Page 284 - The Effect of Hydrogen and Hydrides - ebook first test
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Figure 5-11:   Bulk formation free energies of the ,  and zirconium hydride phases, obtained from point defect modelling at
                             various temperatures (from [Thuinet & Besson, 2012]).



                                                                          
                                  




                                                                       
                                                                             
                                                           and 35 mJ/m 2                        
                         ≈ 0 and 35 mJ/m 2

                                                                                               
                                                                                 



                                  
                                                      
                                                               
                                                      (%) ≫    (%)
                                                    33
                                                             11
                                                       ̅ ≈ 0.
                                                          
                                                                            < 0.6%.
                                                                      ̅ = 0
                                                                         
                                 ′
                     
                            
                                               
                                        
                     (%)/   (%)(   ) >    (%)/   (%)(),
                          11
                                             11
                   33
                                      33
                                                                
                                         
                                                                                             











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