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Shock induced polymorphism phase transitions in high density glass

Liu Xun Cao Xiu-Xia Zhou Xian-Ming Li Jun Li Jia-Bo

Shock induced polymorphism phase transitions in high density glass

Liu Xun, Cao Xiu-Xia, Zhou Xian-Ming, Li Jun, Li Jia-Bo
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  • Plate impact experiments are conducted on high density glass (HDG) with an initial density of ~4.817g/cm3 (Brand ZF6) at a two-stage light gas gun facility. A copper flyer plate is used as a standard sample. Experimental shock pressure is between 52.1GPa and 167.8GPa. A multi-wavelength pyrometer and optical analyzer technique are used to determine the Hugoniot curve, sound velocity and shock temperature of HDG. The experiment results reveal that polymorphism phase transitions occur in HDG under compression, and the onset pressures are ~23, ~78 and ~120GPa, respectively. The measured sound velocity first increases and arrives at about 78GPa, then decreases rapidly, and increases again with pressure increasing. Beyond ~120 GPa, the longitudinal sound velocity turns in to bulk sound velocity, indicating the melting of HDG. Measured shock temperatures also show discontinuities at ~78 and ~120GPa, after which its increase rate becomes small and consistent with the calculated Lindemann melting line, confirming the above HDG phase transformation behaviors. Our Hugoniot data are consistent well with LASL shock Hugoniot data of HDG, which shows discontinuity only at about 23GPa, indicating that the phase transitions at 78 and 120GPa are not first-order ones. Our shock data and the gained knowledge of dynamic response behavior of HDG are valuable for improving the accuracies in sound velocity measurements for metals and non-metals at pressures over a megabar range.
    • Funds:
    [1]

    Yu Y Y, Tan H, Hu J B, Dai C D 2008 Chin. Phys. B 17 264

    [2]

    Peng J X, Jing F Q, Wang L L, Li D H 2005 Acta Phys. Sin. 54 2194 (in Chinese) [彭建祥、经福谦、王礼立、李大红 2005 物理学报 54 2194]

    [3]

    Wang Y G, Chen D P, He H L, Wang L L, Jing F Q 2006 Acta Phys. Sin. 55 4202 (in Chinese) [王永刚、陈登平、贺宏亮、王礼立、经福谦 2006 物理学报 55 4202]

    [4]

    Yu Y Y, Tan H, Hu J B, Dai C D, Chen D N, Wang H R 2008 Acta Phys. Sin. 57 2352 (in Chinese) [俞宇颖、谭 华、胡建波、戴诚达、陈大年、王焕然 2008 物理学报 57 2352]

    [5]

    Hu J B, Yu Y Y, Dai C D, Tan H 2005 Acta Phys. Sin. 54 5750 (in Chinese) [胡建波、俞宇颖、戴诚达、谭 华 2005 物理学报 54 5750]

    [6]

    Tan H 2006 Introduction to Experimental Shock-Wave Physics (Beijing: National Defense Industry Press) p148 (in Chinese) [谭 华 2006 实验冲击波物理导引(北京:国防工业出版社)第148页]

    [7]

    Hu J B, Zhou X M, Tan H 2008 Acta Phys. Sin. 57 2347 (in Chinese) [胡建波、周显明、谭 华 2008 物理学报 57 2347]

    [8]

    Duffy T S, Ahrens T J 1995 J. Geophys. Res. 100 529

    [9]

    Hu J B, Zhou X M, Dai C D, Tan H, Li J B 2008 J. Appl. Phys. 104 083520

    [10]

    Santamara P D, Ross M, Errandonea D, Mukherjee G D, Mezouar M, Boehler R 2009 J. Chem. Phys. 130 124509

    [11]

    Liu Z L, Cai L C, Chen X R, Jing F Q 2008 Phys. Rev. B 77 024103

    [12]

    Hixson R S, Boness D A, Shaner J W, Moriarty J A 1989 Phys. Rev. Lett. 62 637

    [13]

    McQueen R G, Hopson J W, Fritz J N 1982 Rev. Sci. Instrum. 53 1982 245

    [14]

    Alexander C S, Chhabildas L C, Reinhart W D, Templeton D W 2008 Int. J. Impact Eng. 35 1376

    [15]

    McQueen R G, Fritz J N, Morris C E 1984 Shock Wave in Condensed Matter (1983) (Amsterdam: Elsevier Science) p95

    [16]

    Brown J M, Shaner J W 1984 Shock Wave in Condensed Matter (1983) (Amsterdam: Elsevier Science) p91

    [17]

    Millett J C F, Bourne N K, Rosenberg Z 2000 J. Appl. Phys. 87 8457

    [18]

    Bourne N K, Millett J C F 2001 J. Appl. Phys. 89 5368

    [19]

    Mattsson A E 2004 Shock Compression of Condensed Matter (2003) (America institute of physics) 743

    [20]

    Carter W J 1973 High Temp.-High Press. 5 316

    [21]

    Hayes D, Hixson R S, McQueen R G 2000 Shock Compression of Condensed Matter (1999) (America institute of physics) 483

    [22]

    Meyers M A 1994 Dynamic behavior of materials (New York: Wiley-interscience) p101

    [23]

    McQueen R G, March S P, Taylor J W, Fritz J N, Carter W J 1970 High Velocity Impact Phenomena (New York:Academic) p312

    [24]

    Boslough M B, Ahrens T J 1989 Rev. Sci. Instrum. 60 3711

    [25]

    Marsh S P 1980 LASL Shock Hugoniot Data (Berkeley: University of California Press) p392

    [26]

    Li J, Zhou X M, Li J B, Li S N, Zhu W J, Wang X, Jing F Q 2007 Acta Phys. Sin. 56 6557 (in Chinese) [李 俊、周显明、李加波、李赛男、祝文军、王 翔、经福谦 2007 物理学报 56 6557]

    [27]

    Jing F Q 1999 Introduction to Experimental Equation of State (Beijing: Science Press) P213,384 (in Chinese) [经福谦 1999 实验物态方程导引 (北京:科学出版社)] 第213—384页

    [28]

    Heinz D L, Jeanloz R 1984 Phys. Rev. B 30 6045

    [29]

    Akins J A, Ahrens T J 2002 J. Geophys. Lett. 29 101394

    [30]

    Smart R M, Glasser F P 1974 J. Am. Ceram. Soc. 57 378

    [31]

    Furukawa Toshihharu, Brawer S A, White W B 1979 J. Am. Ceram. Soc. 62 351

    [32]

    Nellis W J, Yoo C S 1983 J. Geophys. Res. 95 21749

    [33]

    Prakapenka V P, Shen Guoyin, Dubrovinsky L S, Rivers M L, Sutton S R 2004 J. Phys. Chem. Solids 65 1537

    [34]

    Lyzenga G A, Ahrens T J 1983 J. Geophys. Res. 88 2431

  • [1]

    Yu Y Y, Tan H, Hu J B, Dai C D 2008 Chin. Phys. B 17 264

    [2]

    Peng J X, Jing F Q, Wang L L, Li D H 2005 Acta Phys. Sin. 54 2194 (in Chinese) [彭建祥、经福谦、王礼立、李大红 2005 物理学报 54 2194]

    [3]

    Wang Y G, Chen D P, He H L, Wang L L, Jing F Q 2006 Acta Phys. Sin. 55 4202 (in Chinese) [王永刚、陈登平、贺宏亮、王礼立、经福谦 2006 物理学报 55 4202]

    [4]

    Yu Y Y, Tan H, Hu J B, Dai C D, Chen D N, Wang H R 2008 Acta Phys. Sin. 57 2352 (in Chinese) [俞宇颖、谭 华、胡建波、戴诚达、陈大年、王焕然 2008 物理学报 57 2352]

    [5]

    Hu J B, Yu Y Y, Dai C D, Tan H 2005 Acta Phys. Sin. 54 5750 (in Chinese) [胡建波、俞宇颖、戴诚达、谭 华 2005 物理学报 54 5750]

    [6]

    Tan H 2006 Introduction to Experimental Shock-Wave Physics (Beijing: National Defense Industry Press) p148 (in Chinese) [谭 华 2006 实验冲击波物理导引(北京:国防工业出版社)第148页]

    [7]

    Hu J B, Zhou X M, Tan H 2008 Acta Phys. Sin. 57 2347 (in Chinese) [胡建波、周显明、谭 华 2008 物理学报 57 2347]

    [8]

    Duffy T S, Ahrens T J 1995 J. Geophys. Res. 100 529

    [9]

    Hu J B, Zhou X M, Dai C D, Tan H, Li J B 2008 J. Appl. Phys. 104 083520

    [10]

    Santamara P D, Ross M, Errandonea D, Mukherjee G D, Mezouar M, Boehler R 2009 J. Chem. Phys. 130 124509

    [11]

    Liu Z L, Cai L C, Chen X R, Jing F Q 2008 Phys. Rev. B 77 024103

    [12]

    Hixson R S, Boness D A, Shaner J W, Moriarty J A 1989 Phys. Rev. Lett. 62 637

    [13]

    McQueen R G, Hopson J W, Fritz J N 1982 Rev. Sci. Instrum. 53 1982 245

    [14]

    Alexander C S, Chhabildas L C, Reinhart W D, Templeton D W 2008 Int. J. Impact Eng. 35 1376

    [15]

    McQueen R G, Fritz J N, Morris C E 1984 Shock Wave in Condensed Matter (1983) (Amsterdam: Elsevier Science) p95

    [16]

    Brown J M, Shaner J W 1984 Shock Wave in Condensed Matter (1983) (Amsterdam: Elsevier Science) p91

    [17]

    Millett J C F, Bourne N K, Rosenberg Z 2000 J. Appl. Phys. 87 8457

    [18]

    Bourne N K, Millett J C F 2001 J. Appl. Phys. 89 5368

    [19]

    Mattsson A E 2004 Shock Compression of Condensed Matter (2003) (America institute of physics) 743

    [20]

    Carter W J 1973 High Temp.-High Press. 5 316

    [21]

    Hayes D, Hixson R S, McQueen R G 2000 Shock Compression of Condensed Matter (1999) (America institute of physics) 483

    [22]

    Meyers M A 1994 Dynamic behavior of materials (New York: Wiley-interscience) p101

    [23]

    McQueen R G, March S P, Taylor J W, Fritz J N, Carter W J 1970 High Velocity Impact Phenomena (New York:Academic) p312

    [24]

    Boslough M B, Ahrens T J 1989 Rev. Sci. Instrum. 60 3711

    [25]

    Marsh S P 1980 LASL Shock Hugoniot Data (Berkeley: University of California Press) p392

    [26]

    Li J, Zhou X M, Li J B, Li S N, Zhu W J, Wang X, Jing F Q 2007 Acta Phys. Sin. 56 6557 (in Chinese) [李 俊、周显明、李加波、李赛男、祝文军、王 翔、经福谦 2007 物理学报 56 6557]

    [27]

    Jing F Q 1999 Introduction to Experimental Equation of State (Beijing: Science Press) P213,384 (in Chinese) [经福谦 1999 实验物态方程导引 (北京:科学出版社)] 第213—384页

    [28]

    Heinz D L, Jeanloz R 1984 Phys. Rev. B 30 6045

    [29]

    Akins J A, Ahrens T J 2002 J. Geophys. Lett. 29 101394

    [30]

    Smart R M, Glasser F P 1974 J. Am. Ceram. Soc. 57 378

    [31]

    Furukawa Toshihharu, Brawer S A, White W B 1979 J. Am. Ceram. Soc. 62 351

    [32]

    Nellis W J, Yoo C S 1983 J. Geophys. Res. 95 21749

    [33]

    Prakapenka V P, Shen Guoyin, Dubrovinsky L S, Rivers M L, Sutton S R 2004 J. Phys. Chem. Solids 65 1537

    [34]

    Lyzenga G A, Ahrens T J 1983 J. Geophys. Res. 88 2431

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  • Received Date:  23 November 2009
  • Accepted Date:  30 December 2009
  • Published Online:  05 April 2010

Shock induced polymorphism phase transitions in high density glass

  • 1. (1)College of Physical and Technology, Sichuan University, Chengdu 610065,China; (2)College of Physical and Technology, Sichuan University, Chengdu 610065,China; Laboratory for Shockwave and Detonation Physics, Institute of Fluid Physics ,China Academy of Engineering Physics, Mianyang 621900,China; (3)Laboratory for Shockwave and Detonation Physics, Institute of Fluid Physics ,China Academy of Engineering Physics, Mianyang 621900,China

Abstract: Plate impact experiments are conducted on high density glass (HDG) with an initial density of ~4.817g/cm3 (Brand ZF6) at a two-stage light gas gun facility. A copper flyer plate is used as a standard sample. Experimental shock pressure is between 52.1GPa and 167.8GPa. A multi-wavelength pyrometer and optical analyzer technique are used to determine the Hugoniot curve, sound velocity and shock temperature of HDG. The experiment results reveal that polymorphism phase transitions occur in HDG under compression, and the onset pressures are ~23, ~78 and ~120GPa, respectively. The measured sound velocity first increases and arrives at about 78GPa, then decreases rapidly, and increases again with pressure increasing. Beyond ~120 GPa, the longitudinal sound velocity turns in to bulk sound velocity, indicating the melting of HDG. Measured shock temperatures also show discontinuities at ~78 and ~120GPa, after which its increase rate becomes small and consistent with the calculated Lindemann melting line, confirming the above HDG phase transformation behaviors. Our Hugoniot data are consistent well with LASL shock Hugoniot data of HDG, which shows discontinuity only at about 23GPa, indicating that the phase transitions at 78 and 120GPa are not first-order ones. Our shock data and the gained knowledge of dynamic response behavior of HDG are valuable for improving the accuracies in sound velocity measurements for metals and non-metals at pressures over a megabar range.

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