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</o:shapelayout></xml><![endif]--></head><body bgcolor=white lang=EN-CA link=blue vlink=purple><div class=WordSection1><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>Dear Lanny<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><div><p class=MsoNoSpacing style='margin:0mm;margin-bottom:.0001pt'><b><span style='font-size:13.5pt;font-family:"Arial","sans-serif"'>With the School Lunch Cooker I let the burner extend 1”/25mm above the cook top and used 2”/50mm tall pot holders. This puts the heat on the pot and shields the stove top with a layer of dead air.<o:p></o:p></span></b></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>I have another interpretation that may be useful. You did the right thing, but the layer of air is not at all dead. What happens is that the buoyancy of the hot molecules is much stronger than the effect of turbulence. Even though the gap under the pot is large, it is not hot ‘down there’ on the lower surface. The heat rapidly rises into the pot. An implementation that most will find useful is to extend the burner higher than the top deck as you have done, then have the larger gap, then put a ring of similar height (a little higher) at about the OD of the pot. <o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>This creates a heat transfer zone that is not easily blown around by transient winds.<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>The suggestion that the space should be small with a high velocity to bring the heat close to the pot is based on the presumption that the hottest molecules do not rise with more force than the turbulent force. In fact the buoyancy force is about 30 times the turbulent force. The heat is always at the top when the flow is in the 200 mm/sec range. “Top” in this case means the top 2mm of the cross section. It is cool right at the surface where the heat flux is taking place.<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>The suggestion that ‘more heat’ gets into the pot if the velocity is high confuses the heat transfer rate with the heat transfer efficiency. They are both efficiencies (ratios) but of different things.<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>Regards<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'>Crispin<o:p></o:p></span></p><p class=MsoNormal><span style='font-size:11.0pt;font-family:"Calibri","sans-serif";color:#1F497D;mso-fareast-language:EN-US'><o:p> </o:p></span></p></div></div></body></html>