) through mathematical modeling, where we also use the
                      non-linear expression of the incidence rate. This incidence rate expression is proved to be
                      more realistic than the corresponding bilinear incidence rate [21].
                            Here, we use the COVID-19 features to develop a model and utilized some data that
                      are either real, estimated, or from the literature. In order to identify the most sensitive
                      parameter associated with the model basic reproduction number R0 , a sensitivity analysis
                      was conducted.
                            We organize this paper as follows: in Section 1, we give the introduction; Section 2 is
                      the model formulation; in Section 3, we analyse the model qualitatively, which includes
                      computing the reproduction number using a technique called the next generation ma-
Vaccines 2022, 1, 0                                                                                                  3 of 21
                      2. Model Formulation
                           In this part, we modify an existing COVID-19 model proposed by Pal Bajiya et al.
                      in [22]. The modification procedure is presented below. We define N (t) as the total human
                      population at time t divided into six sub-populations: high-risk susceptible S1 , low-risk
                      susceptible S2 , exposed E, infected I, hospitalized H, and recovered R individuals:
N ( t ) = S1 ( t ) + S2 ( t ) + E ( t ) + I ( t ) + H ( t ) + R ( t ) . (1)
                          Our model also accounts for certain demographic impacts by assuming that all sub-
                      populations have a natural death rate (µ > 0) and a net inflow of humans to the two
                      susceptible population at a rate Λ. Next, we define the incident fraction as follows:
                                                                          β( I + ϵH )
                                                                   η=                 ,                                 (2)
                                                                               N
                      where β is the effective contact rate, and ϵ is a modification factor that measures hospital in-
                      efficacy.
                            The high-risk susceptible population S1 (t) are those that are unvaccinated, human
                      with underlying medical conditions demonstrated to have a higher risk of death due to
                      COVID-19 [23], as well as the elderly [24]. Undocumented migrants associated with limited
                      access to healthcare because of legal, administrative, social barriers, etc., are also part
                      of this population. The high-risk susceptible population S1 (t) is reduced by the natural
                      death rate µ and the force of infection η. The parameter σ1 incorporates the impact of
                      the non-pharmaceutical intervention (wearing masks, physical or social distancing, and
                      washing hands regularly) by individuals in S1 on the number of contacts,
                                                    dS1
                                                        = (1 − ρ)Λ − ((1 − σ1 )η + µ)S1 .
                                                     dt
                           Similarly, the low-risk susceptible population S2 (t) includes those that are not in S1 (t),
                      and are recruited either by birth, or screened of COVID-19 by the authorities at the point of
                      entry through any of the borders. S2 (t) also reduced by natural death rate µ and force of
                      infection η, following effective contacts with an infected individual. Here, σ2 represents
                      the same interventions with S1 . High-risk individuals must take additional precautions in
                      addition to the above-mentioned actions to reduce transmission, this implies 0 ≤ σ2 < σ1 ,
                                                        dS2
                                                            = ρΛ − ((1 − σ2 )η + µ)S2 .
                                                         dt
                            Exposed individuals E(t) stands for the number of people who were exposed to the
                      virus. They are generated by the population of susceptible (high or low risk) humans that
                      become exposed or contact with the infected persons, and decreases as a result of infection
                      at a rate α and natural death at the rate µ,
                                              dE
                                                 = η ((1 − σ1 )S1 + (1 − σ2 )S2 ) − (α + µ) E.
                                              dt
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                           Infected individuals I (t) stands for the number of people who are infected but have
                      not been detected. It is reduced by either hospitalization at the rate of ν2 , recovery without
                      being hospitalized at a rate ν1 , the natural death µ, and COVID-19 induced death at a rate δ,
                                                         dI
                                                            = αE − (ν1 + ν2 + µ + δ) I.
                                                         dt
                           Hospitalized individuals H (t) are those who have been diagnosed with COVID-19
                      and have been isolated by the authorities. They are reduced due to recovery at the rate τ,
                      the natural death µ, and COVID-19 induced death at a rate δ,
                                                           dH
                                                              = ν2 I − (τ + µ + δ) H.
                                                           dt
                           Recovered individuals R(t) represents the number of recovered, undiagnosed individ-
                      uals, who are not being officially identified and those that recovered due to the impact of
                      isolation. The only decline in this population is due to the natural death rate µ,
                                                              dR
                                                                 = ν1 I + τH − µR.
                                                              dt
                            Table 1 contains the model’s state variables, whereas Table 2 lists the model parameters
                      and their descriptions. Based on the assumptions stated above, Figure 1, below, describes
                      the flow transmission of the infection from one compartment to another. The interactions is
                      represented by the system of non-linear ordinary differential equations below:
                                               dS1
                                                      = (1 − ρ)Λ − ((1 − σ1 )η + µ)S1 ,
                                                dt
                                               dS2
                                                      = ρΛ − ((1 − σ2 )η + µ)S2 ,
                                                dt
                                                dE
                                                      = η ((1 − σ1 )S1 + (1 − σ2 )S2 ) − (α + µ) E,
                                                dt                                                                       (3)
                                                dI
                                                      = αE − (ν1 + ν2 + µ + δ) I,
                                                 dt
                                               dH
                                                      = ν2 I − (τ + µ + δ) H,
                                                dt
                                                dR
                                                      = ν1 I + τH − µR.
                                                dt
                                          Variables                                         Description
                                              S1                            Number of high-risk susceptible population
                                              S2                            Number of low-risk susceptible population
                                              E                                 Number of exposed population
                                               I                                Number of infected population
                                              H                                Number of hospitalize population
                                              R                                Number of recovered population
                                              N                                     Total human population
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                             Parameter                                                  Description
                                 Λ                                          Recruitment rate
                                 β                                        Effective contact rate
                                 ρ                       Fraction of newly recruited individuals moving to S2
                                 σ1                             Rate of reduction in infectiousness in S1
                                 σ2                             Rate of reduction in infectiousness in S2
                                 µ                                       The natural death rate
                                 α              The rate of progression from exposed population to infected population
                                 ϵ                                    The rate of hospital inefficacy
                                 ν1                                  The recovery rate of infected in
                                 ν2                          The hospitalization rate of infected individuals
                                 τ                          The recovery rate of the hospitalized individuals
                                 δ                               The COVID-19 induced mortality rate
                            The basic dynamic characteristics of the model will now be discussed. Since the model
                      tracks populations of humans. In the same way as [25], the following theorem shows that
                      all the state variables are non-negative for all time t > 0.
                      Theorem 1. Consider the model (3) with initial conditions S1 (0) > 0, S2 (0) ≥ 0, E(0) ≥ 0,
                      I (0) ≥ 0, H (0) ≥ 0, and R(0) ≥ 0 then the solution is positive in R6+ .
                                                   dS1
                                                       = (1 − ρ)Λ − ((1 − σ1 )η + µ)S1 ,
                                                    dt
                      we have
                                                         dS1
                                                             ≥ −((1 − σ1 )η + µ)S1 .
                                                          dt
                           Solving for S1                                        R
                                                       S1 ( t ) ≥ S1 ( 0 ) e −       ((1−σ1 )η +µ)dt
                                                                                                       ,
                      which implies that
                                                   S1 (t) ≥ 0, since ((1 − σ1 )η + µ) > 0.
                           Similarly, S2 (t), E(t), I (t), H (t), R(t) can be demonstrated to be positive. Therefore,
                      the solution of the model (3) is a positive quantity in R6+ for all t ≥ 0.
Vaccines 2022, 1, 0                                                                                                  6 of 21
                                                                                               Λ
                                               D = {(S1 , S2 , E, I, H, R) ∈ R6+ |0 : N ≤        }.
                                                                                               µ
                                                  dN
                                                     = Λ − µN − δ( I + H ) ≤ Λ − µN,
                                                  dt
                                                               dN
                                                                  + µN ≤ Λ,
                                                               dt
                      therefore
                                                                              Λ
                                                       N (t) ≤ N (0)e−µt +      (1 − e−µt ),
                                                                              µ
                      where N (0) is the initial values, i.e., N (t) = N (0) at t = 0.
                                                                                           Λ
                          Following from [26], it can be observed that N (t) −→            µ   as t −→ ∞. Hence, N (t) is
                                                  Λ
                      bounded as 0 ≤ N (t) ≤      µ.   So, all solutions in   R6+   of the model (3) eventually enter in
                      D.
                           The proposed model is well presented epidemiologically and mathematically from
                      above in the region D . As a result, analysing the qualitative dynamics of model in D
                      is adequate.
                      3. Model Analysis
                          The model system (3) admits two equilibria: disease free equilibrium (DFE) and
                      endemic equilibrium (EE).
                                                                             (1 − ρ)Λ ρΛ
                                                                                                    
                                                  0 0 0 0         0   0
                                        DFE = (S1 , S2 , E , I , H , R ) =           ,   , 0, 0, 0, 0 .
                                                                                 µ     µ
                                                                                                               
                                  0    β((1 − σ1 )(1 − ρ) + (1 − σ2 )ρ)       βϵ((1 − σ1 )(1 − ρ) + (1 − σ2 )ρ)
                             F = 0                   0                                       0                 ,      (4)
                                  0                   0                                       0
                                                                                          
                                                   α+µ                0                0
                                              V =  −α         ν1 + ν2 + µ + δ         0   .                           (5)
                                                     0               −ν2             τ+µ+δ
                           Therefore, the basic reproduction R0 is as follows
                                                  αβ(ϵν2 + τ + µ + δ)((σ1 − σ2 )ρ + (1 − σ1 ))
                                           R0 =                                                .                        (6)
                                                     (ν1 + ν2 + µ + δ)(α + µ)(τ + µ + δ)
                           The basic reproduction number R0 defined as the number of new infections in a
                      population induced by a single infected person within a given period of time. If the R0 < 1,
                      the DFE is said to be locally stable, otherwise is said to be unstable [17].
Vaccines 2022, 1, 0                                                                                                                            7 of 21
                                    Theorem 3. The disease free equilibrium point DFE of the model (3) is said to be locally asymptoti-
                                    cally stable (LAS) if R0 < 1 and unstable if R0 > 1.
λ3 + c1 λ2 + c2 λ + c3 = 0. (9)
                                    where
                                    c1 = k 4 + k 3 + k 1 ,
                                    c2 = k1 k3 + k1 k4 + k3 k4 − αβk2 ,
                                    c3 = k1 k3 k4 − αβk2 k4 − αβϵν2 k2 = k1 k3 k4 − αβk2 (k4 + ϵν2 )
                                    = k1 k3 k4 (1 − αβk2k(1kk43+
                                                               k4
                                                                 ϵν2 )
                                                                       )
                                    = k 1 k 3 k 4 (1 − R0 ).
                                          According to Routh–Hurwitz criterion, the sufficient and necessary condition for
                                    stability is
                                                                         c1 > 0, c3 > 0, c1 c2 − c3 > 0.              (10)
                                          Because all of the model parameters are positive, the first inequality in (10) is automat-
                                    ically satisfied, the second inequality is satisfied when R0 < 1. As a result c1 c2 − c3 > 0 as
                                    long as c3 > 0 holds. Hence, the disease free equilibrium DFE of the model (3) is locally
                                    asymptotically stable when R0 < 1 and unstable whenever R0 > 1.
                                    Theorem 4. The disease-free equilibrium (DFE) of the model (3) is globally asymptotically stable
                                    (GAS) if R0 < 1.
                                    where f 1 , f 2 , and f 3 > 0 are the Lyapunov coefficient. The corresponding derivative of L0
                                    ( dL 0
                                       dt ) is given by
                                                                    µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                                                          L˙0 = −                      −                    + f 1 Ė + f 2 İ + f 3 Ḣ.          (12)
                                                                            S1                   S2
                                                      µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                                            L˙0 = −                      −                    + f 1 (η (1 − σ1 )S1 + η (1 − σ2 )S2 − k1 E)
                                                              S1                   S2                                                            (13)
                                               + f 2 (αE − k3 I ) + f 3 (ν2 I − k4 H ).
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                                            At the DFE, we linearize the (14). We note that near the DFE,
                                                               (1− ρ ) Λ            ρΛ                   S1                     S2
                                                        S1 ≤      µ      , S2   ≤    µ   and therefore   N    ≤ (1 − ρ) and     N    ≤ ρ.
                                            Using this relation, we have
                              µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                      L˙0 ≤ −                    −                    + f 1 ( β( I + ϵH )(1 − ρ)(1 − σ1 ) + β( I + ϵHρ(1 − σ2 ))
                                      S1                   S2                                                                                      (14)
                        − f 1 k1 E + f 2 (αE − k3 I ) + f 3 (ν2 I − k4 H ).
                                                      µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                                            L˙0 ≤ −                      −                    + f 1 ( β( I + ϵH )k2 − k1 E) + f 2 (αE − k3 I )
                                                              S1                   S2                                                              (15)
                                               + f 3 (ν2 I − k4 H ).
                                            We choose
                                                                                                                 αβϵk2
                                                                             f 1 = α, f 2 = k1 , and f 3 =        k4
                                      (15) becomes,
                                                   µ ( S 1 − S 10 ) 2   µ(S2 − S20 )2
                                            L˙0 ≤ −                   −               + α( β( I + ϵH )k2 − k1 E) + k1 (αE − k3 I )
                                                           S1                S2                                                                    (16)
                                                ϵα
                                               + (ν2 I − k4 H ).
                                                k4
                                                             µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                                                                                                                               
                                                                                                                αβ(ϵν2 + k4 )
                                                       =−                       −                    + Ik1 k3                 −1 .                 (17)
                                                                     S1                   S2                       k1 k3 k4
                                                                       µ ( S 1 − S 10 ) 2   µ ( S 2 − S 20 ) 2
                                                               =−                         −                    + Ik1 k3 [ R0 − 1].                 (18)
                                                                               S1                   S2
                                           Clearly, dL
                                                     dt ≤ 0 whenever R0 ≤ 0. As a result, and according to the Lasalle invariance
                                                       0
                                                                            Λ (1 − ρ )
                                                               S1∗ =                       ,
                                                                        (1 − σ1 )η ∗ + µ
                                                                                ρΛ
                                                               S2∗ =                       ,
                                                                        (1 − σ2 )η ∗ + µ
                                                                           η ∗ Λ((1 − σ2 )(1 − σ1 )η ∗ + k2 µ)
                                                               E∗ =                                              ,
                                                                        k1 ((1 − σ1 )η ∗ + µ)((1 − σ2 )η ∗ + µ)
                                                                                                                                                   (19)
                                                                           αη ∗ Λ((1 − σ2 )(1 − σ1 )η ∗ + k2 µ)
                                                               I∗ =                                                ,
                                                                        k1 k3 ((1 − σ1 )η ∗ + µ)((1 − σ2 )η ∗ + µ)
                                                                           αν2 η ∗ Λ((1 − σ2 )(1 − σ1 )η ∗ + k2 µ)
                                                              H∗ =                                                    ,
                                                                        k1 k3 k4 ((1 − σ1 )η ∗ + µ)((1 − σ2 )η ∗ + µ)
                                                                        αη ∗ Λ(k4 ν1 + τν2 )((1 − σ2 )(1 − σ1 )η ∗ + k2 µ)
                                                               R∗ =                                                        .
                                                                          µk1 k3 k4 ((1 − σ1 )η ∗ + µ)((1 − σ2 )η ∗ + µ)
                                      where
                                                                                             β( I ∗ + ϵH ∗ )
                                                                                     η∗ =                    ,                                     (20)
                                                                                                    N∗
                                      and N ∗ = S1∗ + S2∗ + E∗ + I ∗ + H ∗ + R∗
Vaccines 2022, 1, 0                                                                                                                9 of 21
aη ∗2 + bη ∗ + c = 0. (21)
                                   where
                                         a = k5 k6 (αµk4 + αµν2 + ατν2 + αk4 ν1 + µk3 k4 ),
                                         b = µρk1 k3 k4 k5 + αµ2 k2 k4 + αµ2 k2 ν2 + αµτk2 ν2 + αµk2 k4 ν1 + µ2 k2 k3 k4 + µk1 k3 k4 k6 −
                                         βαϵµk5 k6 ν2 − βαµk4 k5 k6 − µρk1 k3 k4 k6 ,
                                         c = µ2 k1 k3 k4 − βαϵµ2 k2 ν2 − βαµ2 k2 k4 = µ2 k1 k3 k4 (1 − R0 ),
                                   where k5 = 1 − σ1 and k6 = 1 − σ2 .           √
                                                                                    2
                                       From the Equation (21) we have η ∗ = −b± 2ab −4ac .
                                       Clearly, a is greater than zero. When R0 > 1, we have the following:
                                                        c < 0,
                                                                        √                     √
                                                                 −b +    b2 − 4ac         −b − b2 − 4ac
                                                         =⇒                       > 0 and               < 0.
                                                                        2a                     2a
                                         This shows that there is a unique endemic equilibrium point.
                                         When R0 < 1, we have
                                                                   c > 0,
                                                                   =⇒ ac > 0 therefore − 4ac < 0,
                                                                   =⇒ if b2 > 4ac then b2 − 4ac > 0,
                                                                             p
                                                                   =⇒ −b ± b2 − 4ac < 0,
                                                                   otherwise no real roots of (21).
Theorem 5. The unique endemic equilibrium of (3) is GAS in D if R0 > 1, provided that
                                                                                   Iη ∗
                                                                                     
                                                                         η
                                                                   1− ∗       1− ∗        ≥0                                         (22)
                                                                        η          I η
                                   and
                                                                                          Hη ∗
                                                                                              
                                                                               η
                                                                            1− ∗        1− ∗         ≥0                              (23)
                                                                              η           H η
                                   are satisfied.
                                   Proof. In this case, we use the approach in [29–31] to establish the proof. If we consider a
                                   Lyapunov function:
                                                                                                       
                                        ∗     ∗    S1                ∗   ∗    S2                ∗      ∗  E
                      L1 (t) = ω1 S1 − S1 − S1 ln ∗ + ω2 S2 − S2 − S2 ln ∗ + ω3 E − E − E ln ∗
                                                  S1                          S2                          E
                                                                                                                       (24)
                                                                   ∗   ∗    I                 ∗      ∗   H
                                                        +ω4 I − I − I ln ∗ + ω5 H − H − H ln ∗ .
                                                                           I                             H
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                                                       S1∗ ˙             S2∗ ˙             E∗
                                                                                         
                                      ˙
                                     L1 (t) = ω1 1 −        S1 + ω 2 1 −      S2 + ω 3 1 −      Ė
                                                       S1                S2                E
                                                                                                                          (26)
                                                                         I∗               H∗
                                                                                          
                                                               + ω4 1 −       İ + ω5 1 −      Ḣ.
                                                                          I               H
                                 S1∗ ˙              S1∗
                                                     
                         ω1 1 −       S1 = ω 1 1 −         ((1 − ρ)Λ − ((1 − σ1 )η + µ)S1 )
                                 S1                 S1
                                                    S∗
                                                       
                                         = ω1 1 − 1 ((1 − ρ)Λ − (1 − σ1 )ηS1 − µS1 )
                                                    S1
                                                    S1∗
                                                       
                                         = ω1 1 −          ((1 − σ1 )η ∗ S1∗ + µS1∗ − (1 − σ1 )ηS1 − µS1 )
                                                    S1
                                                    S1∗
                                                       
                                         = ω1 1 −          ((1 − σ1 )η ∗ S1∗ − (1 − σ1 )ηS1 − µS1 + µS1∗ )
                                                    S1
                                                    S1∗
                                                                                      
                                                                                    ηS1
                                         = ω1 1 −          ((1 − σ1 )η S1 1 − ∗ ∗ − µ(S1 − S1∗ ))
                                                                       ∗ ∗
                                                                                                             (27)
                                                    S1                              η S1
                                                              
                                                                    S ∗                     
                                                                                                    S ∗ 
                                                                                   ηS
                                         = ω1 (1 − σ1 )η ∗ S1∗ 1 − 1         1 − ∗ 1∗ − ω1 1 − 1 µ(S1 − S1∗ )
                                                                    S1             η S1             S1
                                                              
                                                                    S ∗               
                                                                                                (S1 − S1∗ )2
                                                                                   ηS
                                         = ω1 (1 − σ1 )η ∗ S1∗ 1 − 1         1 − ∗ 1∗ − ω1 µ
                                                                    S1             η S1             S1
                                                              
                                                                    S ∗               
                                                                                   ηS
                                         ≤ ω1 (1 − σ1 )η ∗ S1∗ 1 − 1         1 − ∗ 1∗
                                                                    S1             η S1
                                                              
                                                                               S ∗       
                                                                     ηS                η
                                         = ω1 (1 − σ1 )η ∗ S1∗ 1 − ∗ 1∗ − 1 + ∗ ,
                                                                    η S1       S1     η
Vaccines 2022, 1, 0                                                                                            11 of 21
                      and
                              S∗                       S2∗
                                                        
                        ω2 1 − 2 S˙2 = ω2 1 −                 (ρΛ − ((1 − σ2 )η + µ)S2 )
                              S2                       S2
                                                       S2∗
                                                          
                                     = ω2 1 −                 (ρΛ − (1 − σ2 )ηS2 − µS2 )
                                                       S2
                                                       S2∗
                                                          
                                     = ω2 1 −                 ((1 − σ2 )η ∗ S2∗ + µS2∗ − (1 − σ2 )ηS2 − µS2 )
                                                       S2
                                                       S2∗
                                                          
                                     = ω2 1 −                 ((1 − σ2 )η ∗ S2∗ − (1 − σ2 )ηS2 − µS2 + µS2∗ )
                                                       S2
                                                       S2∗
                                                                                         
                                                                                       ηS
                                     = ω2 1 −                 ((1 − σ2 )η ∗ S2∗ 1 − ∗ 2∗ − µ(S1 − S2∗ ))        (28)
                                                       S2                              η S2
                                                                       S∗                              S∗
                                                                                                     
                                                                                      ηS2
                                          =   ω2 (1 − σ2 )η ∗ S2∗ 1 − 2         1 − ∗ ∗ − ω2 1 − 2 µ(S2 − S2∗ )
                                                                       S2             η S2             S2
                                                                 
                                                                       S ∗               
                                                                                                   (S2 − S2∗ )2
                                                                                      ηS2
                                          =   ω2 (1 − σ2 )η ∗ S2∗ 1 − 2         1 − ∗ ∗ − ω2 µ
                                                                       S2             η S2             S2
                                                                 
                                                                       S ∗               
                                                                                      ηS2
                                          ≤   ω2 (1 − σ2 )η ∗ S2∗ 1 − 2         1− ∗ ∗
                                                                       S2             η S2
                                                                 
                                                                                  S ∗       
                                                                        ηS  2             η
                                          =   ω2 (1 − σ2 )η ∗ S2∗ 1 − ∗ ∗ − 2 + ∗ ,
                                                                       η S2       S2     η
                      and
                                           E∗                   E∗
                                                                 
                               ω3       1−      Ė = ω3 1 −           (η (1 − σ1 )S1 + η (1 − σ2 )S2 − k1 E)
                                           E                     E
                                                                E∗
                                                                   
                                                   = ω3 1 −           (η (1 − σ1 )S1 + η (1 − σ2 )S2
                                                                 E
                                                                                                
                                                          ∗          ∗ E       ∗             ∗ E
                                                   − η (1 − σ1 )S1 ∗ + η (1 − σ2 )S2 ∗ )
                                                                       E                       E
                                                          
                                                                E ∗                  
                                                                                          ηS1      E
                                                                                                      
                                                                         ∗          ∗
                                                   = ω3 1 −           (η (1 − σ1 )S1 ∗ ∗ − ∗
                                                                 E                       η S1      E
                                                                                   
                                                                        ηS        E
                                                   + η ∗ (1 − σ2 )S2∗ ∗ 2∗ − ∗ )                                  (29)
                                                                       η S2      E
                                                                         
                                                                               E ∗  ηS          E
                                                                                                     
                                                                                            1
                                                   = ω3 η ∗ (1 − σ1 )S1∗ 1 −                   −
                                                                                E      η ∗ S1∗   E∗
                                                                               E∗
                                                                                                  
                                                                                       ηS2        E
                                                   + ω3 η ∗ (1 − σ2 )S2∗ 1 −                   −
                                                                               E       η ∗ S2∗   E∗
                                                                                             ηS E∗
                                                                                                       
                                                                            ηS       E
                                                   = ω3 (1 − σ1 )η ∗ S1∗ ∗ 1∗ − ∗ − ∗ 1 ∗ + 1
                                                                           η S1     E        η S1 E
                                                                                            ηS2 E∗
                                                                                                      
                                                                    ∗ ∗    ηS2      E
                                                   + ω3 (1 − σ2 )η S2 ∗ ∗ − ∗ − ∗ ∗ + 1 ,
                                                                           η S2     E       η S2 E
Vaccines 2022, 1, 0                                                                                                12 of 21
                      and
                                                    I∗                 I∗
                                                                       
                                             ω4 1 −      İ = ω4 1 −        (αE − k3 I )
                                                     I                  I
                                                                       I∗
                                                                                          
                                                                                          I
                                                            = ω4 1 −          αE − αE∗ ∗
                                                                        I                I
                                                                            ∗  E                                   (30)
                                                                           I               I
                                                            = ω4 αE∗ 1 −             −
                                                                            I     E∗     I∗
                                                                                   I∗ E
                                                                                              
                                                                       E       I
                                                            = ω4 αE∗      −      −       +   1   ,
                                                                       E∗     I∗   IE∗
                      and
                                                       H∗                    H∗
                                                                             
                                           ω5       1−      Ḣ = ω5 1 −           (ν2 I − k4 H )
                                                       H                     H
                                                                             H∗
                                                                                                 
                                                                                                ∗ H
                                                               = ω5 1 −             ν2 I − ν2 I
                                                                             H                   H∗
                                                                                  ∗                                (31)
                                                                         ∗       H         I      H
                                                               = ω5 ν2 I 1 −                 − ∗
                                                                                 H        I∗     H
                                                                           
                                                                              I    H         ∗
                                                                                           H I
                                                                                                    
                                                                         ∗
                                                               = ω5 ν2 I        − ∗−             +1 .
                                                                             I∗    H       H I∗
                                                                       S1∗            ηS1 E∗
                                                                                                    
                                           ˙                 ∗ ∗                E                 η
                                          L1 (t) ≤ (1 − σ1 )η S1 2 −        − ∗− ∗ ∗ + ∗
                                                                       S1       E     η S1 E η
                                                                         ∗
                                                                                      ηS E∗
                                                                                                    
                                                                       S        E                 η
                                                 +(1 − σ2 )η ∗ S2∗ 2 − 2 − ∗ − ∗ 2 ∗ + ∗
                                                                       S2       E     η S2 E η
                                                                                           I∗ E
                                                                                                    
                                                                               E      I
                                                          +(1 − σ1 )η ∗ S1∗       −     −       +  1                   (32)
                                                                               E∗    I∗    IE∗
                                                                                           I∗ E
                                                                                                    
                                                                               E      I
                                                          +(1 − σ2 )η ∗ S2∗       −     −       +  1
                                                                               E∗    I∗    IE∗
                                                                                         H∗ I
                                                                                                   
                                                                             I     H
                                                        +(1 − σ2 )η ∗ S2∗ ∗ − ∗ −               + 1   .
                                                                            I      H     H I∗
                                                                           S1∗           ηS1 E∗
                                                                                                     
                                                                                   E                η
                                                                      2−       − ∗− ∗ ∗ + ∗ =
                                                                            S1     E     η S1 E η
                                                             ∗            ∗           ∗   Iη ∗
                                                            
                                               η          Iη            S       ηS E              E      I
                                         −1 + ∗      1− ∗        + 3 − 1 − ∗ 1∗ − ∗ − ∗ + ∗
                                               η          I η           S1      η S E     I η     E     I
                                                ∗                            1 ∗
                                                                ηS1 E∗
                                                                                           
                                                 S1                                  Iη           E      I
                                          ≤−         −1 −        ∗  ∗  −1 − ∗ −1 − ∗ + ∗                    (33)
                                                 S1             η S1 E               I η          E     I
                                                                              ∗
                                                                               S ηS1 E∗ Iη ∗
                                                                                             
                                                                                                  E      I
                                                                   ≤ − ln 1 ∗ ∗ ∗              − ∗+ ∗
                                                                               S1 η S1 EI η       E     I
                                                                                            
                                                                        I           I           E      E
                                                                    = ∗ − ln ∗ + ln ∗ − ∗ .
                                                                       I           I           E       E
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Likewise,
                                                                                S2∗          ηS2 E∗
                                                                                                         
                                                                                       E                η
                                                                           2−       − ∗− ∗ ∗ + ∗ =
                                                                                S2     E     η S2 E η
                                                                 ∗           ∗          ∗    Hη ∗
                                                                
                                                       η      Hη           S      ηS E                E    H
                                                  −1 + ∗    1− ∗     + 3 − 2 − ∗ 2∗ − ∗ − ∗ + ∗
                                                      η       H η          S2     η S2 E     H η     E     H
                                                         ∗
                                                                    ηS2 E∗             Hη ∗
                                                                                            
                                                         S2                                           E    H
                                                    ≤−      −1 −     ∗  ∗  −1 −          ∗
                                                                                             −1 − ∗ + ∗                         (34)
                                                         S2         η S2 E             H η           E     H
                                                                                ∗
                                                                                 S2 ηS2 E∗ Hη ∗
                                                                                                
                                                                                                      E    H
                                                                       ≤ − ln        ∗  ∗    ∗
                                                                                                  − ∗+ ∗
                                                                                 S2 η S2 EH η        E     H
                                                                                                
                                                                           H           H            E      E
                                                                        = ∗ − ln             + ln ∗ − ∗ .
                                                                           H          H∗           E       E
                                     Similarly, we have
                                   H∗ I
                                                  ∗                            ∗ 
                           I   H                     H I          I     H          H I      I     H
                             − ∗−       +1 = −            −1 +      −      ≤ − ln       +      −
                          I∗  H    H I∗              H I∗        I∗    H∗          H I∗    I∗    H∗
                                      ∗                                                                                 (36)
                                      H            I       I   H      I         I     H         H
                              ≤ − ln       − ln        +     −     =     − ln      −    + ln        .
                                       H          I∗      I∗   H∗    I∗        I∗    H∗        H∗
                                  4. Numerical Simulations
                                         In addition to the theoretical results from the model analysis, it is also crucial that
                                  the model equations are simulated in order to gain an understanding of the model. This
                                  simulations were conducted using MATLAB R2022b on a mid-range personal laptop that
                                  features an i7 processor and 8GB of RAM on a Windows 11 operating system. In the
                                  Supplementary Materials, a copy of the simulation code that was used can be found. While
                                  it is a challenge to find suitable data for model simulation, the lack of an appropriate answer
                                  to this question continues to be a major problem. We used parameters provided in the
Vaccines 2022, 1, 0                                                                                                              14 of 21
                                   existing literature to simulate and perform a sensitivity analysis of our model. Occasionally,
                                   we assumed the values which can be seen in Table 3.
                                         We begin the numerical simulation of our model by first letting β = 0.2693 so that
                                   R0 = 0.9380 < 1 for various initial conditions. When R0 < 1 Figure 2a–d shows that
                                   the system has a DFE that is asymptotically stable which supports the result stated in
                                   Theorem 3. In Figure 3, we examine the scenario in which R0 = 2.3986 > 1 for various
                                   initial conditions. When R0 > 1 Figure 3a–d shows that the system has a DFE and it is
                                   unstable whenever R0 > 1.
(a) (b)
(c) (d)
                                   Figure 2. Time series plot of the model (3) with different initial conditions (described by a color
                                   scheme). The parameter values are given in Table 3 with β = 0.2693 so that R0 = 0.9380 < 1; (a) the
                                   high-risk susceptible, (b) the low-risk susceptible, (c) exposed, and (d) infectious.
Vaccines 2022, 1, 0                                                                                               15 of 21
(a) (b)
(c) (d)
                      Figure 3. Time series plot of the model (3) with different initial conditions (described by a color
                      scheme). The parameter values are given in Table 3 with β = 0.6886 so that R0 = 2.3986 > 1; (a) the
                      high-risk susceptible, (b) the low-risk susceptible, (c) exposed, and (d) infectious.
                      Sensitivity Analysis
                            In mathematical modeling, numerous parameter values are uncertain, this could be
                      due to incorrect parameter estimation and uncertainty regarding the accurate values of the
                      parameters. Therefore, it is reasonable to carry out sampling and sensitivity analysis to
                      identify the parameters that significantly affect the output of our model. We used a Sam-
                      pling and Sensitivity Analysis Tool (SaSAT) in [36] to recognise these parameters. This is an
                      efficient tool that enables us to analyze the sensitivity. We first have values and boundaries
                      assigned to our parameters as in Table 3. We then applied uniform probability distributions
                      to each of the parameters, in accordance with the suggestion of [36]. We evaluated Partial
                      Rank Correlation Coefficients (PRCC) with 1000 samples for each parameter per run, which
                      was resulted from the Latin hypercube sampling (LHS).
                            Figure 4 shows how varying the parameters of model (3) changes the behavior of R0 .
                      The five (5) most sensitive parameters affecting R0 are β, τ, σ2 , ν1 , and ϵ. Rising the value of
                      the recovery rate of the hospitalized individuals, rate of reduction in infectiousness of the
                      low-risk susceptible which is proportional to rising the value of σ1 might cause the value of
                      R0 to drop. Meanwhile, reducing the contact rate, hospital inefficacy might also cause the
                      value of R0 to drop significantly. This study demonstrate that isolating and hospitalizing
                      the infected persons reduces the spread of infection. Figure 5 shows the change in behavior
                      of R0 while varying the value of the most sensitive parameters.
Vaccines 2022, 1, 0                                                                                              16 of 21
                      Figure 4. Tornado plot for the model parameter sensitivities affecting the basic reproduction num-
                      ber R0 .
(a) (b)
(c) (d)
                      Figure 5. Cont.
Vaccines 2022, 1, 0                                                                                                   17 of 21
(e) (f)
                      Figure 5. Response surface plot showing the change in behavior of R0 while varying the value
                      of the most sensitive parameters. (a) Plot of R0 vs. τ and β. (b) Plot of R0 vs. τ and µ. (c) Plot of
                      R0 vs. ν1 and µ. (d) Plot of R0 vs. σ2 and σ1 . (e) Plot of R0 vs. ϵ and β (f) Plot of R0 vs. ν2 and β.
(a) (b)
                      Figure 6. The effect of the vaccine on infected COVID-19 individuals for ν3 = 0.25 and ν3 = 0.75.
                      (a) ν3 = 0.25. (b) ν3 = 0.75.
(a) (b)
                      Figure 7. The effect of the vaccine on hospitalized COVID-19 individuals for ν3 = 0.25 and ν3 = 0.75.
                      (a) ν3 = 0.25. (b) ν3 = 0.75.
(a) (b)
                      Figure 8. The effect of the vaccine on recovered individuals for ν3 = 0.25 and ν3 = 0.75. (a) ν3 = 0.25.
                      (b) ν3 = 0.75.
                      COVID-19. Understanding the influence of the NPIs on both low and high-risk individuals,
                      the impact of the vaccine on the high-risk population can help us inform public health
                      policy as it was discussed in [37]. It is equally vital to evaluate the impact of hospital
                      efficacy/inefficacy.
                            In this paper, we present a model which explains the transmission and spread of
                      COVID-19, incorporating a fraction ρ low-risk and the remaining (1 − ρ) high-risk of the
                      human population. The model also captures NPIs by both low- and high-risk individuals,
                      to reduce infection transmission and insisted that the high-risk individuals take more
                      intervention than the low-risk, similar to what is mentioned in [38]. The model was later
                      extended by incorporating the vaccination of some high-risk individuals and vaccine
                      efficacy. This study has been able to draw some important conclusions both mathematically
                      and biologically, which are summarized below.
                            Many models of the SEIR form in literature, see [21,22,39,40], did not take into con-
                      sideration the segregation in the susceptible class into low- and high-risk individuals.
                      However, considering this division is essential in providing more insight into the transmis-
                      sion dynamics of the disease, as well as guiding the relevant authorities in introducing and
                      providing plans to curtail the spread of the disease.
                      (i)   A GAS DFE occurs in the model without vaccination every time the associated basic
                            reproduction number is less than 1 and there are multiple endemic equilibria, which
                            is a GAS in a particular case.
                      (ii) Based on numerical simulations it is indicated that if some high-risk individuals
                            were vaccinated and moved to low-risk, the disease could be reduced to a minimum.
                            However, this is dependent on the coverage of vaccinations.
                      (iii) The Latin Hypercube Sampling to create 1000 samples and the resulting Partial Rank
                            Correlation Coefficients (PRCCs) were used to perform a sensitivity study of the
                            model parameter values. A tornado plot is used to visually display the results. The
                            parameters τ, (hospitalized recovery rate), σ1,2 , (reduction in infectiousness of risk
                            individuals), according to sensitivity analysis, greatly lessen an epidemic if increased.
                            However, if the rates of person-to-person interaction and hospital inefficacy are
                            reduced, transmission also decreases.
                           In order to stop the epidemic, it is crucial to improve vaccination of the high-risk
                      individuals. Law enforcement must also be strengthened in order to restrict undocu-
                      mented immigration.
                      Author Contributions: All authors contributed equally to the manuscript and typed. All authors
                      have read and agreed to the published version of the manuscript.
                      Funding: This research was funded Petchra by “Pra Jom Klao Ph.D. Research Scholarship from King
                      Mongkut’s University of Technology”.
                      Data Availability Statement: There are no underlying data.
                      Acknowledgments: The authors are grateful to the editors and reviewers for their anticipated
                      thoughtful and insightful comment that will improved the manuscript.
                      Conflicts of Interest: The authors declare no conflicts of interest.
Vaccines 2022, 1, 0                                                                                                                      20 of 21
                                    Abbreviations
                                    The following abbreviations are used in this manuscript:
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