| 000 | 03717nlm1a2200409 4500 | ||
|---|---|---|---|
| 001 | 664964 | ||
| 005 | 20231030041947.0 | ||
| 035 | _a(RuTPU)RU\TPU\network\36149 | ||
| 090 | _a664964 | ||
| 100 | _a20210603a2021 k y0engy50 ba | ||
| 101 | 0 | _aeng | |
| 135 | _adrcn ---uucaa | ||
| 181 | 0 | _ai | |
| 182 | 0 | _ab | |
| 200 | 1 |
_aNonlinear Mixed Convective Flow over a Moving Yawed Cylinder Driven by Buoyancy _fM. P. Prabhugouda, F. S. Hadapad, M. A. Sheremet |
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| 203 |
_aText _celectronic |
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| 300 | _aTitle screen | ||
| 320 | _a[References: 40 tit.] | ||
| 330 | _aThe fluid flow over a yawed cylinder is useful in understanding practical significance for undersea applications, for example, managing transference and/or separation of the boundary layer above submerged blocks and in suppressing recirculating bubbles. The present analysis examines nonlinear mixed convection flow past a moving yawed cylinder with diffusion of liquid hydrogen. The coupled nonlinear control relations and the border restrictions pertinent to the present flow problem are nondimensionalized by using nonsimilar reduction. Further, implicit finite difference schemes and Quasilinearization methods are employed to solve the nondimensional governing equations. Impact of several nondimensional parameters of the analysis on the dimensionless velocity, temperature and species concentration patterns and also on Nusselt number, Sherwood number and friction parameter defined at the cylinder shell is analyzed through numerical results presented in various graphs. Velocity profiles can be enhanced, and the coefficients of friction at the surface can be reduced, for increasing values of velocity ratio parameters along chordwise as well as spanwise directions. Species concentration profile is reduced, while the Sherwood number is enhanced, for growth of the Schmidt number and yaw angles. Furthermore, for an increasing value of yaw angle, skin-friction coefficient in chordwise direction diminishes in opposing buoyancy flow case, whereas the results exhibit the opposite trend in assisting buoyancy flow case. Moreover, very importantly, for increasing magnitude of nonlinear convection characteristic, the liquid velocity and surface friction enhance in spanwise direction. Further, for increasing magnitude of combined convection characteristics, velocity profiles and coefficient of friction at the surface enhance in both spanwise and chordwise directions. Moreover, we have observed that there is no deviation for zero yaw angle in Nusselt number and Sherwood number. | ||
| 461 | _tMathematics | ||
| 463 |
_tVol. 9, iss. 11 _v[1275, 18 p.] _d2021 |
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| 610 | 1 | _aэлектронный ресурс | |
| 610 | 1 | _aтруды учёных ТПУ | |
| 610 | 1 | _amixed convection | |
| 610 | 1 | _ayawed cylinder | |
| 610 | 1 | _adouble diffusion | |
| 610 | 1 | _anonlinear convection | |
| 610 | 1 | _aquasilinearization technique | |
| 610 | 1 | _aсмешанная конвекция | |
| 610 | 1 | _aдиффузия | |
| 700 | 1 |
_aPrabhugouda _bM. P. |
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| 701 | 1 |
_aHadapad _bF. S. |
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| 701 | 1 |
_aSheremet _bM. A. _cphysicist _cProfessor of Tomsk Polytechnic University, Doctor of Physical and Mathematical Sciences _f1983- _gMikhail Aleksandrovich _2stltpush _3(RuTPU)RU\TPU\pers\35115 |
|
| 712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИнженерная школа энергетики _bНаучно-образовательный центр И. Н. Бутакова (НОЦ И. Н. Бутакова) _h8025 _2stltpush _3(RuTPU)RU\TPU\col\23504 |
| 801 | 2 |
_aRU _b63413507 _c20210603 _gRCR |
|
| 856 | 4 | _uhttps://doi.org/10.3390/math9111275 | |
| 942 | _cCF | ||