Simulation and verification of supersonic axisymetric H2-O2 ignition
碩士 === 中華大學 === 機械與航太工程研究所 === 93 === Axisymetric Navier-Stoke equations coupled with chemical kinetic equations were used to solve the supersonic H2-O2 combustion solutions. The numerical scheme is based on central difference with Jameson’s artificial viscosity, 4-stage Runge-Kutta time marching al...
Main Authors: | , |
---|---|
Other Authors: | |
Format: | Others |
Language: | zh-TW |
Published: |
2005
|
Online Access: | http://ndltd.ncl.edu.tw/handle/55762833400120491170 |
id |
ndltd-TW-093CHPI0598022 |
---|---|
record_format |
oai_dc |
spelling |
ndltd-TW-093CHPI05980222016-06-08T04:13:34Z http://ndltd.ncl.edu.tw/handle/55762833400120491170 Simulation and verification of supersonic axisymetric H2-O2 ignition 超音速軸對稱氫氧火焰之模擬與驗證 hsu sheng hsiang 徐勝翔 碩士 中華大學 機械與航太工程研究所 93 Axisymetric Navier-Stoke equations coupled with chemical kinetic equations were used to solve the supersonic H2-O2 combustion solutions. The numerical scheme is based on central difference with Jameson’s artificial viscosity, 4-stage Runge-Kutta time marching algorithm. Three difference chemical kinetic schemes, global 2-step, seven species 7-step, and seven species 8-step were used. The solutions show that seven species 7-step and seven species 8-step are very similar. However, the solution of the global 2-step chemical kinetic provides very little reaction, as suggested try previous researchers. The current numerical prediction gives the ignition position at 12.7 D downstream. However, the experimental result shows an ignition position at 8.25 D downstream. The current H2O formation region is also thinner than the region form experimental measurement. Modification of the inlet pressure, inlet Mach number, artificial viscosity, and grid mesh does not alter the current simulation. 楊一龍 2005 學位論文 ; thesis 56 zh-TW |
collection |
NDLTD |
language |
zh-TW |
format |
Others
|
sources |
NDLTD |
description |
碩士 === 中華大學 === 機械與航太工程研究所 === 93 === Axisymetric Navier-Stoke equations coupled with chemical kinetic equations were used to solve the supersonic H2-O2 combustion solutions. The numerical scheme is based on central difference with Jameson’s artificial viscosity, 4-stage Runge-Kutta time marching algorithm. Three difference chemical kinetic schemes, global 2-step, seven species 7-step, and seven species 8-step were used. The solutions show that seven species 7-step and seven species 8-step are very similar. However, the solution of the global 2-step chemical kinetic provides very little reaction, as suggested try previous researchers. The current numerical prediction gives the ignition position at 12.7 D downstream. However, the experimental result shows an ignition position at 8.25 D downstream. The current H2O formation region is also thinner than the region form experimental measurement. Modification of the inlet pressure, inlet Mach number, artificial viscosity, and grid mesh does not alter the current simulation.
|
author2 |
楊一龍 |
author_facet |
楊一龍 hsu sheng hsiang 徐勝翔 |
author |
hsu sheng hsiang 徐勝翔 |
spellingShingle |
hsu sheng hsiang 徐勝翔 Simulation and verification of supersonic axisymetric H2-O2 ignition |
author_sort |
hsu sheng hsiang |
title |
Simulation and verification of supersonic axisymetric H2-O2 ignition |
title_short |
Simulation and verification of supersonic axisymetric H2-O2 ignition |
title_full |
Simulation and verification of supersonic axisymetric H2-O2 ignition |
title_fullStr |
Simulation and verification of supersonic axisymetric H2-O2 ignition |
title_full_unstemmed |
Simulation and verification of supersonic axisymetric H2-O2 ignition |
title_sort |
simulation and verification of supersonic axisymetric h2-o2 ignition |
publishDate |
2005 |
url |
http://ndltd.ncl.edu.tw/handle/55762833400120491170 |
work_keys_str_mv |
AT hsushenghsiang simulationandverificationofsupersonicaxisymetrich2o2ignition AT xúshèngxiáng simulationandverificationofsupersonicaxisymetrich2o2ignition AT hsushenghsiang chāoyīnsùzhóuduìchēngqīngyǎnghuǒyànzhīmónǐyǔyànzhèng AT xúshèngxiáng chāoyīnsùzhóuduìchēngqīngyǎnghuǒyànzhīmónǐyǔyànzhèng |
_version_ |
1718297518643609600 |