Experimental investigation of liquid spall in laser shock-loaded tin

• Published in: Journal of applied physics Vol. 101; no. 1; pp. 013506 - 013506-7
• Main Authors: de Rességuier, T., Signor, L., Dragon, A., Boustie, M., Roy, G., Llorca, F.
• Format: Journal Article
• Language: English
• Published: United States American Institute of Physics 01.01.2007
• Subjects: CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; Engineering Sciences; EQUATIONS OF STATE; Fluid mechanics; Fluids mechanics; High Energy Physics - Experiment; LASERS; LIQUID METALS; Mechanics; ONE-DIMENSIONAL CALCULATIONS; Physics; PRESSURE RANGE GIGA PA; REFLECTION; REFLECTIVITY; SHOCK WAVES; SIMULATION; SOLIDIFICATION; SPALLATION; STRESSES; TEMPERATURE DISTRIBUTION; TENSILE PROPERTIES; Thermics; TIME RESOLUTION; TIN
• ISSN: 0021-8979; 1089-7550
• DOI: 10.1063/1.2400800

When a metal is shocked above its melting pressure or melted on release, the tensile stresses generated upon reflection of the compressive pulse from a free surface are induced into a liquid state. Instead of the well-known spallation process observed in solid targets, cavitation is expected in the melted material, and liquid fragments are ejected from the free surface. Their size, velocity, and temperature distributions are issues of increasing interest, as well as their impact on other nearby materials, but data are limited on the subject. Here, we present an experimental study performed on tin samples subjected to high pressure laser shocks (ranging from about 50 to 200 GPa ) of short duration ( ∼ 5 ns ) . The results include post-test observations of the ejecta recovered after impact on a polycarbonate shield and time-resolved measurements of the free surface velocity through the shield. For shock pressures below some 80 GPa , the velocity profiles are compared to the predictions of one-dimensional simulations involving a multiphase equation of state. For higher loading pressures, the emergence of the shock at the free surface produces a rapid loss of reflectivity so the particle velocity cannot be determined. In all cases, solidified fragments of tin are recovered on the shield. Their sizes, their shapes, and the induced damage depend significantly on shock pressure, and are indicative of a very wide range of ejection velocities. The data provide a basis for a phenomenological description of the process.