Abstract
The forced convective boundary layer flow of viscous incompressible time-dependent fluid containing water-based nanofluids and gyrotactic microorganisms simultaneously, from a flat surface with leading edge accretion (or ablation), is theoretically investigated in the present study. In doing so, the governing conservation equations are rendered into a nonlinear system of ordinary differential equations by means of utilizing appropriate coordinates transformations. MAPLE symbolic software is employed to solve these equations, which are subjected to impose boundary conditions using the Runge–Kutta–Fehlberg fourth-fifth order numerical method. It is noteworthy that the results of the present study are in an excellent agreement with previous solutions available in literature. The effect of selected parameters on velocity, temperature, nanoparticle volume fraction and motile microorganism density function is then investigated. Tabular solutions are included for the skin friction, heat transfer rate, nano-particle mass transfer rate and microorganism transfer rate. Applications of the study arise in advanced micro-flow devices to bio-modified nanomaterials processing.
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Abbreviations
- \(\tilde{b}\) :
-
Chemotaxis constant \(({\text{m}})\)
- \(C\) :
-
Nano-particles volume fraction \(( - )\)
- \(C_{\text{w}}\) :
-
Wall nano-particle volume fraction \(( - )\)
- \(C_{\infty }\) :
-
Ambient nano-particle volume fraction \(( - )\)
- \(C_{{{\text{f}}_{{\bar{x}}} }}\) :
-
Local skin friction coefficient along the \(\bar{x}\) \(( - )\)
- \(c_{\text{p}}\) :
-
Specific heat at constant pressure \(\left( {\frac{\text{J}}{\text{kgK}}} \right)\)
- \(D_{\text{B}}\) :
-
Brownian diffusion coefficient \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(D_{n}\) :
-
Microorganism diffusion coefficient \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(D_{\text{T}}\) :
-
Thermophoresis diffusion coefficient \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(f(\eta )\) :
-
Dimensionless stream function \(( - )\)
- \(\vec{j}\) :
-
Vector flux of microorganisms \(\left( {\frac{\text{kg}}{{{\text{m}}^{2} {\text{s}}}}} \right)\)
- \(k\) :
-
Thermal conductivity \(\left( {\frac{\text{W}}{\text{mK}}} \right)\)
- \(Lb\) :
-
Bioconvection Lewis number \(\left( {Lb = \frac{{\alpha_{{}} }}{{D_{n} }}} \right)\,\,\,( - )\)
- \(Le\) :
-
Lewis number \(\left( {Le = \frac{\alpha }{{D_{\text{B}} }}} \right)\,\,\,( - )\)
- \(Nb\) :
-
Brownian motion parameter \(\left( {Nb = \frac{{\tau D_{\text{B}} \left( {C_{\text{w}} - C_{\infty } } \right)}}{{\alpha_{{}} }}} \right)\,\,\,( - )\)
- \(Nn_{{\bar{x}}}\) :
-
Local density number of motile microorganisms \(\,\,( - )\)
- \(Nt\) :
-
Thermophoresis parameter \(\left( {Nt = \frac{{\tau D_{\text{T}} \left( {T_{\text{w}} - T_{\infty } } \right)}}{\alpha T_{\infty }}} \right)\,\,\,( - )\)
- \(Nu_{{\bar{x}}}\) :
-
Local Nusselt number \(( - )\)
- \(n\) :
-
Number of motile microorganisms \(( - )\)
- \(n_{\text{w}}\) :
-
Wall motile microorganisms \(( - )\)
- \(Pe\) :
-
Bioconvection Péclet number \(\left( {Pe = \frac{{\tilde{b}W_{\text{c}} }}{{D_{n} }}} \right)\,\,\,( - )\)
- \(Pr\) :
-
Prandtl number \(\left( {Pr = \frac{\upsilon }{\alpha }} \right)\,\,\,( - )\)
- \(Re\) :
-
Reynolds number \(\left( {\frac{{\bar{U}_{\infty } \bar{x}}}{\upsilon }} \right)\) \(\left( - \right)\)
- \(Sh_{{\bar{x}}}\) :
-
Local Sherwood number \(( - )\)
- \(s\) :
-
Wall mass flux (Stefan blowing)\(\left( {\frac{{C_{\text{w}} - C_{\infty } }}{{1 - C_{\text{w}} }}} \right)\) \(( - )\)
- \(\bar{t}\) :
-
Dimensional time \(({\text{s}})\)
- \(T\) :
-
Nanofluid temperature \(({\text{K}})\)
- \(T_{\text{w}}\) :
-
Wall temperature \((K)\)
- \(T_{\infty }\) :
-
Ambient temperature \(({\text{K}})\)
- \(\bar{U}_{\infty }\) :
-
Dimensional ambient velocity \(\left( {\frac{\text{m}}{\text{s}}} \right)\)
- \(\bar{u}\) :
-
Velocity components along the \(\bar{x}\)-axis \(\left( {\frac{\text{m}}{\text{s}}} \right)\)
- \(\overrightarrow {{\bar{v}}}\) :
-
Velocity vector \(\left( {\frac{\text{m}}{\text{s}}} \right)\)
- \(\tilde{\bar{v}}\,\) :
-
Average swimming velocity vector of microorganism \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(\bar{v}\) :
-
Velocity components along the \(\bar{y}\)-axis \(\left( {\frac{\text{m}}{\text{s}}} \right)\)
- \(W_{\text{c}}\) :
-
Maximum cell swimming speed \(\left( {\frac{\text{m}}{\text{s}}} \right)\)
- \(\bar{x}\) :
-
Dimensional coordinate along the surface \(({\text{m}})\)
- \(\bar{y}\) :
-
Coordinate normal to the surface \((m)\)
- \(\alpha {}_{{}}\) :
-
Effective thermal diffusivity \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(\gamma {}_{{}}\) :
-
Leading edge accretion/ablation \(( - )\)
- \(\eta\) :
-
Independent similarity variable \(( - )\)
- \(\theta (\eta )\) :
-
Dimensionless temperature \(( - )\)
- \(\mu\) :
-
Dynamic viscosity \(\left( {\frac{\text{kg}}{\text{ms}}} \right)\)
- \(\upsilon\) :
-
Kinematic viscosity \(\left( {\frac{{{\text{m}}^{2} }}{\text{s}}} \right)\)
- \(\rho\) :
-
Fluid density \(\left( {\frac{\text{kg}}{{{\text{m}}^{3} }}} \right)\)
- π :
-
Pi \(( - )\)
- \((\rho c)_{\text{f}}\) :
-
Volumetric heat capacity of the fluid \(\left( {\frac{\text{J}}{{{\text{m}}^{3} {\text{K}}}}} \right)\)
- \((\rho c)_{\text{p}}\) :
-
Volumetric heat capacity of the nanoparticle material \(\left( {\frac{\text{J}}{{{\text{m}}^{3} {\text{K}}}}} \right)\)
- \(\sigma\) :
-
Dimensionless time variable \(\left( {\bar{U}_{\infty }^{{}} \,\bar{t}/\bar{x}} \right)\) \(( - )\)
- \(\tau\) :
-
Ratio of the effective heat capacity of the nanoparticle material to the fluid heat capacity \(\left( {\frac{{(\rho c)_{\text{p}} }}{{(\rho c)_{\text{f}} }}} \right)\left( - \right)\)
- \(\phi (\eta )\) :
-
Dimensionless nanoparticles volume fraction \(( - )\)
- \(\chi (\eta )\) :
-
Dimensionless number of motile microorganisms \(( - )\)
- \(\psi\) :
-
Streamline function \(( - )\)
- \((\,\,\,)'\) :
-
Ordinary differentiation with respect to \(\eta\)
- \((\,\,\,)_{\text{w}}\) :
-
Condition at wall
- \((\,\,\,)_{\infty }\) :
-
Condition in free stream
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The authors acknowledge financial support from Universiti Sains Malaysia, RU Grant 1001/PMATHS/8011013.
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Basir, M.F.M., Uddin, M.J., Bég, O.A. et al. Influence of Stefan blowing on nanofluid flow submerged in microorganisms with leading edge accretion or ablation. J Braz. Soc. Mech. Sci. Eng. 39, 4519–4532 (2017). https://doi.org/10.1007/s40430-017-0877-7
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DOI: https://doi.org/10.1007/s40430-017-0877-7