TY - JOUR
T1 - Generation of shock trains in free liquid jets with a nanosecond green laser
AU - Ursescu, Daniel
AU - Aleksandrov, Veselin
AU - Matei, Dan
AU - Dancus, Ioan
AU - De Almeida, Matias D.
AU - Stan, Claudiu A.
N1 - Publisher Copyright:
© 2020 American Physical Society.
PY - 2020/12/8
Y1 - 2020/12/8
N2 - Shock wave trains in liquid jets were previously generated only by ablation with femtosecond x-ray lasers. Here we show that shock trains in water microjets can be also generated using nanosecond green laser pulses with 1- to 10-mJ energy. The ablation of 15-, 20-, 30-, and 70-μm water microjets opened a gap in the jets and launched an initial shock wave. Fully developed shock trains were observed in the 30- and 70-μm jets up to 250-ns delays, and these trains were also transmitted inside the nozzles. A few tens of nanoseconds after the pulse, the shock dynamics and its pressure became similar to the ones generated by x-ray lasers, with a more rapid pressure decay in thinner jets. At time delays exceeding 100 ns in the 30-μm jets, the leading shock pressure stabilized to an approximately constant pressure of 40 MPa. The energy density deposited in the jets was estimated at 30 MJ/cm3 by comparing the jet gaps in the green and x-ray laser experiments, and matched previous estimates for optical ablation in water. The pressure decay in the 30-μm jets was modeled based on the pressure decay observed in x-ray laser experiments.
AB - Shock wave trains in liquid jets were previously generated only by ablation with femtosecond x-ray lasers. Here we show that shock trains in water microjets can be also generated using nanosecond green laser pulses with 1- to 10-mJ energy. The ablation of 15-, 20-, 30-, and 70-μm water microjets opened a gap in the jets and launched an initial shock wave. Fully developed shock trains were observed in the 30- and 70-μm jets up to 250-ns delays, and these trains were also transmitted inside the nozzles. A few tens of nanoseconds after the pulse, the shock dynamics and its pressure became similar to the ones generated by x-ray lasers, with a more rapid pressure decay in thinner jets. At time delays exceeding 100 ns in the 30-μm jets, the leading shock pressure stabilized to an approximately constant pressure of 40 MPa. The energy density deposited in the jets was estimated at 30 MJ/cm3 by comparing the jet gaps in the green and x-ray laser experiments, and matched previous estimates for optical ablation in water. The pressure decay in the 30-μm jets was modeled based on the pressure decay observed in x-ray laser experiments.
UR - http://www.scopus.com/inward/record.url?scp=85097582054&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85097582054&partnerID=8YFLogxK
U2 - 10.1103/PhysRevFluids.5.123402
DO - 10.1103/PhysRevFluids.5.123402
M3 - Article
AN - SCOPUS:85097582054
SN - 2469-990X
VL - 5
JO - Physical Review Fluids
JF - Physical Review Fluids
IS - 12
M1 - 123402
ER -