
A mathematical model was built using delay differential equations to investigate the effect of active and passive immunotherapies in delaying the progression of Parkinson's Disease. The model described the dynamics between healthy and infected neurons and alpha-synuclein with innate and adaptive immune responses. The model was examined qualitatively and numerically. The qualitative analysis produced two equilibrium points. The local stability of the free and endemic equilibrium points was established depending on the basic reproduction number, R0. Numerical simulations were executed to show the agreement with the qualitative results. Moreover, a sensitivity analysis on R0 was conducted to examine the critical parameters in controlling R0. We found that if treatment is administered in the early stages of the disease with short time delays, alpha-synuclein is combated, inhibiting activated microglia and T cells and preserving healthy neurons. It can be concluded that administering time of immunotherapies plays a significant role in hindering the advancement of Parkinson's disease.
Citation: Salma M. Al-Tuwairqi, Asma A. Badrah. Modeling the dynamics of innate and adaptive immune response to Parkinson's disease with immunotherapy[J]. AIMS Mathematics, 2023, 8(1): 1800-1832. doi: 10.3934/math.2023093
[1] | Anusmita Das, Kaushik Dehingia, Hemanta Kumar Sharmah, Choonkil Park, Jung Rye Lee, Khadijeh Sadri, Kamyar Hosseini, Soheil Salahshour . Optimal control of effector-tumor-normal cells dynamics in presence of adoptive immunotherapy. AIMS Mathematics, 2021, 6(9): 9813-9834. doi: 10.3934/math.2021570 |
[2] | Eminugroho Ratna Sari, Lina Aryati, Fajar Adi-Kusumo . An age-structured SIPC model of cervical cancer with immunotherapy. AIMS Mathematics, 2024, 9(6): 14075-14105. doi: 10.3934/math.2024685 |
[3] | Fahad Al Basir, Konstantin B. Blyuss, Ezio Venturino . Stability and bifurcation analysis of a multi-delay model for mosaic disease transmission. AIMS Mathematics, 2023, 8(10): 24545-24567. doi: 10.3934/math.20231252 |
[4] | Theyazn H. H. Aldhyani, Abdullah H. Al-Nefaie, Deepika Koundal . Modeling and diagnosis Parkinson disease by using hand drawing: deep learning model. AIMS Mathematics, 2024, 9(3): 6850-6877. doi: 10.3934/math.2024334 |
[5] | Noufe H. Aljahdaly, Nouf A. Almushaity . A diffusive cancer model with virotherapy: Studying the immune response and its analytical simulation. AIMS Mathematics, 2023, 8(5): 10905-10928. doi: 10.3934/math.2023553 |
[6] | Ahmed J. Abougarair, Mohsen Bakouri, Abdulrahman Alduraywish, Omar G. Mrehel, Abdulrahman Alqahtani, Tariq Alqahtani, Yousef Alharbi, Md Samsuzzaman . Optimizing cancer treatment using optimal control theory. AIMS Mathematics, 2024, 9(11): 31740-31769. doi: 10.3934/math.20241526 |
[7] | Ru Meng, Yantao Luo, Tingting Zheng . Stability analysis for a HIV model with cell-to-cell transmission, two immune responses and induced apoptosis. AIMS Mathematics, 2024, 9(6): 14786-14806. doi: 10.3934/math.2024719 |
[8] | Sahabuddin Sarwardi, Hasanur Mollah, Aeshah A. Raezah, Fahad Al Basir . Direction and stability of Hopf bifurcation in an eco-epidemic model with disease in prey and predator gestation delay using Crowley-Martin functional response. AIMS Mathematics, 2024, 9(10): 27930-27954. doi: 10.3934/math.20241356 |
[9] | Turki D. Alharbi, Md Rifat Hasan . Global stability and sensitivity analysis of vector-host dengue mathematical model. AIMS Mathematics, 2024, 9(11): 32797-32818. doi: 10.3934/math.20241569 |
[10] | A. M. Elaiw, A. S. Shflot, A. D. Hobiny . Stability analysis of SARS-CoV-2/HTLV-I coinfection dynamics model. AIMS Mathematics, 2023, 8(3): 6136-6166. doi: 10.3934/math.2023310 |
A mathematical model was built using delay differential equations to investigate the effect of active and passive immunotherapies in delaying the progression of Parkinson's Disease. The model described the dynamics between healthy and infected neurons and alpha-synuclein with innate and adaptive immune responses. The model was examined qualitatively and numerically. The qualitative analysis produced two equilibrium points. The local stability of the free and endemic equilibrium points was established depending on the basic reproduction number, R0. Numerical simulations were executed to show the agreement with the qualitative results. Moreover, a sensitivity analysis on R0 was conducted to examine the critical parameters in controlling R0. We found that if treatment is administered in the early stages of the disease with short time delays, alpha-synuclein is combated, inhibiting activated microglia and T cells and preserving healthy neurons. It can be concluded that administering time of immunotherapies plays a significant role in hindering the advancement of Parkinson's disease.
Parkinson's disease (PD) is a familiar neurodegenerative disease. The death of dopaminergic neurons that secrete dopamine in the Substantia Nigra pars Compacta (SNc), a brain region, is the primary cause. Also, the autopsies of Parkinson's patients exhibited the presence of Lewy bodies, which are an aggregation of misfolded alpha-synuclein (α-syn) protein [1,2,3,4,5]. The aggregation of α-syn protein within a neuron obstructs the cell's autophagy leading to neuronal death [6,7]. As a result, the protein is released into the extracellular surroundings inducing again neuronal loss [4,8,9,10]. The pathological α-syn acts as a prion-like protein and spreads from cell to cell [11,12,13] causing toxic in recipient cells [5,7,14,15].
The immune system defends the body from foreign antigens. Microglia are innate immune cells in the central nervous system (CNS) that constantly check the brain's environment [16,17] with an immediate non-selective response against viruses [18,19]. The activation of microglia leads to the release of anti-inflammatory cytokines to protect and alert neighboring cells [20]. Moreover, they act fast to absorb and dispose of misfolded α-syn [21,22,23] to prevent neurodegeneration. However, activated microglia amid severe inflammation may fail to be regulated, causing damage to healthy neurons [20].
Adaptive immune cells are more sophisticated than innate immune cells. It provides more vital protection to the immune system since it develops a memory of antigens when encountered in the future. It is slower than the innate immune cells and takes one to two weeks to confront the antigen. The effector response takes place in two phases: The first phase is antigen recognition, cell preparation, and activation by antigen-specific T and B cells. The second stage is the effector response by activating the T cells and their exit from the lymphatic system to the disease site, alternatively, by releasing antibodies from B cells into the bloodstream. There are two types of T cells: Helper T cells (CD4+), whose function is to recognize antigens and activate the cellular response to remove disease-causing agents and stimulate B cells. The other type is cytotoxic T cells (CD8+), which are responsible for antiviral and antitumor activity [18,19]. Lymphatic tissues contain antigen-presenting cells (APCs) whose function is to produce the necessary cytokines for T cells and B cells lymphocyte maintenance [18]. They are cells that can break protein into peptides and present them with the major histocompatibility complex (MHC) at the cell surface to interact with the appropriate T cells [24]. Mature T cells are activated when the T cell receptor (TCR) recognizes the antigenic peptide complexed with MHC on an APC [25].
Microglia cells release pro-inflammatory cytokines when they encounter antigens. The persistent inflammation of the innate immune system causes an increase in the permeability of the blood-brain barrier, whose primary function is to protect the brain environment from any damage. T cells infiltrate the CNS through the blood-brain barrier and release inflammatory cytokines, and neurons eventually die due to the presence of persistent inflammation and a cytotoxic environment. Several studies have confirmed the presence of high levels of T cells in the SNc after death in Parkinson's patients compared to healthy controls [18,26].
Immunotherapy is a therapeutic strategy to modulate the immune response to confer neuroprotection in Parkinson's patients by reducing microglia activation, inhibiting pro-inflammatory T cell responses, increasing neuronal support, and removing unfolded protein. There are two types of immunotherapy; the first is active immunization, which offers the patient fragments of the pathogen protein to produce antibodies inside the body to give a long-lasting response due to eliminating the α-syn aggregation. The second is passive immunization, where patients are injected with antibodies against the antigen. Active immunization does not require repeated doses; however, passive immunization needs repeated doses [15]. An example of active immunization is PD01A, developed by AFFiRiS, which involves delivering a vaccine with a short antigen peptide that mimics a portion of α-syn and helps stimulate in vivo antibodies recognize the α-syn aggregation and not the monomeric form. Preclinical trials showed decreased α-syn scores and improved memory and motor defects. As for passive immunization, PRX002 is the first α-syn therapy developed by Prothena. Multiple ascending-dose trials of PRX002 in PD patients have shown a significant reduction of α-syn [18].
Mathematical models participated in understanding the dynamics of neurodegeneration diseases [27,28]. For example, in Alzheimer's disease, Puri and Li [29] modeled the interaction between amyloid-β, neurons, microglia, and astrocytes. They found that activated microglia play a significant role in forming neuropathy. In [30], Hao and Friedman used nonlinear partial differential equations to describe the dynamics between neurons, astrocytes, microglia, macrophages, amyloid-β aggregation, and hyperphosphorylated tau proteins. They suggested a therapeutic approach to slow the progression of the disease.
For PD models, Kuznetsova and Kuznetsova [31] presented a model that explains the aggregation of α-syn within a neuron cell. They concluded that deficiency in the degradation mechanisms is the primary cause for α-syn accumulation. Moreover, they demonstrated in [32], using two models, α-syn transmission, active and diffusive, in both healthy and diseased axons. They discovered that α-syn aggregation in Lewy bodies appears in diseased axons. In [33], Sneppen et al. formed a model describing the connection between α-syn aggregation and proteasome activity. They found that α-syn aggregation is contained when the ratio between the proteasome and α-syn is below a critical level.
The immune system protects the CNS by eliminating any form of toxicity in the brain. The clearance process creates inflammations which result in damaged neurons. The immune system's overactive response may cause neurodegeneration that leads to PD. In [34], we discussed the impact of the extracellular α-syn on the progression of PD. The model represented the relations between neurons, extracellular α-syn, and innate immune response. The model represented the relations between neurons, extracellular α-syn, and innate immune response. A reduction in extracellular α-syn and a reduction in inflammation induced by activated microglia in the CNS were examined as therapeutic interventions. We found that there is no apparent effect of the latter on delaying neuronal deterioration. Treatments that reduce extracellular α-syn, whether alone or in combination with other treatments, preserve neurons and delay Parkinson's disease.
This work investigates the effect of active and passive immunotherapies on delaying the progression of PD. The model includes the immune responses from both the innate and adaptive systems. We model the dynamics between neurons, extracellular α-syn, activated microglia, and activated T cells using delay differential equations. Delay differential equations have been used in the literature to model diseases see for example [35]. To our knowledge, this is a novel PD model that examines the impact of both active and passive immunotherapies on the dynamics of PD progression. Also, the administering time of the therapies can be explored by using delay differential equations.
The paper is outlined as follows. In Section 2, we formulate the model and present a description of the variables and parameters. The feasible region of the model is demonstrated in Section 3. The stability of the equilibrium points is investigated in Section 4. Finally, Numerical simulations adjacent to parameters analysis are illustrated in Section 5. A brief conclusion is given in Section 6.
We propose a model describing the dynamics related to the interaction between neurons, extracellular α-syn, and innate and adaptive immune cells. The model consists of five compartments: The density of healthy neurons, N(t); the density of infected neurons in the brain, I(t); the density of extracellular α-syn, αS(t); the density of the activated microglia, M(t); and the density of the activated T cells, T(t).
We assume that healthy neurons are produced at a rate of σ during neurogenesis and die during apoptosis at the rate of μ1. Extracellular α-syn infects healthy neurons at the rate of β. As a result, healthy neurons move to the infected neuron compartment. α-syn accumulates within the infected neurons, causing their death at the rate of d1. During the lysis of the infected neurons, a percentage e of survived α-syn wander off into the extracellular. Infected neurons and extracellular α-syn in the CNS lead to innate immune response and trigger microglia activation. Consequently, microglia secrete cytokines yielding the death of neurons and extracellular α-syn at the rate of a1. The inflammation due to microglia activation increases the permeability of the blood-brain barrier, causing the movement of α-syn beyond the CNS. This leads to the response of adaptive immune cells; therefore, T cells are activated. The infiltration of activated T cells propagates inflammation causing the death of neurons and extracellular α-syn at the rate of a2. We assume that the activation of microglia and T cells inhibits at the rate of μ2, μ3, respectively.
Inflammation plays a significant role in protecting the CNS; however, at the same time, damage to neurons occurs. The therapeutic approach to PD is to eliminate the excess of α-syn from the extracellular space and improve the immune system's tolerance for α-syn. Two types of immunotherapies can be delivered to PD patients, active and passive immunization. The active involves immunization with a short antigenic peptide, which imitates α-syn. The passive is to deliver anti α-syn antibodies to the brain. We embody immunotherapies in the model by assuming that after a time τ, extracellular α-syn are eliminated by a percentage of ϵ1. Accordingly, due to the immunization, the activation of microglia and T cells is inhibited by a percentage of ϵ2 and ϵ3, respectively. The model dynamics are depicted in Figure 1.
The model is formulated by the following system of nonlinear delay differential equations where the parameters belong to the interval (0,1] (see Table 1 for a summary of all the variables and parameters in the model):
N′(t)=σ−βN(t)αS(t)−a1N(t)−a2N(t)−μ1N(t),I′(t)=βN(t)αS(t)−d1I(t)−a1I(t)−a2I(t),αS′(t)=ed1I(t)−a1αS(t)−a2αS(t)−ϵ1~αS(t,τ),M′(t)=a1I(t)+a1αS(t)−ϵ2˜M(t,τ)−μ2M(t),T′(t)=a1I(t)+(a1+a2)αS(t)−ϵ3˜T(t,τ)−μ3T(t). | (2.1) |
Symbol | Definition | Units |
t | Time | day |
τ | Delay time | day |
N | Density of healthy neurons in the brain | g/ml |
I | Density of infected neurons in the brain | g/ml |
αS | Density of extracellular α-syn in the brain | g/ml |
M | Density of activated microglia | g/ml |
T | Density of activated T cell | g/ml |
σ | Density of new neurons per day due to neurogenesis | g/ml/day |
β | Neuron infection rate | ml/g/day |
μ1 | Apoptosis rate of neurons | day−1 |
μ2 | Annihilation rate of activated microglia | day−1 |
μ3 | Annihilation rate of activated T cell | day−1 |
d1 | Death rate of infected neurons due to α-syn aggregations | day−1 |
a1 | Activation rate of microglia due to extracellular α-syn and infected neurons | day−1 |
a2 | Activation rate of T cell due to extracellular α-syn and infected neurons | day−1 |
e | Percentage of α-syn survival from death of infected neurons | . |
ϵ1 | Percentage of extracellular α-syn clearance due to immunotherapy | . |
ϵ2 | Percentage of inhibited activated microglia due to immunotherapy | . |
ϵ3 | Percentage of inhibited activated T cells due to immunotherapy | . |
The development of the densities in the extracellular α-syn, ~αS(t,τ), the activated microglia, ˜M(t,τ) and the activated T cells, ˜T(t,τ) are described as follows:
(∂∂t+∂∂τ)~αS(t,τ)=−(a1+a2)~αS(t,τ), ~αS(t,0)=ed1I(t),(∂∂t+∂∂τ)˜M(t,τ)=−μ2˜M(t,τ), ˜M(t,0)=a1I(t)+a1αS(t),(∂∂t+∂∂τ)˜T(t,τ)=−μ3˜T(t,τ), ˜T(t,0)=a1I(t)+(a1+a2)αS(t). | (2.2) |
Here, we used the same approach as in [36] to model the development. Moreover, we express the boundary conditions when τ=0, that is, ~αS(t,0), ˜M(t,0) and ˜T(t,0) in terms of the state variables. By using the method of characteristic coordinates for first order partial differential equations in [37], we solve the first order partial differential equations in (2.2). We obtain the following solutions:
~αS(t,τ)=ed1I(t−τ)e−(a1+a2)τ, |
˜M(t,τ)=a1(I(t−τ)+αS(t−τ))e−μ2τ, |
˜T(t,τ)=(a1I(t−τ)+(a1+a2)αS(t−τ))e−μ3τ. |
Hence, system (2.1) can be rewritten as follows:
N′(t)=σ−βN(t)αS(t)−a1N(t)−a2N(t)−μ1N(t),I′(t)=βN(t)αS(t)−d1I(t)−a1I(t)−a2I(t),αS′(t)=ed1I(t)−a1αS(t)−a2αS(t)−ϵ1ed1I(t−τ)e−(a1+a2)τ,M′(t)=a1I(t)+a1αS(t)−ϵ2a1(I(t−τ)+αS(t−τ))e−μ2τ−μ2M(t),T′(t)=a1I(t)+(a1+a2)αS(t)−ϵ3(a1I(t−τ)+(a1+a2)αS(t−τ))e−μ3τ−μ3T(t). | (2.3) |
This section demonstrates the well-posedness of model (2.3) by establishing its positivity and boundedness in a feasible region. Also, it explores the model's equilibrium points and their existence criteria and calculates the basic reproduction number using the next-generation method.
Theorem 3.1. If the initial values of model (2.3) are non-negative, N(0)≥0, I(0)≥0, αS(0)≥0, M(0)≥0, and T(0)≥0, then the solutions of the model, N(t), I(t), αS(t), M(t), and T(t), are non-negative for all t>0.
Proof. Let N(0), I(0), αS(0), M(0) and T(0) be non-negative. From system (2.3), we have,
N′|N=0=σ≥0, |
I′|I=0=βNαS≥0, for all αS≥0. |
Thus, N(t) and I(t) are non-negative. Similarly,
αS′|αS=0=ed1(I(t)−ϵ1e−(a1+a2)τI(t−τ)). |
For τ=0,
αS′|αS=0=ed1I(t)(1−ϵ1)≥0, |
since ϵ1≤1. For τ>0, αS′|αS=0≥0, since e−(a1+a2)τ<1. Therefore, αS is non-negative. Applying the same approach, we find,
M′|M=0=a1(I(t)+αS(t)−ϵ2(I(t−τ)+αS(t−τ))e−μ2τ)≥0, |
T′|T=0=a1(I(t)−ϵ3I(t−τ)e−μ3τ)+(a1+a2)(αS(t)−ϵ3αS(t−τ)e−μ3τ)≥0. |
Hence, the solution (N(t),I(t),αS(t),M(t),T(t)) is non-negative for all t>0.
Theorem 3.2. The feasible region of model (2.3),
Ω∗={(N,I,αS,M,T)∈R5+:0≤N≤σa1+a2+μ1, 0≤I≤σa1+a2+μ1,0≤αS≤ed1σ(a1+a2+μ1)(a1+a2), 0≤M≤a1σ(ed1+a1+a2)μ2(a1+a2+μ1)(a1+a2),0≤T≤σ(ed1+a1)μ3(a1+a2+μ1)}, |
is positively invariant.
Proof. From the first equation in (2.3), we obtain
N′≤σ−(a1+a2+μ1)N. |
Thus,
ddt[N exp{∫t0(a1+a2+μ1)dρ}]≤σ exp{∫t0(a1+a2+μ1)dρ}. |
Integration yields,
N(t)≤N0e−(a1+a2+μ1)t+σ(a1+a2+μ1)−σ(a1+a2+μ1)e−(a1+a2+μ1)t. |
Thus, limsupt→∞N(t)≤σ/(a1+a2+μ1). Consequently, I(t)≤σ/(a1+a2+μ1), since infected neurons I are a part from the healthy neurons N. From the third equation in (2.3), we have
αS′≤ed1I−(a1+a2)αS≤ed1σ(a1+a2+μ1)−(a1+a2)αS. |
Integration gives,
αS(t)≤αS0−ed1σ(a1+a2+μ1)(a1+a2)e−(a1+a2)t+ed1σ(a1+a2+μ1)(a1+a2). |
Therefore, limsupt→∞αS(t)≤ed1σ/[(a1+a2+μ1)(a1+a2)]. Similarly, from the rest of the equations in (2.3), we have
limsupt→∞M(t)≤a1σ(ed1+a1+a2)μ2(a1+a2+μ1)(a1+a2), |
limsupt→∞T(t)≤σ(ed1+a1)μ3(a1+a2+μ1). |
Next, we prove that Ω∗ is a positively invariant set. Let (N(0), I(0), αS(0),M(0), T(0)) be in Ω∗, From (2.3), we have
N′+I′+αS′+M′+T′=σ−(a1+a2+μ1)N−d1I−a2I+a1(αS+I)+ed1I−μ2M−μ3T−ϵ1ed1I(t−τ)e−(a1+a2)τ−ϵ2a1(I(t−τ)+αS(t−τ))e−μ2τ−ϵ3(a1I(t−τ)+(a1+a2)αS(t−τ))e−μ3τ. |
Then
N′+I′+αS′+M′+T′≤σ−(a1+a2+μ1)N−(d1+a2−a1−ed1)I+a1αS−μ2M−μ3T. |
At the boundary,
N′+I′+αS′+M′+T′≤σ−(a1+a2+μ1)σ(a1+a2+μ1)−(d1+a2−a1−ed1)σ(a1+a2+μ1)+a1ed1σ(a1+a2+μ1)(a1+a2)−μ3σ(ed1+a1)μ3(a1+a2+μ1)−μ2a1σ(ed1+a1+a2)μ2(a1+a2+μ1)(a1+a2). |
After simplifying, we get
N′+I′+αS′+M′+T′≤−σ(d1+a2)(a1+a2+μ1)−a1σ(a1+a2)(a1+a2)(a1+a2+μ1)<0. |
Hence, the solution (N(t),I(t),αS(t),M(t),T(t)) stays in Ω∗. Therefore, Ω∗ is positively invariant.
Equilibrium points of model (2.3) are calculated by equating the right-hand side equations to zero, that is,
σ−βN(t)αS(t)−a1N(t)−a2N(t)−μ1N(t)=0, | (3.1) |
βN(t)αS(t)−d1I(t)−a1I(t)−a2I(t)=0, | (3.2) |
ed1I(t)−a1αS(t)−a2αS(t)−ϵ1ed1I(t−τ)e−(a1+a2)τ=0, | (3.3) |
a1I(t)+a1αS(t)−ϵ2a1(I(t−τ)+αS(t−τ))e−μ2τ−μ2M(t)=0, | (3.4) |
a1I(t)+(a1+a2)αS(t)−ϵ3(a1I(t−τ)+(a1+a2)αS(t−τ))e−μ3τ−μ3T(t)=0. | (3.5) |
At equilibrium, we have
limt→∞I(t)=limt→∞I(t−τ),limt→∞αS(t)=limt→∞αS(t−τ). |
If αS=0, then from (3.3), I=0. Substituting for αS=I=0 in (3.4) and (3.5), we get, M=T=0. Consequently, from (3.1), we obtain, N0=σ/(a1+a2+μ1). Hence, the model has a free equilibrium point, E0=(N0,0,0,0,0), which exists always with no conditions.
Next, we find the basic reproduction number using the free equilibrium point and the next-generation method [38]. The infected compartments in model (2.3) are I and αS. Let X=(I,αS)T, then Eqs (3.2) and (3.3) can be rewritten as X′=T(X)−V(X), where
T=[βN(t)αS(t)0]and V=[(d1+a1+a2)I(t)(a1+a2)αS(t)+ϵ1ed1I(t−τ)e−(a1+a2)τ−ed1I(t)]. |
By evaluating the Jacobian of T and V at the free equilibrium point, we have the following matrices T and V, respectively:
T=[0βN000]and V=[(d1+a1+a2)0ed1(ϵ1e−(a1+a2)τ−1)(a1+a2)]. |
The inverse of V is
V−1=[1d1+a1+a20ed1(1−ϵ1e−(a1+a2)τ)(d1+a1+a2)(a1+a2)1a1+a2]. |
Hence, the next-generation matrix is
K=TV−1=[βN0ed1(1−ϵ1e−(a1+a2)τ)(d1+a1+a2)(a1+a2)βN0a1+a200]. |
The reproduction number is the spectral radius of K, that is,
R0=βN0ed1(1−ϵ1e−(a1+a2)τ)(d1+a1+a2)(a1+a2). | (3.6) |
Alternatively,
R0=σβed1(1−ϵ1e−(a1+a2)τ)(d1+a1+a2)(a1+a2)(a1+a2+μ1), | (3.7) |
where N0=σ/(a1+a2+μ1).
To find the endemic equilibrium point of the model, that is, E∗=(N∗,I∗,αS∗,M∗,T∗), we solve the Eqs (3.1)–(3.5). From Eq (3.1), we obtain
N∗=σβαS∗+a1+a2+μ1. |
Substituting N∗ in Eq (3.2), yields
I∗=σβαS∗(βαS∗+a1+a2+μ1)(d1+a1+a2). |
Inserting I∗ into Eq (3.3), we have
ed1(1−ϵ1e−(a1+a2)τ)βσ(d1+a1+a2)(βαS∗+a1+a2+μ1)=(a1+a2). |
Hence,
αS∗=ed1(1−ϵ1e−(a1+a2)τ)−(a1+a2+μ1)(a1+a2)(a1+a2+d1)β(a1+a2+d1)(a1+a2). |
Rewriting αS∗ in terms of R0 as
αS∗=(a1+a2+μ1)(R0−1)β. |
From Eq (3.4), we obtain
M∗=a1(I∗+αS∗)(1−ϵ2e−μ2τ)μ2. |
Finally, from Eq (3.5), we get
T∗=(a1(I∗+αS∗)+a2αS∗)(1−ϵ3e−μ3τ)μ3. |
We summarize the results in the following theorem.
Theorem 3.3. Model (2.3) has two equilibrium points:
● Free equilibrium point, E0=(N0,0,0,0,0) exists always, where N0=σa1+a2+μ1.
● Endemic equilibrium point, E∗=(N∗,I∗,αS∗,M∗,T∗) exists when R0>1, where,
N∗=σR0(a1+a2+μ1),I∗=σ(R0−1)R0(a1+a2+d1),αS∗=(a1+a2+μ1)(R0−1)β, |
M∗=a1(I∗+αS∗)(1−ϵ2e−μ2τ)μ2,T∗=(a1(I∗+αS∗)+a2αS∗)(1−ϵ3e−μ3τ)μ3. |
Using the linearization method for delay differential equations [38,39], we examine the local stability of the equilibrium points of model (2.3). For global stability of the free equilibrium point, the theorems of Castillo-Chavez and Song [40] are utilized in the same manner as in [41].
Theorem 4.1. The free equilibrium point, E0=(N0,0,0,0,0), of model (2.3) is locally asymptotically stable if R0<0.5(1−ϵ1e−(a1+a2)τ).
Proof. First, we prove the stability of E0 for τ=0. The Jacobian matrix of model (2.3) evaluated at E0 is:
J(E0)=[−(a1+a2+μ1)0−βN0000−(d1+a1+a2)βN0000ed1(1−ϵ1)−(a1+a2)000a1(1−ϵ2)a1(1−ϵ2)−μ200a1(1−ϵ3)(a1+a2)(1−ϵ3)0−μ3]. |
The characteristic equation, |J(E0)−λI|=0, gives
(−μ3−λ)(−μ2−λ)(−(a1+a2+μ1)−λ)[λ2+(2a1+2a2+d1)λ+(a1+a2)(a1+a2+d1)(1−βN0ed1(1−ϵ1)(a1+a2)(a1+a2+d1))]=0. |
Thus,
(−μ3−λ)(−μ2−λ)(−(a1+a2+μ1)−λ)[λ2+(2a1+2a2+d1)λ+(a1+a2)(a1+a2+d1)(1−R0)]=0. |
Clearly, λ1=−μ2, λ2=−μ3 and λ3=−(a1+a2+μ1). As for λ4,5, they satisfy the equation:
P(λ)=λ2+α1λ+α2=0, | (4.1) |
where
α1=2a1+2a2+d1,α2=(a1+a2)(a1+a2+d1)(1−R0). |
All terms of the quadratic equation (4.1) are positive if R0|τ=0<1. Hence, the eigenvalues λ4,5 are negative. Therefore, for τ=0, E0 is locally asymptotically stable if R0|τ=0<1.
Next, we investigate the stability of E0 for τ>0. The Jacobian matrix of model (2.3) evaluated at E0 is
J(E0)=J1(E0)+J2(E0), |
where
J1(E0)=[−(a1+a2+μ1)0−βN0000−(d1+a1+a2)βN0000ed1−(a1+a2)000a1a1−μ200a1(a1+a2)0−μ3], |
J2(E0)=[00000000000−ed1ϵ1e−(a1+a2)τ0000−a1ϵ2e−μ2τ−a1ϵ2e−μ2τ000−a1ϵ3e−μ3τ−(a1+a2)ϵ3e−μ3τ00]. |
The characteristic equation for delay differential equations is |J1(E0)+J2(E0)e−λτ−λI|=0. Then
(−μ3−λ)(−μ2−λ)(−(a1+a2+μ1)−λ)[(d1+a1+a2+λ)(a1+a2+λ)−βN0ed1(1−ϵ1e−(a1+a2)e−λτ)]=0. | (4.2) |
Clearly, λ1=−μ2, λ2=−μ3 and λ3=a1+a2+μ1. For λ4,5, they satisfy the equation:
P(λ)=λ2+(d1+2a1+2a2)λ+(d1+a1+a2)(a1+a2)−βN0ed1(1−ϵ1e−(a1+a2)τe−λτ)=0. | (4.3) |
Rewrite (4.3) as:
P(λ)=(λ2+aλ+b)+ce−λτ=0, | (4.4) |
where
a=d1+2a1+2a2,b=(d1+a1+a2)(a1+a2)−βN0ed1,c=βed1N0ϵ1e−(a1+a2)τ. |
Separate P(λ) as:
P(λ)=P1(λ)+P2(λ)e−λτ=0, |
where
P1(λ)=λ2+aλ+b,P2(λ)=c. |
Assume that λ=iw, where w∈R, Then,
P(iw)=P1(iw)+P2(iw)e−iwτ=0. |
Using Euler's formula, we have
P(iw)=P1(iw)+P2(iw)(cos(wτ)−isin(wτ))=0. |
Now,
P1(iw)=−w2+iaw+b,P2(iw)=c. |
Let
P1(iw)=R1(w)+iQ1(w),P2(iw)=R2(w)+iQ2(w), |
where R1, R2, Q1 and Q2 are the real and imaginary parts of P1 and P2, respectively. Then
R1(w)=−w2+b,Q1(w)=aw,R2(w)=c,Q2(w)=0. |
Thus,
P(iw)=R1(w)+iQ1(w)+R2(w)(cos(wτ)−isin(wτ))=0. |
This equation equals zero if and only if the real and the imaginary parts are zero. Therefore,
R1(w)=−R2(w)cos(wτ),Q1(w)=R2(w)sin(wτ). |
By squaring the above two equations, we have
R21(w)=R22(w)cos2(wτ),Q21(w)=R22(w)sin2(wτ). |
Adding these two equations, we obtain
R21(w)+Q21(w)−R22(w)=0. |
That is,
w4+(a2−2b)w2+b2−c2=0. |
Let u=w2, then we get
u2+(a2−2b)u+b2−c2=0. | (4.5) |
We explore the criteria for Eq (4.5) to have negative roots. If a2−2b and b2−c2 are positive, then the roots are negative. Now,
a2−2b=d21+2a1d1+2a2d1+4a1a2+2a21+2a22+2βN0ed1>0, |
b2−c2=(d1+a1+a2)2(a1+a2)2−(βN0ed1)2ϵ21e−2(a1+a2)τ−2(d1+a1+a2)(a1+a2)(βN0ed1)+(βN0ed1)2=(d1+a1+a2)2(a1+a2)2(1−2βN0ed1(d1+a1+a2)(a1+a2))+(βN0ed1)2(1−ϵ21e−2(a1+a2)τ)=(d1+a1+a2)2(a1+a2)2(1−2R0(1−ϵ1e−(a1+a2)τ))+(βN0ed1)2(1−ϵ21e−2(a1+a2)τ). |
If R0<0.5(1−ϵ1e−(a1+a2)τ), then b2−c2>0. Note that ϵ1e−(a1+a2)τ<1. Thus, The roots of Eq (4.5) are negative if R0<0.5(1−ϵ1e−(a1+a2)τ). But w∈R, then the eigenvalues λ≠iw. Therefore, the eigenvalues do not change their signs to a positive sign when τ increases and remain negative as they were when τ=0. Hence, E0 is locally asymptotically stable if R0<0.5(1−ϵ1e−(a1+a2)τ).
Theorem 4.2. The endemic equilibrium point, E∗=(N∗,I∗,αS∗,M∗,T∗), of model (2.3) is locally asymptotically stable if R0>2(1−ϵ1e−(a1+a2)τ).
Proof. First, we prove the stability of E∗ for τ=0. The Jacobian matrix of model (2.3) evaluated at E∗ is:
J(E∗)=[−(βαS∗+a1+a2+μ1)0−βN∗00βαS∗−(d1+a1+a2)βN∗000ed1(1−ϵ1)−(a1+a2)000a1(1−ϵ2)a1(1−ϵ2)−μ200a1(1−ϵ3)(a1+a2)(1−ϵ3)0−μ3]. |
The characteristic equation, |J(E∗)−λI|=0, yields
(−μ3−λ)(−μ2−λ){−βαS∗(βN∗ed1(1−ϵ1))−(βαS∗+a1+a2+μ1+λ)×[(d1+a1+a2+λ)(a1+a2+λ)−βN∗ed1(1−ϵ1)]}=0. |
It is easy to see that λ1=−μ2 and λ2=−μ3. As for λi (i=3,4,5), they satisfy the equation:
P(λ)=λ3+γ2λ2+γ1λ+γ0=0, | (4.6) |
where,
γ2=βαS∗+3a1+3a2+d1+μ1,γ1=(βαS∗+a1+a2+μ1)(2a1+2a2+d1)+(a1+a2+d1)(a1+a2)(1−βN∗ed1(1−ϵ1)(a1+a2+d1)(a1+a2))=(βαS∗+a1+a2+μ1)(2a1+2a2+d1)+(a1+a2+d1)(a1+a2)(1−βσed1(1−ϵ1)R0|τ=0(a1+a2+d1)(a1+a2)(a1+a2+μ1))=(βαS∗+a1+a2+μ1)(2a1+2a2+d1),γ0=(βαS∗+a1+a2+μ1)(a1+a2+d1)×(a1+a2)(1−βN∗ed1(1−ϵ1)(a1+a2+d1)(a1+a2))+β2αS∗N∗ed1(1−ϵ1)=β2αS∗N∗ed1(1−ϵ1). |
We can see that γ2, γ1 and γ0 are all positive. Thus, the eigenvalues λ3,4,5 are negative. Hence, for τ=0, E∗ is locally asymptotically stable.
We continue the proof by exploring the stability of E∗ for τ>0. The Jacobian matrix of model (2.3) evaluated at E∗ is
J(E∗)=J1(E∗)+J2(E∗), |
where
J1(E∗)=[−(βαS∗+a1+a2+μ1)0−βN∗00βαS∗−(d1+a1+a2)βN∗000ed1−(a1+a2)000a1a1−μ200a1(a1+a2)0−μ3], |
J2(E∗)=[00000000000−ed1ϵ1e−(a1+a2)τ0000−a1ϵ2e−μ2τ−a1ϵ2e−μ2τ000−a1ϵ3e−μ3τ−(a1+a2)ϵ3e−μ3τ00]. |
The characteristic equation is |J1(E∗)+J2(E∗)e−λτ−λI|=0, we have
(−μ3−λ)(−μ2−λ)[(−(βαS∗+a1+a2+μ1)−λ)×[(d1+a1+a2+λ)(a1+a2+λ)−βN∗ed1(1−ϵ1e−(a1+a2)e−λτ)]−βαS∗(βN∗ed1(1−ϵ1e−(a1+a2)e−λτ))]=0. | (4.7) |
We find that λ1=−μ2, λ2=−μ3 and λi (i=3,4,5) satisfy the following equation:
P(λ)=λ3+[d1+3a1+3a2+βαS∗+μ1]λ2+[(d1+a1+a2)(a1+a2)−βN∗ed1(1−ϵ1e−(a1+a2)τe−λτ)+(d1+2a1+2a2)(βαS∗+a1+a2+μ1)]λ+(d1+a1+a2)(a1+a2)(βαS∗+a1+a2+μ1)−βN∗ed1(1−ϵ1e−(a1+a2)τe−λτ)(a1+a2+μ1)=0. | (4.8) |
Rewrite (4.8) as
P(λ)=(λ3+r2λ2+r1λ+r0)+(z1λ+z0)e−λτ=0, | (4.9) |
where
r2=d1+3a1+3a2+βαS∗+μ1,r1=(d1+a1+a2)(a1+a2)−βN∗ed1+(d1+2a1+2a2)(βαS∗+a1+a2+μ1),r0=(d1+a1+a2)(a1+a2)(βαS∗+a1+a2+μ1)−(a1+a2+μ1)βN∗ed1,z1=βN∗ed1ϵ1e−(a1+a2)τ,z0=(a1+a2+μ1)βN∗ed1ϵ1e−(a1+a2)τ. |
Separate P(λ) as
P(λ)=P1(λ)+P2(λ)e−λτ=0, |
where
P1(λ)=λ3+r2λ2+r1λ+r0,P2(λ)=z1λ+z0. |
Assume that λ=iw, where w∈R. Then,
P(iw)=P1(iw)+P2(iw)e−iwτ=0. |
Using Euler's formula, we get
P(iw)=P1(iw)+P2(iw)(cos(wτ)−isin(wτ))=0. |
Now,
P1(iw)=−iw3−r2w2+ir1w+r0,P2(iw)=iz1w+z0. |
Let
P1(iw)=R1(w)+iQ1(w),P2(iw)=R2(w)+iQ2(w). |
Where R1, R2,Q1 and Q2 are the real and imaginary parts of P1 and P2, respectively. Then
R1(w)=−r2w2+r0,Q1(w)=−w3+r1w,R2(w)=z0,Q2(w)=z1w. |
Thus,
P(iw)=R1(w)+iQ1(w)+(R2(w)+iQ2(w))(cos(wτ)−isin(wτ))=0. |
This equation equals to zero if and only if the real and the imaginary parts are zero. Therefore,
R1(w)=−R2(w)cos(wτ)−Q2(w)sin(wτ),Q1(w)=R2(w)sin(wτ)−Q2(w)cos(wτ). |
By squaring the above two equations and adding them, we have
R21(w)+Q21(w)−R22(w)−Q22(w)=0. |
That is,
w6+(r22−2r1)w4+(r21−2r0r2−z21)w2+r20−z20=0. |
Let u=w2, we get
u3+(r22−2r1)u2+(r21−2r0r2−z21)u+r20−z20=0. | (4.10) |
For Eq (4.10) to have negative roots, we must show that r22−2r1>0, r21−2r0r2−z21>0 and r20−z20>0. First, we start with the coefficient of u2,
r22−2r1=(d1+2a1+2a2+βαS∗+a1+a2+μ1)2−2(d1+a1+a2)(a1+a2)+2βN∗ed1−2(d1+2a1+2a2)(βαS∗+a1+a2+μ1),r22−2r1=(d1+a1+a2)2+(a1+a2)2+(βαS∗+a1+a2+μ1)2+2βN∗ed1+2(d1+a1+a2)(a1+a2)−2(d1+a1+a2)(a1+a2)+2(d1+a1+a2)(βαS∗+a1+a2+μ1)+2(a1+a2)(βαS∗+a1+a2+μ1)−2(d1+2a1+2a2)(βαS∗+a1+a2+μ1),r22−2r1=(d1+a1+a2)2+(a1+a2)2+(βαS∗+a1+a2+μ1)2+2βN∗ed1. |
Thus, r22−2r1 is positive. Next, we compute r21−2r0r2−z21,
r21−2r0r2−z21=[(d1+a1+a2)(a1+a2)+(d1+2a1+2a2)(βαS∗+a1+a2+μ1)]2+β2N∗2e2d21−2βN∗ed1(d1+a1+a2)(a1+a2)−2βN∗ed1(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+2(d1+3a1+3a2+βαS∗+μ1)(a1+a2+μ1)βN∗ed1−2(d1+3a1+3a2+βαS∗+μ1)(d1+a1+a2)(a1+a2)×(βαS∗+a1+a2+μ1)−(βN∗ed1ϵ1e−(a1+a2)τ)2,r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+(d1+2a1+2a2)2(βαS∗+a1+a2+μ1)2+2(d1+a1+a2)(a1+a2)(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)−2βN∗ed1(d1+a1+a2)(a1+a2)−2βN∗ed1(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+2(d1+2a1+2a2+βαS∗+a1+a2+μ1)(a1+a2+μ1)βN∗ed1−2(d1+2a1+2a2+βαS∗+a1+a2+μ1)(d1+a1+a2)(a1+a2)×(βαS∗+a1+a2+μ1),r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+((d1+a1+a2)+(a1+a2))2(βαS∗+a1+a2+μ1)2−2βN∗ed1(d1+a1+a2)(a1+a2)−2βN∗ed1(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+2(d1+2a1+2a2+βαS∗+a1+a2+μ1)(a1+a2+μ1)βN∗ed1−2(d1+a1+a2)(a1+a2)(βαS∗+a1+a2+μ1)2,r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+((d1+a1+a2)2+(a1+a2)2)(βαS∗+a1+a2+μ1)2−2βN∗ed1(d1+a1+a2)(a1+a2)−2βN∗ed1(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+2(d1+2a1+2a2+βαS∗+a1+a2+μ1)(a1+a2+μ1)βN∗ed1,r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+((d1+a1+a2)2+(a1+a2)2)(βαS∗+a1+a2+μ1)2−2βN∗ed1(d1+a1+a2)(a1+a2)−2βN∗ed1(d1+2a1+2a2)(βαS∗+a1+a2+μ1)+2βN∗ed1(d1+a1+a2)(a1+a2)+2βN∗ed1(a1+a2)2+2βN∗ed1μ1(d1+2a1+2a2)+2βN∗ed1(βαS∗+a1+a2+μ1)(a1+a2)+2βN∗ed1μ1(βαS∗+a1+a2+μ1),r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+((d1+a1+a2)2+(a1+a2)2)(βαS∗+a1+a2+μ1)2−2βN∗ed1(d1+a1+a2)(βαS∗+a1+a2+μ1)−2βN∗ed1(a1+a2)(βαS∗+a1+a2+μ1)+2βN∗ed1(a1+a2)2+2βN∗ed1μ1(d1+2a1+2a2)+2βN∗ed1(βαS∗+a1+a2+μ1)(a1+a2)+2βN∗ed1μ1(βαS∗+a1+a2+μ1),r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+((d1+a1+a2)2+(a1+a2)2)(βαS∗+a1+a2+μ1)2−2βN∗ed1(d1+a1+a2)(βαS∗+a1+a2+μ1)+2βN∗ed1(a1+a2)2+2βN∗ed1μ1(d1+2a1+2a2)+2βN∗ed1μ1(βαS∗+a1+a2+μ1),r21−2r0r2−z21=(d1+a1+a2)2(a1+a2)2+β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+(a1+a2)2(βαS∗+a1+a2+μ1)2+(d1+a1+a2)(βαS∗+a1+a2+μ1)×[(d1+a1+a2)(βαS∗+a1+a2+μ1)−2βN∗ed1]+2βN∗ed1(a1+a2)2+2βN∗ed1μ1(d1+2a1+2a2)+2βN∗ed1μ1(βαS∗+a1+a2+μ1). |
Thus, the term r21−2r0r2−z21 is positive if A is positive, where
A=(d1+a1+a2)(βαS∗+a1+a2+μ1)×[(d1+a1+a2)(βαS∗+a1+a2+μ1)−2βN∗ed1]. |
By using βαS∗+a1+a2+μ1=R0(a1+a2+μ1) and N∗=σ/R0(a1+a2+μ1), we get
A=R0(d1+a1+a2)(a1+a2+μ1)×[R0(d1+a1+a2)(a1+a2+μ1)−2βσed1R0(a1+a2+μ1)]=(d1+a1+a2)[R20(d1+a1+a2)(a1+a2+μ1)2−2βσed1]=2βσed1(d1+a1+a2)[R0(1−ϵ1e−(a1+a2)τ)(a1+a2+μ1)2(a1+a2)−1]. |
Therefore, A>0 if R0>2(a1+a2)(1−ϵ1e−(a1+a2)τ)(a1+a2+μ1). Finally,
r20−z20=(d1+a1+a2)2(a1+a2)2(βαS∗+a1+a2+μ1)2+(a1+a2+μ1)2β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)−2βN∗ed1(d1+a1+a2)(a1+a2)(βαS∗+a1+a2+μ1)(a1+a2+μ1),r20−z20=(a1+a2+μ1)2β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+R20(d1+a1+a2)2(a1+a2)2(a1+a2+μ1)2−2βσed1(d1+a1+a2)(a1+a2)(a1+a2+μ1),r20−z20=(a1+a2+μ1)2β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+2βσed1(d1+a1+a2)(a1+a2)(a1+a2+μ1)×[R20(d1+a1+a2)(a1+a2)(a1+a2+μ1)2βσed1−1],r20−z20=(a1+a2+μ1)2β2N∗2e2d21(1−ϵ21e−2(a1+a2)τ)+2βσed1(d1+a1+a2)(a1+a2)(a1+a2+μ1)[R0(1−ϵ1e−(a1+a2)τ)2−1]. |
Thus, r20−z20 is positive if R0>2(1−ϵ1e−(a1+a2)τ).
Since
2(1−ϵ1e−(a1+a2)τ)>2(a1+a2)(1−ϵ1e−(a1+a2)τ)(a1+a2+μ1), |
then, all coefficient are positive if R0>2(1−ϵ1e−(a1+a2)τ)=R∗0. Consequently, The roots of Eq (4.10) are negative if R0>R∗0. But w∈R, then the eigenvalues λ≠iw. Therefore, the eigenvalues do not change their signs to a positive sign when τ increases and remain negative as they were when τ=0. Hence, E∗ is locally asymptotically stable if R0>R∗0.
Next, we prove the global stability of the free equilibrium point when τ=0 by using Castillo-Chavez and Song approach in [40]. First, we introduce the following lemma.
Lemma 4.3. Consider a disease model system written in the form:
dXdt=F(X,Y),dYdt=G(X,Y),G(X,0)=0, | (4.11) |
where X∈Rm denotes the non-disease compartments and Y∈Rn denotes the disease compartments. U0=(X0,0) denotes the disease free equilibrium of system (4.11). Assuming the conditions (C1) and (C2) below:
(C1) For dXdt=F(X,0), X0 is globally asymptotically stable,
(C2) G(X,Y)=AY−ˆG(X,Y), with ˆG(X,Y)≥0 for (X,Y)∈Ω,
where A=∂G∂Y(X0,0) has all non-negative off-diagonal elements and Ω is the region where the model makes biological sense.
If system (4.11) satisfies the above two conditions then the following theorem holds.
Theorem 4.4. The free equilibrium point E0=(N0,0,0,0,0) of model (2.3) is globally asymptotic stable with respect to Ω∗ if R0<1, τ=0 and that assumptions (Cl) and (C2) of Lemma 4.3 are satisfied.
Proof. Apply Lemma 4.3 to system (2.3), Consider X=(N,M,T)T and Y=(I,αS)T. When I=αS=0, the non-infected subsystem is X′(t)=F(X,Y), which can be rewritten as follows
N′(t)=σ−(a1+a2+μ1)N,M′(t)=−μ2M,T′(t)=−μ3T, |
where F(X,Y) is the right-hand side of the subsystem. Solving the equations, we obtain
N(t)=(N(0)−σa1+a2+μ1)e−(a1+a2+μ1)t+σa1+a2+μ1,M(t)=M(0)e−μ2t,T(t)=T(0)e−μ3t, |
where N(0), M(0) and T(0) are the initial values. Then limt→∞N(t)=σa1+a2+μ1=N0, limt→∞M(t)=0=M0, and limt→∞T(t)=0=T0. Thus, regardless of the initial values, the non-infected subsystem tends to the free equilibrium point, X0=(N0,M0,T0). Hence, the condition (C1) from Lemma 4.3 is satisfied.
Next, we consider the infected subsystem of system (2.3) when τ=0, that is,
I′(t)=βNαS−(d1+a1+a2)I,αS′(t)=ed1I−a1αS−a2αS−ϵ1ed1I. | (4.12) |
Rewrite the subsystem in (4.12) in matrix form as:
dYdt=[βNαS−(d1+a1+a2)Ied1I−a1αS−a2αS−ϵ1ed1I]=G(X,Y). |
To satisfy the condition (C2), we must express G(X,Y)=AY−ˆG(X,Y) such that A=∂G∂Y(X0,0). Now,
G(X,Y)=[βNαS−(d1+a1+a2)Ied1I−a1αS−a2αS−ϵ1ed1I]=[βNαS−(d1+a1+a2)I−βαSN0+βαSN0ed1I−a1αS−a2αS−ϵ1ed1I]=[−(d1+a1+a2)βN0ed1(1−ϵ1)−(a1+a2)][IαS]−[βαS(N0−N)0]=AY−˜G(X,Y). |
Clearly, A=∂G∂Y(X0,0) and has non-negative off-diagonal elements. Also, ˜G(X,Y)≥0 for (X,Y)∈Ω∗ since N≤N0 in Ω∗. Thus, the condition (C2) in Lemma 4.3 is satisfied. Hence, E0 is globally asymptotically stable if R0<1 and τ=0.
The numerical simulations in this section are performed using MATLAB function dde23. First, we illustrate the agreement between the numerical and the qualitative results of model (2.3). Then, sensitivity analysis of the basic reproduction number, R0, is investigated for the model's parameters. Finally, we examine the role of immunotherapies in controlling the progression of PD.
The qualitative analysis showed that if R0<1, the free equilibrium point is stable. If R0>1, the endemic equilibrium point exists and is stable. We conduct experiments by solving model (2.3) numerically. The model's parameters are chosen to satisfy the existence and stability conditions. Some parameters are referenced to [30], which has similar biological processes and the rest are estimated. Tables 2 and 3 display the parameters values satisfying R0<1 and R0>1, respectively.
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 10−4 | g/ml/day | Estimated |
β | 0.5 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 3.4×10−4 | day−1 | [30] |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.5 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 5×10−3 | g/ml/day | Estimated |
β | 0.8 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 0.1 | day−1 | Estimated |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.9 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Figure 2 illustrates the time variation of the models' compartments in case R0<1 for three different initial histories. We see in the figure that the solution curves tend to the free equilibrium point E0=(0.0025,0,0,0,0). Similarly, in Figure 3, the solution curves in case R0>1 tend to the endemic equilibrium point E∗=(0.0811,0.0124,0.0269,0.1019,0.0757). Hence, the numerical simulations agreed with the qualitative analysis.
The basic reproduction number depends on the models' parameters. Each parameter either increases or decreases the value of R0. We demonstrate the sensitivity of R0 to the parameters in model (2.3) analytically and numerically. Analytically, we evaluate the partial derivative of R0 with respect to one parameter at a time. If the result of the differentiation is positive (negative), then R0 increases (decreases) as the parameter increases. The differentiation of R0 is the following:
∂R0∂d1=eβσ(1−ϵ1e−(a1+a2)τ)(a1+a2+d1)2(a1+a2+μ1)>0,∂R0∂σ=ed1β(1−ϵ1e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)>0,∂R0∂e=d1βσ(1−ϵ1e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)>0,∂R0∂β=ed1σ(1−ϵ1e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)>0,∂R0∂μ1=−ed1βσ(1−ϵ1e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)2<0,∂R0∂ϵ1=−ed1βσ(e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)<0,∂R0∂τ=ed1βσϵ1(a1+a2)e−(a1+a2)τ)(a1+a2)(a1+a2+d1)(a1+a2+μ1)>0,∂R0∂a1=1(a1+a2)2(a1+a2+d1)2(a1+a2+μ1)2×{ed1βσϵ1e−(a1+a2)ττ(a1+a2)(a1+a2+d1)(a1+a2+μ1)−ed1βσ(1−ϵ1e−(a1+a2)τ)((a1+a2+μ1)(2a1+2a2+d1)+(a1+a2+d1)(a1+a2))},∂R0∂a2=1(a1+a2)2(a1+a2+d1)2(a1+a2+μ1)2×{ed1βσϵ1e−(a1+a2)ττ(a1+a2)(a1+a2+d1)(a1+a2+μ1)−ed1βσ(1−ϵ1e−(a1+a2)τ)((a1+a2+μ1)(2a1+2a2+d1)+(a1+a2+d1)(a1+a2))}. | (5.1) |
From (5.1), we see that the basic reproduction number decreases when the parameters: μ1 and ϵ1 increase. However, it increases when the parameters: σ, e, β, τ and d1 increase. As for the parameters a1 and a2, we can not determine the sign of the derivative; however, numerically R0 decreases with increasing a1 and a2. No change occurs when varying the parameters: ϵ2, ϵ3, μ2 and μ3 since R0 does not depend on them. These results are displayed in Figure 4. In the figure, we numerically graph the dependence of R0 to one parameter at a time. We allow one parameter to vary while fixing the others at a specific value given in Table 3.
Next, we compute the normalized sensitivity index (elasticity) of R0 with respect to the models' parameters by using the formula in [38]:
SI[p]=pR0∂R0∂p, | (5.2) |
where p denotes any parameter. We use the values in Table 3 for the parameters.
Table 4 illustrates the elasticity of R0, meaning that a 1% increase in the parameter's value leads to an increase or decrease in the percentage of R0. For example, an increase of 1% in σ, e, β, d1 and τ leads to an increase in R0 by 1%, 1%, 1%, 0.2857% and 0.0846%, respectively. Whereas, an increase of 1% in μ1, a1, a2, and ϵ1 yield a decrease in R0 by 0.0047, 1.0982, 1.0982, and 0.0423, respectively. Also, the table shows that the highest decline in R0 is due to the increase of a1 and a2. This is expected since these parameters represent the activation of the immune cells to combat the extracellular α-syn. The alterations of R0 corresponding to the parameters in Figure 4 are consistent with the sensitivity index in Table 4.
Parameter (p) | Sensitivity Index (R0) |
τ | 0.0846 |
σ | 1 |
β | 1 |
μ1 | −0.0047 |
μ2 | 0 |
μ3 | 0 |
d1 | 0.2857 |
a1 | −1.0982 |
a2 | −1.0982 |
e | 1 |
ϵ1 | −0.0423 |
ϵ2 | 0 |
ϵ3 | 0 |
We incorporated in model (2.3) two immunotherapy approaches for PD, the active and passive immunization. In the active approach, PD patients are vaccinated with a short antigenic peptide imitating α-syn to help produce antibodies against extracellular α-syn, where the formation of the antibodies needs time. However, in the passive approach, PD patients are vaccinated with antibodies directly. The parameters in the model representing the effect of immunotherapy are ϵ1, the clearance percentage of extracellular α-syn; ϵ2, the inhibited percentage of activated microglia; and ϵ3, the inhibited percentage of activated T cells. We assume that these parameters have larger values in passive immunization than in active immunization. This is since the construction of antibodies in active immunization needs time which is not the case in the passive approach. Therefore, we let ϵ1=0.6, ϵ2=0.5, and ϵ3=0.5 in the passive approach. But in the active approach, the parameters take the values: ϵ1=0.2, ϵ2=0.15, and ϵ3=0.15.
First, we examine the effect of active immunization with different administration times. In the model, τ symbolizes the time delay for the immunization. We assume the time delays are: 10, 40, and 60 days. The rest of the parameters in the model are chosen when R0>1, the endemic case (see Table 3). Figure 5 illustrates the impact of the active approach with different time delays compared with the no-treatment case (ϵ1=ϵ2=ϵ3=0). Although we see a decline in the size of the compartment N during the beginning period of active immunization, the equilibrium level of N is higher than in the no-treatment case. Moreover, we find that the shorter the time delay for the delivery of active immunization, the highest value of the equilibrium level of N. Conversely, the size of the other compartments: I, αS, M, and T elevates at the beginning of active immunization; however, it reaches a lower equilibrium level than in the no-treatment case. Also, the shorter the time delay for administrating active immunization, the lowest value of the equilibrium level of the compartments.
Second, we study the effect of passive immunization with different time delays for vaccine delivery. As previously, we compare the results with the no-treatment case. In Figure 6, we find that the size of compartment N declines but with a higher equilibrium level than in the no-treatment case. However, if the delay of the vaccine is short (τ=10), no drop is shown in N, and neurons are preserved at an equilibrium level. As for the remaining compartments, a rise in their sizes is shown but with a lower equilibrium level than in the no-treatment case. Also, if the vaccine is delivered in a short time delay, α-syn declines, and as a result, infected neurons decrease, and the activation of microglia and T cells is inhibited.
Finally, in Figure 7, we compare the two therapeutic approaches with the no-treatment case for two-time delays: τ=10 and τ=60. We see that the two immunotherapy approaches impact preserving healthy neurons with different equilibrium levels, which are better than the no-treatment case. However, the best approach is the passive immunization given at an early stage with a short delay. Meanwhile, active immunization with a short delay is far better than passive immunization administered after a long delay. A similar result is shown in the figure for the remaining compartments, where a decrease in their equilibrium levels is the outcome of immunotherapy.
Hence, the analysis shows that passive immunization might be far better than active immunization when both are dispensed with a short delay. However, if passive immunization is delayed for a long time, then active immunization is a good therapy if dispensed with a short delay. This indicates that administering time for immunization is significant in postponing the degeneration of healthy neurons.
We conclude that active and passive immunotherapy affects the progression of PD. If treatment is administered in the early stages of the disease with short time delays, α-syn are combated, leading to the inhibition of activated microglia and T cells. Consequently, healthy neurons are maintained. On the contrary, the longer the time offered treatment, the more deteriorated conditions for PD patients.
We built a model to include the innate and adaptive immune responses. The model aimed to investigate the effect of immunotherapy on the progression of Parkinson's disease. Two strategies of immunotherapy were analyzed, the active and passive immunization. The timing of administrating the immunization is crucial. Therefore, the model was formulated using delay differential equations. The qualitative analysis of the model produced two equilibrium points: The free and the endemic equilibrium points. The local stability of the equilibrium points depended on the basic reproduction number, R0. If R0 was less than unity, the free equilibrium point was stable. Conversely, if R0 was greater than unity, the endemic equilibrium point existed and was stable. Numerical experiments were performed with different initial histories to show the agreement with the qualitative results. Moreover, a sensitivity analysis was conducted on R0 to scrutinize the parameters involved in decreasing and increasing the value of R0. We explored the two therapeutic approaches numerically with different time delays. We concluded that active and passive immunotherapy affects the progression of PD. If treatment was administered in the early stages of the disease with short time delays, α-syn were combated, leading to the inhibition of activated microglia and T cells. Consequently, healthy neurons were maintained. On the contrary, the longer the time offered treatment, the more deteriorated conditions for PD patients.
For future work, this model can be modified to include in the dynamics two compartments: The resting microglia and the T helper cells. This may describe the dynamics of Parkinson's disease with immunotherapy comprehensively, leading to detailed analysis to reach more meaningful results.
The authors declare that there is no conflicts of interest.
[1] |
M. J. Benskey, R. G. Perez, F. P. Manfredsson, The contribution of alpha synuclein to neuronal survival and function–Implications for Parkinson's disease, J. Neurochem., 137 (2016), 331–359, https://doi.org/10.1111/jnc.13570 doi: 10.1111/jnc.13570
![]() |
[2] |
S. Mehra, S. Sahay, S. K. Maji, α-Synuclein misfolding and aggregation: Implications in Parkinson's disease pathogenesis, Biochim. Biophys. Acta Proteins Proteom., 1867 (2019), 890–908. https://doi.org/10.1016/j.bbapap.2019.03.001 doi: 10.1016/j.bbapap.2019.03.001
![]() |
[3] |
R. M. Meade, D. P. Fairlie, J. M. Mason, Alpha-synuclein structure and Parkinson's disease, Mol. Neurodegener., 14 (2019), 29. https://doi.org/10.1186/s13024-019-0329-1 doi: 10.1186/s13024-019-0329-1
![]() |
[4] |
A. D. Schwab, M. J. Thurston, J. Machhi, K. E. Olson, K. L. Namminga, H. E. Gendelman, et al., Immunotherapy for Parkinson's disease, Neurobiol. Dis., 137 (2020), 104760. https://doi.org/10.1016/j.nbd.2020.104760 doi: 10.1016/j.nbd.2020.104760
![]() |
[5] |
J. Shin, H. J. Kim, B. Jeon, Immunotherapy targeting neurodegenerative proteinopathies: α-synucleinopathies and tauopathies, J. Movement Disorders, 13 (2020), 11–19. https://doi.org/10.14802/jmd.19057 doi: 10.14802/jmd.19057
![]() |
[6] |
H. J. Lee, E. D. Cho, K. W. Lee, J. H. Kim, S. G. Cho, S. J. Lee, Autophagic failure promotes the exocytosis and intercellular transfer of α-synuclein, Exp. Mol. Med., 45 (2013), e22. https://doi.org/10.1038/emm.2013.45 doi: 10.1038/emm.2013.45
![]() |
[7] |
C. R. Overk, E. Masliah, Pathogenesis of synaptic degeneration in Alzheimer's disease and Lewy body disease, Biochem. Pharmacol., 88 (2014), 508–516. https://doi.org/10.1016/j.bcp.2014.01.015 doi: 10.1016/j.bcp.2014.01.015
![]() |
[8] |
A. Recasens, B. Dehay, J. Bové, I. Carballo-Carbajal, S. Dovero, A. Pérez-Villalba, et al., Lewy body extracts from parkinson disease brains trigger α-synuclein pathology and neurodegeneration in mice and monkeys, Ann. Neurol., 75 (2014), 351–362. https://doi.org/10.1002/ana.24066 doi: 10.1002/ana.24066
![]() |
[9] |
Y. Chu, J. H. Kordower, The prion hypothesis of Parkinson's disease, Curr. Neurol. Neurosci. Rep., 15 (2015), 28. https://doi.org/10.1007/s11910-015-0549-x doi: 10.1007/s11910-015-0549-x
![]() |
[10] |
R. L. Mosley, J. A. Hutter-Saunders, D. K. Stone, H. E. Gendelman, Inflammation and adaptive immunity in parkinson's disease, Cold Spring Harbor Perspectives in Medicine, 2012, 1–18. https://doi.org/10.1101/cshperspect.a009381 doi: 10.1101/cshperspect.a009381
![]() |
[11] |
J. Y. Li, E. Englund, J. L. Holton, D. Soulet, P. Hagell, A. J. Lees, et al., Lewy bodies in grafted neurons in subjects with parkinson's disease suggest host-to-graft disease propagation, Nat. Med., 14 (2008), 501–503. https://doi.org/10.1038/nm1746 doi: 10.1038/nm1746
![]() |
[12] |
J. H. Kordower, Y. Chu, R. A. Hauser, T. B. Freeman, C. W. Olanow, Lewy body–like pathology in long-term embryonic nigral transplants in parkinson's disease, Nat. Med., 14 (2008), 504–506. https://doi.org/10.1038/nm1747 doi: 10.1038/nm1747
![]() |
[13] |
A. C. Hoffmann, G. Minakaki, S. Menges, R. Salvi, S. Savitskiy, A. Kazman, et al., Extracellular aggregated alpha synuclein primarily triggers lysosomal dysfunction in neural cells prevented by trehalose, Sci. Rep., 9 (2019), 1–18. https://doi.org/10.1038/s41598-018-35811-8 doi: 10.1038/s41598-018-35811-8
![]() |
[14] |
P. Desplats, H. J. Lee, E. J. Bae, C. Patrick, E. Rockenstein, L. Crews, et al., Inclusion formation and neuronal cell death through neuron-to-neuron transmission of α-synuclein, Proc. Natl. Acad. Sci. U. S. A., 106 (2009), 13010–13015. https://doi.org/10.1073/pnas.0903691106 doi: 10.1073/pnas.0903691106
![]() |
[15] |
S. Kwon, M. Iba, C. Kim, E. Masliah, Immunotherapies for aging-related neurodegenerative diseases-emerging perspectives and new targets, Neurotherapeutics, 17 (2020), 935–954. https://doi.org/10.1007/s13311-020-00853-2 doi: 10.1007/s13311-020-00853-2
![]() |
[16] |
C. Arcuri, C. Mecca, R. Bianchi, I. Giambanco, R. Donato, The pathophysiological role of microglia in dynamic surveillance, phagocytosis and structural remodeling of the developing cns, Front. Mol. Neurosci., 10 (2017), 191. https://doi.org/10.3389/fnmol.2017.00191 doi: 10.3389/fnmol.2017.00191
![]() |
[17] |
T. Town, V. Nikolic, J. Tan, The microglial "activation" continuum: From innate to adaptive responses, J. Neuroinflammation, 2 (2005), 24. https://doi.org/10.1186/1742-2094-2-24 doi: 10.1186/1742-2094-2-24
![]() |
[18] |
V. Vedam-Mai, Harnessing the immune system for the treatment of parkinson's disease, Brain Res., 1758 (2021), 147308. https://doi.org/10.1016/j.brainres.2021.147308 doi: 10.1016/j.brainres.2021.147308
![]() |
[19] | A. M. Schonhoff, G. P. Williams, Z. D. Wallen, D. G. Standaert, A. S. Harms, Chapter 6–innate and adaptive immune responses in parkinson's disease, Prog. Brain Res., 252 (2020), 169–216. |
[20] |
A. M. Jurga, M. Paleczna, K. Z. Kuter, Overview of general and discriminating markers of differential microglia phenotypes, Front. Cell. Neurosci., 14 (2020), 198. https://doi.org/10.3389/fncel.2020.00198 doi: 10.3389/fncel.2020.00198
![]() |
[21] |
E. J. Bae, H. J. Lee, E. Rockenstein, D. H. Ho, E. B. Park, N. Y. Yang, et al., Antibody-aided clearance of extracellular α-synuclein prevents cell-to-cell aggregate transmission, J. Neurosci., 32 (2012), 13454–13469. https://doi.org/10.1523/JNEUROSCI.1292-12.2012 doi: 10.1523/JNEUROSCI.1292-12.2012
![]() |
[22] |
J. Y. Vargas, C. Grudina, C. Zurzolo, The prion-like spreading of α-synuclein: From in vitro to in vivo models of Parkinson's disease, Ageing Res. Rev., 50 (2019), 89–101. https://doi.org/10.1016/j.arr.2019.01.012 doi: 10.1016/j.arr.2019.01.012
![]() |
[23] |
D. Chatterjee, J. H. Kordower, Immunotherapy in Parkinson's disease: Current status and future directions, Neurobiol. Dis., 132 (2019), 104587. https://doi.org/10.1016/j.nbd.2019.104587 doi: 10.1016/j.nbd.2019.104587
![]() |
[24] | J. Cruse, R. Lewis, H. Wang, Immunology guidebook, Academic Press, 2004. https://doi.org/10.1016/B978-0-12-198382-6.X5022-5 |
[25] |
F. A. Bonilla, H. C. Oettgen, Adaptive immunity, J. Allergy Clinical Immunology, 125 (2010), S33–S40. https://doi.org/10.1016/j.jaci.2009.09.017 doi: 10.1016/j.jaci.2009.09.017
![]() |
[26] |
F. Garretti, D. Agalliu, C. S. Lindestam Arlehamn, A. Sette, D. Sulzer, Autoimmunity in parkinson's disease: The role of α-synuclein-specific T cells, Front. Immunol., 10 (2019), 303. https://doi.org/10.3389/fimmu.2019.00303 doi: 10.3389/fimmu.2019.00303
![]() |
[27] |
A. Lloret-Villas, T. M. Varusai, N. Juty, C. Laibe, N. Le Novere, H. Hermjakob, et al., The impact of mathematical modeling in understanding the mechanisms underlying neurodegeneration: Evolving dimensions and future directions, CPT: Pharmacometrics Syst. Pharmacol., 6 (2017), 73–86. https://doi.org/10.1002/psp4.12155 doi: 10.1002/psp4.12155
![]() |
[28] |
Y. Sarbaz, H. Pourakbari, A review of presented mathematical models in Parkinson's disease: Black- and gray-box models, Med. Biol. Eng. Comput., 54 (2016), 855–868. https://doi.org/10.1007/s11517-015-1401-9 doi: 10.1007/s11517-015-1401-9
![]() |
[29] |
I. K. Puri, L. Li, Mathematical modeling for the pathogenesis of alzheimer's disease, PloS One, 5 (2010), e15176. https://doi.org/10.1371/journal.pone.0015176 doi: 10.1371/journal.pone.0015176
![]() |
[30] |
W. Hao, A. Friedman, Mathematical model on Alzheimer's disease, BMC Syst. Biol., 10 (2016), 108. https://doi.org/10.1186/s12918-016-0348-2 doi: 10.1186/s12918-016-0348-2
![]() |
[31] |
I. A. Kuznetsov, A. V. Kuznetsov, What can trigger the onset of Parkinson's disease–A modeling study based on a compartmental model of α-synuclein transport and aggregation in neurons, Math. Biosci., 278 (2016), 22–29. https://doi.org/10.1016/j.mbs.2016.05.002 doi: 10.1016/j.mbs.2016.05.002
![]() |
[32] |
I. A. Kuznetsov, A. V. Kuznetsov, Mathematical models of α-synuclein transport in axons, Comput. Methods Biomech. Biomed. Eng., 19 (2016), 515–526. https://doi.org/10.1080/10255842.2015.1043628 doi: 10.1080/10255842.2015.1043628
![]() |
[33] |
K. Sneppen, L. Lizana, M. H. Jensen, S. Pigolotti, D. Otzen, Modeling proteasome dynamics in Parkinson's disease, Phys. Biol., 6 (2009), 036005. https://doi.org/10.1088/1478-3975/6/3/036005 doi: 10.1088/1478-3975/6/3/036005
![]() |
[34] |
A. Badrah, S. Al-Tuwairqi, Modeling the dynamics of innate immune response to parkinson disease with therapeutic approach, Phys. Biol., 19 (2022), 056004. https://doi.org/10.1088/1478-3975/ac8516 doi: 10.1088/1478-3975/ac8516
![]() |
[35] |
J. Yang, X. Wang, F. Zhang, A differential equation model of HIV infection of CD+4 T cells with delay, Discrete Dyn. Nat. Soc., 2008 (2008), 903678. https://doi.org/10.1155/2008/903678 doi: 10.1155/2008/903678
![]() |
[36] |
S. Çakan, Dynamic analysis of a mathematical model with health care capacity for COVID-19 pandemic, Chaos Solitons Fract., 139 (2020), 110033. https://doi.org/10.1016/j.chaos.2020.110033 doi: 10.1016/j.chaos.2020.110033
![]() |
[37] | M. B. Finan, A first course in quasi-linear partial differential equations for physical sciences and engineering, 2019. |
[38] | M. Martcheva, An introduction to mathematical epidemiology, New York: Springer, 2015. https://doi.org/10.1007/978-1-4899-7612-3 |
[39] | O. Nonthakorn, Biological models with time delay, PhD thesis, Worcester Polytechnic Institute, 2016. |
[40] | C. Castillo-Chavez, Z. Feng, W. Huang, On the computation of R0 and its role in global stability, Math. Approaches Emerg Re-emerg. Infect. Dis., 125 (2002), 229–250. |
[41] | Z. S. Kifle, L. L. Obsu, Mathematical modeling for COVID-19 transmission dynamics: A case study in ethiopia, Results Phys., 105191. https://doi.org/10.1016/j.rinp.2022.105191 |
1. | Chunhua Feng, Oscillatory Behavior of the Solutions for a Parkinson’s Disease Model with Discrete and Distributed Delays, 2024, 13, 2075-1680, 75, 10.3390/axioms13020075 | |
2. | Roshana Mukhtar, Chuan-Yu Chang, Muhammad Asif Zahoor Raja, Naveed Ishtiaq Chaudhary, Muhammad Junaid Ali Asif Raja, Chi-Min Shu, Design of fractional innate immune response to nonlinear Parkinson's disease model with therapeutic intervention: Intelligent machine predictive exogenous networks, 2025, 191, 09600779, 115947, 10.1016/j.chaos.2024.115947 | |
3. | Roshana Mukhtar, Chuan-Yu Chang, Muhammad Asif Zahoor Raja, Naveed Ishtiaq Chaudhary, Nabeela Anwar, Iftikhar Ahmad, Chi-Min Shu, Intelligent exogenous networks with Bayesian distributed backpropagation for nonlinear single delay brain electrical activity rhythms in Parkinson's disease system, 2025, 145, 09521976, 110281, 10.1016/j.engappai.2025.110281 | |
4. | Roshana Mukhtar, Chuan-Yu Chang, Aqib Mukhtar, Muhammad Junaid Ali Asif Raja, Naveed Ishtiaq Chaudhary, Zeshan Aslam Khan, Muhammad Asif Zahoor Raja, A novel fractional Parkinson's disease onset model involving α-syn neuronal transportation and aggregation: A treatise on machine predictive networks, 2025, 194, 09600779, 116269, 10.1016/j.chaos.2025.116269 |
Symbol | Definition | Units |
t | Time | day |
τ | Delay time | day |
N | Density of healthy neurons in the brain | g/ml |
I | Density of infected neurons in the brain | g/ml |
αS | Density of extracellular α-syn in the brain | g/ml |
M | Density of activated microglia | g/ml |
T | Density of activated T cell | g/ml |
σ | Density of new neurons per day due to neurogenesis | g/ml/day |
β | Neuron infection rate | ml/g/day |
μ1 | Apoptosis rate of neurons | day−1 |
μ2 | Annihilation rate of activated microglia | day−1 |
μ3 | Annihilation rate of activated T cell | day−1 |
d1 | Death rate of infected neurons due to α-syn aggregations | day−1 |
a1 | Activation rate of microglia due to extracellular α-syn and infected neurons | day−1 |
a2 | Activation rate of T cell due to extracellular α-syn and infected neurons | day−1 |
e | Percentage of α-syn survival from death of infected neurons | . |
ϵ1 | Percentage of extracellular α-syn clearance due to immunotherapy | . |
ϵ2 | Percentage of inhibited activated microglia due to immunotherapy | . |
ϵ3 | Percentage of inhibited activated T cells due to immunotherapy | . |
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 10−4 | g/ml/day | Estimated |
β | 0.5 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 3.4×10−4 | day−1 | [30] |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.5 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 5×10−3 | g/ml/day | Estimated |
β | 0.8 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 0.1 | day−1 | Estimated |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.9 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Parameter (p) | Sensitivity Index (R0) |
τ | 0.0846 |
σ | 1 |
β | 1 |
μ1 | −0.0047 |
μ2 | 0 |
μ3 | 0 |
d1 | 0.2857 |
a1 | −1.0982 |
a2 | −1.0982 |
e | 1 |
ϵ1 | −0.0423 |
ϵ2 | 0 |
ϵ3 | 0 |
Symbol | Definition | Units |
t | Time | day |
τ | Delay time | day |
N | Density of healthy neurons in the brain | g/ml |
I | Density of infected neurons in the brain | g/ml |
αS | Density of extracellular α-syn in the brain | g/ml |
M | Density of activated microglia | g/ml |
T | Density of activated T cell | g/ml |
σ | Density of new neurons per day due to neurogenesis | g/ml/day |
β | Neuron infection rate | ml/g/day |
μ1 | Apoptosis rate of neurons | day−1 |
μ2 | Annihilation rate of activated microglia | day−1 |
μ3 | Annihilation rate of activated T cell | day−1 |
d1 | Death rate of infected neurons due to α-syn aggregations | day−1 |
a1 | Activation rate of microglia due to extracellular α-syn and infected neurons | day−1 |
a2 | Activation rate of T cell due to extracellular α-syn and infected neurons | day−1 |
e | Percentage of α-syn survival from death of infected neurons | . |
ϵ1 | Percentage of extracellular α-syn clearance due to immunotherapy | . |
ϵ2 | Percentage of inhibited activated microglia due to immunotherapy | . |
ϵ3 | Percentage of inhibited activated T cells due to immunotherapy | . |
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 10−4 | g/ml/day | Estimated |
β | 0.5 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 3.4×10−4 | day−1 | [30] |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.5 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Symbol | Value | Units | Reference |
τ | 50 | day | Estimated |
σ | 5×10−3 | g/ml/day | Estimated |
β | 0.8 | ml/g/day | Estimated |
μ1 | 1.9×10−4 | day−1 | [30] |
μ2 | 6×10−3 | day−1 | [30] |
μ3 | 0.015 | day−1 | [30] |
d1 | 0.1 | day−1 | Estimated |
a1 | 2×10−2 | day−1 | [30] |
a2 | 2×10−2 | day−1 | [30] |
e | 0.9 | . | Estimated |
ϵ1 | 0.3 | . | Estimated |
ϵ2 | 0.3 | . | Estimated |
ϵ3 | 0.3 | . | Estimated |
Parameter (p) | Sensitivity Index (R0) |
τ | 0.0846 |
σ | 1 |
β | 1 |
μ1 | −0.0047 |
μ2 | 0 |
μ3 | 0 |
d1 | 0.2857 |
a1 | −1.0982 |
a2 | −1.0982 |
e | 1 |
ϵ1 | −0.0423 |
ϵ2 | 0 |
ϵ3 | 0 |