A multiple-relaxation-time lattice Boltzmann method with Beam-Warming scheme for a coupled chemotaxis-fluid model

Zhonghua Qiao; Xuguang Yang; Zhonghua Qiao; Xuguang Yang

doi:10.3934/era.2020066

Electronic Research Archive

2020, Volume 28, Issue 3: 1207-1225. doi: 10.3934/era.2020066

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A multiple-relaxation-time lattice Boltzmann method with Beam-Warming scheme for a coupled chemotaxis-fluid model

Zhonghua Qiao ^{1
,},
Xuguang Yang ^{2
,
,}

1.
Department of Applied Mathematics, The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong, China
2.
School of Mathematics and Computational Science, Hunan First Normal University, Changsha, China

Received: 01 April 2020 Revised: 01 June 2020
Primary: 65Z05, 65N06; Secondary: 76D99

In this work, a multiple-relaxation-time (MRT) lattice Boltzmann method (LBM) is proposed to solve a coupled chemotaxis-fluid model. In the evolution equation of the proposed LBM, Beam-Warming (B-W) scheme is used to enhance the numerical stability. In numerical experiments, at first, the comparison between the classical LBM and the present LBM with B-W scheme is carried out by simulating blow up phenomenon of the Keller-Segel (K-S) model. Numerical results show that the stability of the present LBM with B-W scheme is better than the classical one. Then, the second order convergence rate of the proposed B-W scheme is verified in the numerical study of the coupled Navier-Stokes (N-S) K-S model. Finally, through solving the coupled chemotaxis-fluid model, the formation of falling bacterial plumes is numerically investigated. Numerical results agree well with existing ones in the literature.

Keywords:

Citation: Zhonghua Qiao, Xuguang Yang. A multiple-relaxation-time lattice Boltzmann method with Beam-Warming scheme for a coupled chemotaxis-fluid model[J]. Electronic Research Archive, 2020, 28(3): 1207-1225. doi: 10.3934/era.2020066

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Abstract

1. Introduction

Coronavirus disease 2019 (COVID-19) is a contagious disease caused by severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2). The virus was first identified in Wuhan, China, in December 2019, and it quickly spread to other parts of mainland China and many other countries [1]–[6]. Due to the rapid spread of the virus with consequences worldwide, the World Health Organization (WHO) declared a public health emergency of international concern on January 30, 2020, and a pandemic on March 11, 2020 [7],[8]. The transmission of COVID-19 has become a global health threat. As of April 17, 2020, there was a total of 2,230,439 COVID-19 cases reported worldwide, with 150,810 deaths and 564,210 recovered cases [9]. According to the WHO's COVID-19 global report, over 21.2 million people had been infected with the virus as of August 16, 2020, with over 761,779 deaths [10]. Moreover, till October 14, 2021, more than 239,426,728 cases of infection and at least 4,878,373 deaths have been confirmed in Africa, Asia, Europe, North America, Oceania, South America and Antarctica. This has become one of the deadliest pandemics in history according to the Center for Systems Science and Engineering (CSSE) at Johns Hopkins University (JHU) [11].

Studying and analyzing complex infectious disease models are difficult tasks and require some computational tools and mathematical approaches. In systems biology, mathematical presentations and computational simulations are effective tools and will help further understanding and future predictions about model dynamics. The models of COVID-19 are complicated, and they are required some mathematical tools to improve interventions and healthcare strategies. Recently, several studies about COVID-19 were suggested based on mathematical tools and computational simulations to understand this pandemic and its control approaches. In [12]–[14], the SEIR model was modified by several researchers to understand the impacts of social distancing, rapid testing, vaccination and contaminated objects in controlling the spread of COVID-19. One of the most important key elements in the spreading of COVID-19 is the basic reproduction number (also called basic reproductive ratio). This quantity, denoted by R₀, represents the number of secondary infections induced by a single primary infection in a population where everyone is susceptible [15]. According to developed techniques of mathematical epidemiology models, R₀ plays an important role for understanding epidemiological ideas and identifying key critical parameters for such models, and R₀ may have different values for reported cases of coronavirus. According to a published study, the basic reproduction number was computed using incidence data in the city of Jakarta from March 3, 2020, to May 10, 2020. The median value of R₀ was about 1.75 during the first interval. After the rigorous social distancing implemented, this value was about 1.22. In addition, the basic reproduction number has been calculated for different infectious disease models. Consequently, this quantity was calculated for a mathematical model of the CD8+ T-cell response to human T cell leukemia/lymphoma virus type I (HTLV-I) infection, given in [16].

According to published studies given in [14],[17],[18], the concept of sensitivity analysis has been presented to detect model sensitive parameters, including local sensitivities for each model state with respect to model parameters. Such sensitivities are computed by using three different methods: non-normalization, half-normalization and full-normalization. Accordingly, there was another method of sensitivity analysis given in [19]. They suggested the partial rank correlation coefficient (PRCC) technique to determine how the glioma-immune model output is affected by changes in specific parameter values.

Optimal control analysis is another effective method to identify the model critical parameters and to suggest control strategies. This technique has been used with the COVID-19 pandemic for deriving control policies. Recently, this technique has been used to find some control strategies for the COVID-19 pandemic in Indonesia, given in [20]. Then, there was a study about mathematical modeling with optimal control analysis for the spread of the COVID-19 pandemic with a case study of Brazil and cost-effectiveness; this was given in [21]. More recently, there was another approach that suggested a mathematical model with optimal control to highlight the negative impact of quarantine on diabetic people, with cost-effectiveness, presented in [22]. The reader can also find more relevant works about different approaches and mathematical models of the COVID-19 pandemic and its control strategies in [23]–[29].

Although there are many mathematical models that have been suggested for prediction of the COVID-19 pandemic, such models can be further improved and analyzed in terms of real data. Calculating the basic reproduction number with local sensitivities can improve the model outcomes further. An issue that has not been considered enough is elasticity of basic reproduction number with respect to model parameters. This helps us to identify the most critical model parameters in spreading this disease. Another issue of modeling such phenomena is validating the model results. Therefore, comparing the model predictions with real data can also indicate the accuracy and reliability of such models.

Estimating the model initial parameters for the suggested SEIR model is an important step forward in this study compared to the other existing studies about the confirmed cases of COVID-19 in the Kurdistan Region of Iraq. Therefore, we suggest the Metropolis–Hastings (MH) algorithm to estimate such model parameters, and then we use them in computational simulations. Such estimated parameters can also provide a good agreement between the model results and the daily infected cases. Another novelty here is the data collection of COVID-19 infected cases in the area that provides the future predictions and interventions. Accordingly, we have collected the daily confirmed cases of COVID-19 from January 10, 2021, to March 22, 2021. The collected real data here give us a great understanding about this disease in the area and suggested more interventions and strategies to control this pandemic. Interestingly, identifying the critical model parameters based on sensitivity and elasticity methods becomes another novelty for the suggested SEIR model.

This paper has some contributions. The main contribution is suggesting the simplified SEIR model for COVID-19 disease to predict the spreading of the disease in the Kurdistan Region of Iraq. We use this model to compare the model results and the daily infected cases more easily and correctly. Another contribution here is identifying the model critical parameters. Consequently, we suggest the local sensitivity methods to calculate the model sensitivities between the model variables and parameters. Additionally, the elasticity between the basic reproduction number, R₀, and model parameters are also calculated and helps to identify the key critical parameters in spreading this disease.

The organization of this paper is as follows. In Section 2, we construct the SEIR model based on our assumptions and model transmissions. Using the next generation matrix, we derive the formula of the basic reproduction number, calculate the elasticity between R₀ and model parameters and show the model local sensitivities based on the estimated values, as discussed in Section 3. We perform our computational model simulations of daily infected cases in Section 4. Finally, some conclusions and suggestions are given in Section 5.

2. A mathematical model of the spread of the COVID-19 pandemic

Many infectious disease models have been suggested to understand the transmission rates of COVID-19. The SEIR model has been commonly applied in many infectious diseases. This model consists of four compartments, namely, susceptible S(t), exposed E(t), infected I(t) and recovered R(t) individuals. Several authors modified the SEIR model for studying the transmission of pathogens. Among them, in [30], a modified SEIR model was used to describe the 2009 influenza A (H1N1) pandemic within local regions in Japan. It was also used for the Ebola epidemic occurring in the West African nations of Guinea, Liberia and Sierra Leone [31]. In this paper, we use the SEIR model for COVID-19 disease that describes the spreading of COVID-19 in the Kurdistan Region of Iraq. Accordingly, we develop the previously published work given in [32], and we add a parameter that shows a rate of recovery of the individuals from the exposed class. The model network of SEIR shown in Figure 1 includes various compartments with their transmissions. The model compartments and transmission rates are defined in Table 1.

Figure 1. The SEIR model network of the COVID-19 pandemic that includes model populations with their reaction rates.

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The chemical reactions of the model can be expressed as follows:

µ µ µ µ

$\begin{array}{l} n u l l \overset{Λ}{\to} S, S \overset{µ S}{\to} n u l l, S \overset{\frac{β S I}{N}}{\to} E, \\ E \overset{µ E}{\to} n u l l, E \overset{α E}{\to} R, E \overset{k E}{\to} I, \\ I \overset{γ E}{\to} R, I \overset{µ I}{\to} n u l l, R \overset{µ R}{\to} n u l l . \end{array}$ (1)

Furthermore, all parameters and initial states with their biological meanings are shown in Table 1. We use the concepts of standard chemical kinetics and the mass action law to derive a system of non–linear ordinary differential equations [33],[34]. Then, the system of nonlinear ordinary differential equations takes the following form:

$\begin{array}{l} \frac{d S}{d t} = Λ - \frac{β S I}{N} - µ S, \\ \frac{d E}{d t} = \frac{β S I}{N} - k E - α E - µ E, \\ \frac{d I}{d t} = k E - γ I - µ I, \\ \frac{d R}{d t} = α E + γ I - µ R, \end{array}$ (2)

with non-negative initial conditions S(0) = S₀ > 0, E(0) = E₀ > 0, I(0) = I₀ > 0, R(0) = R₀ ≥ 0. All parameters are defined as contact rates between individual categories.

Table 1. The model reaction constants and initial individuals for the SEIR model with their biological meanings.

Symbol	Biological definition
S(0)	Initial susceptible individuals
E(0)	Initial exposed individuals
I(0)	Initial symptomatic infected individuals
R(0)	Initial recovered individuals
β	Infection rate
Λ	Recruitment rate
k	Transition rate of exposed individuals to the infected class
α	Transition rate of exposed individuals to the recovered class
γ	Natural recovery rate
µ	Natural death rate

| Show Table

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3. Methods

Infectious disease models cannot be well understood only by biological techniques. Model analysis techniques and computational simulations can serve a great role in predicting and analyzing the model dynamics and identifying critical model parameters. Recently, some techniques of model analysis have been applied such as sensitivity and elasticity methods. They are useful tools to determine which variable or parameter is sensitive to a specific condition [12],[17],[18]. Calculating the basic reproduction numbers at the equilibrium points can also provide a great environment to discuss infectious disease models more widely and accurately [13],[14]. Here, in this study, we focus on three important techniques of model analysis: basic reproduction numbers, local sensitivity and elasticity methods. More details about the suggested techniques are discussed in the following sections.

3.1. Next generation method

In epidemiology, the next-generation matrix is used to derive the basic reproduction number for a compartmental model of the spread of infectious disease. This method was proposed by Diekmann et al. (1990) [35] and van den Driessche and Watmough (2002) [36]. One of the most important parameters for epidemiological models is the basic reproduction number [37]. Using Equation 2, we can easily derive R₀ at an equilibrium point E₀. The suggested model here includes two infected states, E and I, and two uninfected states, S and R. Let X be a vector of infected classes and Y be a vector of uninfected classes. They are shown below:

$X = [\begin{matrix} E \\ I \end{matrix}], Y = [\begin{matrix} S \\ R \end{matrix}] .$

To find equilibrium points for the model, let us set the right-hand side of Equation 2 equal to zero. Then, the equilibrium points are obtained. The first equilibrium is the COVID-19-free equilibrium point, which is represented by

$E_{0} = (\frac{Λ}{µ}, 0, 0, 0) .$ (3)

The second type of equilibrium is called the endemic equilibrium point. It is given below:

$E^{*} = (S^{'}, E^{'}, I^{'}, R^{'}),$ (4)

where $S^{'}, E^{'}, I^{'}, R^{'}$ are positive and defined as follows:

$\begin{array}{l} S^{'} = \frac{N}{β k} (k + α + µ) (γ + µ + d), E^{'} = \frac{β k Λ - µ N (k + α + µ) (γ + µ + d)}{β k (k + α + µ)}, \\ I^{'} = \frac{β k Λ - µ N (k + α + µ) (γ + µ + d)}{β (k + α + µ) (γ + µ + d)}, R^{'} = \frac{α E^{'} + γ I^{'}}{µ} . \end{array}$

Using the next generation method, we have the vector functions

$M (S, E, I, R) = [\begin{matrix} \frac{β S I}{N} \\ 0 \end{matrix}], G (S, E, I, R) = [\begin{matrix} (k + α + µ) E \\ - k E + (γ + µ) I \end{matrix}] .$

Then, the Jacobian matrices for M, G at E₀ are given below:

$H = {[\frac{\partial M (S, E, I, R)}{\partial (E, I)}]}_{(\frac{Λ}{µ}, 0, 0, 0)} = [\begin{matrix} 0 & \frac{β Λ}{µ N} \\ 0 & 0 \end{matrix}], W = {[\frac{\partial G (S, E, I, R)}{\partial (E, I)}]}_{(\frac{Λ}{µ}, 0, 0, 0)} = [\begin{matrix} (k + α + µ) & 0 \\ - k & (γ + µ) \end{matrix}] .$

Since W is a non-singular matrix, W⁻¹ can be calculated:

$W^{- 1} = \frac{1}{(k + α + µ) (γ + µ)} [\begin{matrix} (γ + µ) & 0 \\ k & (k + α + µ) \end{matrix}] .$

Therefore, the basic reproduction number is the spectral radius of HW⁻¹. Thus, the basic reproduction number for Equation 2 is

$R_{0} = \frac{β k Λ}{µ N (k + α + µ) (γ + µ)} .$ (5)

3.2. Elasticity of R₀

The concept of elasticity for infectious disease models has an effective role in determining the sensitivity between R₀ and the model parameters. For calculating such coefficients, the following main formula is used:

$Γ_{ω}^{R_{0}} = \frac{\partial R_{0}}{\partial ω} * \frac{ω}{R_{0}},$ (6)

where ω is the set of all parameters. Using Equation 5, we can calculate the elasticity index of R₀ for each model parameter. They are given below:

$\begin{array}{l} Γ_{Λ}^{R_{0}} = \frac{\partial R_{0}}{\partial Λ} * \frac{Λ}{R_{0}} = 1, \\ Γ_{k}^{R_{0}} = \frac{\partial R_{0}}{\partial k} * \frac{k}{R_{0}} = \frac{(α + µ)}{(k + α + µ)}, \\ Γ_{α}^{R_{0}} = \frac{\partial R_{0}}{\partial α} * \frac{α}{R_{0}} = \frac{- α}{(k + α + µ)}, \\ Γ_{γ}^{R_{0}} = \frac{\partial R_{0}}{\partial γ} * \frac{γ}{R_{0}} = \frac{- γ}{(γ + µ)}, \\ Γ_{β}^{R_{0}} = \frac{\partial R_{0}}{\partial β} * \frac{β}{R_{0}} = 1, \\ Γ_{µ}^{R_{0}} = \frac{\partial R_{0}}{\partial µ} * \frac{µ}{R_{0}} = - (1 + \frac{µ}{(k + α + µ)} + \frac{µ}{(γ + µ)}) . \end{array}$

Using the estimated parameters, we can compute the model elasticity; see Table 2.

Table 2. Elasticity values of R₀ regarding model parameters.

Parameter	$Γ_{ω}^{R_{0}}$
Λ	1
k	0.14039612
α	−0.403487536
γ	−0.9996225141
β	1
µ	−1.0004274882

| Show Table

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The results given in Table 2 show the positive and negative signs for the model elasticity. These give us the direct or indirect relations between R₀ and the model parameters. For example, this coefficient is positive for the set of parameters {Λ, k, β}. This means that when these parameters, {Λ, k, β}, are increased, the value of R₀ is also increased, and this virus spreads further. On the other hand, the signs of {γ, α, µ} are negative. This means that the value of the basic reproduction number can be reduced by increasing such parameters. Interestingly, β is the most significant positive parameter that can be utilized to reduce R₀. For example, if the value of β is decreased by 10%, then the basic reproduction number will be reduced to R₀ = 0.52886708. Furthermore, reducing the contact rate between individuals can impact the number of infected people from the disease.

3.3. Sensitivity analysis

The concept of local sensitivity analysis is another step forward for studying infection disease models and identifying the model critical elements. This is simply used for determining the sensitivity of each model species with respect to the model parameters. This method was recently considered in [14],[17],[18],[38]. Assume that there are p compartments (y_i for i = 1,2,...,p) and q parameters (b_j for j = 1,2,...,q) in an infectious disease model. The model balanced equations are represented by the following system of differential equations:

$\frac{d y_{i}}{d t} = f_{i} (y, b),$

where $y \in ℝ^{p}, b \in ℝ^{q}$ . The model sensitivities can be computed with three different techniques: non normalizations, half normalizations and full normalizations.

The full-normalization sensitivities are given as follows:

$S_{b_{j}}^{y_{i}} = \frac{b_{j}}{y_{i}} \frac{d y_{i}}{d b_{j}} .$ (7)

The half-normalization sensitivities are defined as follows:

$S_{b_{j}}^{y_{i}} = \frac{1}{y_{i}} \frac{d y_{i}}{d b_{j}} .$ (8)

The non-normalization sensitivities can be expressed as follows:

$S_{b_{j}}^{y_{i}} = \frac{d y_{i}}{d b_{j}},$ (9)

where $S_{b_{j}}^{y_{i}}$ stands for sensitivity for each variable y_i with respect to each parameter b_j. We apply the idea of local sensitivity for the proposed COVID-19 model (Equation 2). The model initial populations are S₀ = 6 × 10⁶, E₀ = 105.26, I₀ = 1027 and R₀ = 1027, and the model estimated parameters are α = 0.23, k = 0.34, γ = 0.08, β = 0.17, µ = 0.00003, and Λ = 182.46. They are used in computational simulations using SimBiology Toolbox for MATLAB. The results provide a wide range of means of identifying the key critical model parameters. According to the non-normalization technique, susceptible individuals, S, are very sensitive to the natural death, µ. This is clearly shown in Figure 2a. In addition, all model states are also sensitive to these parameters: {β, α, γ} (see Figure 2b). This means that natural death rate, infection rate, natural recovery rate and transition rate between exposed individuals and recovered individuals have a great impact on the model populations, while the rate of natural birth has less impact on the model states. In addition, using the half-normalization method shows that the most sensitive parameter for all model states is the natural death µ. In addition, the exposed and infected individuals are also very sensitive to the set of parameters {β, γ}; see Figure 3. According to the full-normalization technique shown in Figure 4, the model parameters {Λ, µ} are the less critical model parameters, whereas the remaining model parameters are the most sensitive parameters. Interestingly, all model results here provide a wide range of means of studying such models biologically and give more suggestions. This is because identifying critical model parameters helps us to further model improvements and suggest control strategies and vaccination programs.

Figure 2. Local sensitivity analysis using non-normalization technique given in Equation 7 for proposed model (Equation 2) using MATLAB: (a) calculating the local sensitivity of all model variables and model parameters, (b) calculating the local sensitivity of all model variables and model parameters excluding µ.

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Figure 3. Local sensitivity analysis using half-normalization technique given in Equation 8 for proposed model (Equation 2) using MATLAB. This calculation includes all model variables and model parameters.

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Figure 4. Local sensitivity analysis using full-normalization technique given in Equation 9 for proposed model (Equation 2) using MATLAB: (a) calculating the local sensitivity of all model variables and model parameters, (b) calculating the local sensitivity of all model variables and model parameters excluding β.

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4. Computational simulations and discussions

Computational techniques are effective tools and frequently required to analyze some complex infectious disease models. The estimated parameter values and initial populations are obtained from the real data in the Kurdistan Region of Iraq given in the Appendices. The model estimated parameters are α = 0.23, k = 0.34, γ = 0.08, β = 0.17, µ = 0.00003, Λ = 182.46, and the model initial variables are S₀ = 6 × 10⁶, E₀ = 105.26, I₀ = 1027, R₀ = 1027. Using System Biology Toolbox (SBedit) in MATLAB, we determine the numerical approximate solutions of the model (Equation 2); see Figures 5 and 6. Numerical simulations are calculated in two-dimensional planes. All model computational results here are very interesting and provide some biological aspects. Firstly, it can be seen that Figure 5 shows the model dynamics of susceptible, exposed, asymptomatic infected and recovered people. We have noticed that the number of healthy people decreases gradually and becomes stable after 500 days, while the dynamics of recovered people increases and then becomes more flat after 500 days as well. Then, from 200 to 600 days, the numbers of exposed and infected individuals change dramatically. More interestingly, Figure 6 shows the comparison of total populations between the real data cases shown in Table 3 and the model equations given in Equation 2. For example, the total populations of infected people for the model equations and real data are given in Figure 6a. Then, Figure 6b shows the total populations of recovered individuals for model equations and real data. The results show good agreement between the real data and the model results. Finally, it is clear that our model results are fitted for the confirmed cases in Kurdistan. This means that the suggested model here can further be used to predict and give more control strategies.

Figure 5. Computational simulations here show the total populations for susceptible, exposed, asymptomatic infected and recovered people in MATLAB using initial populations S₀ = 6 × 10⁶, E₀ = 105.26, I₀ = 1027, R₀ = 1027 and estimated parameters α = 0.23, k = 0.34, γ = 0.08, β = 0.17, µ = 0.00003, Λ = 182.46.

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Figure 6. Numerical results here show the comparison between model results given in Equation 2 and real data of confirmed cases for the COVID-19 pandemic in the Kurdistan Region, Iraq, given in Table 3: (a) the total population of infected people, (b) the total population of recovered people.

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5. Conclusions

Control strategies and preventions for the COVID-19 pandemic may not be well understood only by healthcare techniques and biological concepts. Mathematical models and computational simulations have been widely used for further improvements and identifying the model critical parameters. Therefore, identifying such parameters becomes an issue that can be further studied, and more techniques can be proposed. Sensitivity of model parameters helps international efforts to suggest more control strategies and preventions. Accordingly, the suggested SEIR model in this study plays an effective role in identifying the model critical elements using elasticity and sensitivity of R₀. Thus, the model sensitivities were calculated using three different techniques: non normalizations, half normalizations, and full normalizations. The results showed that the most effective parameters for spreading this disease are contact rate among people, transition rate from exposed class to the infected class and natural recovery rate. Interestingly, identifying the model critical parameters here will help to suggest further interventions and control strategies in the Kurdistan Region of Iraq. The suggested SEIR model can be further developed and can have added more transmission rates between model states. For example, the vaccination compartment with its contact rates can be added to the model. This helps to study this disease more widely and accurately. Further techniques of model analysis such as optimal control will also be applied to the model to find more control strategies.

References

[1]	The Keller-Segel model for chemotaxis with prevention of overcrowding: linear vs. nonlinear diffusion. SIAM J. Math. Anal. (2006) 38: 1288-1315.
[2]	Z. Chai, H. Liang, R. Du and B. Shi, A lattice Boltzmann model for two-phase flow in porous media, SIAM J. Sci. Comput., 41 (2019), B746–B772. doi: 10.1137/18M1166742
[3]	Z. H. Chai and T. S. Zhao, Lattice Boltzmann model for the convection-diffusion equation, Phy. Rev. E, 87 (2013), 063309.
[4]	Lattice Boltzmann method for fluid flows. Annu. Rev. Fluid Mech. (1998) 30: 329-364.
[5]	Sinking, merging and stationary plumes in a coupled chemotaxis-fluid model: A high-resolution numerical approach. J. Fluid Mech. (2012) 694: 155-190.
[6]	Numerical study of plume patterns in a chemotaxis-diffusion-convection coupling system. Comput. Fluids (2016) 126: 58-70.
[7]	The Keller-Segel model with logistic sensitivity function and small diffusivity. SIAM J. Appl. Math. (2005) 66: 286-308.
[8]	C. Dombrowski, L. Cisneros, S. Chatkaew, R. E. Goldstein and J. O. Kessler, Self-concentration and large-scale coherence in bacterial dynamics, Phys. Rev. Lett., 93 (2004), 098103. doi: 10.1103/PhysRevLett.93.098103
[9]	(2004) Chemotaxis. London: Imperial College Press.
[10]	Upwind-difference potentials method for Patlak-Keller-Segel chemotaxis model. J. Sci. Comput. (2012) 53: 689-713.
[11]	Discontinuous Galerkin methods for the chemotaxis and haptotaxisn models. J. Comput. Appl. Math. (2009) 224: 168-181.
[12]	New interior penalyt discontinous Galerkin methods for the Keller-Segel chemotaxis model. SIAM J. Numer. Anal. (2008/2009) 47: 386-408.
[13]	A finit volume scheme for the Patlak-Keller-Segel chemotaxis model. Numer. Math. (2006) 104: 457-488.
[14]	Bioconvection. Fluid Dynam. Res. (2005) 37: 1-20.
[15]	Bioconvection in suspensions of oxytactic bacteria: Linear theory. J. Fluid Mech. (1996) 324: 223-259.
[16]	Lattice-Boltzmann model for bacterial chemotaxis. J. Math. Biol. (2005) 51: 302-332.
[17]	Numerical investigation of falling bacterial plumes caused by bioconvection in a three-dimensional chamber. Eur. J. Mech. B Fluid. (2015) 52: 120-130.
[18]	Recent advances in lattice Boltzmann computing.. Annu. Rev. Comput. Phys. (1995) 3: 195-242.
[19]	Thermodynamic-consistent multiple-relaxation-time lattice Boltzmann equation model for two-phase hydrocarbon fluids with Peng-Robinson equation of state. Int. J. Heat Mass Tran. (2019) 141: 1216-1226.
[20]	Stability of operator splitting methods for systems with indefinite poerators: advection-diffusion-reaction systems. J. Comput. Phys. (2009) 228: 3508-3516.
[21]	Conservative upwind finite-element method for a simplified Keller-Segel system modeling chemotaxis. IMA J. Numer. Anal. (2007) 27: 332-365.
[22]	Numerical investigation of chemotaxic phenomenon in incompressible viscous fluid flow. Comput. Fluids (2014) 103: 290-306.
[23]	B. C. Shi and Z. L. Guo, Lattice Boltzmann model for nonlinear conveciton-diffusion equations, Phy. Rev. E, 79 (2009), 016701.
[24]	Bacterial swimming and oxygen transport near contact lines. Proc. Natl. Acad. Sci. (2005) 102: 2277-2282.
[25]	Fractional step methods applied to a chemotaxis model. J. Math. Biol. (2000) 41: 455-475.
[26]	A lattice Boltzmann analysis of the conjugate natural convection in square enclosure with a circular cylinder. Appl. Math. Model. (2019) 71: 31-44.
[27]	A multiple-relaxation-time Lattice-Boltzmann model for bacterial chemotaxis: Effects of initial concentration, diffusion, and hydrodynamic dispersion on traveling bacterial bands. Bull Math. Biol. (2014) 76: 2449-2475.
[28]	A coupled lattice Boltzmann method to solve Nernst-Planck model for simulating electro-osmotic flows. J. Sci. Comput. (2014) 61: 222-238.
[29]	T. Zhang, B. C. Shi, Z. L. Guo, Z. H. Chai and J. H. Lu, Genearl bounce-back scheme for concentration boundary condition in the lattice Boltzmann method, Phys. Rev. E, 85 (2012), 016701.

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