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1. ¦¨®Ö (nucleation):
        
      ©w¸q¡X The formation of very small (often submicroscopic) particles, or nuclei, of the new phase,
                 which are capable of growing.
 
      A. §¡½è¦¨®Ö (Homogeneous Nucleation)
 
              (driving force)¡X (Gv)
                  
                    GN = net free energy change
                    Gv = bulk free energy difference
                      r   = radius of a nucleus
                     = surface energy
              
              Critical radius of the stable nucleus (r*)
                  
 
      “        Free energy barrier to nucleation
                  
                        
              Effect of supercooling (undercooling)
                  
                  
                       HF = latent heat of fusion
                        TM = melting point
                       T = supercooling
 
      B. «D§¡½è¦¨®Ö (Heterogeneous Nucleation)
              ¤j¦h¼Æ±¡§Î
              interfaces, grain boundaries, precipitates, and inclusions.
              critical nucleus is smaller, rate of formation is greater.
              unknown interactions between nucleus and other ¡§impurities¡¨ difficult to analyze

 

2. µ²´¹¥Íªø (crystal growth)
 
      ©TÅ餤ªºÁû²Éªø®É¶¡¦b°ª·Å¤U·|º¥º¥ªø¤j
      driving force reduction in interfacial area between grains.
 
      A. ©TÅé/²GÅ鶡¥­·Æ¬É­±¤Wªºµ²´¹¥Íªø
      B. ´¹­±¤W¦¨®Ö(Surface Nucleation)«á¡u¶¥¡vªº¥Íªø
      C. µ²´¹ªºÁ³±Û¥Íªø(Spiral Growth)
      D. ´¹¬É¤W¹L§N(undercooling)¹ïµ²´¹¥Íªø³t²vªº¼vÅT
      E. ¿Nµ²¤¤ªºµ²´¹¥Íªø ¡V ´¹¬É²¾°Ê
      F. ±`¥Îªº¤H³y´¹Åé¤èªk (Synthetic Crystals Growing)
              (1)  Czochralski
              (2)  flame fusionc
              (3)  floating-zone
              (4)  hydrothermal


3. ÂX´²§@¥Î (diffusion)
 
      ©w¸q¡X The movement of atoms or molecules in a material.
      [Kinetics¡Xthe totality of time-dependent mass transport and phase transformation phenomena in solids.]
 
      A. ÂX´²§@¥Î¤¶²Ð
              ÂX´²¾÷¨î:ªÅ¦ìÂX´²»P´¡¤Jª«ÂX´²(Vacancy diffusion and Interstitial diffusion)
              ÂX´²§@¥Îªº¬¡¤Æ¯à (activation energy, Q)
              ÂX´²§@¥ÎªººØÃþ (types of diffusion)
              ÂX´²§@¥Îªº¹ê¨Ò-- »É-ÂìÂX´²
              
      B. í©wª¬ºA¤UªºÂX´²(steady-state diffusion, and D is a constant)
              Fick¡¦s First Law
 
      C. ¤£Ã­©wª¬ºA¤UªºÂX´²(non-steady-state diffusion, and D is a constant)
              Fick¡¦s Second Law
              ÂX´²¨Ó·½ªº¤Æ¾Ç¿@«×¥i¤À¬°(1)©T©w©M(2)ÅܤÆ
 
      D. ÂX´²«Y¼Æ(diffusion coefficient, D)ÀH·Å«×ªºÅܤÆ
              
              Arrhenius plot
 
      E. ÂX´²±µ¦X (diffusion bonding)
 
      F. ¿Nµ²§@¥Î (sintering)
              ²yª¬Áû²Éªº¿Nµ²
              ¿Nµ²§@¥Îªº¤TºØÂX´²¾÷¨î¡XÅé¡B´¹¬É¡Bªí­±¡C
              ¿Nµ²§@¥Î¶i¦æ®ÉªºÂX´²±¡§Î
 
      G. ÂX´²§@¥Î¦³§Qªº±¡ªp
              °ª·Å (at high T)
              ÂX´²ªº­ì¤l¤p (the diffusion atom is small [e.g., C in Fe])
              ´¹®æÃP´² (the packing factor of the host structure is low [e.g., bcc vs. fcc])
              Áäµ²®z (the bonds of the host structure are weak [e.g., low-melting materials])
              §÷®Æ¦³¯Ê³´ (there are defects in the material [e.g., vacancies or GB])
 

 

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