Laser absorption measurements of temperature, pressure, CO, and CO2 at near-MHz rates in post-detonation fireballs with comparison to synthetic measurements

C Charles J. Schwartz (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) R Rebekah L. Travis (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) C Cohen Nunes (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) S Steven F. Son (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) D Daniel R. Guildenbecher (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) A Anthony A. Egeln (Sandia National Laboratories 2 , Albuquerque, New Mexico 87185,) R Ryan Houim (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,) C Christopher S. Goldenstein (School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,)

Abstract

A laser absorption spectroscopy (LAS) diagnostic was used to obtain measurements of temperature, pressure, CO, and CO2 at 500 kHz or 1 MHz in post-detonation fireballs produced by hemispherical samples of pentaerythritol tetranitrate (PETN). A quantum-cascade laser was scanned over multiple CO absorption transitions near 2008.5 cm−1 at 1 MHz, while an interband-cascade laser was scanned over a CO2 absorption transition near 2394.8 cm−1 at 500 kHz. Light from each laser was combined onto a single path and passed through a detonation chamber approximately 83 mm above the 12-mm diameter hemispherical PETN charge. The CO and CO2 absorption signals were post-processed to obtain time histories of temperature, pressure, species column pressures (PCOL, PCO2L), and species column mole fractions (XCOL, XCO2L). Additionally, schlieren imaging was performed simultaneously at 500 kHz to aid interpretation of the LAS measurements. Experimental and synthetic (i.e., CFD based) LAS measurements were compared to evaluate the accuracy of the CFD model and its ability to model the turbulent afterburning of the detonation products in air. In general, the experimental measurements exhibit reasonable agreement with the synthetic measurements at early times; thereby supporting the accuracy of the CFD model. Periods of disagreement between experimental and synthetic measurements at later times are most likely due to a reflected shock and detonator cavity jetting, which are not accounted for in the CFD model.

Article Details

Volume / Issue Vol. 139, Issue 7
Published February 21, 2026
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

C

Charles J. Schwartz

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

R

Rebekah L. Travis

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

C

Cohen Nunes

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

S

Steven F. Son

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

D

Daniel R. Guildenbecher

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

A

Anthony A. Egeln

Sandia National Laboratories 2 , Albuquerque, New Mexico 87185,

R

Ryan Houim

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,

C

Christopher S. Goldenstein

School of Mechanical Engineering, Purdue University 1 , West Lafayette, Indiana 47907,