Chapter 6 FUNDAMENTALS OF CONVECTION
Download as PPT, PDF24 likes4,976 views
Chapter 6 of the document covers the fundamentals of convection, focusing on its physical mechanisms, classifications of fluid flows, and the dynamics of velocity and thermal boundary layers. Key concepts such as the Reynolds, Prandtl, and Nusselt numbers are introduced to understand heat and momentum transfer, particularly in laminar and turbulent flows. The chapter also discusses the derivation and solutions of convection equations, emphasizing their practical applications in engineering and daily life.
Chapter 6 FUNDAMENTALS OF CONVECTION
- 1. Chapter 6 FUNDAMENTALS OF CONVECTION Abdul moiz Dota Dept.Food Engineering University of Agriculture Faisalabad Heat and Mass Transfer: Fundamentals & Applications Fourth Edition Yunus A. Cengel, Afshin J. Ghajar McGraw-Hill, 2011
- 2. 2 Objectives • Understand the physical mechanism of convection and its classification • Visualize the development of velocity and thermal boundary layers during flow over surfaces • Gain a working knowledge of the dimensionless Reynolds, Prandtl, and Nusselt numbers • Distinguish between laminar and turbulent flows, and gain an understanding of the mechanisms of momentum and heat transfer in turbulent flow • Derive the differential equations that govern convection on the basis of mass, momentum, and energy balances, and solve these equations for some simple cases such as laminar flow over a flat plate • Nondimensionalize the convection equations and obtain the functional forms of friction and heat transfer coefficients • Use analogies between momentum and heat transfer, and determine heat transfer coefficient from knowledge of friction coefficient
- 3. 3 PHYSICAL MECHANISM OF CONVECTION Conduction and convection both require the presence of a material medium but convection requires fluid motion. Convection involves fluid motion as well as heat conduction. Heat transfer through a solid is always by conduction. Heat transfer through a fluid is by convection in the presence of bulk fluid motion and by conduction in the absence of it. Therefore, conduction in a fluid can be viewed as the limiting case of convection, corresponding to the case of quiescent fluid.
- 4. 4 The fluid motion enhances heat transfer, since it brings warmer and cooler chunks of fluid into contact, initiating higher rates of conduction at a greater number of sites in a fluid. The rate of heat transfer through a fluid is much higher by convection than it is by conduction. In fact, the higher the fluid velocity, the higher the rate of heat transfer. Heat transfer through a fluid sandwiched between two parallel plates.
- 5. 5 Convection heat transfer strongly depends on the fluid properties dynamic viscosity, thermal conductivity, density, and specific heat, as well as the fluid velocity. It also depends on the geometry and the roughness of the solid surface, in addition to the type of fluid flow (such as being streamlined or turbulent). Convection heat transfer coefficient, h: The rate of heat transfer between a solid surface and a fluid per unit surface area per unit temperature difference. Newton’s law of cooling
- 6. 6 The development of a velocity profile due to the no-slip condition as a fluid flows over a blunt nose. A fluid flowing over a stationary surface comes to a complete stop at the surface because of the no-slip condition. No-slip condition: A fluid in direct contact with a solid “sticks” to the surface due to viscous effects, and there is no slip. Boundary layer: The flow region adjacent to the wall in which the viscous effects (and thus the velocity gradients) are significant. The fluid property responsible for the no-slip condition and the development of the boundary layer is viscosity.
- 7. 7 An implication of the no-slip condition is that heat transfer from the solid surface to the fluid layer adjacent to the surface is by pure conduction, since the fluid layer is motionless, and can be expressed as The determination of the convection heat transfer coefficient when the temperature distribution within the fluid is known The convection heat transfer coefficient, in general, varies along the flow (or x-) direction. The average or mean convection heat transfer coefficient for a surface in such cases is determined by properly averaging the local convection heat transfer coefficients over the entire surface area As or length L as
- 8. 8
- 9. 9 Nusselt Number Heat transfer through a fluid layer of thickness L and temperature difference ∆T. In convection studies, it is common practice to nondimensionalize the governing equations and combine the variables, which group together into dimensionless numbers in order to reduce the number of total variables. Nusselt number: Dimensionless convection heat transfer coefficient Lc characteristic length The Nusselt number represents the enhancement of heat transfer through a fluid layer as a result of convection relative to conduction across the same fluid layer. The larger the Nusselt number, the more effective the convection. A Nusselt number of Nu = 1 for a fluid layer represents heat transfer across the layer by pure conduction.
- 10. 10 • We turn on the fan on hot summer days to help our body cool more effectively. The higher the fan speed, the better we feel. • We stir our soup and blow on a hot slice of pizza to make them cool faster. • The air on windy winter days feels much colder than it actually is. • The simplest solution to heating problems in electronics packaging is to use a large enough fan. Convection in daily life
- 11. 1111 CLASSIFICATION OF FLUID FLOWS Viscous versus Inviscid Regions of Flow Viscous flows: Flows in which the frictional effects are significant. Inviscid flow regions: In many flows of practical interest, there are regions (typically regions not close to solid surfaces) where viscous forces are negligibly small compared to inertial or pressure forces. The flow of an originally uniform fluid stream over a flat plate, and the regions of viscous flow (next to the plate on both sides) and inviscid flow (away from the plate).
- 12. 1212 Internal versus External Flow External flow over a tennis ball, and the turbulent wake region behind. External flow: The flow of an unbounded fluid over a surface such as a plate, a wire, or a pipe. Internal flow: The flow in a pipe or duct if the fluid is completely bounded by solid surfaces. • Water flow in a pipe is internal flow, and airflow over a ball is external flow . • The flow of liquids in a duct is called open- channel flow if the duct is only partially filled with the liquid and there is a free surface.
- 13. 1313 Compressible versus Incompressible Flow Incompressible flow: If the density of flowing fluid remains nearly constant throughout (e.g., liquid flow). Compressible flow: If the density of fluid changes during flow (e.g., high-speed gas flow) When analyzing rockets, spacecraft, and other systems that involve high- speed gas flows, the flow speed is often expressed by Mach number Ma = 1 Sonic flow Ma < 1 Subsonic flow Ma > 1 Supersonic flow Ma >> 1 Hypersonic flow c is the speed of sound whose value is 346 m/s in air at room temperature at sea level. Gas flows can often be approximated as incompressible if the density changes are under about 5 percent, which is usually the case when Ma < 0.3. Therefore, the compressibility effects of air can be neglected at speeds under about 100 m/s.
- 14. 1414 Laminar versus Turbulent Flow Laminar flow: The highly ordered fluid motion characterized by smooth layers of fluid. The flow of high-viscosity fluids such as oils at low velocities is typically laminar. Turbulent flow: The highly disordered fluid motion that typically occurs at high velocities and is characterized by velocity fluctuations. The flow of low- viscosity fluids such as air at high velocities is typically turbulent. Transitional flow: A flow that alternates between being laminar and turbulent. Laminar, transitional, and turbulent flows.
- 15. 1515 Natural (or Unforced) versus Forced Flow Forced flow: A fluid is forced to flow over a surface or in a pipe by external means such as a pump or a fan. Natural flow: Fluid motion is due to natural means such as the buoyancy effect, which manifests itself as the rise of warmer (and thus lighter) fluid and the fall of cooler (and thus denser) fluid. In this schlieren image, the rise of lighter, warmer air adjacent to her body indicates that humans and warm- blooded animals are surrounded by thermal plumes of rising warm air.
- 16. 1616 Steady versus Unsteady Flow • The term steady implies no change at a point with time. • The opposite of steady is unsteady. • The term uniform implies no change with location over a specified region. • The term periodic refers to the kind of unsteady flow in which the flow oscillates about a steady mean. • Many devices such as turbines, compressors, boilers, condensers, and heat exchangers operate for long periods of time under the same conditions, and they are classified as steady-flow devices.
- 17. 1717 One-, Two-, and Three-Dimensional Flows • A flow field is best characterized by its velocity distribution. • A flow is said to be one-, two-, or three-dimensional if the flow velocity varies in one, two, or three dimensions, respectively. • However, the variation of velocity in certain directions can be small relative to the variation in other directions and can be ignored. The development of the velocity profile in a circular pipe. V = V(r, z) and thus the flow is two-dimensional in the entrance region, and becomes one-dimensional downstream when the velocity profile fully develops and remains unchanged in the flow direction, V = V(r).
- 18. 1818 VELOCITY BOUNDARY LAYER Velocity boundary layer: The region of the flow above the plate bounded by δδ in which the effects of the viscous shearing forces caused by fluid viscosity are felt. The boundary layer thickness, δδ, is typically defined as the distance y from the surface at which u = 0.99V. The hypothetical line of u = 0.99V divides the flow over a plate into two regions: Boundary layer region: The viscous effects and the velocity changes are significant. Irrotational flow region: The frictional effects are negligible and the velocity remains essentially constant.
- 19. 19 Wall Shear Stress Shear stress: Friction force per unit area. The shear stress for most fluids is proportional to the velocity gradient, and the shear stress at the wall surface is expressed as The fluids that obey the linear relationship above are called Newtonian Fluids. Most common fluids such as water, air, gasoline, and oils are Newtonian fluids. Blood and liquid plastics are examples of non-Newtonian fluids. In this text we consider Newtonian fluids only. µ dynamic viscosity kg/m⋅s or N⋅s/m2 or Pa⋅s 1 poise = 0.1 Pa ⋅ s
- 20. 20 The viscosity of a fluid is a measure of its resistance to deformation, and it is a strong function of temperature. Cf friction coefficient or skin friction coefficient The friction coefficient is an important parameter in heat transfer studies since it is directly related to the heat transfer coefficient and the power requirements of the pump or fan. Wall shear stress: Friction force over the entire surface: Kinematic viscosity, m2 /s or stoke 1 stoke = 1 cm2 /s = 0.0001 m2 /s
- 21. 21
- 22. 2222 THERMAL BOUNDARY LAYER Thermal boundary layer on a flat plate (the fluid is hotter than the plate surface). A thermal boundary layer develops when a fluid at a specified temperature flows over a surface that is at a different temperature. Thermal boundary layer: The flow region over the surface in which the temperature variation in the direction normal to the surface is significant. The thickness of the thermal boundary layer δt at any location along the surface is defined as the distance from the surface at which the temperature difference T − Ts equals 0.99(T∞− Ts). The thickness of the thermal boundary layer increases in the flow direction, since the effects of heat transfer are felt at greater distances from the surface further down stream. The shape of the temperature profile in the thermal boundary layer dictates the convection heat transfer between a solid surface and the fluid flowing over it.
- 23. 2323 Prandtl Number The relative thickness of the velocity and the thermal boundary layers is best described by the dimensionless parameter Prandtl number The Prandtl numbers of gases are about 1, which indicates that both momentum and heat dissipate through the fluid at about the same rate. Heat diffuses very quickly in liquid metals (Pr << 1) and very slowly in oils (Pr >> 1) relative to momentum. Consequently the thermal boundary layer is much thicker for liquid metals and much thinner for oils relative to the velocity boundary layer.
- 24. 24
- 25. 2525 LAMINAR AND TURBULENT FLOWS Laminar and turbulent flow regimes of candle smoke. The behavior of colored fluid injected into the flow in laminar and turbulent flows in a pipe. Laminar: Smooth streamlines and highly ordered motion. Turbulent: Velocity fluctuations and highly disordered motion. Transition: The flow fluctuates between laminar and turbulent flows. Most flows encountered in practice are turbulent. Laminar flow is encountered when highly viscous fluids such as oils flow in small pipes or narrow passages.
- 26. 2626 Reynolds Number The transition from laminar to turbulent flow depends on the geometry, surface roughness, flow velocity, surface temperature, and type of fluid. The flow regime depends mainly on the ratio of inertia forces to viscous forces (Reynolds number). The Reynolds number can be viewed as the ratio of inertial forces to viscous forces acting on a fluid element. Critical Reynolds number, Recr: The Reynolds number at which the flow becomes turbulent. The value of the critical Reynolds number is different for different geometries and flow conditions. At large Reynolds numbers, the inertial forces, which are proportional to the fluid density and the square of the fluid velocity, are large relative to the viscous forces, and thus the viscous forces cannot prevent the random and rapid fluctuations of the fluid (turbulent). At small or moderate Reynolds numbers, the viscous forces are large enough to suppress these fluctuations and to keep the fluid “in line” (laminar).
- 27. 27
- 28. 28 HEAT AND MOMENTUM TRANSFER IN TURBULENT FLOW Most flows encountered in engineering practice are turbulent, and thus it is important to understand how turbulence affects wall shear stress and heat transfer. However, turbulent flow is a complex mechanism dominated by fluctuations, and the theory of turbulent flow is still not fully understood. Therefore, we must rely on experiments and the empirical or semi-empirical correlations developed for various situations. Turbulent flow is characterized by disorderly and rapid fluctuations of swirling regions of fluid, called eddies, throughout the flow. These fluctuations provide an additional mechanism for momentum and energy transfer. The swirling eddies transport mass, momentum, and energy to other regions of flow much more rapidly than molecular diffusion, greatly enhancing mass, momentum, and heat transfer. Turbulent flow is associated with much higher values of friction, heat transfer, and mass transfer coefficients.
- 29. 29
- 30. 30
- 31. 31
- 32. 32 DERIVATION OF DIFFERENTIAL CONVECTION EQUATIONS
- 35. 35
- 36. 36
- 37. 37 Conservation of Energy Equation
- 38. 38
- 39. 39
- 40. 40 SOLUTIONS OF CONVECTION EQUATIONS FOR A FLAT PLATE
- 41. 41
- 42. 42
- 43. 43
- 45. 45
- 46. 46
- 47. 47 NONDIMENSIONALIZED CONVECTION EQUATIONS AND SIMILARITY
- 48. 48
- 49. 49 FUNCTIONAL FORMS OF FRICTION AND CONVECTION COEFFICIENTS
- 50. 50
- 51. 51
- 52. 52 ANALOGIES BETWEEN MOMENTUM AND HEAT TRANSFER
- 53. 53
- 54. 54
- 55. 55
- 56. 56
- 57. 5757 Some important results from convection equations The velocity boundary layer thickness The local skin friction coefficient The thermal boundary layer thickness Local Nusselt number Reynold analogy Modified Reynold analogy or Chilton-Colburn analogy
- 58. 5858 Summary • Physical Mechanism of Convection Nusselt Number • Classification of Fluid Flows • Velocity Boundary Layer Wall shear sttress • Thermal Boundary Layer Prandtl Number • Laminar and Turbulent Flows Reynolds Number • Heat and Momentum Transfer in Turbulent Flow • Derivation of Differential Convection Equations • Solutions of Convection Equations for a Flat Plate • Nondimensionalized Convection Equations and Similarity • Functional Forms of Friction and Convection Coefficients • Analogies Between Momentum and Heat Transfer