Abstract:[1] Radiative heat flux predictions for the Huygens probe entry into Titan's atmosphere are presented in this paper. Radiative heating was computed with the radiation code SPECAIR, assuming a Boltzmann distribution of the excited electronic levels at a characteristic temperature taken as the vibrational temperature of the gas. CN violet is found to be the most intense emitter, followed by CN red, C 2 Swan, and at early trajectory points by the first and second positive systems of N 2 . Solutions of the 1-D rad… Show more
“…Caillault et al [31] showed using Boltzmann distributions in thermo-chemical nonequilibrium, that the radiative heating during entry of Huygens probe is primarily attributable to the CN violet system [transition CN(B → X)] and to a lesser extent to the CN red system [transition CN(A → X)]. Hence, an important aspect of this work is the direct assessment of radiative heat flux from the CN populations for which we propose a simplified model for the intensity based on the CN number density.…”
Section: B Radiative Heat Flux Modeling For Titan Atmospheric Entrymentioning
“…Caillault et al [31] showed using Boltzmann distributions in thermo-chemical nonequilibrium, that the radiative heating during entry of Huygens probe is primarily attributable to the CN violet system [transition CN(B → X)] and to a lesser extent to the CN red system [transition CN(A → X)]. Hence, an important aspect of this work is the direct assessment of radiative heat flux from the CN populations for which we propose a simplified model for the intensity based on the CN number density.…”
Section: B Radiative Heat Flux Modeling For Titan Atmospheric Entrymentioning
“…To investigate this assumption, the line-by-line radiation model Specair [30] was used to calculate the absorption coefficient of the test gas at each of the three test conditions. The Specair model was extensively tested and found to provide accurate predictions of the radiation of Titan mixtures [9].…”
Section: A Self-absorption In the Test Gasmentioning
confidence: 99%
“…However, there is a significant level of disagreement between the models and the published experimental data, which creates a need for further data across a wider range of conditions. At gthe peak heating point of the Titan entry trajectory, the CN radical formed by the dissociation of atmospheric methane and nitrogen is the dominant radiator [8][9][10][11]. Recently, a number of shock tube facilities have been used to investigate the radiative emission in Titan mixtures.…”
“…In order to model the EAST experimental setting, we will use the one-dimensional, shock-fitting Euler code Shocking [13][14][15] that simulates the shock-tube flow field by solving the Rankine-Hugoniot (RH) jump equations to determine the post-shock conditions -i.e. by solving the conservation equations of mass, momentum, and global energy across the shock.…”
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