Consolidation of Mechanically Alloyed Amorphous CoNbZr Powder by HIP

Anovel HIP processing of mechanically alloyed（MA）amorphous powder is developed， based on the densification via viscous flow mechanism， with which it is possible to obtain a fully dense amorphous com− pact of large scale． This study describes the evaluation of viscous flow in a thermal mechanical analyzer （TMA）and the optimization of HIP variables， time， temperature， pressure and heating rate for a nearly full densification of MA amorphous Co7g．5Nb15Zr5．5 powder． The pre−compacted compressive sample of amorphous Co7g．5Nb15Zr5．5 shows a drastic plastic displace− ment after thermal shrinkage in a constant heating rate experiment far below the temperature at the onset of crystallization（鑑）．An analysis of the TMA curve for a porous amorphous compact permits us to derive the displacement rate and the viscosity． The temperature dependence of the newtonian viscosity（η）is fairly well expressed by an Arrhenius typed relation ofη＝ηo exp（221 kJ・mol−1／んT）within the range of the ex− periment in this study． The we11−defined glass temperature（舞）shows a constancy for heating rates above 1．7×10−1K・s−1， but a great increase due to structural relaxation below 8．3×10−2 K・s−1． HIP cmpaction of MA amorphous powder in vacuumed can in a temperature range，馬くT＜7ンunder a I pressure of 196 MPa makes it possible to obtain a high density amorphous product with a diameter of 24 mm at the nearly maximum in our laboratory HIP apparatus． An increase in holding time and／or temperature leads to an increase in relative density of the amorphous HIP compact， approaching to theoretical one． These increases are in good agreement with a HIP map which is constructed based on newtonian viscous flow mechanism with an Arrhenius equation with an increasedηo for MA amorphous powder subjected to exten− SiVe StrUCtUral relaxatiOn． The compressive strength（σF）for the amorphous HIP compact of Co7g．5Nb15Zr5．5 greatly increases with decreasing porosity（瓦）．Apower law of compressive strength is derived asσF＝BP80’5．