Abstract
Dueck’s mathematical model of biofilm is discussed. This model is also generalized to cover all substratum types. This system is based on a nonlinear reaction–diffusion equation that includes a nonlinear term related to square law of microbial death rate. In this paper, the analytical expression of the substrate consumption and flux in a biofilm is obtained by solving the nonlinear differential equation using the Taylor series and the modified Adomian decomposition method. Comparing the results obtained with the numerical method and limiting case results shows the validity and usefulness of these techniques.
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ACKNOWLEDGMENTS
We are very grateful to the reviewers for their comments and suggestion. The authors are also thankful to Shri J. Ramachandran, Chancellor, Col. Dr. G. Thiruvasagam, Vice-Chancellor, Dr. M. Jayaprakashvel, registrar Academy of Maritime Education and Training (AMET), Deemed to be University, Chennai, for their constant encouragement.
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Appendices
APPENDIX A
Analytical solution of nonlinear reaction Eq. (11)using the TSM method. The steady-state nonlinear equation (11) can be written as follows:
By differentiating the above Eq. (A1) successively with respect to “x”, we get the following results.
The boundary condition (12) can be written as
Using this condition in the above Eqs. (A1) to (A4), we get
The concentration of substrates using the Taylor series is
Substituting Eqs. (A5) to (A10) into Eq. (A11), we obtain Eq. (19) in the text.
APPENDIX B
Analytical solution of nonlinear reaction Eq. (14)using the boundary conditions ((15) and (16)) by the modified Adomian decomposition method. In this Appendix, we indicate how Eq. (24) is derived. In order to solve Eq. (14) by means of the modified Adomian decomposition method [46]. We write Eq. (14) in the operator form
where \(L\) and \(N\) are linear and nonlinear terms of Eq. (14). Here, \(N(S) = {{\left( {\frac{S}{{1 + S}}} \right)}^{2}}.\) The operator for spherical substratum is defined as [46]
Applying the inverse operator [46]
on both sides of Eq. (B1) yields
where \(A\) and \(B\) are constants of integration. Let
In view of Eqs. (B4) to (B6) gives
The zero elements is defined as
and the remaining components as the recurrence relation \({{S}_{{i + 1}}}\left( x \right) = \delta {{L}^{{ - 1}}}{{A}_{i}},\) \(i \geqslant 0\)
where \({{A}_{i}}(x) = \frac{1}{{i!}}\frac{{{{d}^{i}}}}{{d{{\lambda }^{i}}}}N\)\({{\left( {\sum\limits_{n = 0}^\infty {{{\lambda }^{i}}{{S}_{i}}} } \right)}_{{\lambda = 0}}}\) are the Adomian polynomials of \({{S}_{1}},{{S}_{2}},...{{S}_{i}}\). We can find \({{A}_{i}}\) as follows:
The remaining polynomials can be easily generated and so on
Adding Eqs. (B11) to (B13), we get the concentration of substrate in the biofilm (Eq. (24)).
NOTATION
L f | biofilm thickness, m |
S f | concentration of substrate in the biofilm, g/m3 |
S 1 | concentration of substrate outside the biofilm, g/m3 |
D f | diffusion coefficient within the biofilm, m2/s |
z | distance from biofilm, m |
ψ | flux of substrate, g/m2 d |
b | microbial death constant, m3/g d |
K | Michaelis-Menten constant, g/m3 |
X f | position of an occupied grid cell above the substratum within the grid, g/m3 |
q | rate constant of substrate consumption, d–1 |
Y | yield per unit amount of substrate consumed in biofilm, g/m3 |
R | radius of the sphere, m |
S | dimensionless concentration of substrate in the biofilm |
S L | dimensionless concentration of substrate outside the biofilm |
x | dimensionless distance from the biofilm |
δ | dimensionless biofilm thickness |
m | dimensionless constant |
SUBSCRIPTS AND SUPERSCRIPTS
f | film |
L, 1 | solution |
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Jeyabarathi, P., Kannan, M. & Rajendran, L. Approximate Analytical Solutions of Biofilm Reactor Problem in Applied Biotechnology. Theor Found Chem Eng 55, 851–861 (2021). https://doi.org/10.1134/S0040579521050213
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DOI: https://doi.org/10.1134/S0040579521050213