Heat and Mass Transfer

❤️‍🔥Heat and Mass Transfer Unit 3 – Convection Heat Transfer

Convection heat transfer involves fluid motion enhancing heat exchange compared to conduction alone. It's crucial in engineering applications like heat exchangers and cooling systems. The process depends on fluid properties, flow characteristics, and temperature differences, quantified by Newton's law of cooling. Convection types include forced, natural, and mixed. Boundary layers, dimensionless numbers, and empirical equations help analyze and predict convective heat transfer. Real-world applications span automotive, HVAC, electronics, and food industries, showcasing convection's importance in thermal management across various fields.

Fundamentals of Convection

  • Convection involves the transfer of heat through the movement of fluids (liquids or gases)
    • Fluid motion enhances heat transfer compared to conduction alone
  • Convective heat transfer occurs due to the combined effects of conduction and fluid motion
  • The rate of convective heat transfer depends on the fluid properties, flow characteristics, and temperature differences
  • Convection plays a crucial role in various engineering applications (heat exchangers, cooling systems, HVAC)
  • The driving force for convective heat transfer is the temperature gradient between the surface and the fluid
  • Convective heat transfer can be quantified using Newton's law of cooling: Q=hA(TsT)Q = hA(T_s - T_\infty)
    • QQ is the convective heat transfer rate (W)
    • hh is the convective heat transfer coefficient (W/m²·K)
    • AA is the surface area (m²)
    • TsT_s is the surface temperature (K)
    • TT_\infty is the fluid temperature far from the surface (K)

Types of Convection

  • Convection can be classified into two main categories: forced convection and natural (or free) convection
  • Forced convection occurs when an external means (pump, fan) is used to drive the fluid motion
    • Examples include air flow over a car's radiator or water flowing through a pipe
  • Natural convection arises from buoyancy forces due to density differences caused by temperature variations in the fluid
    • Hotter fluid rises while cooler fluid sinks, creating a circulatory motion
  • Mixed convection is a combination of forced and natural convection, where both mechanisms influence the heat transfer process
  • The Rayleigh number (RaRa) determines the relative importance of natural convection to forced convection
  • Convection can also be classified as external (flow over a surface) or internal (flow within a confined space)

Boundary Layer Concepts

  • The boundary layer is a thin region near a surface where the fluid velocity changes from zero at the surface to the free-stream velocity
  • Boundary layers develop due to the no-slip condition, which states that the fluid velocity is zero at the surface
  • The velocity boundary layer thickness (δ\delta) is defined as the distance from the surface where the velocity reaches 99% of the free-stream velocity
  • The thermal boundary layer thickness (δt\delta_t) is the distance from the surface where the temperature difference between the fluid and the surface reaches 99% of the total temperature difference
  • The Prandtl number (PrPr) relates the velocity and thermal boundary layer thicknesses: Pr=ναPr = \frac{\nu}{\alpha}
    • ν\nu is the kinematic viscosity (m²/s)
    • α\alpha is the thermal diffusivity (m²/s)
  • Boundary layers can be laminar or turbulent, affecting the heat transfer characteristics
    • Laminar boundary layers have smooth, parallel streamlines and lower heat transfer rates
    • Turbulent boundary layers have chaotic, mixing flow and higher heat transfer rates

Dimensionless Numbers in Convection

  • Dimensionless numbers are used to characterize and analyze convective heat transfer problems
  • The Reynolds number (ReRe) represents the ratio of inertial forces to viscous forces: Re=ρVLμRe = \frac{\rho VL}{\mu}
    • ρ\rho is the fluid density (kg/m³)
    • VV is the fluid velocity (m/s)
    • LL is the characteristic length (m)
    • μ\mu is the dynamic viscosity (kg/m·s)
  • The Nusselt number (NuNu) represents the ratio of convective to conductive heat transfer: Nu=hLkNu = \frac{hL}{k}
    • hh is the convective heat transfer coefficient (W/m²·K)
    • LL is the characteristic length (m)
    • kk is the thermal conductivity (W/m·K)
  • The Prandtl number (PrPr) represents the ratio of momentum diffusivity to thermal diffusivity: Pr=ναPr = \frac{\nu}{\alpha}
  • The Grashof number (GrGr) represents the ratio of buoyancy forces to viscous forces in natural convection: Gr=gβ(TsT)L3ν2Gr = \frac{g\beta(T_s - T_\infty)L^3}{\nu^2}
    • gg is the acceleration due to gravity (m/s²)
    • β\beta is the volumetric thermal expansion coefficient (1/K)

Forced Convection Equations

  • Forced convection equations are used to calculate the heat transfer coefficient and Nusselt number for various flow configurations
  • For external flow over a flat plate, the local Nusselt number can be calculated using the Dittus-Boelter equation: Nux=0.0296Rex4/5Pr1/3Nu_x = 0.0296Re_x^{4/5}Pr^{1/3}
    • Valid for 0.6Pr600.6 \leq Pr \leq 60 and Rex105Re_x \geq 10^5
  • For internal flow in a circular tube, the Nusselt number can be calculated using the Sieder-Tate equation: Nu=0.027Re0.8Pr1/3(μμs)0.14Nu = 0.027Re^{0.8}Pr^{1/3}(\frac{\mu}{\mu_s})^{0.14}
    • Valid for 0.7Pr16,7000.7 \leq Pr \leq 16,700 and Re10,000Re \geq 10,000
    • μ\mu is the fluid viscosity at the bulk temperature
    • μs\mu_s is the fluid viscosity at the surface temperature
  • The Gnielinski correlation can be used for turbulent flow in a circular tube: Nu=(f/8)(Re1000)Pr1+12.7(f/8)1/2(Pr2/31)Nu = \frac{(f/8)(Re - 1000)Pr}{1 + 12.7(f/8)^{1/2}(Pr^{2/3} - 1)}
    • Valid for 0.5Pr20000.5 \leq Pr \leq 2000 and 3000Re5×1063000 \leq Re \leq 5 \times 10^6
    • ff is the friction factor, which can be calculated using the Colebrook equation or Moody chart

Natural Convection Principles

  • Natural convection occurs due to buoyancy forces arising from density differences caused by temperature variations
  • The driving force for natural convection is the Grashof number (GrGr), which represents the ratio of buoyancy forces to viscous forces
  • The Rayleigh number (RaRa) is the product of the Grashof and Prandtl numbers: Ra=GrPrRa = GrPr
    • It characterizes the flow regime in natural convection (laminar, transitional, or turbulent)
  • For natural convection over a vertical plate, the Nusselt number can be calculated using the Churchill and Chu correlation: Nu=(0.825+0.387Ra1/6[1+(0.492/Pr)9/16]8/27)2Nu = (0.825 + \frac{0.387Ra^{1/6}}{[1 + (0.492/Pr)^{9/16}]^{8/27}})^2
    • Valid for Ra1012Ra \leq 10^{12}
  • For natural convection in enclosures (rectangular cavities), the Nusselt number depends on the aspect ratio and Rayleigh number
  • Correlations for natural convection in various geometries (horizontal plates, cylinders, spheres) are available in the literature

Heat Transfer Coefficients

  • The heat transfer coefficient (hh) quantifies the rate of heat transfer between a surface and a fluid
  • It depends on the fluid properties, flow characteristics, and surface geometry
  • Heat transfer coefficients are typically determined experimentally or estimated using empirical correlations
  • The overall heat transfer coefficient (UU) accounts for the combined effects of conduction and convection in a system
    • It is used in the design of heat exchangers and other thermal systems
  • The thermal resistance concept can be used to analyze convective heat transfer in series or parallel arrangements
    • Thermal resistances are analogous to electrical resistances in a circuit
  • The Biot number (BiBi) is a dimensionless parameter that relates the internal conduction resistance to the external convection resistance: Bi=hLckBi = \frac{hL_c}{k}
    • LcL_c is the characteristic length (m)
    • It helps determine whether lumped system analysis can be applied

Real-World Applications

  • Convective heat transfer is encountered in numerous real-world applications across various industries
  • In the automotive industry, convective heat transfer is crucial for engine cooling, radiator design, and cabin air conditioning
  • HVAC (Heating, Ventilation, and Air Conditioning) systems rely on convective heat transfer to maintain comfortable indoor environments
    • Natural convection plays a role in passive cooling strategies (natural ventilation)
    • Forced convection is used in air handling units, fan coil units, and ductwork
  • Heat exchangers, used in power plants, chemical processing, and refrigeration systems, utilize convective heat transfer to efficiently transfer heat between fluids
  • Electronic devices (computer chips, power electronics) require effective convective cooling to dissipate heat and maintain optimal operating temperatures
    • Heat sinks and fans are designed to enhance convective heat transfer
  • In the food industry, convective heat transfer is employed in cooking, baking, and drying processes
    • Ovens, fryers, and dryers rely on forced convection to uniformly heat or remove moisture from food products
  • Renewable energy systems, such as solar thermal collectors and geothermal heat pumps, harness convective heat transfer to capture and utilize thermal energy from the environment


© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.