Prediction of shock standoff distance with modified rotational relaxation time of air mixture
The rotational relaxation time of an air mixture is modified as an approach to improve accuracy when predicting hypersonic shock standoff distance. A novel atomistic quasi-classical trajectory (QCT) method with a modified approach is devised to drastically reduce computational cost, and rigorously m...
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Published in | Physics of fluids (1994) Vol. 33; no. 4 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
01.04.2021
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Online Access | Get full text |
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Summary: | The rotational relaxation time of an air mixture is modified as an approach to improve
accuracy when predicting hypersonic shock standoff distance. A novel atomistic
quasi-classical trajectory (QCT) method with a modified approach is devised to drastically
reduce computational cost, and rigorously model the rotational relaxation time of
N2 in N2–N and N2–N2 collisions. The
calculated full sets of rotational state-to-state transition rates obtained by the QCT
method are fed into the rotational state-resolved master equations to determine the
rotational relaxation time of N2. Clear discrepancies are observed when the
present rotational relaxation time is compared with existing empirical data for
N2. The existing empirical model is utilized to determine the rotational
relaxation time of other atmospheric gas species. Then the present set of rotational
relaxation times for the air mixture is employed to predict the hypersonic shock standoff
distance over a blunt body of the ground and flight experiments. Compared with the results
from the two-temperature model, the rotational nonequilibrium enlarges the hypersonic
shock standoff distance. This increase in shock standoff distance by the rotational
nonequilibrium is attributed to the delay in chemical reactions inside the shock layers.
The accuracy of the predicted measured shock standoff distance is improved by considering
the present rotational relaxation time of the air mixture. |
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ISSN: | 1070-6631 1089-7666 |
DOI: | 10.1063/5.0045842 |