Ex Parte HIRST - Page 8




              Appeal No. 2000-0946                                                                  Page 8                
              Application No. 08/704,217                                                                                  


                     Appellant’s first argument is not persuasive of any error on the examiner’s part                     
              because, as discussed supra, claim 1 does not positively recite structure for                               
              determining or calculating supply voltage from the measured rate of temperature                             
              change.  As for appellant’s second argument, we perceive no requirement in claim 1                          
              that the power source provide a variable voltage.                                                           
                     Appellant’s statement that Figure 4 shows that the rate of change of the heating                     
              element temperature is not proportional to the supply voltage is not well founded.  While                   
              appellant appears to be correct that the voltage applied to the heating element is kept                     
              essentially constant, the changing slope of the current vs. time curve merely                               
              illustrates that the rate of temperature change is a function of other variables, such as                   
              melting of frost on the heating element, for example, in addition to the source voltage.                    
              This is not inconsistent with the examiner’s finding that the rate of temperature change                    
              is proportional to the source voltage.  The supply of a higher voltage, and consequently                    
              a higher current, to the heating element would reasonably be expected to increase the                       
              temperature of the heating element at a higher rate, thereby also increasing the                            
              resistance of the heating element at a higher rate.  While the curve in Figure 4 does                       
              flatten out (i.e., zero slope), regardless of voltage, over certain portions thereof, such as               
              during the melting of the frost, for example, claim 1 does not require that the voltage be                  
              proportional to the rate of temperature change at all times or for any particular length of                 
              time.                                                                                                       








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