TY - JOUR
T1 - Nano-second Laser-induced Plasma Shock Wave in Air for Non-contact Vibration Tests
AU - Hosoya, N.
AU - Nagata, M.
AU - Kajiwara, I.
AU - Umino, R.
N1 - Publisher Copyright:
© 2016, Society for Experimental Mechanics.
PY - 2016/9/1
Y1 - 2016/9/1
N2 - Herein a vibration test method is discussed based on a non-contact, non-destructive excitation input using a laser-induced plasma (LIP) shock wave and a non-contact input estimation using Newton’s second law of motion. We have previously introduced a non-contact vibration test method using an excitation force generated by laser ablation, but it cannot be used when the target structure is lightweight, fragile, and small-sized because a crater with a diameter of several micrometers is created. The LIP generates a highly reproducible shock wave, which become an excitation force to a target structure. This shock wave depends on the gas density, gas specific heat ratio, laser fluence, and ambient environment. If these parameters are constant, the LIP excitation force can be estimated beforehand, allowing only the output measurement to determine the frequency response measurement of an input–output relationship of the target structure. After calibrating the LIP excitation, the frequency response function of a target structure can be obtained.
AB - Herein a vibration test method is discussed based on a non-contact, non-destructive excitation input using a laser-induced plasma (LIP) shock wave and a non-contact input estimation using Newton’s second law of motion. We have previously introduced a non-contact vibration test method using an excitation force generated by laser ablation, but it cannot be used when the target structure is lightweight, fragile, and small-sized because a crater with a diameter of several micrometers is created. The LIP generates a highly reproducible shock wave, which become an excitation force to a target structure. This shock wave depends on the gas density, gas specific heat ratio, laser fluence, and ambient environment. If these parameters are constant, the LIP excitation force can be estimated beforehand, allowing only the output measurement to determine the frequency response measurement of an input–output relationship of the target structure. After calibrating the LIP excitation, the frequency response function of a target structure can be obtained.
KW - Frequency response function measurement
KW - Laser-induced plasma
KW - Non-contact vibration tests
KW - Reliability coefficient
KW - Shock wave
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U2 - 10.1007/s11340-016-0167-9
DO - 10.1007/s11340-016-0167-9
M3 - Article
AN - SCOPUS:84968572427
SN - 0014-4851
VL - 56
SP - 1305
EP - 1311
JO - Experimental Mechanics
JF - Experimental Mechanics
IS - 7
ER -