State-resolved modeling of Sharma and Gillespie's shock-tube experiment

2022 ◽  
Author(s):  
Alexander J. Fangman ◽  
Daniil Andrienko
1993 ◽  
Author(s):  
STEPHANE MOREAU ◽  
PIERRE-YVES BOURQUIN ◽  
DEAN CHAPMAN ◽  
ROBERT MACCORMACK

2005 ◽  
Vol 2005.7 (0) ◽  
pp. 87-88
Author(s):  
Kazumichi KOBAYASHI ◽  
Satoru MIKAMI ◽  
Tatsuki OTA ◽  
Takeru YANO ◽  
Shigeo FUJIKAWA ◽  
...  

1970 ◽  
Vol 41 (2) ◽  
pp. 689-697 ◽  
Author(s):  
H. D. Glenn ◽  
B. K. Crowley

Author(s):  
J Falcovitz ◽  
O Igra ◽  
D Igra

We consider a classical shock tube with Helium-filled driver section, and a driven section filled with a He– Ar gaseous mixture of continuously varying composition. We simulate a shock tube experiment, where the driven section composition starts out with pure Ar and ends with pure He (denoted ‘ − ’), or vice versa (denoted ‘+’). The initial pressures are 2 and 0.01 MPa. Two alternate initial species compositions are assumed: ‘Molar fraction’ – a linear distribution of the molar fraction; ‘Mass Fraction’ – a linear distribution of the mass fraction. Wave patterns arising in every case are presented and discussed.


2008 ◽  
Vol T132 ◽  
pp. 014015 ◽  
Author(s):  
T A Ota ◽  
C J Barton ◽  
D A Holder

2019 ◽  
Vol 209 ◽  
pp. 376-388 ◽  
Author(s):  
Jia Cheng ◽  
Chun Zou ◽  
Qianjin Lin ◽  
Shibo Liu ◽  
Yunpeng Wang ◽  
...  

1966 ◽  
Vol 34 (2) ◽  
pp. 127-129
Author(s):  
James D. Hood

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