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1.
Domestic stack is considered to investigate the double-diffusive laminar natural convection. The working fluid is a gaseous mixture that has similar physical properties to carbon dioxide. Knowing the patterns of gaseous mixture distribution and determining the carbon deposit regions can help in carbon capture problems. The present study uses the finite element method to numerically examine the double ratio-diffusive physical phenomena in a rectangular-trapezoidal enclosure and to simulate the stack under a wide range of dimensionless parameters, such as buoyancy ratio 1 N BR 7 $1\le {N}_{{BR}}\le 7$ , Lewis number 2 Le 8 $2\le {Le}\le 8$ , and Rayleigh number 10 3 Le 10 5 ${10}^{3}\le {Le}\le {10}^{5}$ for different aspect ratios. Nine different cases of the geometrical ratio are selected to cover most possible design configurations. The results indicate that increasing the Lewis number leads to augmented solutal transport but reduces heat transfer. However, both heat and mass transfer are observed by increasing the buoyancy ratio. It is worth mentioning that increasing the ratio of upper side length to base length d D $\left(\frac{d}{D}\right)$ from 1 4 $\left(\frac{1}{4}\right)$ to 3 8 $\left(\frac{3}{8}\right)$ leads to a significant increase in mass transfer by 75% and heat transfer enhancement ratio by around 50%.  相似文献   

2.
This article focuses on the study of heat and mass transfer (HMT) fluid flow over an exponentially accelerated vertical plate, which is subjected to an applied magnetic field and viscous dissipation. The research has applications in various manufacturing processes such as wire/fiber drawing, hot rolling, continuous casting, and hot extrusion, where heat transfer to the ambient medium and the hot moving material are of utmost importance. The findings could also be relevant to aerospace engineering applications. The study investigates the time-fractional natural convection phenomenon and utilizes conservation laws to derive the flow guiding equations, which are then made nondimensional. Finite difference discretization is utilized to solve the dimensionless equations implicitly. Then the flow simulation results such as concentration, temperature, and velocity profiles are discussed based on the variation in parameters such as Prandtl number ( P r $Pr$ ), thermal/mass Grashof number ( Gr / Gc ${Gr}/{Gc}$ ), Eckert number ( Ec ${Ec}$ ), magnetic parameter ( M $M$ ), time-fractional order ( λ $\lambda $ ), and Schmidt number ( Sc ) $({Sc})$ . Also, the HMT rate is depicted using the Nusselt number and skin friction plots. It is noted that HMT increases when Sc ${Sc}$ increases and λ $\lambda $ decreases. The change in time-fractional order affects the velocity profiles adjacent to the wall and is more significant in the case of lower values of the Prandtl number.  相似文献   

3.
This study investigates the chemical reaction influence on heat transfer flow of viscous Newtonian fluid over a moving surface under the intensity of nonuniform heat source/sink. Variable fluid viscosity and ohmic heating effects are considered in the model equation. The uniqueness of the present investigation is to scrutinize the significance of nonuniform heat source/sink and ohmic heating on the heat transfer flow of optically thin radiative fluid in a permeable medium. The flow equations of continuity, momentum, thermal and solutal fields are converted by invoking relevant dimensionless variables. Also, the converted nonlinear equations are analyzed numerically by using the fourth order Runge–Kutta Fehlberg approach. The significance of model parameters are scrutinized and discussed in detail via graphs and tables. The important findings of this study are the effects of Joule heating J $J$ , viscous dissipation parameter B r ${B}_{r}$ , variable fluid property parameter ϵ $\epsilon $ and radiation parameter R a ${R}_{a}$ on fluid flow, energy profile and solutal field. The results show that the thermal field depreciates as the Prandtl number increases but escalates against higher values of Joule heating parameter and Brinkman number. Also, the outcome of this study reveals that an enhancement in the values of variable viscosity parameter declines velocity distribution. Concentration distributions behave as a growing function of the Soret number and diminishing function of the Schmidt number. Furthermore, contrasting this study with existing results reveals excellent agreement.  相似文献   

4.
It is imperative to mitigate the convective heat loss from the receiver to improve the overall efficiency of the parabolic dish concentrator. In this study, the reductions of convective heat loss from the cylindrical-hemispherical receiver are numerically analyzed and the model was validated by the experimental data from literature. In the first case, the impact of the glass cover on convective heat loss is examined under conditions of both natural and forced convections at various receiver orientations (γ = 0°, 30°, 60°, and 90°). Numerical results clearly demonstrate that the use of a glass cover significantly reduces the intrusion of surrounding air into the receiver cavity which leads to an enhancement of the stagnation zone inside the cavity and, as a consequence, a noticeable reduction in convective heat loss is observed. To perform analysis of the receiver with glass cover under forced convective condition, the wind velocities over the receiver are considered in the range of 1–6 m/s. The maximum reduction of convective heat loss using the glass cover is achieved to be 58.44% with wind velocity of 5 m/s at γ = 60°. In the second case, the influence of air curtain at the receiver aperture under natural convective heat loss conditions is analyzed. The analysis incorporates three variables: receiver orientation (γ = 0°–60°), nozzle width ( L noz ${L}_{\mathrm{noz}}$ = 0.002–0.004 m), and nozzle outlet velocity ( V noz ${V}_{\mathrm{noz}}$ = 0.5–3.5 m/s). The results show that the air curtain minimizes the outflow of receiver inside air and results in an improvement in the stagnation zone inside the cavity. The maximum effectiveness of the air curtain is found to be 43.2% at nozzle width of L noz ${L}_{\mathrm{noz}}$ = 0.004 m and nozzle velocity of V noz ${V}_{\mathrm{noz}}$ = 1.5 m/s at receiver orientation of 60°. It is also noteworthy that the optimal nozzle velocity decreases with the increase of nozzle widths.  相似文献   

5.
In this research endeavor, Casson fluid flow and melting heat transfer due to a curved nonlinearly stretching sheet are investigated. The sheet is naturally permeable and the flow is considered in a porous medium. For flow in a porous medium, a modified Darcy's resistance term for Casson fluid is considered in the momentum equation. In the energy equation, heat transport characteristics, including viscous dissipation, are taken into account. Mass transport is also studied together with the impact of chemical reaction of higher order. The governing nonlinear partial differential equations of flow, heat, and mass transport are reduced to nondimensional ordinary differential equations using adequate similarity transformations and then solved numerically employing the bvp4c technique and Runge–Kutta fourth-order method on MATLAB. The impacts of numerous occurring parameters on relevant fields (velocity field, temperature field, and concentration field) are depicted and discussed by plotting graphs. We concluded the curvature parameter, K $K$ reduces the pace of the flow. The impacts of the stretching index, m $m$ and melting parameter, M e $Me$ are also found to reduce flow and temperature field. Furthermore, we noted that the reaction parameter, K n ${K}_{n}$ and its order, n $n$ exhibit opposite impacts on the concentration field. Moreover, the numerical values of skin-friction coefficient and Nusselt number calculated employing bvp4c and Runge–Kutta fourth-order technique are expressed in tabular mode, and these are found in an excellent match. For validation of the results, skin-friction coefficient values were computed using the Runge–Kutta fourth-order technique and bvp4c solver, compared with the existing results, and a good agreement was found.  相似文献   

6.
The current work deals with the numerical investigation of mixed convection occurring from two hot cylinders placed inside vented ducts under different sizes of inflow and locations of outflow opening vents. The mathematical formulation is solved based on the finite volume approach. The location of the outflow section is changed to left, center, and right of enclosure. Impacts of inflow section sizes ( O ${O}$ 1 = 0.125 and O ${O}$ 1 = 0.25), locations of outflow section ( O 2 ${O}_{2}$ = 0.125 $0.125$ ), space between cylinders ( 0.3 S 0.45 $0.3\le S\le 0.45$ ), Reynolds number ( 200 R e 400 $200\le Re\le 400$ ), and Richardson number ( 0.1 Ri 20 $0.1\le {Ri}\le 20$ ) are implemented. Findings display that the average Nusselt number (Nu) is exceeded by 20% for low Ri ${Ri}$ due to the effect of nonsymmetrical inflow and outflow sections as compared with the case of equal opening vents. For large Ri, a higher Nu is obtained for nonequal opening vents in comparison with the case of equal opening vents by 10%. The difference in the average Nu between left and right cylinders is about 11%. Findings display that the enhancement in Nu due to the large spacing size between cylinders as compared with those of low spacing size is about 35%. The variations of Nu display the opening vents ratio, Re, S $S$ , and Ri ${Ri}$ have an extreme action on the characteristics of flow and temperature fields.  相似文献   

7.
This study involvesthe numerical modeling of steady thermal radiation and chemical reaction on non-Newtonian fluid motion via a bidirectional stretching surface. We have taken convective boundary conditions, and heat sources on the stretching surface. The working fluid of the present study is Casson fluid (“non-Newtonian”) with couple stress. The self-similarity forms of the nonlinear thermal radiative flow model are obtained by using similarity variables. Furthermore, the numerical results are computed with the help of fourth-order Runge–Kutta–Fehlberg method with a shooting algorithm after reducing nonlinear partial differential equations have been translated into strong ordinary differential equations (ODEs). Impacts of the various flow physical parameters especially Biot number, nonlinear thermal radiation, and heat source parameters containing nonlinear ODEs are discussed in detail for distinct numerical values. A comparison of calculated results with the known numerical results made with the previously published literature is mentioned and obtained a good agreement. Finally, we found that the R e x 1 / 2 C f x $R{e}_{x}^{1/2}{C}_{fx}$ (“coefficient of skin friction”) declines along x * , y * $x* ,\,y* $ directions, respectively, with β $\beta $ via λ $\lambda $ while the opposite direction follows M $M$ with respect to λ $\lambda $ and the R e x 1 / 2 N u x $R{e}_{x}^{-1/2}N{u}_{x}$ (“heat transfer rate”), R e x 1 / 2 S h $R{e}_{x}^{-1/2}Sh$ (“mass transfer rate”) increase with Γ $\Gamma $ via γ 1 ${\gamma }_{1}$ while opposite direction follows γ 1 ${\gamma }_{1}$ with respect to γ 2 ${\gamma }_{2}$ .  相似文献   

8.
This study covers a simulation on conjugate free convective in a porous enclosure containing a side wall thickness and partially heated and cooled from sides under the considerations of local thermal nonequilibrium (LTNE) and non-Darcy flow. Interest has been focused on how the side wall thickness and the locations of cooled and heated parts affect the effectiveness of the Nusselt number (Nu). Three different cases of localized heating and cooling locations have been implemented for the following ranges: scaled heat transfer coefficient ( 0.1 H 100 $0.1\le H\le 100$ ), wall to fluid thermal conductivity ratio ( 0.1 R k 100 $0.1{\le R}_{k}\le 100$ ), modified Rayleigh number ( 200 Ra * 1000 $200\le {Ra}* \le 1000$ ), wall width ( 0.1 Z ˆ 0.5 $0.1\le \hat{Z}\le 0.5$ ), inertial parameter ( 10 4 F s / P r * 10 2 ${10}^{-4}{\le F}_{s}/{P}_{r}^{* }\le {10}^{-2}$ ), and thermal conductivity ratio ( 0.1 K r 100 $0.1\le {K}_{r}\le 100$ ). Outcomes show that Z ˆ $\hat{Z}$ and the locations of cooled and heated parts have remarkable impacts on all the Nusselt numbers. The intensity of LTNE region considerably relies on Ra * ${Ra}{* }$ , K r ${K}_{r}$ and H $H$ . The total average NuT is highly dependent on R k ${R}_{k}$ , Ra * ${Ra}{* }$ , Z ˆ $\hat{Z}$ , F s / P r * ${F}_{s}/{P}_{r}^{* }$ , and K r ${K}_{r}$ as compared to H. The increase in Z ˆ $\hat{Z}$ leads to change of the convective mechanism to conductive mode. The rise in R k ${R}_{k}$ guides to increase Nu, where R k ${R}_{k}$ can control the flow strength. The actions of F s / P r * ${F}_{s}/{P}_{r}^{* }$ on Nuf is more evident than Nus. For low H and Kr, the size of LTNE zone is considerably affected by H as compared to Kr although Kr has a high influence on Nu. For high Kr and H, the LTNE zone has closely vanished. Findings display that the Case 2 provided the highest Nu for all tested parameters except the case of K r = 0.1 ${K}_{r}=0.1$ . Finally, it is evident that for the problems that employed solid conduction wall with localized heating and cooling sections, Case 2 is recommended for future use in the applications that implement a porous medium and depend on free convection.  相似文献   

9.
The given investigation concerns the study of non-Newtonian Oldroyd-B fluid flow across a permeable surface along with nonlinear thermal radiation, chemical reactions, and heat sources. Equations modified are thus numerically evaluated by employing bvp4c-technique. Obtained outcomes are exhibited graphically. Pictorial notations are used to investigate the consequences of necessary parameters of velocity, energy, and mass. Acquired outcomes provide promising agreement with already established consequences provided in the open literature. The obtained results guided that magnetic field parameter ( M $M$ ), porosity parameter ( K p $Kp$ ), Deborah number β 1 ${\beta }_{1}$ reduce momentum boundary layer thickness, furthermore, growth in the relevant Deborah number β 2 ${\beta }_{2}$ improves the corresponding momentum boundary layer.  相似文献   

10.
Some properties of time-dependent that modify Brinkman equations for fluid flow in a cylindrical tube filled with Bidisperse Porous Material are discussed in this article. The fluid velocities through the fracture and porous phases of the Bidisperse Porous Medium (BDPM) resulting from the application of pressure gradient are described by two coupled second-order partial differential equations. Laplace transform technique, D'Alembert and Riemann-Sum Approximation Methods are used to obtain a semianalytical solution for the model. The choice of the D'Alembert is made to systematically decouple the coupled governing equations without altering their initial orders. The role of the coupling parameter: The coefficient of momentum transfer ( η ) $(\eta )$ in the flow formation is considered. Accordingly, three cases are analyzed: (a) weak coupling ( η = 0 ) $(\eta =0)$ which described the fluid flow in the absence of the coupling parameter, (b) the strong coupling resulting from a large value of the coupling parameter ( η ) $(\eta \to \infty )$ , and (c) fluid momentum for any arbitrary value of η $\eta $ . It is observed that fluid stability is attained when Da f ${{Da}}_{f}$ and Da p ${{Da}}_{p}$ are decreased; a finding that agrees with the findings of Nield and Kuznetsov and Magyari. Also, the maximum velocity in the fracture phase of the BDPM is attained when the coefficient of momentum transfer is neglected ( η = 0 ) $(\eta =0)$ while an opposing flow formation is demonstrated in the fracture and porous phases of BDPM as η $\eta $ is increased.  相似文献   

11.
In this study, the water convection flow within a right-angled, inclined, and isosceles triangle enclosure for various inclination angles was numerically analyzed using the lattice Boltzmann method with the multirelaxation time model. On the hypotenuse side, the enclosure is thermally insulated, while the left and horizontal walls are kept, respectively, at cold and hot temperatures. This study was conducted to show the effects of two key parameters, the tilt angle ϕ $\phi $ and the Rayleigh number R a $Ra$ , whose changes span from 0 ${0}^{\circ }$ to 31 5 $31{5}^{\circ }$ and 5 × 1 0 3 $5\times 1{0}^{3}$ to 1 0 6 $1{0}^{6}$ , respectively. The effect of these variables is presented in terms of streamlines, isotherms, velocity profiles, temperature plots, and the average Nusselt number. Furthermore, the impact of the size of a hot square obstruction inside the cavity on the isotherms and streamlines has been investigated. The findings demonstrate that the rate of heat transport is enhanced as the Rayleigh number increases. This result is in good agreement with earlier research without tilting the cavity. Depending on the Rayleigh number, the tilt angle has a significant effect on the rate of heat transmission.  相似文献   

12.
This paper investigates the heat and mass transfer under magnetohydrodynamic mixed convection flow of a binary gas mixture in a four-sided lid-driven square cavity. The enclosure's left wall is sinusoidally heated and acts as a source term, while the right wall functions as a sink. The cavity's horizontal walls are adiabatic and impermeable to mass transfer. The governing equations under Boussinesq approximation and stream function-vorticity formulation are solved using the alternating-direction-implicit scheme, a finite-difference method. The numerical scheme's consistency and stability are demonstrated using the matrix method. The MATLAB code is written, validated against some existing studies, and used to perform numerical simulations. The numerical solutions are graphically examined by visualizing the streamline, isotherm, and concentration contours for nondimensional parameters, such as Hartmann number ( 0 H a 100 ) $(0\le Ha\le 100)$ , heat absorption or generation coefficient ( 2 ϕ 2 ) $(-2\le \phi \le 2)$ , Richardson number ( 0.01 R i 100 ) $(0.01\le Ri\le 100)$ , and buoyancy ratio ( 6 N 6 ) $(-6\le N\le 6)$ . The magnetic field modifies the temperature and concentration distribution in the cavity, depending on the convection mode. The magnetic field forces the fluid to stagnate in different regions of the cavity, depending on the mode of convection. It was found that the difference between the maximum and minimum temperature and concentration at the cavity's midpoint increases up to 13 and 10 times, respectively, in the natural convection compared with the forced convection. The average Nusselt number on the vertical walls of the cavity is maximum in natural convection in the absence of a magnetic field but reaches a minimum value at H a = 100 $Ha=100$ in forced and mixed convection. The average Sherwood number on the cavity's vertical walls decreases with the magnetic field in mixed and natural convection.  相似文献   

13.
The present numerical study focuses on the cooling by natural convection and surface radiation of two electronic components generating two different and uniform volumetric powers. These components are modeled by two square bodies placed inside a closed square cavity with a cold straight wall. Two configurations are analyzed based on the position of the two heat-generating bodies. In the first one (horizontal position configuration), the two bodies are located at the same height of the cavity, while they are placed at different heights in the second case (vertical position configuration). The effects of two Rayleigh numbers ( 0 ( Ra 1 , Ra 2 ) 10 6 $0\le ({{Ra}}_{1},{{Ra}}_{2})\le {10}^{6}$ ), the conductivity ratio ( 0.01 K 100 $0.01\le K\le 100$ ), and the emissivity ( 0 ε 1 $0\le \varepsilon \le 1$ ) on the heat transfer characteristics and the flow structure are analyzed. The data is displayed as streamlines, isotherms, velocity, and maximum temperature profiles, and local heat transfer on the active wall. The obtained results indicate that the choice of the appropriate configuration depends mainly on the deviation between the two Rayleigh numbers. Furthermore, the maximum temperature of a specific block decreases as the quantity of heat generated by the other block rises. We can also see that the maximum temperature of the two blocks decreases by about 50 % $50 \% $ with the increase in the emissivity (from 0 $0$ to 1 $1$ ) or the conductivity ratio (from 0.1 $0.1$ to 1 $1$ ).  相似文献   

14.
The major scope of this research is to scrutinize the effects of multiple slips on unstable magnetohydrodynamic micropolar fluid past a stretched sheet with a non-Darcy porous medium. In the momentum equation, the non-Darcy porous medium effect is also taken into consideration. The effects of uneven heat source/sink and thermal radiation in the energy equation are also analyzed. By implementing the similarity transmission, the mathematical modeling of the set of managing partial differential equations is reframed into nonlinear ordinary differential equations. These equations are numerically solved by applying Matlab built-in solver bvp5c. The implications of foremost parameters such as micropolar parameter, magnetic parameter, permeability parameter, Prandtl, Eckert, and Schmidt numbers, Chemical reaction, slip parameters on velocity, microrotation, temperature as well as concentration profiles are displayed pictorially and explained. It is worthwhile to mention that the improving values of micropolar parameter K $K$ escalate the velocity as well as microrotation profiles. However, the upsurge in non-Darcy porous medium F s ${F}_{s}$ will cause a declining nature in the velocity profile. Also, an enhancement in the unsteadiness parameter A $A$ brings about a lessening in all the profiles. Increment in all the three usual slip parameters will bring a declining nature in the respective profiles. An increase in Schmidt number will give a deduction nature in velocity as well as concentration profile. Moreover, the physical quantities are defined and Nusselt numbers are formulated in the table, and it enlarges while boosting up P r $Pr$ and R $R$ , whilst a reverse nature is noticed for others. This present study compared with the earlier studies in special cases holds a better agreement.  相似文献   

15.
The current work investigates the effect of an arc-shaped vertical control plate on the heat and mass transfer in uniform flow past an isothermally heated circular cylinder. The control plate is positioned downstream at various distances from the circular cylinder's surface. The governing equations are discretized by the higher order compact (HOC) finite difference scheme, and then this system of discretized equations is solved by using a bi-conjugate gradient stabilized iterative method for Prandtl number P r = 0.7 $Pr=0.7$ , Reynolds number R e = 150 $Re=150$ . To investigate the effect of an arc-shaped control plate on heat and mass transfer, we consider a range of nondimensional distances between the circular cylinder and the control plate, 0.5 d R 0 8 $0.5\le d\unicode{x02215}{R}_{0}\le 8$ , where d $d$ is the control plate's distance and R 0 ${R}_{0}$ is the cylinder's radius. The exact timing and location of the bifurcation points are calculated by using topological aspect-based structural bifurcation analysis. Significant effects of various locations of the control plate on periodic wake and heat transfer are observed. It is found that the increasing distance of the control plate from the cylinder delays the occurrence of the structural bifurcation and shifts the bifurcation points upwards in the upper half and downwards in the lower half of the cylinder. Our study shows that the specific location of the control plate can fully suppress the vortex shedding. Time-averaged total Nusselt number can be drastically reduced by increasing the distance between the control plate and the cylinder. With proper positioning, the vertical control plate can lessen the time-averaged drag force by up to 22.5 % $22.5 \% $ when compared to a cylinder without a control plate. Overall, this work presents many new phenomena that have not been reported before.  相似文献   

16.
Fluid flow coupled with temperature effects has attained prime importance due to its huge applications in different fields like casting and welding industries, geothermal extraction, and lubrication technologies. The present study is a novel numerical method for computations for fluid flow with temperature effects in a rectangular domain. A control volume method is employed as a numerical method for solving continuity, momentum, and energy equations. Owing to the difficulties associated with solving these governing equations, numerical computations are presented in the computational grid by using the control volume method. A modified algorithm is suggested for the current problem. The magnitude of the velocity, temperature, and pressure at different nodes in horizontal and vertical directions of the computational domain is investigated. Along the diagonal nodes, the pressure declines and then grows consistently. The temperature for mercury ( P r = 0.015 ) $(Pr=0.015)$ is higher than for water ( P r = 6.57 ) $(Pr=6.57)$ at a particular node.  相似文献   

17.
The present article provides a three-dimensional numerical investigation of thermal convection and entropy generation. The lattice Boltzmann method, coupled with the finite difference approach, is applied to perform numerical simulations. The validation of these numerical approaches for thermal convection simulation and entropy calculation is performed by comparing our numerical results with those in the published literature for the case of benchmark problems. The physical geometry studied in this paper concerns a hot obstacle having the shape of a plus sign (+) placed in the center of a cubic enclosure. This cube is filled with air of a Prandtl number of 0.71 and characterized by two cold vertical walls. The heat exchange between the fluid and the hot body is studied as a function of the Rayleigh number ( 10 3 Ra 10 7 ${10}^{3}\le {Ra}\le {10}^{7}$ ). The performed simulations show that the heat transfer rate can be increased by about 429% by switching from Ra = 10 3 ${Ra}={10}^{3}$ to 10 7 ${10}^{7}$ . The entropy generation due to fluid friction, heat transfer, and total entropy are also calculated and discussed. For an irreversibility coefficient φ = 10 4 ${\varphi }={10}^{-4}$ , the analysis of the results showed that for low values of the Rayleigh number ( Ra = 10 3 ${Ra}={10}^{3}$ ), the entropy production due to temperature gradients predominates over that produced by viscous effects. In the cases of Ra = 10 4 ${Ra}={10}^{4}$ and 10 5 ${10}^{5}$ , entropy generation is due to both fluid friction and heat transfer. However, when the Rayleigh number becomes large ( Ra 10 6 ${Ra}{\ge 10}^{6}$ ), entropy generation due to viscosity predominates over entropy production related to heat exchange. These results have important implications for the optimization and design of heat transfer systems in various industrial applications.  相似文献   

18.
A numerical study of mixed convective heat transfer in a lid-driven square enclosure containing a hot elliptic cylinder is conducted. The impacts of the Grashof number  ( 10 3 Gr 1 0 6 ) $({10}^{3}\le {Gr}\le 1{0}^{6})$ , Reynolds number ( 1.0 R e 100 ) $(1.0\le Re\le 100)$ , cylinder tilt angle  ( 0 ° ϕ 90 ° ) $({0}^{^\circ }\le \phi \le {90}^{^\circ })$ , and aspect ratio ( 1.0 A R 3.0 ) $(1.0\le AR\le 3.0)$ have been examined for a fluid of P r $Pr$ of 0.71. The horizontal enclosure walls are insulated, while its vertical walls are restricted to a nonvarying temperature Tc, whereas a sinusoidal temperature of T h + T sin ( π x / L ) ${T}_{h}+\unicode{x02206}T\unicode{x0200A}\sin (\pi x/L)$ is imposed on the wall of the elliptical cylinder. The governing equations are solved using COMSOL Multiphysics 5.6 software. The fluid dynamic and the heat transport profiles between the enclosure and the elliptical cylinder walls are represented by the stream function, isothermal contours, and average Nusselt number. Results established that for all the considered aspect ratios, the thermal heating range of 10 3 Gr 1 0 4 ${10}^{3}\le {Gr}\le 1{0}^{4}$ is predominantly a conduction mechanism. The critical position of the ellipse where the inclination effect becomes insignificant is determined by the Grashof number and aspect ratio when the Re = 100. The strength of vortices and cell numbers are significantly influenced by the aspect ratio, particularly when the Gr = 1 0 4 ${Gr}=1{0}^{4}$ . When A R = 1.0 $AR=1.0$ , the average heat transfer from the cylinder remains the same regardless of the cylinder's orientation. The impact of cylinder orientation on heat transfer from the cylinder wall is minimal for 1.5 A R 2.0 $1.5\le AR\le \phantom{\rule{}{0ex}}2.0$ . For AR values of 2.5 A R 3.0 $2.5\le AR\le \phantom{\rule{}{0ex}}3.0$ , increasing the inclination angle does not result in improved heat transfer. The influence of the increasing inclination angle on the right wall diminishes as the angle increases, except when the Grashof number is greater than 105, where the rate of heat transfer is enhanced for inclination angles beyond 45°.  相似文献   

19.
The onset of convection in a Newtonian liquid-containing system is investigated using a two-frequency boundary temperature. The consequences of three types of two-frequency boundary temperature modulations have been thoroughly investigated: (i) in-phase, (ii) out-of-phase, and (iii) bottom-wall. The combined effect of two frequencies with sinusoidal and nonsinusoidal wave types is also documented under these various types of boundary temperature modulations. To facilitate the study, the Venezian method is approved and the critical Rayleigh number and its correction are calculated. The parameters resulting from the study's two frequencies of modulation are the mixing angle, χ $\chi $ , the amplitudes, β , δ $\beta ,\delta $ , and the set of coprime integers, ( r 1 , r 2 ) $({r}_{1},{r}_{2})$ . The system's thermodynamics determines the range of these parameters. The research discovered that out-of-phase two-frequency boundary temperature modulation is the most stable, while in-phase is the least stable. Besides that, any combination of wave type with square wave type yields the most excellent stability. Furthermore, the two-frequency boundary temperature modulation is more stable than the single-frequency and no-modulation cases.  相似文献   

20.
In this article, the natural convection of stratified fluid driven by the asymmetric heating and cooling of the surfaces of the concentric cylinders filled with an anisotropic porous matrix is investigated. The stratified fluid is confined between the outer surface of the inner cylinder and the inner surface of the outer cylinder while the onset transient natural convection is induced by the asymmetric heat heating/cooling of the inner surface of the outer cylinder while the outer surface of the inner cylinder is maintained at a constant temperature T = 1 $T=1$ . The present problem is governed by a pair of coupled second-order partial differential equations. To obtain the expressions for the temperature and velocity fields, the coupled mathematical equations describing the problem are systematically uncoupled such that their original orders remain unaltered. The research established that if the temperature of the outer surface of the inner cylinder equals the temperature of the inner surface of the outer cylinder, a symmetric flow occurs where two maxima velocities are observed close to the surfaces Z = 1 $Z=1\phantom{\rule{}{0ex}}$ and λ $\lambda $ of the annulus, respectively. Furthermore, for some constraints on certain values of some physical quantities in the flow solutions, the present work excellently compares with the research conducted by Jha and Oni.  相似文献   

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