2020
DOI: 10.3390/cryst10030168
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Analysis of Eyring–Powell Fluid Flow Used as a Coating Material for Wire with Variable Viscosity Effect along with Thermal Radiation and Joule Heating

Abstract: This article examines a wire coating technique that considers how viscoelastic Eyring–Powell fluid is studied with magnetohydrodynamic (MHD) flow, thermal transfer, and Joule heating effects. Temperature-dependent variable and flexible viscosity models are considered. The interface boundary layer equalities which describe flux and thermal convective phenomena are evaluated using a dominant numerical technique—the so-called Runge–Kutta 4th-order method. A permeable matrix which behaves like a dielectric to avoi… Show more

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Cited by 33 publications
(19 citation statements)
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“…Now, obtain the solutions of steady flow from (8)(9)(10)(11) as 𝑓(𝜂) = 𝑓 0 (𝜂), 𝑔(𝜂) = 𝑔 0 (𝜂), 𝜃(𝜂) = 𝜃 0 (𝜂),and ∅(𝜂) = ∅ 0 (𝜂), it is assumed { 𝑓(𝜂, 𝜏) = 𝑓 0 (𝜂) + 𝑒 −𝜀𝜏 𝐹(𝜂, 𝜏) 𝑔(𝜂, 𝜏) = 𝑔 0 (𝜂) + 𝑒 −𝜀𝜏 𝐺(𝜂, 𝜏) 𝜃(𝜂, 𝜏) = 𝜃 0 (𝜂) + 𝑒 −𝜀𝜏 𝐻(𝜂, 𝜏) ∅(𝜂, 𝜏) = ∅ 0 (𝜂) + 𝑒 −𝜀𝜏 𝐽(𝜂, 𝜏) (25) Sumera Dero (et al) where the unidentified eigenvalue is 𝜀 where its value needs to fix a stable branch. In addition, 𝐹(𝜂, 𝜏), 𝐺(𝜂, 𝜏), 𝐻(𝜂, 𝜏), and 𝐽(𝜂, 𝜏) all their derivatives are assumed small relative to 𝑓 0 (𝜂), 𝑔 0 (𝜂), 𝜃 0 (𝜂), and ∅ 0 (𝜂).…”
Section: Temporal Stability Analysismentioning
confidence: 99%
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“…Now, obtain the solutions of steady flow from (8)(9)(10)(11) as 𝑓(𝜂) = 𝑓 0 (𝜂), 𝑔(𝜂) = 𝑔 0 (𝜂), 𝜃(𝜂) = 𝜃 0 (𝜂),and ∅(𝜂) = ∅ 0 (𝜂), it is assumed { 𝑓(𝜂, 𝜏) = 𝑓 0 (𝜂) + 𝑒 −𝜀𝜏 𝐹(𝜂, 𝜏) 𝑔(𝜂, 𝜏) = 𝑔 0 (𝜂) + 𝑒 −𝜀𝜏 𝐺(𝜂, 𝜏) 𝜃(𝜂, 𝜏) = 𝜃 0 (𝜂) + 𝑒 −𝜀𝜏 𝐻(𝜂, 𝜏) ∅(𝜂, 𝜏) = ∅ 0 (𝜂) + 𝑒 −𝜀𝜏 𝐽(𝜂, 𝜏) (25) Sumera Dero (et al) where the unidentified eigenvalue is 𝜀 where its value needs to fix a stable branch. In addition, 𝐹(𝜂, 𝜏), 𝐺(𝜂, 𝜏), 𝐻(𝜂, 𝜏), and 𝐽(𝜂, 𝜏) all their derivatives are assumed small relative to 𝑓 0 (𝜂), 𝑔 0 (𝜂), 𝜃 0 (𝜂), and ∅ 0 (𝜂).…”
Section: Temporal Stability Analysismentioning
confidence: 99%
“…In addition, 𝐹(𝜂, 𝜏), 𝐺(𝜂, 𝜏), 𝐻(𝜂, 𝜏), and 𝐽(𝜂, 𝜏) all their derivatives are assumed small relative to 𝑓 0 (𝜂), 𝑔 0 (𝜂), 𝜃 0 (𝜂), and ∅ 0 (𝜂). Now, substituting the correlation (25) in Equations (20)(21)(22)(23)(24), we get the following resultant Linearized Eigenvalue Problem (LEVP) system as follows:…”
Section: Temporal Stability Analysismentioning
confidence: 99%
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“…Furthermore, Ishaq et al [15] explored two dimensional nanofluid film stream of Eyring-Powell liquid with variable warmth transmission in the presence of MHD on a shaky permeable extending sheet and announced that porosity parameter diminishes the movement of the fluid movies, and enlarging the nanoparticle concentration effectively expands the rubbing characteristic of Eyring-Powell nanofluid. In recent times, various researches have been made in the field of Eyring-Powell nanofluids that can be found in references [16][17][18][19][20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%
“…The unsteady state of mixed convection flow of micropolar fluid moving along an inclined stretching plate has been scrutinized by Kasim et al [12]. Furthermore, some interesting studies regarding fluid flow and heat transfer for various aspects have been investigated, as reported in [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29].…”
Section: Introductionmentioning
confidence: 99%