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Electrothermal blood streaming conveying hybridized nanoparticles in a non-uniform endoscopic conduit

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Abstract

The novelty of nanoparticles in transferrals of medications and biological fluids via electrokinetic mechanism has been competently recognized. Due to the impressive role of nanoparticles suspended in blood or physiological fluids in medical fields, the current research article is planned to formulate an effective mathematical model to analyze the dynamism of bloodstream infused with hybridized nanoparticles in a non-uniform endoscopic conduit (space between two coaxial tubes) under the interactivities of electroosmosis, peristalsis, and buoyancy forces. The dual impact of heat source, Joule heating, and convectively cooling wall condition is examined. The geometrical shapes (sphere, brick, cylinder, and platelet) of nanoparticles injected into blood are accounted for in the formulation of modelled equations. The blood doped with hybridized nanoparticles is regarded as an electrolyte solution. The lubrication and Debye-Hückel linearization estimations are invoked in order to linearize the flow equations. Analytical solutions for the resulting leading equations are computed by implementing an analytical approach. The amendments in the physiognomies under variations in sundry parameters are explained through the line, bar graphs, and numerical tables. Outcomes admit that the flow of ionized blood is significantly amended across the endoscopic conduit due to the electrostatic body force. Blood is warmed or cooled with positive or negative values of Joule heating parameter. Blood is cooled with augmenting volumetric concentration of hybridized nanoparticles. The trap** phenomenon is also described by designing streamline plots. The size of confined blood boluses expands due to the thin electric double layer (EDL). The novel findings of this hemodynamic simulation furnish significant applicabilities in modelling of transportation of medications and drugs, physiological fluid mixers, testing and assessment of human diseases, detection of bacteria and viruses, etc.

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Abbreviations

List of symbols:

Description

a :

Dimensionless wave amplitude

a :

Wave amplitude

b 0 :

Radius of outer tube inlet

B i :

Biot number

c :

Wave velocity

\(c_{i}^{\prime }s\) :

Expressions

c p :

Specific heat capacity at constant pressure

e :

Net electronic charge

\((E_{\bar {R}}, E_{\bar {Z}})\) :

Electric filed components

F :

Volumetric flow rate

\(f_{i}^{\prime }s\) :

Expressions

F i, F o :

Friction forces for inter and outer tubes

\(_{0}\tilde {F}_{1}\) :

Regularized confluent hypergeometric function

I 0, I 1 :

First kind modified Bessel functions of zero th and first order

g :

Acceleration due to gravity

G r :

Thermal Grashof number

h :

Convective heat transfer coefficient

J 0, J 1 :

Bessel functions of first kind of zero and first order

k :

Non-uniform parameter

\(\bar {k}\) :

Thermal conductivity of blood

K B :

Boltzmann constant

n :

Nanoparticles’ shape factor

n 0 :

Average number of cations and anions

n +, n :

Number of densities of cations and anions

p :

Dimensionless blood pressure

\(\bar {P}\) :

Blood pressure

P r :

Prandtl number

Q :

Mean volume flow rate

Q 0 :

Heat source

R 0 :

Inner tube radius

(r 1, r 2):

Dimensionless radii of inner and outer tubes

(R 1, R 2):

Radii of inner and outer tubes

R e :

Reynolds number

S :

Joule heating parameter

t :

Dimensionless time

\(\bar {t}\) :

Time

T :

Blood temperature

T a :

Average temperature of electrolytic solution

T 0, T 1 :

Constant temperatures at inner tube and outer tube

(u,w):

Dimensionless velocity components in (r, z)

\((\bar {u}, \bar {w})\) :

Velocity components in moving frame (\(\bar {r}\), \(\bar {z}\))

\((\bar {U}, \bar {W})\) :

Velocity components in fixed frame (\(\bar {R}\), \(\bar {Z}\))

U h s :

Helmholtz-Smoluchowski velocity parameter

Y 0, Y 1 :

Second kind Bessel functions of zero the and first order

\(\tilde {z}\) :

Valence of ions

\(\bar {Z}\) :

Axial distance from inlet,

Z :

Heat transfer coefficient at outer wall

β :

Thermal expansion coefficient

δ :

Dimensionless wave number

𝜖 :

Amplitude ratio

ε :

A constant

ε 0 :

Dielectric permittivity of medium

𝜃 :

Dimensionless temperature

κ :

Electro-osmotic parameter

λ :

Wavelength

μ :

Dynamic viscosity of blood

ρ :

Fluid density

ρ e :

Net ionic charge density of electrolyte

σ :

Electric conductivity of blood

\(\omega _{i}^{\prime }s\) :

Expressions

Φ:

Non-dimensional electric potential

\(\bar {\Phi }\) :

Electric potential

(ϕ 1,ϕ 2):

Solid volume fractions of Ag and Al2O3-NPs

χ :

Heat source parameter

ψ :

Stream function

s 1 :

Silver nanoparticles (Ag-NPs)

s 2 :

Aluminum oxide nanoparticles (Al2O3-NPs)

f :

Base fluid (blood)

nf :

Nano-blood

hnf :

Hybrid nano-blood

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Acknowledgements

The authors are very grateful to the honourable editor and referees for their constructive comments and valued suggestions to enhance the superiority of the manuscript.

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Appendix

Appendix

$$\begin{array}{@{}lll@{}} c_{1}&=& \frac{Y_{0}(-i \kappa r_{1})}{J_{0}(i \kappa r_{2}) Y_{0}(-i \kappa r_{1})-J_{0}(i \kappa r_{1}) Y_{0}(-i \kappa r_{2})},\\ c_{2}&=& \frac{J_{0}(i \kappa r_{1})}{J_{0}(i \kappa r_{1}) Y_{0}(-i \kappa r_{2})-J_{0}(i \kappa r_{2}) Y_{0}(-i \kappa r_{1})},\\ f_{1}&=&B_{i}-\frac{B_{i}}{4 x_{4}}(S x_{3}+\chi)({r_{2}^{2}}-{r_{1}^{2}})-\frac{1}{2} r_{2} (S x_{3}+\chi),\\ f_{2}&=&B_{i} \log{\frac{r_{2}}{r_{1}}}+\frac{x_{4}}{r_{2}},\\ c_{3}&=&-\frac{f_{1}}{f_{2}},\\ f_{3}&=&r_{2} B_{i} [{r_{2}^{2}} \log{r_{1}}(S x_{3}+\chi)-{r_{1}^{2}} \log {r_{2}} (S x_{3}+\chi)-4 x_{4} \log{r_{2}}]\\ &+&x_{4} [2 {r_{2}^{2}} \log {r_{1}}(S x_{3}+\chi)-{r_{1}^{2}} (S x_{3}+\chi)-4 x_{4}],\\ f_{4}&=&4 x_{4} [r_{2} B_{i} \log{\frac{r_{2}}{r_{1}}}+x_{4}],\\ c_{4}&=&-\frac{f_{3}}{f_{4}},\\ f_{5}&=& - Gr \kappa x_{2} [(S x_{3}+\chi)({r_{1}^{6}} -3 {r_{2}^{2}} {r_{1}^{4}}+3 {r_{2}^{4}} {r_{1}^{2}})+{r_{2}^{6}} \chi],\\ f_{6}&=& Gr \kappa {r_{2}^{6}} S x_{2} x_{3}+192 r_{1} U x_{4} [\kappa r_{1} \{c_{1} (I_{0}(\kappa r_{1}) +I_{0}(\kappa r_{2}))\\ &+&c_{2}\left(Y_{0}(-i \kappa r_{1})+Y_{0}(-i \kappa r_{2})\right)\}-4 i c_{2} Y_{1}(-i \kappa r_{1})],\\ f_{7}&=& -192 U_{hs} x_{4} [2 c_{1} \kappa {r_{1}^{2}} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{1}^{2}}\right) +r_{2} \{c_{1} \kappa r_{2} (I_{0}(\kappa r_{1})+I_{0}(\kappa r_{2})) -4 i c_{2} Y_{1}(-i \kappa r_{2})\}],\\ f_{8}&=& -192 \kappa x_{4} [(2 x_{1} ({r_{1}^{2}}-F)+{r_{2}^{2}} \{-2 x_{1}+U_{hs} (-2 c_{1} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{2}^{2}}\right)\\ &+&c_{2} Y_{0}(-i \kappa r_{1})+c_{2} Y_{0}(-i \kappa r_{2}))\}]-12 c_{3} Gr \kappa x_{2} x_{4} [-{r_{1}^{4}}+{r_{2}^{4}}+4 {r_{2}^{2}} {r_{1}^{2}}\log{\frac{r_{1}}{r_{2}}}],\\ f_{9}&=& 192 \kappa x_{1} x_{4} [{r_{1}^{2}} (\log{\frac{r_{1}}{r_{2}}}-1)+{r_{2}^{2}} (\log{\frac{r_{1}}{r_{2}}}+1)],\\ c_{5}&=&-\frac{1}{f_{9}}(f_{5}+f_{6}+f_{7}+f_{8}),\\ f_{10}&=& Gr \kappa \chi x_{2} [{r_{1}^{8}} \log{r_{2}}+{r_{2}^{2}} {r_{1}^{6}} (3-4 \log{r_{1}})+3 {r_{2}^{4}} {r_{1}^{4}} (\log{r_{1}r_{2}}-2)+{r_{2}^{6}} {r_{1}^{2}} (3-4 \log{r_{2}})+{r_{2}^{8}} \log{r_{1}}],\\ f_{11}&=& Gr \kappa {r_{1}^{2}} S x_{2} x_{3}[{r_{1}^{6}} \log{r_{2}}+{r_{2}^{2}} {r_{1}^{4}} (3-4 \log{r_{1}})+3 {r_{2}^{4}} {r_{1}^{2}}(\log{r_{1}r_{2}}-2)+{r_{2}^{6}}(3-4 \log{r_{2}})],\\ f_{12}&=& Gr \kappa {r_{2}^{8}} S x_{2} x_{3} \log{r_{1}}+192 {r_{1}^{3}} U_{hs} x_{4} [\kappa r_{1} \{c_{1} I_{0}(\kappa r_{2}) + c_{1}(\log{r_{1}}-1)\\ &+&c_{2} Y_{0}(-i \kappa r_{2})\}+4 i c_{2} \log{r_{2}} Y_{1}(-i \kappa r_{1})],\\ f_{13}&=& -192 \kappa {r_{1}^{4}} U_{hs} x_{4} [c_{1} \log{r_{1}} I_{0}(\kappa r_{2})+c_{1} \log{r_{2}}(I_{0}(\kappa r_{1})+1)+c_{2} \log{r_{1}} Y_{0}(-i \kappa r_{2})],\\ f_{14}&=& -192 {r_{1}^{2}} U_{hs} x_{4} \log{r_{2}} [\kappa {r_{1}^{2}} \{-2c_{1} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{1}^{2}}\right) +c_{2} Y_{0}(-i \kappa r_{1})\}+4 i c_{2} r_{2} Y_{1}(-i \kappa r_{2})],\\ f_{15}&=& -192 r_{1} {r_{2}^{2}} U_{hs} x_{4} [\kappa r_{1} \{c_{1} I_{0}(\kappa r_{1})+c_{1} I_{0}(\kappa r_{2})-2 c_{1}+c_{2} Y_{0}(-i \kappa r_{1})\} +4 i c_{2} \log{r_{1}} Y_{1}(-i \kappa r_{1})],\\ f_{16}&=& 192 \kappa {r_{1}^{2}} {r_{2}^{2}} U_{hs} x_{4}[2 \log{r_{1}} \{c_{1} I_{0}(\kappa r_{1})+c_{2} Y_{0}(-i \kappa r_{1})\}-c_{2} Y_{0}(-i \kappa r_{2})],\\ f_{17}&=&384 \kappa {r_{1}^{2}} {r_{2}^{2}} U_{hs} x_{4} [-c_{1} \log{r_{1}} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{1}^{2}}\right) +\log{r_{2}} \{(c_{1} I_{0}(\kappa r_{2})+c_{2} Y_{0}(-i \kappa r_{2})\}],\\ f_{18}&=&-192 {r_{2}^{2}} U_{hs} x_{4} [2 c_{1} \kappa {r_{1}^{2}} \log{r_{2}} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{2}^{2}}\right) +r_{2} \{c_{1} \kappa r_{2}-4 i c_{2} \log{r_{1}} Y_{1}(-i \kappa r_{2})\}], \end{array}$$
$$\begin{array}{@{}rcl@{}} f_{19}&=&192 \kappa {r_{2}^{4}} U_{hs} x_{4} [c_{1} I_{0}(\kappa r_{1})-c_{1} \log{r_{1}}(I_{0}(\kappa r_{2})+1)+c_{2} Y_{0}(-i \kappa r_{1})],\\ f_{20}&=&-192 \kappa {r_{2}^{4}} U_{hs} x_{4} [-2c_{1} \log{r_{1}} {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{2}^{2}}\right) +c_{1} \log{r_{2}} (I_{0}(\kappa r_{1})-1)+c_{2} \log{r_{1}} Y_{0}(-i \kappa r_{2})],\\ f_{21}&=& -192 \kappa x_{4}[c_{2} {r_{2}^{4}} U_{hs} \log{r_{2}} Y_{0}(-i \kappa r_{1})-2 {r_{2}^{2}} x_{1} (F \log{r_{1}}+{r_{1}^{2}})\\ &+&{r_{1}^{2}} x_{1} \{2 F \log{r_{2}}-{r_{1}^{2}} (\log{r_{1}}+\log{r_{2}}-1)\}],\\ f_{22}&=&12 \kappa x_{4}[-c_{3} Gr {r_{1}^{6}} x_{2} \log{r_{2}}+c_{3} Gr {r_{2}^{2}} {r_{1}^{4}} x_{2} \log{r_{1}} (4 \log{r_{1}}-3)\\ &-&32 {r_{2}^{2}} {r_{1}^{2}} x_{1}\log{r_{1}r_{2}}+16 {r_{2}^{4}} x_{1} (\log{r_{1}r_{2}}-1)],\\ f_{23}&=& 12 c_{3} Gr \kappa {r_{1}^{2}} {r_{2}^{2}} x_{2} x_{4} [{r_{2}^{2}} (4 \log{r_{1}}-3 \log{r_{2}})-4 {r_{1}^{2}} (\log{r_{1}}-1) \log{r_{2}}],\\ f_{24}&=& -12 c_{3} Gr \kappa {r_{2}^{4}} x_{2} x_{4} [4 {r_{1}^{2}} \log{\frac{r_{1}}{r_{2}}} \log{r_{2}}+{r_{2}^{2}} \log{r_{1}}],\\ f_{25}&=&192 \kappa ({r_{1}^{2}}-{r_{2}^{2}}) x_{1} x_{4} [{r_{1}^{2}} (\log{\frac{r_{1}}{r_{2}}}-1)+{r_{2}^{2}}(\log{\frac{r_{1}}{r_{2}}}+1)],\\ c_{6}&=&-\frac{1}{f_{25}}(f_{10}+f_{11}+f_{12}+f_{13}+f_{14}+f_{15}+f_{16}+f_{17}+f_{18}\\ &+&f_{19}+f_{20}+f_{21}+f_{22}+f_{23}+f_{24}),\\ f_{26}&=&\frac{1}{8 x_{1}}({r_{1}^{4}}-{r_{2}^{4}}),\\ f_{27}&=&192 c_{1} \kappa r_{1} U_{hs} x_{4} [ {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{1}^{2}}\right)-1] +384 i c_{2} U_{hs} x_{4} Y_{1}(-i \kappa r_{1})-Gr \kappa {r_{1}^{5}} x_{2} (S x_{3}+\chi),\\ f_{28}&=& 6 \kappa r_{1} x_{4} [Gr {r_{1}^{2}} x_{2} (4 c_{3} \log{r_{1}}-5c_{3}+4c_{4})-16 x_{1} (2c_{5} \log{r_{1}}-c_{5}+2c_{6})],\\ f_{29}&=& 192 c_{1} \kappa r_{2} U_{hs} x_{4} [ {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{2}^{2}}\right)-1] +384 i c_{2} U_{hs} x_{4} Y_{1}(-i \kappa r_{2})-Gr \kappa {r_{2}^{5}} x_{2} (S x_{3}+\chi),\\ f_{30}&=& 6 \kappa r_{2} x_{4} [Gr {r_{2}^{2}} x_{2}(4 c_{3} \log{r_{2}}-5c_{3}+4c_{4})-16 x_{1}(2 c_{5} \log{r_{2}}-c_{5}+2 c_{6})],\\ f_{31}&=&192 \kappa x_{1} x_{4},\\ f_{32}&=&\frac{1}{384 \kappa x_{1} x_{4}},\\ f_{33}&=& 16 i c_{2} r_{2} U Y_{1}(-i \kappa r_{2})-\kappa {r_{2}^{4}}\left(\frac{dp}{dz}\right),\\ f_{34}&=& 4\kappa {r_{2}^{2}}[2 c_{1} U_{hs} \{ {{}_{0}}\tilde{F}_{1}\left(;2;\frac{1}{4} \kappa^{2} {r_{2}^{2}}\right)-1\}+x_{1} (-2 c_{5} \log{r_{2}}+c_{5}-2c_{6})],\\ f_{35}&=& Gr \kappa x_{2} [6 {r_{2}^{4}} x_{4}(4 c_{3} \log{r_{2}}-5c_{3}+4c_{4})-{r_{2}^{6}}(S x_{3}+\chi)] \end{array}$$

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Das, S., Karmakar, P. & Ali, A. Electrothermal blood streaming conveying hybridized nanoparticles in a non-uniform endoscopic conduit. Med Biol Eng Comput 60, 3125–3151 (2022). https://doi.org/10.1007/s11517-022-02650-9

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