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Recent rigidity results for graphs with prescribed mean curvature

  • This survey describes some recent rigidity results obtained by the authors for the prescribed mean curvature problem on graphs u : MR. Emphasis is put on minimal, CMC and capillary graphs, as well as on graphical solitons for the mean curvature flow, in warped product ambient spaces. A detailed analysis of the mean curvature operator is given, focusing on maximum principles at infinity, Liouville properties, gradient estimates. Among the geometric applications, we mention the Bernstein theorem for positive entire minimal graphs on manifolds with non-negative Ricci curvature, and a splitting theorem for capillary graphs over an unbounded domain?? M, namely, for CMC graphs satisfying an overdetermined boundary condition.

    Citation: Bruno Bianchini, Giulio Colombo, Marco Magliaro, Luciano Mari, Patrizia Pucci, Marco Rigoli. Recent rigidity results for graphs with prescribed mean curvature[J]. Mathematics in Engineering, 2021, 3(5): 1-48. doi: 10.3934/mine.2021039

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  • This survey describes some recent rigidity results obtained by the authors for the prescribed mean curvature problem on graphs u : MR. Emphasis is put on minimal, CMC and capillary graphs, as well as on graphical solitons for the mean curvature flow, in warped product ambient spaces. A detailed analysis of the mean curvature operator is given, focusing on maximum principles at infinity, Liouville properties, gradient estimates. Among the geometric applications, we mention the Bernstein theorem for positive entire minimal graphs on manifolds with non-negative Ricci curvature, and a splitting theorem for capillary graphs over an unbounded domain?? M, namely, for CMC graphs satisfying an overdetermined boundary condition.


    Cancer, the abnormal growth of tumor cells that invade other body parts, is now the second leading cause of death worldwide after cardiovascular disease. So, managing cancer disease by developing new treatment strategies is a new research area for researchers. However, it is essential to understand the dynamics of tumor cells' growth and their complex interactions with the immune system to develop new treatment strategies. To do this, researchers heavily relied on mathematical models.

    Many scientists have studied mathematical modelling of tumor evolution, interaction with different cells, and tumor proliferation by developing various models over the last few decades [1,2,3,4,5,6,7,8]. Allison et al. [9] developed an experiment-based, mathematical model to measure the effect of tumor growth rate, carrying capacity, and cytolytic activity of the effector cells on the progression of a tumor. Li et al. [10] explored the effects of angiogenic growth factors secreted by the tumor associated with the angiogenic process on tumor growth using a nonlinear time-delay model. They observed that the time delay on angiogenic growth is harmless for the model's local and global dynamical properties. In [11], the authors observed the dynamical properties such as stable steady states, unstable steady states, and limit cycles of a tumor micro-environment mathematical model consisting of tumor cells, cytotoxic T cells, and helper T cells by varying the infiltration rates of cytotoxic and helper T cells. Their results showed that the tumor always escaped when the infiltration rates of cytotoxic and helper T cells were both low. Two types of bistability can occur at intermediate values of the infiltration rates of cytotoxic and helper T cells. One is bi-stability between tumor escape and elimination; the other is between tumor escape and tumor coexistence with the immune system, the coexistence state representing either a finite equilibrium state or a time-dependent periodic solution. The tumor is permanently eliminated when the infiltration rates of cytotoxic and helper T cells are high. Ghosh and Banerjee [12] investigated the role of antibodies in cancer elimination by considering the clinical fact that antibodies can directly kill cancerous cells. Their quantitative analysis reveals that the antibodies' effectiveness plays a significant role in killing cancer cells directly. Shu et al. [13] explored the interactions between tumor cells, M1 and M2 macrophages and suggested some new results, such as the dual role of M1 and M2 immune macrophages on the tumor and the balance between the immune system and tumors in the host, which are essential from a biological perspective.

    There are several common treatment modalities for cancer, such as chemotherapy, targeted chemotherapy, radiotherapy, immunotherapy, and surgery. Among these cancer treatments, targeted chemotherapy is a systematic therapy that fights and kills the cancer cells in the tumor site without any significant effect on the effector-normal cells so that the tumor cells can not migrate to other parts of the body [14]. Mathematical modeling of tumor growth and treatment has been approached by several researchers using a variety of models over the past few decades [15,16,17]. De Pillis and his collaborators investigated several mathematical models to measure the impact of chemotherapy [18,19,20], immunotherapy [17,21], chemo-immunotherapy [22], and monoclonal antibody (mAb) therapy [23] on tumor growth and other healthy tissue. In [19], the authors observed "Jeff's phenomenon" for a tumor growth competition model. They obtained new optimal treatment protocols that lower tumor growth and stabilize the normal cell population. A phase-space analysis of a mathematical model of tumor growth with immune response and chemotherapy has been performed, and it has been observed that optimally administered chemotherapy drugs could drive the system into a desirable basin of attraction [18]. In [24], the importance of CD8+ T cell activation in cancer therapy was addressed. Moreover, Pillis et al. developed a cancer treatment model [21] in which they observed that combining chemotherapy and immunotherapy can eliminate the entire tumor rather than the therapies applied alone. An optimally controlled chemo-drug administration was presented in [20], which discussed the role of a quadratic control, a linear control, and a state constraint. In [22], it is observed that CD8+T cells play an active role in chemo-immunotherapy to kill tumor cells. The effectiveness of mAbs treatment on colorectal cancer has been discussed in [23]. An optimal feedback scheme was proposed based on [24] that aims to tumor regression under a better health indicator profile and to improve treatment strategies in the case of mixed immunotherapy and chemotherapy of tumor [25]. Ansarizadeh et al. [26] examined the effectiveness of chemotherapy on tumor regression by developing a model of partial differential equations. They observed that the closer the point of injection of the chemotherapeutic drug is to the invasive fronts, the more regression in tumor cells occurs, and they also observed a clinically verified phenomenon called "Jeff's phenomenon." Arabameri et al. [27] designed a dendritic cell-based immunotherapy model by fitting it with experimental data, which predicted that the successive injection of DC-based vaccines might be very effective in suppressing tumor cells. A combination of stem-cell and chemo-drug therapy models for cancer treatment was investigated in [28], and the results suggested that the combination treatment may cure cancer and improve the patient's life. Recently, Liu and Liu [14] proposed a targeted chemotherapy cancer treatment mathematical model that suggests that the effectiveness of targeted chemotherapy in killing tumor cells is better than regular chemotherapy. The effect and efficacy of the targeted chemotherapeutic drug were investigated in [29], which shows that an adequate dosage of the targeted chemotherapeutic drug of low molecular weight is necessary for removing tumor cells from the infected tumor system.

    In the present study, we will examine the effectiveness of targeted chemotherapy on tumor and normal cells by modifying the model of de Pillis et al. [18], which describes the interaction between tumor cells and healthy tissue or normal cells. In the very next section, we formulate our model. In Section 3, we verified the positive invariance and boundedness of the models' solutions. A steady-state analysis has been performed in Section 4. We have checked the global stability of the tumor-free state in Section 5. A numerical simulation and a concluding remark have been carried out in Sections 6 and 7.

    We consider the model developed by de Pillis et al. [18], in which a set of ordinary differential equations is used to characterize the dynamic interplay between effector cells, tumor cells, and healthy cells. We employ a novel adaptation in the model proposed by de Pillis et al. [18] that a targeted chemotherapy approach slows tumor growth. Traditional chemotherapy drugs kill all cell types at varying rates, which can cause severe side effects like hair loss, fatigue, anaemia, etc. On the other hand, targeted chemotherapy mainly targets tumor cells so that it may have fewer unintended consequences. We describe this attachment by the term kTC in the last equation of the system (2.1), where k denotes the rate of attachments of targeted chemo-drugs with tumor cells. Also, to measure the effectiveness of targeted chemotherapy on immune and normal cells, we introduce a parameter η [14]. Thus, our modification takes the following model:

    {dIdt=s+ρITσ+Tc1ITd1Ia1(1η)CI,dTdt=r1T(1b1T)c2ITc3TNa2CT,dNdt=r2N(1N)c4TNa3(1η)CN,dCdt=ud2CkTC, (2.1)

    and the initial conditions are: I(0)=I0>0, T(0)=T0>0, N(0)=N0>0 and C(0)=C0>0.I(t), T(t), and N(t) represent the densities of effector cells, tumor cells, and normal cells, respectively, at time t and C(t) represents the amount of targeted chemo drug administered at time t. In terms of the model's novelty, we normalized the number of normal cells by taking their carrying capacity equal to one.

    In this section, we will investigate whether the model (2.1) solutions are biologically feasible or not for the considered values of all parameters. To do this, we must show that the solutions of the model are positive and bounded. Using standard comparison theory [30], we get

    dI(t)dt=s+ρITσ+Tc1ITd1Ia1(1η)CIsd1I.

    Integration of the above leads to

    I(t)sd1+I(0)expd1tlimtsup[I(t)]sd1.

    Again,

    dT(t)dt=r1T(1b1T)c2ITc3TNa2CTr1T(1b1T).

    Proceeding as above, we have

    T(t)=1b1+T(0)expr1tlimtsup[T(t)]1b1.

    Similarly, we have

    dN(t)dt=r2N(1N)c4TNa3(1η)CNr2N(1N)N(t)=11+N(0)expr2tlimtsup[N(t)]1,

    and

    dC(t)dt=ud2CkTCud2CC(t)ud2+C(0)expd2tlimtsup[C(t)]ud2.

    Using the considered initial values, we assume that I(t)0,T(t)0,N(t)0 and C(t)0 for all t>0. Consequently, the corresponding domain region for the system (2.1) is

    Δ={(I,T,N,C)R4+|I(t)sd1,T(t)1b1,N(t)1,C(t)ud2}.

    The domain region Δ is positively invariant, which verifies that the model system (2.1) is biologically feasible.

    In this section, we will study the stability of the system and the system's stability around the equilibrium. To do this, we compute dIdt=0, dTdt=0, dNdt=0, and dCdt=0 and get the following equilibrium:

    ● Tumor-free equilibrium: E1(I1,T1,N1,C1) where,

    I1=r1c3r2+{c3a3(1η)a2}ud2c2, T1=0, N1=r2a3(1η)ud2r2,

    C1=ud2.

    The tumor-free equilibrium E1 exists if r1+{c3a3(1η)a2}ud2>c3r2 and r2>a3(1η)ud2.

    ● Co-axial equilibrium: E(I,T,N,C) where,

    I=r1(1b1Tc3r2+c3c4T)+{c3a3(1η)a2}ud2+kTc2,

    N=r2c4Ta3(1η)ud2+kTr2, C=ud2+kT, and from the following quadratic equation, we will calculate the value of T.

    c1IT2{sρI+c1σI+d1I+a1(1η)CI}T+{d1σI+a1σ(1η)CIsσ}=0.

    After substituting the values of I and C, we get

    a11T5+a12T4+a13T3+a14T2+a15T+a16=0, (4.1)

    where,

    a11=r1(c3c4b1)c1k2,a12=(kr1(1c3r2)+d2r1(c3c4b1))c1k+kr1(c3c4b1)(c1d2+(ρc1σd1)k),a13=[kr1(1c3r2)+d2r1(c3c4b1)][c1d2+(ρc1σd1)k]+kr1(c3c4b1)[(ρc1σd1)d2+d1σka1(1η)u]+[r1(1c3r2)d2+c3a3(1η)ua2u]c1kk2s2,a14=[r1(1c3r2)d2+c3a3(1η)ua2u][c1d2σ+(ρc1d1)k](sσk2+2kd2s2)+kr1(c3c4b1)[d1σd2+a1(1η)u]+[kr1(1c3r2)+d2r1(c3c4b1)][(ρc1σd1)d2+d1σka1(1η)u],
    a15=[r1(1c3r2)d2+c3a3(1η)ua2u][(ρc1σd1)d2+d1σka1(1η)u]+[kr1(1c3r2)+d2r1(c3c4b1)][d1σd2+a1(1η)u](2sσkd2+s2d22),
    a16=(r1(1c3r2)d2+c3a3(1η)ua2u)(d1σd2+a1(1η)u)sσd22.

    The co-axial equilibrium E exists if the roots of the equation (4.1) is positive i.e., T>0 and following inequalities must holds:

    r1(1b1Tc3r2+c3c4T)+{c3a3(1η)a2}ud2+kT>0,and r2>c4T+a3(1η)ud2+kT.

    As N=0 implies that the patients will not be alive, we do not consider those cases where N=0. To investigate the linear stability of the system around the two above stability, we must compute the Jacobian of the system, and the Jacobian is

    M=(m11m120m14m21m22m23m240m32m33m340m420m44), (4.2)

    where

    m11=ρTσ+Tc1Td1a1(1η)C,

    m12=σρI(σ+T)2c1I,

    m14=a1(1η)I,

    m21=c2T, m22=r12r1b1Tc2Ic3Na2C,

    m23=c3T,

    m24=a2T,

    m32=c4N,

    m33=r22r2Nc4Ta3(1η)C,

    m34=a3(1η)N,

    m42=kC,

    m44=d2kT.

    ● The eigenvalues of the Jacobian matrix (4.2) corresponding to the steady-state E1 are: λ11=d1a1(1η)C1, λ12=r1c2I1c3N1a2C1, λ13=r22r2N1a3(1η)C1, and λ14=d2. Clearly, λ11<0 and λ14<0.

    Therefore, E1 will stable if λ12<0r1<c2I1+c3N1+a2C1 and λ13<0r2<2r2N1+a3(1η)C1; otherwise E1 becomes unstable.

    ● The Jacobian corresponding to the stability E is

    M=(m11m120m14m21m22m23m240m32m33m340m420m44), (4.3)

    where

    m11=ρTσ+Tc1Td1a1(1η)C, m12=σρI(σ+T)2c1I, m14=a1(1η)I, m21=c2T, m22=r12r1b1Tc2Ic3Na2C, m23=c3T, m24=a2T, m32=c4N, m33=r22r2Nc4Ta3(1η)C, m34=a3(1η)N, m42=kC, and m44=d2kT.

    At E, the eigen values of the corresponding Jacobian matrix (4.3) are the roots of the following equation

    λ4+A11λ3+A12λ2+A13λ+A14=0, (4.4)

    where

    A11=m11m22m33m44,A12=m11m22+m11m33+m11m44+m22m33+m22m44+m33m44m21m12m23m32m24m42,A13=m11m22(m33+m44)m33m44(m11+m22)+m23m32(m11+m44)+m24m42(m11+m33)+m12m21(m33+m44)m42(m23m34+m14m21),A14=m11m22m33m44+m11m23(m34m42m32m44)+m33m42(m14m21m11m24)m33m44m12m21.

    According to Routh-Hurwitz stability rule, the equilibrium point E will be asymptotically stable if

    A11>0,A13>0,A14>0,A11A12A13>A213+A211A14. (4.5)

    In this section, we will analyze the global stability around E1 in order to investigate the behavior of the system (2.1) far away from the equilibrium point E1. Let us define a Lyapunov function for the model (2.1) at E1 as:

    V(t)=[II1I1lnII1]+T+[NN1N1lnNN1]+[CC1C1lnCC1]. (5.1)

    Differentiating V(t) with respect to t, we get

    dVdt=(1I1I)dIdt+dTdt+(1N1N)dNdt+(1C1C)dCdt=(1I1I)[s+ρITσ+Tc1ITd1Ia1(1η)CI]+[r1T(1b1T)c2ITc3TNa2CT]+(1N1N)[r2N(1N)c4TNa3(1η)CN]+(1C1C)(ud2CkTC)=(1I1I)[ρITσ+Tc1ITd1(II1)a1(1η)CI+a1(1η)C1I1]+(r1Tr1b1T2c2ITc3TNa2TC)+(1N1N)[r2(NN1)r2(N2N21)c4TNa3(1η)N(CC1)a3(1η)C1(NN1)]+(1C1C)[d2(CC1)kTC]=(II1)[ρTσ+Tc1Td1I(II1)a1(1η)(CC1)+a1I(1η)C1(II1)]+(r1r1b1Tc2Ic3Na2C)T+(NN1)[r2(NN1)c4Ta3(1η)(CC1)]+(CC1)(d2C(CC1)kT)=(II1)2[d1I+a1I(1η)C1]+(c1+ρσ+T)(II1)Ta1(1η)(II1)(CC1)r1b1T2c2T(II1)c3T(NN1)a2T(CC1)+r2(NN1)2c4T(NN1)a3(1η)(NN1)(CC1)d2c(CC1)kT(CC1)+(r1c2I1c3N1a2C1)T=PtRPQtP,

    where,

    R=((d1Ia1I(1η)C1)12(c1+c2ρ(σ+T))0a12(1η)12(c1+c2ρ(σ+T))r1b112(c3+c4)12(a2+k)012(c3+c4)r212a3(1η)012(a2+k)12a3(1η)d2C), (5.2)

    P=[II1,T,NN1,CC1] and

    Q=[0,r1+c2I1+c3N1+a2C1,0,0].

    By noting the second component of the vector Q, we must have,

    r1+c2I1+c3N1+a2C1>0c2I1+c3N1+a2C1>r1 (5.3)

    so that QtP0.

    Furthermore, by considering the values of parameters from Table 1, if I=sd1,T=1b1 and C=ud2, then all minors are positive in the matrix R (all eigenvalues of R are also positive), and so PtRP>0. Hence, it is clear that dVdt<0.

    Table 1.  Parameter values for the simulation.
    Parameters Definition Values
    s constant popualtion of effector cells present in the body 0.05
    ρ maximum recruitment of effector cells by tumor cells 1
    σ half saturation constant forthe proliferation term 0.4
    d1 effector cells' natural death rate 0.2
    r1 intrinsic growth rate of tumor cells 0.4
    r2 normal cells' growth rate 0.35
    1b1 maximum carrying capacity of tumor cells 11.5
    d2 decay rate of targeted chemo-drug 0.05
    a1 kill rate of effector cell by targeted chemo-drug 0.2
    a2 kill rate of tumor cell by targeted chemo-drug 0.5
    a3 kill rate of normal cell by targeted chemo-drug 0.25
    c1 effector cells' growth rate due to tumor cells 0.2
    c2 tumor cells' decay rate due to immune cells 0.3
    c3 tumor cells' decay rate due to normal cells 0.2
    c4 normal cells' decay rate due to tumor cells 0.25
    η effectiveness of the targeted chemo-drug 0.01
    k rate of attachments of targeted chemo-drugs with tumor cells 0.01

     | Show Table
    DownLoad: CSV

    Therefore, the tumor-free equilibrium E1 satisfies local stability conditions, making the point globally stable. In biological terms, it means that targeted chemotherapy will kill the tumor cells if

    c2I1+c3N1+a2C1>r1,I=sd1,T=1b1,C=ud2, (5.4)

    must hold.

    Analytical studies can only be completed with numerical verification of the derived results. In this section, we verified our analytical results of the considered system (2.1) graphically using MATHEMATICA, which is very important from a practical point of view. All the simulations have been carried out using the parameter values of Table 1 [14,18]. We take the units of the parameter values to be arbitrary.

    To investigate the effects of drugs on effector cells, tumor cells, and normal cells, we considered three cases: (a) u=0.019, (b) u=0.020 and (c) u=0.021. For u=0.019, there exist only co-axial equilibrium E=(0.198,0.0101,0.725,0.379). The eigenvalues correspond to coaxial equilibrium E are (0.254,0.248,0.0504,0.0096), implies that E is stable. Further, for u=0.020, only the co-axial equilibrium E=(0.184,0.0032,0.715,0.3997) exist and (0.270326,0.250733,0.0501065,0.00282614) are the eigenvalues correspond to it. Hence, E is stable for this case also. Thus, for the cases: (a) u=0.019 (b)u=0.020, only the co-axial equilibria exist, and tumor cells are present at this equilibrium; the drug dose could not be able to eradicate the tumor cells from the body, and hence there is a chance of the rebirth of abnormal cells. However, for the case of u=0.021, there exist only tumor-free equilibrium E1=(0.177,0,0.703,0.42). Corresponding to the equilibrium E1, the eigenvalues are 0.283,0.246,0.05,0.0037; which indicates that E1 is a stable point. Therefore, for u=0.021, no tumor cells are present in the body, and the patient recovers from the disease.

    The above scenarios can be justified in Figure 1. We observe that the density of fast proliferation tumor cells gets suppressed quickly as the amount of drugs increases from u=0.019, u=0.020 to u=0.021 (see Figure 1) and gets stable at zero for u=0.021, suggesting targeted chemotherapy's success. So, the prescribed drugs quickly affected the tumor cells, which is clinically reliable.

    Figure 1.  Density of tumor cell for I(0)=0.6,T(0)=0.4,N(0)=0.9 and C(0)=0.1 when (a) u=0.019 (red) (b) u=0.020 (blue) and (c) u=0.021 (green).

    In Figure 2, we observe that the density of effector cells decreases slowly (compared to tumor cells) while the amount of applied drug doses increases and gets stable at a required level.

    Figure 2.  Density of effector cell for I(0)=0.6,T(0)=0.4,N(0)=0.9 and C(0)=0.1 when (a) u=0.019 (red) (b) u=0.020 (blue) and (c) u=0.021 (green).

    In Figure 3, the density of normal cells is reduced more slowly (compared to tumor cells) while the amount of drugs increases. Also, the normal cells become stable at the desired level.

    Figure 3.  Density of normal cell for I(0)=0.6,T(0)=0.4,N(0)=0.9 and C(0)=0.1 when (a) u=0.019 (red) (b) u=0.020 (blue) and (c) u=0.021 (green).

    The time series diagrams of tumor cells for different tumor growth rates, r1 with drug dose u=0.021, have been presented in Figure 4.

    Figure 4.  Density of tumor cell for I(0)=0.6,T(0)=0.4,N(0)=0.9 and C(0)=0.1 when tumor growth rate (a) r1=0.4 (red) (b) r1=0.42 (blue) and (c) r1=0.44 (green) and u=0.021.

    After investigating the effect of drugs on the cell population, we are now interested in examining the interaction of tumor growth and drug administration. To examine this, we fixed the drug parameter u=0.021 (as at this level, the tumor cells can be eradicated) and varied the tumor growth rate r1. Also, we considered tumor growth rate as r1=0.4,0.42,0.44 along with the parameter Table 1. For r1=0.4, there exist only tumor-free equilibrium E1=(0.177,0,0.703,0.42) corresponding to the eigenvalues (0.283,0.246,0.05,0.0037); indicating E1 is stable. Further, for r1=0.42 and r1=0.44, only the co-axial equilibrium E=(0.205,0.0175,0.691,0.419) and E=(0.240,0.0355,0.680,0.417) exist respectively. The respective eigenvalues are (0.239+0.001i,0.2390.001i,0.0508,0.0178) and (0.241,0.181,0.0553,0.0422); hence, E is stable for both cases. Biologically, the above results can be explained that the prescribed drugs eradicate the density of tumor cells if the tumor growth rate r1 is low. From Figure 4, it can be concluded that the increase in the tumor growth rate decreases the tumor-reducing capability of the system.

    Next, we fixed the value of treatment parameter u=0.0205 and tumor growth rate, r1=0.4, to examine the optimal effects of drugs on the cell population. In this case, the system (2.1) exhibits one biologically valid equilibrium point and this E1=(0.178,0,0.710,0.41), which is tumor-free. The eigenvalues corresponds to E1 are 0.28118,0.248475,0.05,0.0004, which indicates that E1 is asymptotically stable node. From Figure 5, it can be observed that the tumor cells die off over a long period, where as the normal and immune cells are stable at their required level. Also, it is noticed that the system could reduce the density of tumor cells if tumor growth rate, r1=0.4 and drug dose, u=0.0205.

    Figure 5.  Numerical simulations of the model (2.1) showing the time variation in the size of all relative populations of the model. For these simulations, we used the following initial values: I(0)=0.6,T(0)=0.4,N(0)=0.9 with tumor growth rate, r1=0.4 and drug dose, u1=0.0205.

    In Figure 6, it is seen that the trajectory converges to the tumor-free steady state E1 with the basin of attraction in the treatment case, indicating that it is a globally stable point for the system. The steady-state E1 is a stable node, implying that the cell population incorporated with the treatment can suppress the cancer growth to zero with time increase. Biologically, this indicates that the body is recovering from the tumor regardless of the initial condition, which includes tumor growth.

    Figure 6.  Parametric plot of the system (2.1) at E1 equilibrium point by using the parameter values in Table:1 and initial values are I(0)=0.6,T(0)=0.4,N(0)=0.9 and C(0)=0.1 with u=0.0205 and r1=0.4.

    Overall, we observe that if the size of the tumor is small, i.e., the growth rate of tumor r1 is tiny, then it is quite possible to eradicate the tumor from the body using a smaller amount of drugs with less harm to the other healthy cells. If not, we require a high drug dose that can increase the side effects of the drugs.

    We have investigated a modified ODE mathematical model for tumor growth, considering the effector-tumor-normal cells' interaction under targeted chemotherapy. We established the basic characteristics, such as positivity and boundedness of the solutions of the model. To explore the dynamic behavior of the model, we performed a stability analysis of the considered system. We found that the tumor-free steady state is globally stable under the conditions: c2I1+c3N1+a2C1>r1,I=sd1,T=1b1,C=ud2, provided it is locally stable; which suggests that the prescribed treatment can eradicate tumor cells from the body for a threshold value of tumor growth rate. Numerically, it is also observed that the prescribed treatment can eradicate tumor cells from the body without much effect on other healthy cells if the tumor size is small. However, one limitation in our model is that if the tumor size is large, it requires a high amount of drugs and a long period of time, which can harm the patient's body. So, in this regard, we must need an optimum period and drug dose for which the tumor is eradicated [18,19]; and it will be carried out in our future study.

    The authors declare that they have no conflict of interest.



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