Description of viscous dissipation in magnetohydrodynamic flow of nanofluid: Applications of biomedical treatment

Introduction

The saturation of nanoparticles into base fluids develops the nanofluids. The nanofluids acts as effective coolant media in diverse industrial and technological devices in view of the fact that they have well-established characteristics of improving heat transfer rates. Therefore, flow of nanomaterials is very useful in different processes such as heat exchanger, cooling of electronic devices, hybrid power engine, and fuel cells. Nanofluids are also very significant in biomedical treatments such as in cancer therapy, magnetic nanoparticles are used. Magnetic particles, such as polystyrene, amino, carboxyl, polystyrene cross-linked particles, and epoxy and aldehyde magnetic particles, are used for burning cancer cells, in controllable deployment of particle degradation, in biological tags for quantifiable recognition, in development of chemical and biosensors, etc. Choi ¹ inaugurated the work considering the types of fluids. After that, many researchers deliberated the idea of flow with heat transfer phenomenon with various other nanofluids. Ibrahim ² disclosed the aspect of melting in hydromagnetic stagnant nanomaterial flow through stretched plate. Balla et al. ³ exhibited heat transport features in magnetohydrodynamic (MHD) nanoliquid flow via inclined porous cavity. Mixed convection impacts on the flow of stagnation nanofluid over a vertically held stretchable plate are discussed by Othman et al. ⁴ Hydromagnetic flow of radiative nanoliquid caused by stretched sheet is reported by Ganga et al. ⁵ Yin et al. ⁶ studied the heat transport characteristics in nanoliquid flow deformed by rotating stretchable disk. Dogonchi and Ganji ⁷ discussed the characteristics of modified fluxes in radiative nanofluid flow between parallel surfaces considering magnetic effects. Reddy et al. ⁸ explored the MHD radiative nanofluid flow through inclined porous sheet considering heat generation (or absorption). Their investigations motivated few other researchers to work on nanofluids in different conditions.^9–17

Difference of temperature among two distinct types of bodies causes heat transfer phenomenon. Transportation of heat and mass plays an impactful role in crystals growth, formation of polyethylene and papers, cooling of metallic sheet in the cooling bath, cooling of nuclear reactors, castings of metals, latent heat storage, and biomedical aspects includes drug targeting, conduction of heat in tissues, and many others. Fourier ¹⁸ and later on Fick ¹⁹ were initiated to explore the transfer processes of heat and mass, respectively. Their work shows that both energy and concentration profiles are parabolic in nature. Afterward, modification is made by Cattaneo ²⁰ in Fourier’s law in order to add thermal relaxation time factor so that the heat is transferred in the thermal wave form with finite speed. Subsequently, Christov ²¹ modified Cattaneo’s work by considering Oldroyd’s upper-convected derivative model. Stretching flow through a sheet with varying thicknesses considering Cattaneo and Christov theory is discussed by Hayat et al.^22,23 They also discussed the Burgers nanofluid flow considering Cattaneo and Christov dual diffusive models. Nadeem et al. ²⁴ disclosed the characteristics of modified fluxes in viscoelastic fluid with Newtonian heating. Hayat et al. ²⁵ reported thermally stratified flow via non-Fourier heat flux over a stretchable sheet. Influence of modified heat flux in stratified flow through porous media is illustrated by Nadeem and Muhammad. ²⁶ Anjum et al. ²⁷ exposed the properties of second-grade flow due to Riga plate. Sui et al. ²⁸ explored the combined impacts of velocity slip and Cattaneo–Christove double diffusion in the Maxwell nanomaterial past through stretchable sheet. Characteristics of variable physical properties via modified Fourier’ law in Burgers liquid flow is described by Waqas et al. ²⁹ Rana and Nawaz ³⁰ investigated the heat transport features of Sutterby nanofluid flow using modified heat flux. Few recent analyses on Cattaneo–Christov model can be found in the literature.^31–35

From the literature survey, it is revealed that most of the studies considering nanofluid flow with Cattaneo–Christov double diffusive model are not corrected mathematically and physically. Because some extra terms related to Brownian motion and thermophoresis effects appear under the theory of Cattaneo–Christov, which are missing in the literature. Here, our main focus is to cover such analysis in order to optimize the mathematical data with real situations. Moreover, viscous dissipation phenomenon is incorporated with Cattaneo–Christov model for the first time. The study of MHD nanofluid flow with the phenomena of Brownian diffusion and thermophoresis is also performed. First, the problem is modeled using similarity transformations and then the analytical solutions of reduced flow equations through homotopic technique are obtained.^36–40 The figures are sketched to depict the behavior of resulting non-dimensional expressions. The values of drag force (skin friction coefficient) are acquired for involved non-dimensional parameters.

Problem formulation

Consider two-dimensional and steady-state flow of nanofluid passing through a sheet. Stretching sheet with linear velocity U w ( x ) is considered. The axes x and y are considered along the stretched wall and vertical to it. The strength B 0 of magnetic field is implemented so that the magnetic Reynolds number is assumed to be small. The expressions of energy and concentration are modeled utilizing non-conventional fluxes model. Temperature is supposed to be unchanged at the wall surface and ambient fluid. The principles of mass, momentum, energy, and concentration yield ³⁴

∂ u ∂ x + ∂ v ∂ y = 0

(1)

u ∂ u ∂ x + v ∂ u ∂ y = v f ∂ 2 u ∂ y 2 − σ ∗ ρ f B 0 2 u

(2)

( ρ C ) f d T d t − ( ρ C ) p [ D B ∇ C ⋅ ∇ T + D T T ∞ ( ∇ T ) 2 ] = − ∇ ⋅ q +τ T ⋅ L

(3)

d C d t − D T T ∞ ∇ 2 T = − ∇ ⋅ J

(4)

Here, u and v represent the velocity components in x and y directions, respectively; ( ρ C ) p and ( ρ C ) f depict the heat capacity of nanoparticles and nanofluid, respectively; v f and ρ f represent the kinematic viscosity and fluid density, respectively; σ ∗ represents the electrical conductivity of fluid; T ∞ and its ambient temperature T represent the upper wall and fluid temperatures, respectively; C represents the concentration; and D B and D T represent Brownian diffusion and thermophoresis coefficients, respectively.

The heat and mass fluxes models of Cattaneo–Christov are mathematically given by ³⁵

q + δ E ( ∂ q ∂ t + v ⋅ ∇ q + ( ∇ ⋅ v ) q − q ⋅ ∇ v ) = − k ∇ T

(5)

J + δ C ( ∂ J ∂ t + v ⋅ ∇ J + ( ∇ ⋅ v ) J − J ⋅ ∇ v ) = − D B ∇ C

(6)

In case of steady and incompressible flow, Cattaneo–Christov fluid model for thermal and solutal fluxes is described as

q + δ E ( v ⋅ ∇ q − q ⋅ ∇ v ) = − k ∇ T

(7)

J + δ C ( v ⋅ ∇ J − J ⋅ ∇ v ) = − D B ∇ C

(8)

Here, D B represents the mass diffusivity and k represents the thermal conductivity.

Implementing expressions (7) and (8) in expressions (3) and (4) and after utilizing boundary layer approximation, governing equations become

u ∂ T ∂ x + v ∂ T ∂ y + δ E ( u ∂ u ∂ x ∂ T ∂ x + v ∂ v ∂ y ∂ T ∂ y + u 2 ∂ 2 T ∂ x 2 + v 2 ∂ 2 T ∂ y 2 + 2 u v ∂ 2 T ∂ x ∂ y + u ∂ v ∂ x ∂ T ∂ y + v ∂ u ∂ y ∂ T ∂ x ) − τ 1 D B δ E ( u ∂ C ∂ y ∂ 2 T ∂ x ∂ y + u ∂ T ∂ y ∂ C ∂ x ∂ y + v ∂ C ∂ y ∂ 2 T ∂ y 2 + v ∂ T ∂ y ∂ 2 C ∂ y 2 ) + 2 μ ρ C p ( ∂ u ∂ y ) 2 − 2 τ 1 D T T ∞ δ E ( u ∂ T ∂ y ∂ 2 T ∂ x ∂ y + v ∂ T ∂ y ∂ 2 T ∂ y 2 ) + 2 μ δ E ( u ∂ 2 v ∂ x 2 + v ∂ 2 u ∂ y 2 ) = k ρ C p ( ∂ 2 T ∂ y 2 ) + τ 1 D B ( ∂ T ∂ y ∂ C ∂ y ) + τ 1 D T T ∞ ( ( ∂ T ∂ y ) 2 )

(9)

u ∂ C ∂ x + v ∂ C ∂ y + δ C ( ∂ u ∂ x ∂ C ∂ x + v ∂ v ∂ y ∂ C ∂ y + u 2 ∂ 2 C ∂ x 2 + v 2 ∂ 2 C ∂ y 2 + 2 u v ∂ 2 C ∂ x ∂ y + u ∂ v ∂ x ∂ C ∂ y + v ∂ u ∂ y ∂ C ∂ x ) − D T T ∞ δ C ( u ∂ 3 T ∂ x ∂ y 2 + v ∂ 3 T ∂ y 3 ) = D B ( ∂ 2 C ∂ y 2 ) + D T T ∞ ( ∂ 2 T ∂ y 2 )

(10)

corresponding to the conditions at boundary

u = U w ( x ) = a x , v = 0 , T = T w , C = C w at y = 0

(11)

u → 0 , T → T ∞ , C → C ∞ at y → ∞

(12)

Here, T w and T ∞ represent the wall and ambient fluid temperatures, respectively; C w and C ∞ represent the wall and ambient fluid concentrations, respectively; and τ 1 represents the ratio of capacity of nanoparticles and nanofluid.

Using non-dimensional variables

u = a x f ′ ( η ) , v = − a ν f ( η ) , η = a ν y , θ ( η ) = T − T ∞ T w − T ∞ , Φ ( η ) = C − C ∞ C w − C ∞

(13)

Continuity equation vanishes identically, whereas other governing equations are

f ‴ + f f ″ − ( f ′ ) 2 − M f ′ = 0

(14)

θ ″ + Pr E c f ′ ′ 2 + Pr ( N b θ ′ Φ ′ + N t ( θ ′ ) 2 ) + Pr f θ ′ − Pr β e ( f f ′ θ ′ + f 2 θ ″ ) − Pr β e N b ( f θ ″ Φ ′ + f θ ′ Φ ″ ) − 2 β e N t f θ ′ θ ″ − 2 Pr β e E c ( f ′ f ″ 2 − f f ″ f ‴ ) = 0

(15)

Φ ″ + Pr L e f Φ ′ + ( N t N b ) θ ″ − Pr L e β c ( f f ′ Φ ′ + f 2 Φ ″ ) − β c ( N t N b ) f θ ‴ = 0

(16)

f ′ ( 0 ) = 1 , f ( 0 ) = 0 , f ′ ( ∞ ) = 0

(17)

θ ( 0 ) = 1 , θ ( ∞ ) = 0

(18)

Φ ( 0 ) = 1 , Φ ( ∞ ) = 0

(19)

Here, M is the Hartman number; β e and β c are the thermal and solutal relaxation time parameters, respectively; Pr is the Prandtl number; L e is the Lewis number; N t and N b are the thermophoresis and Brownian diffusion parameters, respectively; and E c is the Eckert number and are mathematically defined as follows

M = σ ∗ B 0 2 ρ f a , Pr = v α , β e = a δ E , β c = a δ C , L e = α D B N t = τ D T ( T w − T ∞ ) v T ∞ , N b = τ D B ( C w − C ∞ ) v , E c = u w 2 C p ( T w − T ∞ )

(20)

Mathematical expression for skin friction is

C f = τ w ρ U w 2

(21)

Non-dimensional form is given as

C f R e x 1 / 2 = f ″ ( 0 )

(22)

Here, R e x = U w ( x ) x / ν is the Reynolds number.

Homotopic solutions

The homotopic technique is established on the basic concept of topology known as homotopy. This method was first developed by Liao ³⁶ in 1992, in order to determine the solutions of highly non-linear equations. It has prominent features as compared to other methods, that is (1) it is independent of large or small parameters, (2) it ensures the convergence of homotopic solutions, and (3) it gives us considerable freedom in order to choose the linear operators and base functions. To initiate with this method, it is significant to have linear operators and initial guesses, which are given below

f 0 ( η ) = ( 1 − exp ⁡ ( − η ) )

(23)

θ 0 ( η ) = exp ⁡ ( − η )

(24)

Φ 0 ( η ) = exp ⁡ ( − η )

(25)

L f ( f ) = d 3 f d η 3 − d f d η , L θ ( θ ) = d 2 θ d η 2 − θ , L Φ ( Φ ) = d 2 Φ d η 2 − Φ

(26)

L f [ C 1 + C 2 exp ⁡ ( η ) + C 3 exp ⁡ ( − η ) ] = 0

(27)

L θ [ C 4 exp ⁡ ( η ) + C 5 exp ⁡ ( − η ) ] = 0

(28)

L Φ [ C 6 exp ⁡ ( η ) + C 7 exp ⁡ ( − η ) ] = 0

(29)

Here, C i ( i = 1 , … , 7 ) denotes the arbitrary constants.

Zeroth-order problem

( 1 − p ) L f [ f ⌢ ( η ; p ) − f 0 ( η ) ] = p ℏ f N f [ f ⌢ ( η ; p ) ]

(30)

( 1 − p ) L θ [ θ ⌢ ( η ; p ) − θ 0 ( η ) ] = p ℏ θ N θ [ θ ⌢ ( η ; p ) ]

(31)

( 1 − p ) L Φ [ Φ ⌢ ( η ; p ) − Φ 0 ( η ) ] = p ℏ Φ N Φ [ Φ ⌢ ( η ; p ) ]

(32)

f ⌢ ( 0 ; p ) = 0 , f ⌢ ′ ( 0 ; p ) = 1 , f ⌢ ′ ( ∞ ; p ) = 0

(33)

θ ⌢ ( 0 ; p ) = 1 , θ ⌢ ( ∞ ; p ) = 0

(34)

Φ ⌢ ( 0 ; p ) = 1 , Φ ⌢ ( ∞ ; p ) = 0

(35)

Non-linear operators are

N f [ f ⌢ ( η , p ) ] = ∂ 3 f ⌢ ( η ; p ) ∂ η 3 + f ⌢ ( η ; p ) ∂ 2 f ⌢ ( η ; p ) ∂ η 2 − ( ∂ f ⌢ ( η ; p ) ∂ η ) 2 − M ∂ f ⌢ ( η ; p ) ∂ η

(36)

N θ [ θ ⌢ ( η ; p ) ] = ∂ 2 θ ⌢ ( η , p ) ∂ η 2 + Pr E c ( ∂ 2 f ⌢ ( η ; p ) ∂ η 2 ) 2 + Pr f ⌢ ( η ; p ) ∂ θ ⌢ ( η , p ) ∂ η + Pr ( N b ∂ θ ⌢ ( η , p ) ∂ η ∂ Φ ⌢ ( η , p ) ∂ η + N t ( ∂ θ ⌢ ( η ; p ) ∂ η ) 2 ) − Pr β e ( f ⌢ ( η ; p ) ∂ f ⌢ ( η ; p ) ∂ η ∂ θ ⌢ ( η ; p ) ∂ η ) − Pr β e ( ( f ⌢ ( η ; p ) ) 2 ∂ 2 θ ⌢ ( η ; p ) ∂ η 2 ) − Pr β e N b ( f ⌢ ( η ; p ) ∂ 2 θ ⌢ ( η ; p ) ∂ η 2 ∂ Φ ⌢ ( η ; p ) ∂ η ) − Pr β e N b ( f ⌢ ( η ; p ) ∂ θ ⌢ ( η ; p ) ∂ η ∂ 2 Φ ⌢ ( η ; p ) ∂ η ) − 2 β e N t ( f ⌢ ( η ; p ) ∂ θ ⌢ ( η ; p ) ∂ η ∂ 2 θ ⌢ ( η ; p ) ∂ η ) − 2 Pr β e E c ( ∂ f ⌢ ( η ; p ) ∂ η ( ∂ 2 f ⌢ ( η ; p ) ∂ η 2 ) 2 ) − 2 Pr β e E c ( f ⌢ ( η ; p ) ∂ f ⌢ ( η ; p ) ∂ η ∂ 3 f ⌢ ( η ; p ) ∂ η 3 )

(37)

N Φ [ Φ ⌢ ( η ; p ) ] = ∂ 2 Φ ⌢ ( η , p ) ∂ η 2 + Pr L e f ⌢ ( η ; p ) ∂ Φ ⌢ ( η ; p ) ∂ η + ( N t N b ) ∂ 2 θ ⌢ ( η , p ) ∂ η 2 − Pr L e β c ( f ⌢ ( η ; p ) ∂ f ⌢ ( η ; p ) ∂ η ∂ Φ ⌢ ( η ; p ) ∂ η ) − Pr L e β c ( f ⌢ 2 ( η ; p ) ∂ 2 Φ ⌢ ( η ; p ) ∂ η 2 ) − β c ( N t N b ) f ⌢ ( η ; p ) ∂ 3 θ ⌢ ( η , p ) ∂ η 3

(38)

where p ∈ [ 0 , 1 ] is the embedding parameter and ℏ f , ℏ θ , and ℏ Φ are the non-zero auxiliary parameters.

mth-order problem

L f [ f m ( η ) − χ m f m − 1 ( η ) ] = ℏ f R m f ( η )

(39)

L θ [ θ m ( η ) − χ m θ m − 1 ( η ) ] = ℏ θ R m θ ( η )

(40)

L Φ [ Φ m ( η ) − χ m Φ m − 1 ( η ) ] = ℏ Φ R m Φ ( η )

(41)

f m ( 0 ) = f ′ m ( 0 ) = f ′ m ( ∞ ) = 0

(42)

θ m ( 0 ) = θ m ( ∞ ) = 0

(43)

Φ m ( 0 ) = Φ m ( ∞ ) = 0

(44)

R m f ( η ) = f ‴ m − 1 ( η ) + ∑ k = 0 m − 1 f m − 1 − k f k ′ ′ − ∑ k = 0 m − 1 f ′ m − 1 − k f ′ k − M f ′ m − 1

(45)

R m θ ( η ) = θ ″ m − 1 + Pr E c ∑ k = 0 m − 1 f ″ m − 1 − k f ″ k + Pr ∑ k = 0 m − 1 f m − 1 − k θ ′ k + Pr ( N b ∑ k = 0 m − 1 θ ′ m − 1 − k Φ ′ k + N t ∑ k = 0 m − 1 θ ′ m − 1 − k θ ′ k ) − Pr β e ( ∑ k = 0 m − 1 f m − 1 − k f ′ m − 1 − k θ ′ k + ∑ k = 0 m − 1 f m − 1 − k f m − 1 − k θ ″ k ) − Pr β e N b ( ∑ k = 0 m − 1 f m − 1 − k θ ″ m − 1 − k Φ ′ k + ∑ k = 0 m − 1 f m − 1 − k θ ′ m − 1 − k Φ ″ k ) − 2 Pr β e E c ( ∑ k = 0 m − 1 f ′ m − 1 − k f ″ m − 1 − k f ″ k + ∑ k = 0 m − 1 f m − 1 − k f ″ m − 1 − k f ‴ k ) − 2 β e N t ∑ k = 0 m − 1 f m − 1 − k θ ′ m − 1 − k θ ″ k

(46)

R m Φ ( η ) = Φ ″ m − 1 + Pr L e ∑ k = 0 m − 1 f m − 1 − k Φ ′ k + ( N t N b ) θ ″ m − 1 − Pr L e β c ( ∑ k = 0 m − 1 f m − 1 − k f ′ m − 1 − k Φ ′ k + ∑ k = 0 m − 1 f m − 1 − k f m − 1 − k Φ ″ k ) − β c ( N t N b ) ∑ k = 0 m − 1 f m − 1 − k θ ‴ k

(47)

χ m = { 0 , m ≤ 1 1 , m > 1

(48)

For p = 0 and p = 1 , we can write

f ⌢ ( η ; 0 ) = f 0 ( η ) , f ⌢ ( η ; 1 ) = f ( η )

(49)

θ ⌢ ( η ; 0 ) = θ 0 ( η ) , θ ⌢ ( η ; 1 ) = θ ( η )

(50)

Φ ⌢ ( η ; 0 ) = Φ 0 ( η ) , Φ ⌢ ( η ; 1 ) = Φ ( η )

(51)

and with the variation of p from 0 to 1 , f ⌢ ( η ; p ) , θ ⌢ ( η ; p ) , and Φ ⌢ ( η ; p ) vary from the initial solutions f 0 ( η ) , θ 0 ( η ) , and Φ 0 ( η ) to final solutions f ( η ) , θ ( η ) , and Φ ( η ) , respectively. By Taylor’s series, we have

f ⌢ ( η ; p ) = f 0 ( η ) + ∑ m = 1 ∞ f m ( η ) p m , f m ( η ) = 1 m ! ∂ m f ⌢ ( η ; p ) ∂ p m | p = 0

(52)

θ ⌢ ( η ; p ) = θ 0 ( η ) + ∑ m = 1 ∞ θ m ( η ) p m , θ m ( η ) = 1 m ! ∂ m θ ⌢ ( η ; p ) ∂ p m | p = 0

(53)

Φ ⌢ ( η ; p ) = Φ 0 ( η ) + ∑ m = 1 ∞ Φ m ( η ) p m , Φ m ( η ) = 1 m ! ∂ m Φ ⌢ ( η ; p ) ∂ p m | p = 0

(54)

The value of auxiliary parameter is selected so properly that the series converge at p = 1 , that is

f ( η ) = f 0 ( η ) + ∑ m = 1 ∞ f m ( η )

(55)

θ ( η ) = θ 0 ( η ) + ∑ m = 1 ∞ θ m ( η )

(56)

Φ ( η ) = Φ 0 ( η ) + ∑ m = 1 ∞ Φ m ( η )

(57)

In general, analytical solutions are

f m ( η ) = f m ∗ ( η ) + C 1 + C 2 e η + C 3 e − η

(58)

θ m ( η ) = θ m ∗ ( η ) + C 4 e η + C 5 e − η

(59)

Φ m ( η ) = Φ m ∗ ( η ) + C 6 e η + C 7 e − η

(60)

in which ( f m ∗ , θ m ∗ , Φ m ∗ ( η ) ) are special solutions.

Convergence analysis

Homotopic analysis method (HAM) ensures the convergence of iterative solutions which relies over an auxiliary parameters ℏ f , ℏ θ , and ℏ Φ . The relevant ℏ -curves are sketched in Figures 1–3 for the flow, heat, and mass equations. The allowable ranges of ℏ f , ℏ θ , and ℏ Φ are − 1.6 ≤ ℏ f ≤ − 0.6 , − 1.0 ≤ ℏ θ ≤ − 0.6 , and − 1. ≤ ℏ Φ ≤ − 0.7 , respectively. Furthermore, Table 1 depicts the convergence of series solution. It is revealed that 17th order of approximation is sufficient for series solution convergence.

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Table 1.

Convergence table for Pr ⁡ = 1.2 , N b = L e = 0.8 , N t = 0.2 , E c = β e = β c = 0.1 , and M = 0. 5.

Order of approximation	− f ″ ( 0 )	− θ ′ ( 0 )	− Φ ′ ( 0 )
1	1.0500	0.5588	0.6716
4	1.0990	0.3732	0.5538
8	1.1110	0.3508	0.5201
10	1.1130	0.3477	0.5107
12	1.1140	0.3464	0.5089
15	1.1140	0.3462	0.5037
17	1.1140	0.3462	0.5037

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Figure 1.

Physical interpretation of the problem.

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Figure 2.

h -curve for f .

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Figure 3.

h -curve for θ and Φ .

Discussion

The aim of this portion is to report the graphical demonstration for diverse parameters on flow velocity, nanofluid temperature, and particles concentration. Figure 4 illustrates the velocity distribution corresponding to Hartman number M . Decaying behavior is analyzed for velocity field for escalating Hartman number M . Physically, Lorentz force increments due to higher Hartman number which resists the fluid motion and consequently velocity decays. Figure 5 represents the features of Hartman number M on temperature field. Dominating behavior is noted for larger Hartman number M . Physically, more heat produces due to the resistive force (Lorentz force). Therefore, temperature field increases. Figure 6 reflects the characteristics of temperature field corresponding to Prandtl number (Pr). Decaying behavior of temperature field is observed for higher (Pr). For lower Prandtl number, thermal boundary layer thickness dominates. Dominant Prandtl number illustrates decrement in thermal diffusivity which is responsible for small temperature distribution. Description of Eckert number E c on temperature profile is given in Figure 7. Increment in temperature profile is noted for increased Eckert number E c . Physically, increment in Eckert number generates more heat in the fluid due to high friction forces between fluid particles. Therefore, temperature distribution intensifies. Figure 8 reflects the features of Brownian diffusive parameter N b on fluid temperature. Here, we noted that temperature field increases for increased Brownian diffusive parameter N b . Because collisions of the particles enhance and consequently, kinetic energy will be increased. Therefore, temperature field rises. Figure 9 describes the behavior of Brownian diffusive parameter N b on fluids concentration. The concentration field is decaying function of Brownian parameter N b . In fact, when Brownian parameter increases, the collisions between fluid particles enhance and ensure lower mass transport phenomenon from heated sheet toward the cold fluid. Therefore, concentration field shows decreasing behavior. Behavior of thermophoresis diffusive parameter N t is described in Figure 10 for temperature field. Temperature rises for thermophoretic phenomenon because particles are pushed to cold region from heated plate, therefore, temperature field increases. Figure 11 reflects the behavior of thermophoresis diffusive parameter N t on fluid concentration. For dominant thermophoresis parameter, less nanoparticles are shifted from hot surface to cold surface. Hence, concentration distribution increases. Figure 12 explains the impact of β e on temperature profile. From Figure 12, it can be perceived that by increasing parameter β e , temperature profile shows decreasing behavior, since β e is the thermal relaxation parameter and represents in terms of thermal relaxation time. So by increasing β e , thermal relaxation time for fluid particle also increases and particles will take more time for heat transfer that is why decreasing behavior is shown by temperature field. Figure 13 shows the behavior of β c on concentration field. From Figure 13, it can be predicted that by increasing parameter β c , concentration profile shows a decreasing behavior, since β c is solutal relaxation parameter and represents in terms of solutal relaxation time. So, by increasing β c , solutal relaxation time for fluid particle also increases and particles will take more time for mass transfer that is why concentration profile shows a decreasing behavior. Behavior of Lewis number L e on fluid concentration is given in Figure 14. It is perceived that concentration distribution declines with dominant Lewis number L e . Physically, Lewis number and Brownian motion coefficient have inverse relation. So, the increase in Lewis number L e causes low Brownian coefficient which helps in reducing the concentration distribution. Table 2 depicts the behavior of skin friction coefficient for diverse values of Hartman number M . Decrement in skin friction coefficient is noticed. As Hartman number increases, resistance between particles of fluid increases and as a consequence, skin friction decreases. To validate the present results, Table 3 displays the comparison of different values of skin friction with previously published work of Mabood and Mastroberardino ⁴¹ for diverse values of M . It is revealed that the outcome gives favorable agreement.

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Figure 4.

Description of M on f ' ( η ) .

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Figure 5.

Description of M on θ ( η ) .

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Figure 6.

Description of Pr ⁡ on θ ( η ) .

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Figure 7.

Description of E c on θ ( η ) .

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Figure 8.

Description of N b on θ ( η ) .

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Figure 9.

Description of N b on Φ ( η ) .

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Figure 10.

Description of N t on θ ( η ) .

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Figure 11.

Description of N t on Φ ( η ) .

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Figure 12.

Description of β e on θ ( η ) .

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Figure 13.

Description of β c on Φ ( η ) .

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Figure 14.

Description of L e on Φ ( η )

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Table 2.

Skin friction for diverse values of Hartman number M, when Pr ⁡ = 1.2 , N b = 0.5 , N t = 0.1 , and L e = E c = β e = β c = 0.2 .

M	f ″ ( 0 )
0.0	1.0000
0.2	–1.0188
0.4	–1.0742
0.6	–1.1632

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Table 3.

Comparison of skin friction with other method for various values of M .

M	Mabood and Mastroberardino41	This study
0	1.0000	1.0000
1	–1.41421	–1.41422
5	–2.44948	–2.44949
10	–3.31662	–3.31662

Concluding remarks

In this article, we discuss the characteristics of Cattaneo–Christov heat and mass fluxes in nanoliquid, considering Brownian motion, magnetic effect, and the thermophoresis effect. It is noticed that some extra impacts of thermophoresis phenomenon and Brownian motion will appear due to Cattaneo–Christov heat and mass fluxes. The main surveying points are as follows:

Velocity profile become smaller corresponding to higher Hartman number M .

Brownian motion and thermophoresis parameters result in increment of temperature field.

Brownian parameter is the decreasing function for concentration field, whereas concentration increases for thermophoresis parameter.

Lewis number reduces the concentration field.

Thermal and solutal relaxation time parameters ( β e and β c ) are the decreasing functions for temperature and the concentration profiles, respectively.

Skin friction coefficient enhanced when Hartman number M increased.

It is desired that this study contributes as a boost for sculpting more advanced MHD nanofluid flows notably in cooling of microchips, nuclear reactors, fuels, extraction of geothermal power, microactuation process, and biomedicines. This article may be used in nanodrug delivery, hyperthermia, cancer therapeutics, nano-cryosurgery, magnetic cell separation, and magnetic resonance imaging.