# Analytical Solution for One-Dimensional Transport of Particles considering Dispersion in Deposition Kinetics

Authors: Xingxin Chen; Xinran Zhang; Zhonghan Wu
Journal: Geofluids
 (2019)

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## Abstract

The study of particle transport in porous media is of great significance for pollution mitigation, grouting reinforcement, municipal solid waste landfill management, and groundwater exploitation. We developed an analytical solution for a corrected convection-dispersion model that takes into account the effects of dispersion on deposition kinetics with regard to the particle concentration decay type. The rationality and correctness of the solution were verified using time, distance, deposition coefficient, diffusion coefficient, and decay coefficient. As the time increased, the particle concentration increased from zero to the peak value, then decreased to zero. However, as distance increased, the peak value of particle concentration gradually decreased. The deposition coefficient affected the magnitude of the peak value and the distance corresponding to the peak value. In addition, the greater the attenuation coefficient, the smaller the peak value. Overall, our method’s prediction results showed that considering the effect of dispersion on deposition kinetics produces better results than when this is not considered.


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## Body

## 1. Introduction

Rapid global socioeconomic development is increasing groundwater pollution, which has a serious impact on human lives and productivity. As underground aquifers have complex structures and groundwater flow rates tend to be slow, groundwater pollution is difficult to find and mitigate. It was previously thought that pollutants in aquifers could only be transported via liquids and gases, but it is now understood that pollutants can be adsorbed by small particles carried in water; thus, the presence of such particles promotes the diffusion of pollutants [1–3]. Biological particles (e.g., bacteria, protozoa, and viruses) in aquifers can affect water safety and human health; these are primarily sourced from septic tanks, underground pipeline leaks, sewage leakage, and sludge [4–6]. Thus, the study of particle transport characteristics in porous media is very important for human and ecological health.The conventional particle transportation model has obtained many analytical solutions regarding the direct prediction and inverse problems [7–13], in which the particle flux in porous media is the sum of advective and dispersive fluxes. Nevertheless, this model only considers hydrodynamic particle dispersion in the mass balance equation but does not consider the effect of dispersive flux on retention kinetics. Laboratory tests can provide useful context for the ways in which this model’s deficiencies make prediction results inaccurate [14]. Increasing numbers of experimental studies [12] show that when conditions are not conducive to adsorption, particle deposition along the depth profile appears in a superexponential form, different from the prediction results of the conventional model. In pulse-injected tracers or suspension to the porous medium, conventional model results suggest that the maximum value of the pulse velocity is the same as that of the flow rate and that the concentration curve is symmetrically distributed on both sides of the maximum. However, many test results [13] show that the first half of the concentration distribution is much larger than the second half and that the transport of the maximum concentration is far less than the flow rate.Previous research contains a general framework for solutions to solute transport problems subject to time-dependent boundary conditions that is useful for many applications in science and engineering [15]. However, in this framework, the initial moment of the porous medium is clean (far from the actual situation), limiting its practical and accurate use. In this paper, we present an analytical solution for corrected convection-dispersion models that take into account the effects of dispersion on deposition kinetics and the initial particle concentration, obtained for particle concentration decay types. The solutions were verified using time, distance, deposition coefficient, diffusion coefficient, and decay coefficient [3, 5, 11]. This method is useful for providing benchmarks for complex transport processes, conducting sensitivity analyses of various parameters for particle transport, and estimating parameters for laboratory experiments. Therefore, our results can be widely applied to the treatment of pollutants, grouting reinforcement, municipal solid waste landfill management, and groundwater exploitation.


## 2. Materials and Methods

### 2.1. Assumptions

(1)
The porous medium is saturated, homogeneous, and isotropic
(2)
The study area is a semi-infinite porous medium
(3)
The flow is a one-dimensional steady flow, and the convection and dispersion of the particles are also one-dimensional
(4)
The deposition of particles is irreversible, and the release of deposited particles is neglected


### 2.2. Mathematical Model

Under one-dimensional steady flow conditions, the mass balance equation for particle transport is [10–16]
(1)∂C∂t=D∂2C∂x2−u∂C∂x−ρϕ∂σ∂t,where C is the particle concentration in seepage (ML-3), φ is the porosity, D is the diffusion coefficient (L2T-1), u is the average flow rate in the pore space between the cross sections (LT-1), t is the transport time (T), x is the transport distance (L), ρ is the particle density (ML-3), and σ is the ratio of particle volume deposit on the particle surface to solid medium volume (dimensionless). The deposition kinetic equation that takes into account dispersion [14, 16, 17] gives
(2)ρϕ∂σ∂t=kdep⋅C−kdep⋅Du⋅∂C∂x,where kdep is the deposition coefficient (T-1). Assuming that the dispersivity D=αD⋅u, substitution of equation (2) into equation (1) gives
(3)∂C∂t=D⋅∂2C∂X2+D1−u∂C∂X−kdep⋅C,where αD is the longitudinal dispersivity (L). D1 are coefficients given by
(4)D1=kdep⋅Du.For decay concentration injection, the initial state and boundary conditions are(5)Cx,0=Ci,0≤x<+∞,(6)C0,t=C0exp−α′t,(7)∂C∞,t∂x=0,where Ci is the initial constant concentration in the porous media (M/L), C0 is the initial injection concentration (ML-3), and α′ is the decay coefficient (T-1).


### 2.3. Solving the Model

Laplace transformation oft for equation (3) on both sides and substitution of the initial condition (5) are obtained by
(8)∂2C¯∂X2+D1D−uD∂C¯∂X−kdep+sDC¯=−CiD,where s is a complex variable corresponding to t and C¯ is the Laplace transformation of C.The solution to equation (8) can be obtained by
(9)C¯=C1⋅expu2D−D12Dx+xD12D−u2D2+kdep+sD1/2+C2⋅expu2D−D12Dx−xD12D−u2D2+kdep+sD1/2−CiDk1k2.From the boundary conditions of equations (6) and (7), the values of C1 and C2 can be obtained; thus,
(10)C¯=C0p+α′−Cip+kdep⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2+Cip+kdep,where p is a complex variable corresponding to t in equations (6) and (7). Assuming that
(11)I1=C0p+α′⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2,(12)I2=−Cip+kdep⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2,(13)I3=Cikdep+p,by first letting α=D1−u2/4D+kdep−α′,k=D, in equation (19) of Carslaw and Jaeger [18] and then using a=−D1−u2/4D−kdep in equation (29.2.12) of Abramowitz and Stegun [19], the inverse Laplace transformation of the first term in equation (11) is
(14)L−1I1=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′D⋅erfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′D⋅erfcx2Dt+D1−u24Dt+kdept−α′t.Hence, the result of the inverse Laplace transformation of the second term in equation (12) is given by
(15)L−1I2=−Ci2⋅expu2D−D12Dx−kdeptexp−xD1−u2D⋅erfcx2D⋅t−D1−u2t4D+expxD1−u2D⋅erfcx2D⋅t+D1−u2t4D.The result of the inverse Laplace transformation of the second term in equation (13) is given by
(16)L−1I4=Ci⋅e−kdept.The inverse transformation of equation (3), which is the solution to the present problem, is thus
(17)Cx,t=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′Derfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′Derfcx2Dt+D1−u24Dt+kdept−α′t−Ci2⋅expu2D−D12Dx−kdeptexp−xD1−u2D⋅erfcx2D⋅t−D1−u2t4D+expxD1−u2D⋅erfcx2D⋅t+D1−u2t4D+Ci⋅e−kdept.By lettingCi=0, equation (17) is reduced to the following form:
(18)Cx,t=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′D⋅erfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′D⋅erfcx2Dt+D1−u24Dt+kdept−α′t.The analytical solution of the conventional convection-dispersion model, in which the influence of the dispersion on the deposition kinetics is not considered, can be obtained by lettingCi=0 and D1=0 in equation (17), delivering the following result:
(19)Cx,t=C02⋅expux2D−α′t⋅exp−xu24D2+kdep−α′D⋅erfcx2Dt−u24Dt+kdept−α′t+expxu24D2+kdep−α′D⋅erfcx2Dt+u24Dt+kdept−α′t.


## 2.1. Assumptions

(1)
The porous medium is saturated, homogeneous, and isotropic
(2)
The study area is a semi-infinite porous medium
(3)
The flow is a one-dimensional steady flow, and the convection and dispersion of the particles are also one-dimensional
(4)
The deposition of particles is irreversible, and the release of deposited particles is neglected


## 2.2. Mathematical Model

Under one-dimensional steady flow conditions, the mass balance equation for particle transport is [10–16]
(1)∂C∂t=D∂2C∂x2−u∂C∂x−ρϕ∂σ∂t,where C is the particle concentration in seepage (ML-3), φ is the porosity, D is the diffusion coefficient (L2T-1), u is the average flow rate in the pore space between the cross sections (LT-1), t is the transport time (T), x is the transport distance (L), ρ is the particle density (ML-3), and σ is the ratio of particle volume deposit on the particle surface to solid medium volume (dimensionless). The deposition kinetic equation that takes into account dispersion [14, 16, 17] gives
(2)ρϕ∂σ∂t=kdep⋅C−kdep⋅Du⋅∂C∂x,where kdep is the deposition coefficient (T-1). Assuming that the dispersivity D=αD⋅u, substitution of equation (2) into equation (1) gives
(3)∂C∂t=D⋅∂2C∂X2+D1−u∂C∂X−kdep⋅C,where αD is the longitudinal dispersivity (L). D1 are coefficients given by
(4)D1=kdep⋅Du.For decay concentration injection, the initial state and boundary conditions are(5)Cx,0=Ci,0≤x<+∞,(6)C0,t=C0exp−α′t,(7)∂C∞,t∂x=0,where Ci is the initial constant concentration in the porous media (M/L), C0 is the initial injection concentration (ML-3), and α′ is the decay coefficient (T-1).


## 2.3. Solving the Model

Laplace transformation oft for equation (3) on both sides and substitution of the initial condition (5) are obtained by
(8)∂2C¯∂X2+D1D−uD∂C¯∂X−kdep+sDC¯=−CiD,where s is a complex variable corresponding to t and C¯ is the Laplace transformation of C.The solution to equation (8) can be obtained by
(9)C¯=C1⋅expu2D−D12Dx+xD12D−u2D2+kdep+sD1/2+C2⋅expu2D−D12Dx−xD12D−u2D2+kdep+sD1/2−CiDk1k2.From the boundary conditions of equations (6) and (7), the values of C1 and C2 can be obtained; thus,
(10)C¯=C0p+α′−Cip+kdep⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2+Cip+kdep,where p is a complex variable corresponding to t in equations (6) and (7). Assuming that
(11)I1=C0p+α′⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2,(12)I2=−Cip+kdep⋅expu2D−D12Dx−xD12D−u2D2+kdep+pD1/2,(13)I3=Cikdep+p,by first letting α=D1−u2/4D+kdep−α′,k=D, in equation (19) of Carslaw and Jaeger [18] and then using a=−D1−u2/4D−kdep in equation (29.2.12) of Abramowitz and Stegun [19], the inverse Laplace transformation of the first term in equation (11) is
(14)L−1I1=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′D⋅erfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′D⋅erfcx2Dt+D1−u24Dt+kdept−α′t.Hence, the result of the inverse Laplace transformation of the second term in equation (12) is given by
(15)L−1I2=−Ci2⋅expu2D−D12Dx−kdeptexp−xD1−u2D⋅erfcx2D⋅t−D1−u2t4D+expxD1−u2D⋅erfcx2D⋅t+D1−u2t4D.The result of the inverse Laplace transformation of the second term in equation (13) is given by
(16)L−1I4=Ci⋅e−kdept.The inverse transformation of equation (3), which is the solution to the present problem, is thus
(17)Cx,t=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′Derfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′Derfcx2Dt+D1−u24Dt+kdept−α′t−Ci2⋅expu2D−D12Dx−kdeptexp−xD1−u2D⋅erfcx2D⋅t−D1−u2t4D+expxD1−u2D⋅erfcx2D⋅t+D1−u2t4D+Ci⋅e−kdept.By lettingCi=0, equation (17) is reduced to the following form:
(18)Cx,t=C02⋅expu2D−D12Dx−α′t⋅exp−xD1−u24D2+kdep−α′D⋅erfcx2Dt−D1−u24Dt+kdept−α′t+expxD1−u24D2+kdep−α′D⋅erfcx2Dt+D1−u24Dt+kdept−α′t.The analytical solution of the conventional convection-dispersion model, in which the influence of the dispersion on the deposition kinetics is not considered, can be obtained by lettingCi=0 and D1=0 in equation (17), delivering the following result:
(19)Cx,t=C02⋅expux2D−α′t⋅exp−xu24D2+kdep−α′D⋅erfcx2Dt−u24Dt+kdept−α′t+expxu24D2+kdep−α′D⋅erfcx2Dt+u24Dt+kdept−α′t.


## 3. Results and Discussion

### 3.1. Calculation Examples

We assessed the analytical solutions in terms of time, distance, dispersion coefficient, deposition coefficient, and attenuation coefficient, using model parameters selected from previous studies [20–23]. Figure 1 shows the relationship between particle concentration and time for various distances predicted by equations (18) and (19) using the parameters given in Table 1. Figure 2 shows the relationship between particle concentration and distance for various times predicted by equations (18) and (19) using the parameters given in Table 1.Figure 1
Relationship between particle concentration and time for various distances predicted by equations (18) (solid curves) and (19) (dashed curves), using parameters given in Table 1.Table 1
Model parameters used for simulations shown in Figures1 and 2.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
1
0.36
1
0.001Figure 2
Relationship between particle concentration and distance for various times predicted by equations (18) (solid curves) and (19) (dashed curves), using parameters given in Table 1.Figure1 shows that particle concentration increases from zero to peak concentration very quickly, then decreases back to zero over a longer time period. In other words, the time required for a concentration increase is far less than that required for a concentration decrease and the peak concentration value gradually decreases with increasing distance. In addition, the prediction results from equation (18) are consistently lower than those from equation (19). Figure 2 shows that the particle concentration gradually decreases with increasing distance, while the greater the time, the smaller the concentration at the same distance. The prediction results from both equations (18) and (19) are very close. Overall, neglecting dispersion in the deposition kinetic equation can result in larger errors in the relationship between particle concentration and time.Figure3 shows the relationship between particle concentration and time for two dispersion coefficients predicted by equation (18) using the parameters given in Table 2. Figure 4 shows the relationship between particle concentration and distance for the same two dispersion coefficients using the parameters given in Table 3.Figure 3
Relationship between particle concentration and time for two dispersion coefficients, using parameters given in Table2.Table 2
Model parameters used for simulations shown in Figure3.
kdep (s-1)
x (cm)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
50
0.36
1
0.001Figure 4
Relationship between particle concentration and distance for two dispersion coefficients, using parameters given in Table3.Table 3
Model parameters for simulations shown in Figure4.
kdep (s-1)
t (s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
1000
0.36
1
0.001As the influence of the dispersion coefficient on the concentration curve is small, only two dispersion coefficients were tested in Figures3 and 4. Particle concentration rapidly peaked with increasing time, then gradually decreased to zero; the dispersion coefficients had little influence on particle concentration. Particle concentration decreased with increasing distance; again, the dispersion coefficients had little influence.Figure5 shows the relationship between particle concentration and time for four deposition coefficients predicted by equation (18) using the parameters given in Table 4. Figure 6 shows the relationship between particle concentration and distance for the same four deposition coefficients using the parameters given in Table 5.Figure 5
Relationship between particle concentration and time for four deposition rate coefficients, using parameters given in Table4.Table 4
Model parameters for simulations shown in Figure5.
x (cm)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
100
1
0.36
1
0.001Figure 6
Relationship between particle concentration and distance for four deposition rate coefficients, using parameters given in Table5.Table 5
Model parameters for simulations shown in Figure6.
t (s)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
1000
1
0.36
1
0.001Figure5 shows that the particle concentration rapidly peaked with increasing time, then gradually decreased to zero. The peak value gradually decreased with increasing deposition coefficient, showing that this has a very important influence on particle transportation. Figure 6 shows that when the deposition coefficient was zero, the particle concentration gradually increased from about 0.35 to the peak with increasing distance, then decreased to zero. When the deposition coefficients were 0.004 and 0.006, the particle concentration decreased from 0.35 to zero with increasing distance. Furthermore, when the deposition coefficient was 0.002, the particle concentration showed a transition period between deposition coefficients of 0 and 0.004. Overall, the particle concentration decreased with increasing deposition coefficient, showing that this has a great influence on the shape of such curves.Figure7 shows the relationship between particle concentration and time for four decay coefficients predicted by equation (18) using the parameters given in Table 6. Figure 8 shows the relationship between particle concentration and distance for the same decay coefficients using the parameters given in Table 7.Figure 7
Relationship between particle concentration and time for four decay factors, using parameters given in Table6.Table 6
Model parameters for simulations shown in Figure7.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
x (cm)
0.01
1
0.36
1
100Figure 8
Relationship between particle concentration and distance for four decay factors, using parameters given in Table7.Table 7
Model parameters for simulations shown in Figure8.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
t (s)
0.01
1
0.36
1
500Figure7 shows that when the decay coefficient was zero, the particle concentration peaked rapidly, then did not change further. When the decay coefficient was greater than zero, the concentration peaked rapidly, then gradually decreased to zero over time. In addition, the peak value of the particle concentration decreased with increasing decay coefficient. Figure 8 shows that the particle concentration decreased to zero with increasing distance and also decreased with increasing decay coefficient. Overall, the decay coefficient has a significant effect on particle transport.


## 3.1. Calculation Examples

We assessed the analytical solutions in terms of time, distance, dispersion coefficient, deposition coefficient, and attenuation coefficient, using model parameters selected from previous studies [20–23]. Figure 1 shows the relationship between particle concentration and time for various distances predicted by equations (18) and (19) using the parameters given in Table 1. Figure 2 shows the relationship between particle concentration and distance for various times predicted by equations (18) and (19) using the parameters given in Table 1.Figure 1
Relationship between particle concentration and time for various distances predicted by equations (18) (solid curves) and (19) (dashed curves), using parameters given in Table 1.Table 1
Model parameters used for simulations shown in Figures1 and 2.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
1
0.36
1
0.001Figure 2
Relationship between particle concentration and distance for various times predicted by equations (18) (solid curves) and (19) (dashed curves), using parameters given in Table 1.Figure1 shows that particle concentration increases from zero to peak concentration very quickly, then decreases back to zero over a longer time period. In other words, the time required for a concentration increase is far less than that required for a concentration decrease and the peak concentration value gradually decreases with increasing distance. In addition, the prediction results from equation (18) are consistently lower than those from equation (19). Figure 2 shows that the particle concentration gradually decreases with increasing distance, while the greater the time, the smaller the concentration at the same distance. The prediction results from both equations (18) and (19) are very close. Overall, neglecting dispersion in the deposition kinetic equation can result in larger errors in the relationship between particle concentration and time.Figure3 shows the relationship between particle concentration and time for two dispersion coefficients predicted by equation (18) using the parameters given in Table 2. Figure 4 shows the relationship between particle concentration and distance for the same two dispersion coefficients using the parameters given in Table 3.Figure 3
Relationship between particle concentration and time for two dispersion coefficients, using parameters given in Table2.Table 2
Model parameters used for simulations shown in Figure3.
kdep (s-1)
x (cm)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
50
0.36
1
0.001Figure 4
Relationship between particle concentration and distance for two dispersion coefficients, using parameters given in Table3.Table 3
Model parameters for simulations shown in Figure4.
kdep (s-1)
t (s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
0.01
1000
0.36
1
0.001As the influence of the dispersion coefficient on the concentration curve is small, only two dispersion coefficients were tested in Figures3 and 4. Particle concentration rapidly peaked with increasing time, then gradually decreased to zero; the dispersion coefficients had little influence on particle concentration. Particle concentration decreased with increasing distance; again, the dispersion coefficients had little influence.Figure5 shows the relationship between particle concentration and time for four deposition coefficients predicted by equation (18) using the parameters given in Table 4. Figure 6 shows the relationship between particle concentration and distance for the same four deposition coefficients using the parameters given in Table 5.Figure 5
Relationship between particle concentration and time for four deposition rate coefficients, using parameters given in Table4.Table 4
Model parameters for simulations shown in Figure5.
x (cm)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
100
1
0.36
1
0.001Figure 6
Relationship between particle concentration and distance for four deposition rate coefficients, using parameters given in Table5.Table 5
Model parameters for simulations shown in Figure6.
t (s)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
α′ (s-1)
1000
1
0.36
1
0.001Figure5 shows that the particle concentration rapidly peaked with increasing time, then gradually decreased to zero. The peak value gradually decreased with increasing deposition coefficient, showing that this has a very important influence on particle transportation. Figure 6 shows that when the deposition coefficient was zero, the particle concentration gradually increased from about 0.35 to the peak with increasing distance, then decreased to zero. When the deposition coefficients were 0.004 and 0.006, the particle concentration decreased from 0.35 to zero with increasing distance. Furthermore, when the deposition coefficient was 0.002, the particle concentration showed a transition period between deposition coefficients of 0 and 0.004. Overall, the particle concentration decreased with increasing deposition coefficient, showing that this has a great influence on the shape of such curves.Figure7 shows the relationship between particle concentration and time for four decay coefficients predicted by equation (18) using the parameters given in Table 6. Figure 8 shows the relationship between particle concentration and distance for the same decay coefficients using the parameters given in Table 7.Figure 7
Relationship between particle concentration and time for four decay factors, using parameters given in Table6.Table 6
Model parameters for simulations shown in Figure7.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
x (cm)
0.01
1
0.36
1
100Figure 8
Relationship between particle concentration and distance for four decay factors, using parameters given in Table7.Table 7
Model parameters for simulations shown in Figure8.
kdep (s-1)
D (cm2/s)
u (cm/s)
C0 (mg/ml)
t (s)
0.01
1
0.36
1
500Figure7 shows that when the decay coefficient was zero, the particle concentration peaked rapidly, then did not change further. When the decay coefficient was greater than zero, the concentration peaked rapidly, then gradually decreased to zero over time. In addition, the peak value of the particle concentration decreased with increasing decay coefficient. Figure 8 shows that the particle concentration decreased to zero with increasing distance and also decreased with increasing decay coefficient. Overall, the decay coefficient has a significant effect on particle transport.


## 4. Conclusion

We developed an analytical solution for a corrected convection-dispersion model that takes into account the effect of dispersion on deposition kinetics with regard to the particle concentration decay type. The rationality and correctness of the solution were verified using the time, distance, deposition coefficient, diffusion coefficient, and decay coefficient. The main conclusions are as follows:(1)
Particle concentration increased from zero to the peak value with increasing time, then decreased to zero. However, particle concentration gradually reduced to zero with increasing transport distance
(2)
Neglecting dispersion in the deposition kinetic equation can result in large errors in the relationship between particle concentration and time
(3)
With regard to time, the peak value of the particle concentration decreased gradually with increasing deposition coefficient, but the time corresponding to the peak value did not change
(4)
With regard to distance, the deposition coefficient affected the magnitude and distance of the peak value of the particle concentration
(5)
With regard to time, the peak value of the particle concentration decreased with increasing decay coefficient. With regard to distance, the peak value decreased with increasing decay coefficient



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