Shock compression of organic polymers and proteins: Ultrafast structural relaxation dynamics and energy landscapes

被引:29
作者
Kim, H [1 ]
Hambir, SA [1 ]
Dlott, DD [1 ]
机构
[1] Univ Illinois, Sch Chem Sci, Urbana, IL 61801 USA
关键词
D O I
10.1021/jp994153o
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The response of organic polymers and proteins including poly(methyl methacrylate) (PMMA) and the protein bovine serum albumin (BSA) to a short duration 4.5 GPa shock pulse, termed a "nanoshock", is studied using ultrafast coherent Raman spectroscopy (CARS) to monitor density-dependent vibrational frequency shifts of a dye molecule probe. In conventional shock compression experiments, a two-part response of PMMA to fast compression is usually explained with a phenomenological viscoelastic model. The molecular basis for this two-part response is discussed here using an energy landscape model to describe large-amplitude structural relaxation of shocked supercooled liquids. The polymers and the protein show an instantaneous response to the steeply rising shock front, viewed as a vertical transition to a new region of the energy landscape with radically different topography. A slower similar to 300 ps response is also observed, attributed to large-amplitude structural relaxation along the rugged shocked energy landscape. A viscoelastic model is used to determine an effective shock viscosity eta approximate to 3 Pa.s for the solid samples. This extremely small value (compared to eta > 10(12) Pa.s expected for supercooled liquids) is explained as a result of the very large strain rate and the extensive plastic deformation, which causes even seemingly rigid solids to flow. After the short duration (similar to 2 ns) nanoshock unloads and the samples become frozen, for at least tens of nanoseconds, in a state where the dye vibrational shift indicates a negative pressure of about -1 GPa. The negative pressure means the local density near the dye has decreased, the sample has become more permeable, and the sample is unstable to spontaneous expansion of the polymer chains. The energy landscape model provides a framework for understanding the fast cycle of compression and expansion and how to optimize the generation and detection of large-amplitude structural relaxation processes.
引用
收藏
页码:4239 / 4252
页数:14
相关论文
共 66 条
[1]   PHOTOMECHANICAL BASIS OF LASER-ABLATION OF BIOLOGICAL TISSUE [J].
ALBAGLI, D ;
DARK, M ;
PERELMAN, LT ;
VONROSENBERG, C ;
ITZKAN, I ;
FELD, MS .
OPTICS LETTERS, 1994, 19 (21) :1684-1686
[2]  
Ashcroft N. W., 1973, SOLID STATE PHYS
[3]  
Barbara P. F., 1990, ADV PHOTOCHEM, V15, P1, DOI [DOI 10.1002/9780470133453.CHL, DOI 10.1103/PhysRevLett.88.158101]
[4]   LASER INTERFEROMETER FOR MEASURING HIGH VELOCITIES OF ANY REFLECTING SURFACE [J].
BARKER, LM ;
HOLLENBACH, RE .
JOURNAL OF APPLIED PHYSICS, 1972, 43 (11) :4669-+
[5]   SHOCK-WAVE STUDIES OF PMMA, FUSED SILICA, AND SAPPHIRE [J].
BARKER, LM ;
HOLLENBACH, RE .
JOURNAL OF APPLIED PHYSICS, 1970, 41 (10) :4208-+
[6]   Laser flash photolysis studies of some rhodamine dyes - Characterisation of the lowest excited singlet state of Rhodamine 3B, Sulforhodamine B and Sulforhodamine 101 [J].
Beaumont, PC ;
Johnson, DG ;
Parsons, BJ .
JOURNAL OF THE CHEMICAL SOCIETY-FARADAY TRANSACTIONS, 1998, 94 (02) :195-199
[7]   COMPARISON OF A VISCOELASTIC THEORY OF SOLVATION DYNAMICS TO TIME-RESOLVED EXPERIMENTS IN A NONPOLAR SOLUTION [J].
BERG, M .
CHEMICAL PHYSICS LETTERS, 1994, 228 (4-5) :317-322
[8]   Viscoelastic continuum model of nonpolar solvation. 1. Implications for multiple time scales in liquid dynamics [J].
Berg, M .
JOURNAL OF PHYSICAL CHEMISTRY A, 1998, 102 (01) :17-30
[9]   A viscoelastic continuum model of non-polar solvation. II. Vibrational dephasing in moderate to high-viscosity liquids and glasses [J].
Berg, MA ;
Hubble, HW .
CHEMICAL PHYSICS, 1998, 233 (2-3) :257-266
[10]  
BLOOMQUIST DD, 1979, B AM PHYS SOC, V24, P714