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# Unsteady Flow and Heat Transfer of a Casson Micropolar Nanofluid over a Curved Stretching/Shrinking Surface

1 Department of Mathematics, DCC-KFUPM, Dhahran, 31261, Saudi Arabia

2 Interdisciplinary Research Center for Hydrogen and Energy Storage, KFUPM, Dhahran, 31261, Saudi Arabia

3 Department of Mathematics, Riphah International University, Faisalabad Campus, Faisalabad, 38000, Pakistan

4 Mechanical Engineering Department, King Fahd University of Petroleum and Minerals, Dhahran, 31261, Saudi Arabia

5 Department of Mathematics, AIR University, Islamabad, 44000, Pakistan

* Corresponding Author: Muhammad A. Sadiq. Email:

(This article belongs to the Special Issue: Electro- magnetohydrodynamic Nanoliquid Flow and Heat Transfer)

*Fluid Dynamics & Materials Processing* **2023**, *19*(2), 471-486. https://doi.org/10.32604/fdmp.2022.021133

**Received** 29 December 2021; **Accepted** 07 April 2022; **Issue published** 29 August 2022

## Abstract

We present the results of an investigation into the behavior of the unsteady flow of a Casson Micropolar nanofluid over a shrinking/stretching curved surface, together with a heat transfer analysis of the same problem. The body force acting perpendicular to the surface wall is in charge of regulating the fluid flow rate. Curvilinear coordinates are used to account for the considered curved geometry and a set of balance equations for mass, momentum, energy and concentration is obtained accordingly. These are turned into ordinary differential equations using a similarity transformation. We show that these equations have dual solutions for a number of different combinations of various parameters. The stability of such solutions is investigated by applying perturbations on the steady states. It is found that high values of the Micropolar and Casson parameters cause the flow to move more slowly. However, when compared to a shrunken surface, a stretched surface produces a greater Micro-rotation flux.## Keywords

Nomenclature

| Micropolar parameter |

| Suction/injection parameter |

| Wall temperature |

| Non dimensional parameter |

| Modified Hartman number |

| Reynolds number |

| Vertex viscosity |

| Micro-gyration |

| Heat capacity of fluid |

| Angular velocity components |

| Arc length |

| Velocity components |

| Brownian motion parameter |

| Curvature parameter |

| Wall shear stress |

| Velocity vector r-dircetion |

| Eckert number |

| Cassan fluid parameter |

| Reynolds number |

| Sherwood number |

| Lewis number |

| Thermophoresis parameter |

| Prandtl number |

| Micro-gyration |

| Radius of curvature |

| Stretching parameter |

| Fluid density |

| Dimensionless parameter |

| Viscosity of kinematic |

| Thermal diffusivity |

| Ratio between heat capacity and base fluid |

T(K) | Temperature |

| Dynamic viscosity |

| Wall temperature |

| Ambient temperature |

| Raduis of curvature |

COVID-19 has altered our way of life, causing us to become more aware of the limitations that we as humans confront. Scientists and clinicians around the world are scrambling to figure out what is causing the epidemic of the COVID-19 virus and what they can do to stop it. Scientists have concluded, as a result of recent investigations, that nanotechnology can be used to address a wide range of clinical difficulties, including the Coronavirus pandemic [1]. Nanotechnology has the potential to be used to prevent and identify diseases in their early stages. The nanoparticles, when introduced into human immune system, have the potential to target diseases at the cellular level. Nanoparticles have the extra advantage of delivering molecular adjuvants for loaded antigens, which can improve the efficacy and safety of a vaccine while also increasing its efficacy. In order to target delivery at the cellular level, a large number of vaccines are being produced on the basis of nanoparticles (Lipid nanoparticles). The BioNTech/Pfizer and Moderna mRNA Corona virus vaccines, for example, make use of Lipid nanoparticles to deliver treatments more efficiently to the patient. Aside from that, face masks constructed of nanomaterials are more capable of providing efficient air filtering and can also be reused for a longer period of time, giving them an added edge in overcoming the shortage of high-quality masks.

Nanotechnology operates at the nanometric scale, and as a result, it is the study of a wide range of systems and technologies that operate at this scale. Nanofluids, which are based on nanomaterials, are becoming increasingly used in a variety of industrial and technical operations. Yoo et al. [2] were the first to propose the concept of nanofluids in the year 1995, and since then, nanofluids have become a popular topic of discussion among scientists. Yoo et al. [2] investigated the prospect of increasing energy exchange among fluids by incorporating various nanoparticles into the mix. Fetecau et al. [3] developed a precise solution for the flow of nanoliquids by employing a fractional model. Meanwhile, Khan et al. [4] presented the challenge of thin film electrically guided nanoliquids sprayed over a stretching cylinder in their paper Tinny film electrically steered nanoliquids sprayed over a stretching cylinder in their paper. A study conducted by Mekheimer et al. [5] using gyrotactic suspended nanoparticles and micro organisms to investigate the discharge of Prandtl fluid flow by utilizing chemical reaction, radiation, and magnetic field effects has just been published. Meanwhile, Ahmed et al. [6] investigated the Fa lkner-Skan problem with double stratification in the flow of nanofluids by employing single/multiple wall carbon nanotubes in the flow of single/multiple wall carbon nanotubes [7]. We out a comparative investigation of ethylene glycol-based nanofluid flows, employing electro-osmotic and peristaltic pumping techniques. To examine Hybrid nanoliquid slip flows, Wahid et al. [8] used an exponentially stretching/shrinking permeable sheet that was stretched and shrunk exponentially. Because of the increasing demand for nanoliquid flows in numerous fields of research and development, we find a wealth of studies on nanoliquid flows conducted by a large number of other researchers [9,10].

Micropolar fluids are a class of non-Newtonian fluids in which we are interested in the micro-motion of fluid particles and are therefore named as such. Eringen [11] was the first to propose the concept of micro components in fluids, back in 1966. The formation of a boundary layer of micro-structured liquids, on the other hand, was predicted by Willson [12]. With the use of Lubrication approximation theory, Asghar et al. [13] were able to obtain a reduced version of the flow equation to represent Micropolar slime. In the contemporary age, Abbas et al. [14] investigated the prospect of increasing energy transformation among Micro-rotational nanoliquids by employing the Ota, Yamada, and Xue models of hybrid nanoliquids, which were developed by Ota, Yamada, and Xue. For their part, Ismail et al. [15] used generated magnetic field effects to analyze the flow of micro-structured fluids while conducting their experiments. With the help of a magnetic curved surface, Abbas et al. [16] investigated the unsteady flow of Micropolar fluid flows. Raza et al. [17] discovered dual solutions in their investigation of Micropolar fluid flows utilizing thermal radiations, which was published just a few months ago.

Casson fluid is yet another essential non-Newtonian liquid that is becoming increasingly important in our daily lives, according to the National Institute of Standards and Technology. Casson fluids include a variety of sauces, jellies, and soups, amongst other things. Casson [18] was the first to derive the constitutive equations for Casson fluid and to illustrate the properties of various polymers. He published his results in 1959. McDonald [19] pointed out in 1974 that the flow of blood is a good representation of the Casson fluid model. Under-discussed fluid classes find use in a diverse range of fields including medical, biology, the food industry, and several sorts of drilling procedures, just to name a few. Because of the wide range of applications for which this essential class of fluids is used, many researchers keep a close eye on it in their laboratories. Through the use of the homotopy approach, Nadeem et al. [20] found the optimal solutions of Casson nanoliquid flows. The authors of another paper [21] concluded that skin friction along the wall is lower in Newtonian fluids than in non-Newtonian Casson-nanofluids when comparing the two types of fluids. When it comes to the flow of Casson nanoliquids, Mustafa et al. [22] used general power law velocity dispersal to analyze the phenomenon. Sarkar et al. [23] investigated the evolution of Casson nanoliquids in the aggregation of wedge angle and melting processes, respectively. In a similar vein, Ibrar et al. [24] investigated the flow of Casson nanoliquids with magnetic current using single and multiple wall carbon nanotubes, respectively. Nayak et al. [25] used entangled motile gyrotactic micro-creatures to examine the flow of Casson nanoliquids utilizing chemical processes in order to better understand their behavior. Several researchers, including Khan et al. [26], have investigated the possibility of a dual solution in the evolution of Casson fluid flows across a Stretching/Shrinking sheet.

We believe that unsteady fluid mix is appropriate based on the literature research and to the best of our knowledge. Nanofluids flows across a curved Stretching/Shrinking surface using the Micropolar Casson-Buongiorno model have not been investigated previously. Based on the findings of the studies given in [27,28], we determined that it was reasonable to unleash the dual solution phenomena utilizing the fluid flows under consideration. Stability testing will be carried out in order to better understand and identify the most appropriate solutions that will be physically feasible. To achieve this goal, we will introduce a form of exponential function into our steady state system to represent perturbation to it. This results in the stable situation being turned into an eigen value problem, from which acceptable eigen values are selected and noted for future reference.

Consider the case of a liquid mixture. As illustrated in Fig. 1, a Casson Micropolar nanofluid is discharged across a bent stretching/shrinking surface that has been wrapped in a circle of radius R. For our two-dimensional frame of reference

When

Eqs. (1)–(4) represent velocity and angular velocity profile, Eqs. (5) and (6) represent temperature profile and concentration of nano particles.

To simplify the above equations, we will use these transformations:

After solving Eqs. (2)–(6) we get

The boundary conditions for above flow problem are:

Moreover, some of the important physical measures are Skin friction coefficient

where,

Moreover, the dimensionless form these measures are:

where

Under specified parametric combinations, the numerical simulation of Eqs. (9)–(13) yields dual solutions to the equations. It is therefore essential to choose the most appropriate solution that is both realistic and viable. The stability analysis will be conducted in accordance with the methodologies established by the authors Weidman et al. [27] and Rosca et al. [28], respectively. In order to accomplish this, we establish another variable

Simplifying Eqs. (3)–(6) using transforming variables from (17) we have

Subject to boundary conditions

Also, when

We have steady solution of the system of Eqs. (9)–(12) with boundary condition (13), in the form

We assume the following variables to generate the perturbation:

Here functions

and the corresponding boundary conditions are

For

Keeping in view the work done by authors in [27,28], we investigate the steady solutions

The boundary conditions are as follows:

For

As per findings of authors Weidman et al. [27] and Rosca et al. [28], the stability analysis will give smallest values for

4 Discussion on Numerical Solutions

We will now investigate impacts of various embedded parameters on different profiles.

Velocity Profile

Adding higher values of the material parameter K for second solution causes the micro-rotational profile

This is seen in Fig. 10, which illustrates the lower temperature profile of a bent channel. It is because we decreased the surface area with the fluid when we raised K*, and this resulted in a drop in liquid temperature. Thermophoresis aids in increasing the thermal flux in both solutions, as seen in Figs. 11 and 12. To put it another way: Large values of the parameter

For both solutions, large values of parameter

We also compare our present values of

Some parametric options have been shown to have dual solutions in previous sections, as demonstrated by numerical simulations of Eqs. (9)–(13). For this reason, we used a numerical eigenvalue system of Eqs. (29)–(33) to determine the best solution. For positive lowest eigen values, we noticed that our solutions show an initial deterioration. Furthermore, we found that the solutions remained unstable when the eigen values were negative. Table 2 shows the least eigen values that were identified as a result of these solutions. Our findings show that the first options are more feasible than the second ones. According to [27,28], there were similar findings.

The performance of the Casson Micropolar nanoliquid flow mixer and energy transfer were examined in this study. We discovered that for some parametric values, our equations yield two solutions. As a result, we needed to do a stability analysis in order to select the best solution. Our steady state system was perturbed by exponential functions. Because exponential functions converge more quickly than some other function, this is why they are used. It was easy for us to identify the proper eigenvalues because they agreed so well with our possible solutions. The MATLAB solver bvp4c has stopped working.

We arrived at the following key observations:

• We witnessed that the profile

• The profile

• The profile

• For second solution, the function

• The profile

• The function

Acknowledgement: Authors are thanks to KFUPM for providing adequate resources for this research.

Funding Statement: The authors received no specific funding for this study.

Conflicts of Interest: The authors declare that they have no conflicts of interest to report regarding the present study.

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*Fluid Dyn. Mater. Proc.*, vol. 19, no. 2, pp. 471-486. 2023. https://doi.org/10.32604/fdmp.2022.021133

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