4.3 Article

Determination of JWL parameters from underwater explosion test of spherical explosives by continuous velocity probe

期刊

JOURNAL OF ENERGETIC MATERIALS
卷 39, 期 4, 页码 479-493

出版社

TAYLOR & FRANCIS INC
DOI: 10.1080/07370652.2020.1822461

关键词

Pressure-conducted velocity probe; underwater explosion; spherical charge; impedance matching; JWL-EOS

资金

  1. National Natural Science Foundation of China [11272081, 11672067, 11972201]
  2. Research Fund Project of Ningbo University [XYL20014]
  3. Open Fund of Key Laboratory of Impact and Safety Engineering of Ministry of Education [CJ202008]

向作者/读者索取更多资源

This paper presents a new method for determining the Jones-Wilkins-Lee equation of state (JWL-EOS) through underwater explosion tests with spherical charges. Through field tests using RDX, the JWL-EOS parameters were successfully adjusted to plot the adiabatic curves of pressure versus relative volume.
Underwater explosion test has been proven to be a simple way to measure the equation of state of detonation products. In order to further develop this technology, a new method for determining Jones-Wilkins-Lee equation of state (JWL-EOS) by underwater explosion test with spherical charge was designed based on the self-developed pressure-conducted velocity probe in this paper. First of all, we established an experimental system for the measurement of near-field shock wave of spherical charge using the novel probe, which made it possible to continuously record the velocities of detonation wave and shock wave in a given direction. Four field tests were performed using powdery cyclotrimethylene trinitramine (RDX) and the time history curves of detonation-shock wave front were obtained, by which we determined the velocity of detonation (VoD) and initial shock wave velocity. Besides, the detonation pressure was calculated applying impedance matching technique based on interface continuity conditions and acoustic approximation. We also analyzed the attenuation law of peak pressure of near-field shock wave by fitting the full-scale shock wave data. Applying numerical calculation and test-and-error process, we adjusted the six JWL-EOS parameters (A, B, C, R-1,R-2, and omega) constantly to make the error between numerical and experimental attenuation coefficients of peak pressure of shock wave fall within +/- 1%. Finally, the JWL-EOS parameters of powdery RDX of each test were determined, and the adiabatic curves of pressure versus relative volume were plotted as well.

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