Heat pipes

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Heat pipes

  1. 1. A Presentation on Heat PipesSubmitted to: Submitted By:Dr.-Ing. Jyotirmay Mathur Subhash PatelAssociate Professor (2011PME5264)MNIT, Jaipur
  2. 2. Heat Pipe Background• 1800s – A. M. Perkins and J. Perkins developed Perkins tube• 1944 – R. S. Gaugler introduced the use of a wicking structure• 1964 – G. M. Grover published research and coined the “Heat Pipe” name
  3. 3. Transfer of Heat Heat Added Heat Released Heat Sink Heat Pipe Heat Processor*Drawing is not to scale.
  4. 4. Heat Transfer within a Heat Pipe Heat Absorbed Container Heat Released Wick Structure Evaporation Condensation Wick Structure Heat Absorbed Container Heat Released*Drawing is not to scale.
  5. 5. Component of heat pipe Container• Metal Tubing, usually copper or aluminum.• Provides a medium with high thermal conductivity.• Shape of tubing can be bent or flattened.
  6. 6. Working Fluid• Pure liquids such as helium, water and liquid silver• Impure solutions cause deposits on the interior of the heat pipe reducing its overall performance.• The type of liquid depends on the temperature range of the application.
  7. 7. Examples of Working Fluid BOILING PT. AT USEFUL MELTING ATM. PRESSUREMEDIUM RANGE PT. (° C ) (° C) (° C)Helium - 271 - 261 -271 to -269Ammonia - 78 - 33 -60 to 100 Water 0 100 30 to 200 Silver 960 2212 1800 to 2300
  8. 8. Choosing the Working Fluid Chi(1976) developed a parameter of gauging the effectiveness of a working fluid called the liquid transport factor: l Nl l lWhere is the latent heat of vaporization and is the surface tension. Subscript refers to the liquid (Peterson, 1994).
  9. 9. The wicking structure Axial Groove WickCreated by carving out grooves on the interior coreof the Heat Pipe.
  10. 10. Screen Mesh WickUtilizes multiple wire layers to create a porous wick.Sintering can be used.
  11. 11. Sintered Powder WickUtilizes densely packed metal spheres.Sintering must be used to solidify the spheres.
  12. 12. Purpose of the Wick• Transports working fluid from the Condenser to the Evaporator.• Provides liquid flow even against gravity.
  13. 13. How the Wick Works• Liquid flows in a wick due to capillary action.• Intermolecular forces between the wick and the fluid are stronger than the forces within the fluid.• A resultant increase in surface tension occurs.
  14. 14. Thermodynamic Cycle• 1-2 Heat applied to evaporator through external sources vaporizes working fluid to a saturated(2’) or superheated (2) vapor.• 2-3 Vapor pressure drives vapor through adiabatic section to condenser.• 3-4 Vapor condenses, releasing heat to a heat sink.• 4-1 Capillary pressure created by menisci in wick pumps condensed fluid into evaporator section.• Process starts over.
  15. 15. Ideal Thermodynamic Cycle(Faghiri, 1995)
  16. 16. Heat Pipe Applications• Electronics cooling- small high performance components cause high heat fluxes and high heat dissipation demands. Used to cool transistors and high density semiconductors.• Aerospace- cool satellite solar array, as well as shuttle leading edge during reentry.• Heat exchangers- power industries use heat pipe heat exchangers as air heaters on boilers.• Other applications- production tools, medicine and human body temperature control, engines and automotive industry.
  17. 17. Types of Heat Pipes• Thermosyphon- gravity assisted wickless heat pipe. Gravity is used to force the condensate back into the evaporator. Therefore, condenser must be above the evaporator in a gravity field.• Leading edge- placed in the leading edge of hypersonic vehicles to cool high heat fluxes near the wing leading edge. (Faghiri, 1995)• Rotating and revolving- condensate returned to the evaporator through centrifugal force. No capillary wicks required. Used to cool turbine components and armatures for electric motors.• Cryogenic- low temperature heat pipe. Used to cool optical instruments in space. (Peterson, 1994)
  18. 18. Types of Heat Pipes• Flat Plate- much like traditional cylindrical heat pipes but are rectangular. Used to cool and flatten temperatures of semiconductor or transistor packages assembled in arrays on the top of the heat pipe. (Faghiri,1995)
  19. 19. Types of Heat Pipes• Micro heat pipes- small heat pipes that are noncircular and use angled corners as liquid arteries. Characterized by the equation: rc /rh 1 where rc is the capillary radius, and rh is the hydraulic radius of the flow channel. Employed in cooling semiconductors (improve thermal control), laser diodes, photovoltaic cells, medical devices.
  20. 20. Types of Heat Pipes• Variable conductance- allows variable heat fluxes into the evaporator while evaporator temperature remains constant by pushing a non- condensable gas into the condenser when heat fluxes are low and moving the gas out of the condenser when heat fluxes are high, thereby, increasing condenser surface area. They come in various forms like excess-liquid or gas- loaded form. The gas-loaded form is shown below. Used in electronics cooling. (Faghiri,1995)
  21. 21. Types of Heat Pipes• Capillary pumped loop heat pipe- for systems where the heat fluxes are very high or where the heat from the heat source needs to be moved far away. In the loop heat pipe, the vapor travels around in a loop where it condenses and returns to the evaporator. Used in electronics cooling. (Faghiri, 1995)
  22. 22. Main Heat Transfer Limitations• Capillary limit- occurs when the capillary pressure is too low to provide enough liquid to the evaporator from the condenser. Leads to dry out in the evaporator. Dry out prevents the thermodynamic cycle from continuing and the heat pipe no longer functions properly.• Boiling Limit- occurs when the radial heat flux into the heat pipe causes the liquid in the wick to boil and evaporate causing dry out.
  23. 23. Heat Transfer Limitations• Entrainment Limit- at high vapor velocities, droplets of liquid in the wick are torn from the wick and sent into the vapor. Results in dry out.• Sonic limit- occurs when the vapor velocity reaches sonic speed at the evaporator and any increase in pressure difference will not speed up the flow; like choked flow in converging-diverging nozzle. Usually occurs during startup of heat pipe.• Viscous Limit- at low temperatures the vapor pressure difference between the condenser and the evaporator may not be enough to overcome viscous forces. The vapor from the evaporator doesn’t move to the condenser and the thermodynamic cycle doesn’t occur.
  24. 24. The stages in the design :( i) Select wick and Wall materials(ii) Select working fluids Criteria - limitations - pressure -priming -handling -purity etc .(iii) Examine wick types : Homogeneous rejected Arterial selected
  25. 25. The stages in the design :(iv) Determine artery sizes(v) Examine radial resistance to heat flow(vi) Examine overall pressure balance of proposed design(vii) Select final configuration on basis of (vi) and such features as manufacturing difficulties etc.
  26. 26. Container Design• Things that should be considered for container design: – Operating temperature range of the heat pipe. – Internal operating pressure and container structural integrity. – Evaporator and condenser size and shape. – Possibility of external corrosion. – Prevent leaks. – Compatibility with wick and working fluid.• Stresses: – Since the heat pipe is like a pressure vessel it must satisfy ASME pressure vessel codes.
  27. 27. Container Design• Typical materials: – Aluminum – Stainless steel – Copper – Composite materials – High temperature heat pipes may use refractory materials or linings to prevent corrosion.
  28. 28. Sample DesignA heat pipe is required which will be capable oftransferring a minimum of 15 W at vapourtemperatures between 0 and 80 0C over a distance of1 m in zero gravity (a satellite application) .Restraints on t he design are such that the evaporatorand condenser sections are each 8 cm long , locatedat each end of t he heat pipe , and the maximumpermissible temperature drop between the outside wallof the evaporator and the outside Hall of thecondenser is 6 0 C. Because of Height and volumelimitation, the cross - sectional area of the vapourspace should not exceed 0 . 197 cm 2 • The heat pipemust also with -stand bonding temperatures.
  29. 29. Selection of Material• The selection of wick and wall material is based in various criteria.• In this problem mass being an important parameter• So Aluminium alloy (HT30) is chosen for the wall, and Stainless Steel for the Wick.
  30. 30. Selection of Working Fluid Working fluid compatible with the wall and wick materials, based on available data, includes:• Freon 11• Freon 113• Acetone• Ammonia The limitations on heat transport must now be examined for each working fluid.
  31. 31. Heat pipe Compatibility• Working fluid/ material compatibility. (Faghiri, 1995)
  32. 32. Conclusion on Selection of Working Fluid• After the various examination like Sonic Limit, Entrainment Limit, Wicking Limit, Priming of the Wick Acetone is Selected.• Properties of Acetone are shown
  33. 33. ACETONE
  34. 34. Detail Design
  35. 35. Circumferential liquid distribution• The circumferential wick thickness is limited by the fact that the temperature drop between the vapour space and the outside surface of the heat pipe and vice versa should be 3 0 c maximum Assuming that the temperature drop through the aluminum wall is negligible , the thermal conductivity of the wick may be determined and used in steady state condition.
  36. 36. Final Analysis
  37. 37. Computational Study of Improving the Efficiency of Photovoltaic Panels in the UAEThe efficiency of photovoltaic cells decreases astemperature increases, therefore cooling is essential atelevated illumination situations for instance concentratingsystems, or hot and humid conditions.•With the average temperature in the UAE reaching up to42 C in the summer the cell temperature could reach upto 80 C which decreases the output power by up to0.65%/K, fill factor to 0.2%/K and conversion efficiencyto 0.08%/K of the PV module, above the operatingtemperature .
  38. 38. •a reduction by 20 C will give an increase inefficiency between 0.6 and 1%.•The overall reduction in the highest possibleoutput power (Pmax) of a solar cell decreases asthe cell temperature increase, shown in Fig.
  39. 39. Heat Produced by Photovoltaic Cells•When PV modules are exposed to sunlight it convertsonly 10% to 15% of the light to electricity the rest isconverted to heat.•PV panels are rated at 25 C and isolation of 1 kW/m².The power output of PV cells can be estimated from theexpected Nominal Operating Cell Temperature (NOCT),defined as the open circuit temperature of the module at800 W/m² irradiance (on cell surface), air temperature of20 C, 1 m/s wind velocity and mounted with an openback.
  40. 40. Ross, R.G. (1980) approximation can beused to calculate the cell temperature (T cell)
  41. 41. Heat Pipe Selection•The two main assessments for the heat pipe design isthe selection of the heat pipe’s working fluid andenvelope (wick) materials for compatibility with theheat pipe.•The second main decision is the designing of the wickto cool the PV panel reliably, under any orientation andenvironmental conditions.
  42. 42. Heat Pipe Materials•Falling under the temperature range of -20 to 1000 C,two potential heat pipe wall and wick materials arealuminum and copper.•In this study copper is selected for its higher thermalconductivity as compared to aluminum.•Compatible working fluids for copper according tosurveys by Dunn and Reay, Brennan and Kroliczek andAnderson are:Compatible with copper: Water, Methanol, EthanolIncompatible/Unsuitable with copper: Ammonia ,Acetone
  43. 43. Heat Pipe Fluid Selection SelectionTypical results of the compatibility of working fluidand wall material are being shown in Fig. and it isshown that the power output of copper/water heat pipeis six times greater than the other fluids.
  44. 44. Description of the Proposed Finned Heat Pipe• After the choice of heat pipe and working fluid, the next step was the selection of fin arrangements. In this case, the fins were arranged according to the constrained of the need to fit between the rear side of the PV panel and the result of cooling the panel.• The 3D profile of the proposed arrangement used is shown in Fig.
  45. 45. •the glass provides protection for the solar cells and insome cases anti-reflection coatings are applied forreduction in light scattering. T•The PV panel is attached to an aluminum frame to beis beneficial for the proposed finned heat pipearrangement due to the high conductivity thataluminum can achieve.•The proposed finned heat pipe arrangement consist acopper heat pipe with attached aluminum fins and analuminum saddle acting as a heat sink for the finnedheat pipe.
  46. 46. ResultsThe climatic conditions in the UAE lead to thecorresponding cell temperatures given by the Ross, R.G.
  47. 47. Results
  48. 48. Results
  49. 49. Results
  50. 50. Discussions•the use of fins on heat pipe is more efficient as comparedto heat pipes alone.•the cooling of PV panels to its maximum operatingefficiency by maintaining the solar cell operatingtemperature under the UAE’s climatic conditions can beobtained with the help of the proposed finned heat pipe.•This study confirms the advantages of a finned heat pipefor practical use, especially in the high-temperatureregion.•The proposed finned heat pipe can be used to passivelyremove the heat, accepting high heat flux by naturalconvection, at a much lower heat flux.
  51. 51. REFERENCES• Computational Study of Improving the Efficiency of Photovoltaic Panels in the UAE: Ben Richard Hughes, Ng Ping Sze Cherisa, and Osman Beg, World Academy of Science, Engineering and Technology 73 2011.• Fundamentals of Heat Pipes by Widah Saied• Heat Pipes by P.D. Dunn and D.A. Reay• Nptel
  52. 52. Nomenclature
  53. 53. Nomenclature
  54. 54. THANK YOU

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