Ex Parte Scheidecker et al - Page 10



          Appeal No. 2005-2005                                                        
          Application 10/273,845                                                      
          material (spec. at 3).  One of ordinary skill in the art would              
          have appreciated that the flexural modulus of the material is a             
          result effective variable depending on the usage and determining            
          the optimum values of result effective variables is ordinarily              
          within the skill of the art.  See In re Boesch, 617 F.2d 272,               
          205 USPQ 215 (CCPA 1980).  In this case, one skilled in the art             
          would have known to select a material with a lower flexural                 
          modulus if impact resistance was not needed, such as for coating            
          of wires to resist modest compression loads as in the background            
          of WO 98/52197 (pages 3-6).  Moreover, it is not clear how far              
          different the material is in WO 98/52197 because if the flexural            
          modulus before expansion E1 is 200 MPa and the material is                  
          expanded 100%, so that the expanded density D2 is one-half the              
          nonexpanded density D1, the modulus after expansion E2 = E1(D2/D1)2         
          = 200(.5)2 = 50 MPa (equation at bottom of page 18).  Thus, the             
          limitation of a "tensile strength between 10.0 MPa and 50.0 MPa"            
          seems prima facie obvious.                                                  
               We leave it to the examiner to address the merits of the               
          dependent claims.  Some of the relevant teachings have been noted           
          above.                                                                      

                                     CONCLUSION                                       

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