NATURAL (Aka: FREE) CONVECTION NATURAL CONVECTION

Total Page:16

File Type:pdf, Size:1020Kb

NATURAL (Aka: FREE) CONVECTION NATURAL CONVECTION NATURAL (aka: FREE) CONVECTION NATURAL CONVECTION Many familiar heat transfer applications involve natural convection as the primary mechanism of heat transfer. Examples? cooling of hot food warming of cold drinks 2 1 Buoyancy force: upward force exerted by a fluid on a body completely or partially immersed in it in a gravitational field The “chimney effect” induces upward flow of hot combustion gases through a chimney due to the buoyancy differences. 3 at rest except in the Free Convection vicinity of the hot surface Heat transfer that occurs in a quiescent fluid due to convection currents induced by buoyancy forces n Heat transfer equation is the same as for forced convection. n Volume expansivity, β, is a property that indicates the variation in density with temperature: for an ideal gas 2 In natural convection, the flow rate is established by the dynamic balance of buoyancy and friction. An interferometer produces a map of interference fringes (lines of constant temperature). Smooth and parallel lines in (a) indicate laminar flow. Eddies and irregularities in (b) indicate turbulent flow. Lines are closest near the surface indicating a higher temperature gradient. Isotherms in natural convection over a hot plate in air 5 FLUID MOTION The thickness of the boundary layer increases in the flow direction. Fluid velocity is zero at the outer edge of the velocity boundary layer AND at the surface of the plate. At the surface, the fluid temperature is equal to the plate temperature. In the case of cold surfaces, the shape of the velocity and temperature profiles remains the same but their direction is reversed. Typical velocity and temperature profiles for natural convection over a hot vertical plate at temperature Ts inserted in a fluid at temperature T∞. 6 3 The Grashof Number The Grashof number Gr is a measure of the relative magnitudes of the buoyancy force and viscous force acting on the fluid: g βρ2(T −T )L3 g β(T −T )L3 Gr = s f char = s f char L µ2 υ2 g = gravitational acceleration (m/s2) β = volume expansivity (1/K) (β=1/T for ideal gases) o Ts = surface temperature ( C) o Tf = fluid temperature ( C) Lchar = characteristic length (m) ρ = density (kg/m3) µ = dynamic viscosity (N-s/m2) ν = kinematic viscosity (m2/s) The Grashof number is the main criterion in determining whether fluid flow is laminar or turbulent in natural convection. For vertical plates, the critical Grashof number is about 109. 7 External flow involves both natural and forced convection. The relative importance of each mode is determined by Gr/Re2: • Gr/Re2 >> 1 (Natural convection dominates; forced convection is negligible) • Gr/Re2 << 1 (Forced convection dominates; natural convection is negligible) • Gr/Re2 ≈ 1 BOTH effects are significant (mixed convection) 8 4 9 Natural Convection over Surfaces Depends on: surface geometry & orientation variation of surface temperature thermophysical properties of the fluid Most natural convection relations are based on experimental studies: Nu = f (Gr Pr) Rayleigh number = Ra =Gr Pr% Nu =C(Gr Pr)n C and n depend on surface geometry and flow regime n = 1/4 for laminar flow n = 1/3 for turbulent flow Fluid properties evaluated at the film temperature: Tfilm = (Ts + Tf)/2 10 5 Dimensionless parameters ρvL vL Re = = µ υ Horizontal Plates For a hot surface in a cool environment: If the hot surface is facing up, the heated Natural convection on the fluid rises freely, inducing strong natural upper and lower surfaces of convection currents. Effective heat a horizontal hot plate: transfer. If the hot surface is facing down, the plate blocks the heated fluid from rising. Heat transfer is impeded. Characteristic length: Lc = a/4 for a horizontal square surface of length a Lc = D/4 for a horizontal circular surface of diameter D 12 6 Inclined Plates A hot plate in a cooler environment: lower surface has weak Natural convection occurs on the upper and lower surfaces of convection currents à rate of an inclined hot plate. heat transfer is lower than that for a vertical plate upper surface has a thicker boundary layer à rate of heat transfer is higher than that for a vertical plate (opposite occurs for a cold plate in a warmer environment) 13 Horizontal Cylinders and Spheres The boundary layer over a hot horizontal Natural convection cylinder starts to develop at the bottom, over a horizontal hot increasing in thickness along the cylinder: circumference, and forming a rising plume at the top. Local Nusselt number is highest at the bottom and lowest at the top when the boundary layer flow remains laminar. (The opposite is true in the case of a cold horizontal cylinder in a warmer fluid) 14 7 Example 1… (to do in class) A square plate (50 cm on a side) is in a 30oC room. One surface of the plate is maintained at 90oC and the other surface is insulated. Determine the rate of heat transfer from the plate by natural convection if the plate is: (a) Vertical (b) Horizontal with the hot surface facing down (c) Horizontal with the hot surface facing up 8 .
Recommended publications
  • Convection Heat Transfer
    Convection Heat Transfer Heat transfer from a solid to the surrounding fluid Consider fluid motion Recall flow of water in a pipe Thermal Boundary Layer • A temperature profile similar to velocity profile. Temperature of pipe surface is kept constant. At the end of the thermal entry region, the boundary layer extends to the center of the pipe. Therefore, two boundary layers: hydrodynamic boundary layer and a thermal boundary layer. Analytical treatment is beyond the scope of this course. Instead we will use an empirical approach. Drawback of empirical approach: need to collect large amount of data. Reynolds Number: Nusselt Number: it is the dimensionless form of convective heat transfer coefficient. Consider a layer of fluid as shown If the fluid is stationary, then And Dividing Replacing l with a more general term for dimension, called the characteristic dimension, dc, we get hd N ≡ c Nu k Nusselt number is the enhancement in the rate of heat transfer caused by convection over the conduction mode. If NNu =1, then there is no improvement of heat transfer by convection over conduction. On the other hand, if NNu =10, then rate of convective heat transfer is 10 times the rate of heat transfer if the fluid was stagnant. Prandtl Number: It describes the thickness of the hydrodynamic boundary layer compared with the thermal boundary layer. It is the ratio between the molecular diffusivity of momentum to the molecular diffusivity of heat. kinematic viscosity υ N == Pr thermal diffusivity α μcp N = Pr k If NPr =1 then the thickness of the hydrodynamic and thermal boundary layers will be the same.
    [Show full text]
  • Laws of Similarity in Fluid Mechanics 21
    Laws of similarity in fluid mechanics B. Weigand1 & V. Simon2 1Institut für Thermodynamik der Luft- und Raumfahrt (ITLR), Universität Stuttgart, Germany. 2Isringhausen GmbH & Co KG, Lemgo, Germany. Abstract All processes, in nature as well as in technical systems, can be described by fundamental equations—the conservation equations. These equations can be derived using conservation princi- ples and have to be solved for the situation under consideration. This can be done without explicitly investigating the dimensions of the quantities involved. However, an important consideration in all equations used in fluid mechanics and thermodynamics is dimensional homogeneity. One can use the idea of dimensional consistency in order to group variables together into dimensionless parameters which are less numerous than the original variables. This method is known as dimen- sional analysis. This paper starts with a discussion on dimensions and about the pi theorem of Buckingham. This theorem relates the number of quantities with dimensions to the number of dimensionless groups needed to describe a situation. After establishing this basic relationship between quantities with dimensions and dimensionless groups, the conservation equations for processes in fluid mechanics (Cauchy and Navier–Stokes equations, continuity equation, energy equation) are explained. By non-dimensionalizing these equations, certain dimensionless groups appear (e.g. Reynolds number, Froude number, Grashof number, Weber number, Prandtl number). The physical significance and importance of these groups are explained and the simplifications of the underlying equations for large or small dimensionless parameters are described. Finally, some examples for selected processes in nature and engineering are given to illustrate the method. 1 Introduction If we compare a small leaf with a large one, or a child with its parents, we have the feeling that a ‘similarity’ of some sort exists.
    [Show full text]
  • Chapter 6 Natural Convection in a Large Channel with Asymmetric
    Chapter 6 Natural Convection in a Large Channel with Asymmetric Radiative Coupled Isothermal Plates Main contents of this chapter have been submitted for publication as: J. Cadafalch, A. Oliva, G. van der Graaf and X. Albets. Natural Convection in a Large Channel with Asymmetric Radiative Coupled Isothermal Plates. Journal of Heat Transfer, July 2002. Abstract. Finite volume numerical computations have been carried out in order to obtain a correlation for the heat transfer in large air channels made up by an isothermal plate and an adiabatic plate, considering radiative heat transfer between the plates and different inclination angles. Numerical results presented are verified by means of a post-processing tool to estimate their uncertainty due to discretization. A final validation process has been done by comparing the numerical data to experimental fluid flow and heat transfer data obtained from an ad-hoc experimental set-up. 111 112 Chapter 6. Natural Convection in a Large Channel... 6.1 Introduction An important effort has already been done by many authors towards to study the nat- ural convection between parallel plates for electronic equipment ventilation purposes. In such situations, since channels are short and the driving temperatures are not high, the flow is usually laminar, and the physical phenomena involved can be studied in detail both by means of experimental and numerical techniques. Therefore, a large experience and much information is available [1][2][3]. In fact, in vertical channels with isothermal or isoflux walls and for laminar flow, the fluid flow and heat trans- fer can be described by simple equations arisen from the analytical solutions of the natural convection boundary layer in isolated vertical plates and the fully developed flow between two vertical plates.
    [Show full text]
  • Chapter 5 Dimensional Analysis and Similarity
    Chapter 5 Dimensional Analysis and Similarity Motivation. In this chapter we discuss the planning, presentation, and interpretation of experimental data. We shall try to convince you that such data are best presented in dimensionless form. Experiments which might result in tables of output, or even mul- tiple volumes of tables, might be reduced to a single set of curves—or even a single curve—when suitably nondimensionalized. The technique for doing this is dimensional analysis. Chapter 3 presented gross control-volume balances of mass, momentum, and en- ergy which led to estimates of global parameters: mass flow, force, torque, total heat transfer. Chapter 4 presented infinitesimal balances which led to the basic partial dif- ferential equations of fluid flow and some particular solutions. These two chapters cov- ered analytical techniques, which are limited to fairly simple geometries and well- defined boundary conditions. Probably one-third of fluid-flow problems can be attacked in this analytical or theoretical manner. The other two-thirds of all fluid problems are too complex, both geometrically and physically, to be solved analytically. They must be tested by experiment. Their behav- ior is reported as experimental data. Such data are much more useful if they are ex- pressed in compact, economic form. Graphs are especially useful, since tabulated data cannot be absorbed, nor can the trends and rates of change be observed, by most en- gineering eyes. These are the motivations for dimensional analysis. The technique is traditional in fluid mechanics and is useful in all engineering and physical sciences, with notable uses also seen in the biological and social sciences.
    [Show full text]
  • Forced and Natural Convection
    FORCED AND NATURAL CONVECTION Forced and natural convection ...................................................................................................................... 1 Curved boundary layers, and flow detachment ......................................................................................... 1 Forced flow around bodies .................................................................................................................... 3 Forced flow around a cylinder .............................................................................................................. 3 Forced flow around tube banks ............................................................................................................. 5 Forced flow around a sphere ................................................................................................................. 6 Pipe flow ................................................................................................................................................... 7 Entrance region ..................................................................................................................................... 7 Fully developed laminar flow ............................................................................................................... 8 Fully developed turbulent flow ........................................................................................................... 10 Reynolds analogy and Colburn-Chilton's analogy between friction and heat
    [Show full text]
  • Convectional Heat Transfer from Heated Wires Sigurds Arajs Iowa State College
    Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 1957 Convectional heat transfer from heated wires Sigurds Arajs Iowa State College Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Physics Commons Recommended Citation Arajs, Sigurds, "Convectional heat transfer from heated wires " (1957). Retrospective Theses and Dissertations. 1934. https://lib.dr.iastate.edu/rtd/1934 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. CONVECTIONAL BEAT TRANSFER FROM HEATED WIRES by Sigurds Arajs A Dissertation Submitted to the Graduate Faculty in Partial Fulfillment of The Requirements for the Degree of DOCTOR 01'' PHILOSOPHY Major Subject: Physics Signature was redacted for privacy. In Chapge of K or Work Signature was redacted for privacy. Head of Major Department Signature was redacted for privacy. Dean of Graduate College Iowa State College 1957 ii TABLE OF CONTENTS Page I. INTRODUCTION 1 II. THEORETICAL CONSIDERATIONS 3 A. Basic Principles of Heat Transfer in Fluids 3 B. Heat Transfer by Convection from Horizontal Cylinders 10 C. Influence of Electric Field on Heat Transfer from Horizontal Cylinders 17 D. Senftleben's Method for Determination of X , cp and ^ 22 III. APPARATUS 28 IV. PROCEDURE 36 V. RESULTS 4.0 A. Heat Transfer by Free Convection I4.0 B. Heat Transfer by Electrostrictive Convection 50 C.
    [Show full text]
  • Forced Convection Heat Transfer Convection Is the Mechanism of Heat Transfer Through a Fluid in the Presence of Bulk Fluid Motion
    Forced Convection Heat Transfer Convection is the mechanism of heat transfer through a fluid in the presence of bulk fluid motion. Convection is classified as natural (or free) and forced convection depending on how the fluid motion is initiated. In natural convection, any fluid motion is caused by natural means such as the buoyancy effect, i.e. the rise of warmer fluid and fall the cooler fluid. Whereas in forced convection, the fluid is forced to flow over a surface or in a tube by external means such as a pump or fan. Mechanism of Forced Convection Convection heat transfer is complicated since it involves fluid motion as well as heat conduction. The fluid motion enhances heat transfer (the higher the velocity the higher the heat transfer rate). The rate of convection heat transfer is expressed by Newton’s law of cooling: q hT T W / m 2 conv s Qconv hATs T W The convective heat transfer coefficient h strongly depends on the fluid properties and roughness of the solid surface, and the type of the fluid flow (laminar or turbulent). V∞ V∞ T∞ Zero velocity Qconv at the surface. Qcond Solid hot surface, Ts Fig. 1: Forced convection. It is assumed that the velocity of the fluid is zero at the wall, this assumption is called no‐ slip condition. As a result, the heat transfer from the solid surface to the fluid layer adjacent to the surface is by pure conduction, since the fluid is motionless. Thus, M. Bahrami ENSC 388 (F09) Forced Convection Heat Transfer 1 T T k fluid y qconv qcond k fluid y0 2 y h W / m .K y0 T T s qconv hTs T The convection heat transfer coefficient, in general, varies along the flow direction.
    [Show full text]
  • Three-Dimensional Free Convection in Molten Gallium A
    Three-dimensional free convection in molten gallium A. Juel, T. Mullin, H. Ben Hadid, Daniel Henry To cite this version: A. Juel, T. Mullin, H. Ben Hadid, Daniel Henry. Three-dimensional free convection in molten gallium. Journal of Fluid Mechanics, Cambridge University Press (CUP), 2001, 436, pp.267-281. 10.1017/S0022112001003937. hal-00140472 HAL Id: hal-00140472 https://hal.archives-ouvertes.fr/hal-00140472 Submitted on 6 Apr 2007 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. J. Fluid Mech. (2001), vol. 436, pp. 267–281. Printed in the United Kingdom 267 c 2001 Cambridge University Press Three-dimensional free convection in molten gallium By A. JUEL1, T. MULLIN1, H. BEN HADID2 AND D. HENRY2 1Schuster laboratory, The University of Manchester, Manchester M13 9PL, UK 2Laboratoire de Mecanique´ des Fluides et d’Acoustique UMR 5509, Ecole Centrale de Lyon/Universite´ Claude Bernard Lyon 1, ECL, BP 163, 69131 Ecully Cedex, France (Received 22 March 1999 and in revised form 11 December 2000) Convective flow of molten gallium is studied in a small-aspect-ratio rectangular, differentially heated enclosure. The three-dimensional nature of the steady flow is clearly demonstrated by quantitative comparison between experimental temperature measurements, which give an indication of the strength of the convective flow, and the results of numerical simulations.
    [Show full text]
  • Chaotic Flow in a 2D Natural Convection Loop
    International Journal of Heat and Mass Transfer 61 (2013) 565–576 Contents lists available at SciVerse ScienceDirect International Journal of Heat and Mass Transfer journal homepage: www.elsevier.com/locate/ijhmt Chaotic flow in a 2D natural convection loop with heat flux boundaries ⇑ William F. Louisos a,b, , Darren L. Hitt a,b, Christopher M. Danforth a,c a College of Engineering & Mathematical Sciences, The University of Vermont, Votey Building, 33 Colchester Avenue, Burlington, VT 05405, United States b Mechanical Engineering Program, School of Engineering, The University of Vermont, Votey Building, 33 Colchester Avenue, Burlington, VT 05405, United States c Department of Mathematics & Statistics, Vermont Complex Systems Center, Vermont Advanced Computing Core, The University of Vermont, Farrell Hall, 210 Colchester Avenue, Burlington, VT 05405, United States article info abstract Article history: This computational study investigates the nonlinear dynamics of unstable convection in a 2D thermal Received 13 August 2012 convection loop (i.e., thermosyphon) with heat flux boundary conditions. The lower half of the thermosy- Received in revised form 1 February 2013 phon is subjected to a positive heat flux into the system while the upper half is cooled by an equal-but- Accepted 3 February 2013 opposite heat flux out of the system. Water is employed as the working fluid with fully temperature dependent thermophysical properties and the system of governing equations is solved using a finite vol- ume method. Numerical simulations are performed for varying levels of heat flux and varying strengths Keywords: of gravity to yield Rayleigh numbers ranging from 1.5 Â 102 to 2.8 Â 107.
    [Show full text]
  • Numerical Simulation of Williamson Combined Natural and Forced
    entropy Article Numerical Simulation of Williamson Combined Natural and Forced Convective Fluid Flow between Parallel Vertical Walls with Slip Effects and Radiative Heat Transfer in a Porous Medium Mohammad Yaghoub Abdollahzadeh Jamalabadi 1,*, Payam Hooshmand 2, Navid Bagheri 3, HamidReza KhakRah 4 and Majid Dousti 5 1 Department of Mechanical, Robotics and Energy Engineering, Dongguk Universit, Seoul 04620, Korea 2 Young Researchers and Elite Club, Mahabad Branch, Islamic Azad University, Mahabad 433-59135, Iran; [email protected] 3 Department of Energy Engineering, Graduate School of the Environment and Energy, Science and Research Branch, Islamic Azad University, Tehran 1477893855, Iran; [email protected] 4 Department of Mechanical Engineering, College of Engineering, Shiraz Branch, Islamic Azad University, Shiraz 71987-74731, Iran; [email protected] 5 Faculty of Engineering, Zanjan University, Zanjan 38791-45371, Iran; [email protected] * Correspondence: [email protected] or [email protected]; Tel.: +82-22-260-3073 Academic Editor: Milivoje M. Kostic Received: 29 February 2016; Accepted: 8 April 2016; Published: 18 April 2016 Abstract: Numerical study of the slip effects and radiative heat transfer on a steady state fully developed Williamson flow of an incompressible Newtonian fluid; between parallel vertical walls of a microchannel with isothermal walls in a porous medium is performed. The slip effects are considered at both boundary conditions. Radiative highly absorbing medium is modeled by the Rosseland approximation. The non-dimensional governing Navier–Stokes and energy coupled partial differential equations formed a boundary problem are solved numerically using the fourth order Runge–Kutta algorithm by means of a shooting method. Numerical outcomes for the skin friction coefficient, the rate of heat transfer represented by the local Nusselt number were presented even as the velocity and temperature profiles illustrated graphically and analyzed.
    [Show full text]
  • Enhancement of Natural Convection Heat Transfer Coefficient by Using V-Fin Array
    International Journal of Engineering Research and General Science Volume 3, Issue 2, March-April, 2015 ISSN 2091-2730 Enhancement of Natural convection heat transfer coefficient by using V-fin array Rameshwar B. Hagote, Sachin K. Dahake Student of mechanical Engg. Department, MET’s IOE, Adgaon, Nashik (Maharashtra,India). Email. Id: [email protected], Contact No. +919730342211 Abstract— Extended surfaces known as fins are, used to enhance convective heat transfer in a wide range of engineering applications, and offer an economical and trouble free solution in many situations demanding natural convection heat transfer. Fin arrays on horizontal, inclined and vertical surfaces are used in variety of engineering applications to dissipate heat to the surroundings. Studies of heat transfer and fluid flow associated with such arrays are therefore of considerable engineering significance. The main controlling variables generally available to the designer are the orientation and the geometry of the fin arrays. An experimental work on natural convection adjacent to a vertical heated plate with a multiple V- type partition plates (fins) in ambient air surrounding is already done. Boundary layer development makes vertical fins inefficient in the heat transfer enhancement. As compared to conventional vertical fins, this V-type partition plate works not only as extended surface but also as flow turbulator. This V-type partition plate is compact and hence highly economical. The numerical analysis of this technique is done using Computational Fluid Dynamics (CFD) software, Ansys CFX , for natural convection adjacent to a vertical heated plate in ambient air surrounding. In numerical analysis angle of V-fin is further optimized for maximum average heat transfer coefficient.
    [Show full text]
  • On Dimensionless Numbers
    chemical engineering research and design 8 6 (2008) 835–868 Contents lists available at ScienceDirect Chemical Engineering Research and Design journal homepage: www.elsevier.com/locate/cherd Review On dimensionless numbers M.C. Ruzicka ∗ Department of Multiphase Reactors, Institute of Chemical Process Fundamentals, Czech Academy of Sciences, Rozvojova 135, 16502 Prague, Czech Republic This contribution is dedicated to Kamil Admiral´ Wichterle, a professor of chemical engineering, who admitted to feel a bit lost in the jungle of the dimensionless numbers, in our seminar at “Za Plıhalovic´ ohradou” abstract The goal is to provide a little review on dimensionless numbers, commonly encountered in chemical engineering. Both their sources are considered: dimensional analysis and scaling of governing equations with boundary con- ditions. The numbers produced by scaling of equation are presented for transport of momentum, heat and mass. Momentum transport is considered in both single-phase and multi-phase flows. The numbers obtained are assigned the physical meaning, and their mutual relations are highlighted. Certain drawbacks of building correlations based on dimensionless numbers are pointed out. © 2008 The Institution of Chemical Engineers. Published by Elsevier B.V. All rights reserved. Keywords: Dimensionless numbers; Dimensional analysis; Scaling of equations; Scaling of boundary conditions; Single-phase flow; Multi-phase flow; Correlations Contents 1. Introduction .................................................................................................................
    [Show full text]