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1-D Steady Conduction: Plane Wall

1-D Steady Conduction: Plane Wall. Governing Equation:. Dirichlet Boundary Conditions:. Solution:. temperature is not a function of k. Heat Flux:. heat flux/flow are a function of k. Heat Flow:. Notes: A is the cross-sectional area of the wall perpendicular to the heat flow

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1-D Steady Conduction: Plane Wall

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  1. 1-D Steady Conduction: Plane Wall Governing Equation: Dirichlet Boundary Conditions: Solution: temperature is not a function of k Heat Flux: heat flux/flow are a function of k Heat Flow: • Notes: • A is the cross-sectional area of the wall perpendicular to the heat flow • both heat flux and heat flow are uniform  independent of position (x) • temperature distribution is governed by boundary conditions and length of domain  independent of thermal conductivity (k)

  2. 1-D Steady Conduction: Cylinder Wall Governing Equation: Dirichlet Boundary Conditions: Solution: heat flux is non-uniform Heat Flux: heat flow is uniform Heat Flow: heat flow per unit length • Notes: • heat flux is not uniform  function of position (r) • both heat flow and heat flow per unit length are uniform  independent of position (r)

  3. 1-D Steady Conduction: Spherical Shell Governing Equation: Dirichlet Boundary Conditions: Solution: Heat Flux: heat flux is non-uniform heat flow is uniform Heat Flow: • Notes: • heat flux is not uniform  function of position (r) • heat flow is uniform  independent of position (r)

  4. Thermal Resistance

  5. Thermal Circuits: Composite Plane Wall Circuits based on assumption of isothermal surfaces normal to x direction or adiabatic surfaces parallel tox direction Actual solution for the heat rate q is bracketed by these two approximations

  6. Thermal Circuits: Contact Resistance In the real world, two surfaces in contact do not transfer heat perfectly Contact Resistance: values depend on materials (A and B), surface roughness, interstitial conditions, and contact pressure typically calculated or looked up Equivalent total thermal resistance:

  7. fig_02_04

  8. fig_02_05

  9. Fins: The Fin Equation • Solutions

  10. Fins: Fin Performance Parameters • Fin Efficiency • the ratio of actual amount of heat removed by a fin to the ideal amount of heat removed if the fin was an isothermal body at the base temperature • that is, the ratio the actual heat transfer from the fin to ideal heat transfer from the fin if the fin had no conduction resistance • Fin Effectiveness • ratio of the fin heat transfer rate to the heat transfer rate that would exist without the fin • Fin Resistance • defined using the temperature difference between the base and fluid as the driving potential

  11. Fins: Efficiency

  12. Fins: Efficiency

  13. Fins: Arrays • Arrays • total surface area • total heat rate • overall surface efficiency • overall surface resistance

  14. Fins: Thermal Circuit Equivalent Thermal Circuit Effect of Surface Contact Resistance

  15. Fins: Overview Straight fins of (a) uniform and (b) non-uniform cross sections; (c) annular fin, and (d) pin fin of non-uniform cross section. • Fins • extended surfaces that enhance fluid heat transfer to/from a surface in large part by increasing the effective surface area of the body • combine conduction through the fin and convection to/from the fin • the conduction is assumed to be one-dimensional • Applications • fins are often used to enhance convection when h is small (a gas as the working fluid) • fins can also be used to increase the surface area for radiation • radiators (cars), heat sinks (PCs), heat exchangers (power plants), nature (stegosaurus)

  16. Fins: The Fin Equation • Solutions

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