Numerical study of a reacting single coal char particle with different pore structures moving in a hot O2/CO2 atmosphere

Fuel ◽  
2017 ◽  
Vol 206 ◽  
pp. 381-389 ◽  
Author(s):  
Zhicun Xue ◽  
Qinghua Guo ◽  
Yan Gong ◽  
Jianliang Xu ◽  
Guangsuo Yu
Fuel ◽  
2019 ◽  
Vol 256 ◽  
pp. 115967 ◽  
Author(s):  
Zhicun Xue ◽  
Yan Gong ◽  
Qinghua Guo ◽  
Yifei Wang ◽  
Guangsuo Yu

2012 ◽  
Vol 184 (12) ◽  
pp. 2084-2099 ◽  
Author(s):  
Wei He ◽  
Rong He ◽  
Liyong Cao ◽  
Takamasa Ito ◽  
Toshiyuki Suda ◽  
...  

2018 ◽  
Vol 32 (4) ◽  
pp. 4323-4333 ◽  
Author(s):  
Yuan Chen ◽  
Lyuxiao Jiang ◽  
Hui Zhang ◽  
Changdong Sheng

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Mingyan Gu ◽  
Xianhui He ◽  
Jialun Wang ◽  
Fuling Wang ◽  
...  

2016 ◽  
Vol 73 (10) ◽  
pp. 4151-4169
Author(s):  
Tatsuya Yamashita ◽  
Masatsugu Odaka ◽  
Ko-ichiro Sugiyama ◽  
Kensuke Nakajima ◽  
Masaki Ishiwatari ◽  
...  

Abstract Cloud convection of a CO2 atmosphere where the major constituent condenses is numerically investigated under a setup idealizing a possible warm atmosphere of early Mars, utilizing a two-dimensional cloud-resolving model forced by a fixed cooling profile as a substitute for a radiative process. The authors compare two cases with different critical saturation ratios as condensation criteria and also examine sensitivity to number mixing ratio of condensed particles given externally. When supersaturation is not necessary for condensation, the entire horizontal domain above the condensation level is continuously covered by clouds irrespective of number mixing ratio of condensed particles. Horizontal-mean cloud mass density decreases exponentially with height. The circulations below and above the condensation level are dominated by dry cellular convection and buoyancy waves, respectively. When 1.35 is adopted as the critical saturation ratio, clouds appear exclusively as intense, short-lived, quasi-periodic events. Clouds start just above the condensation level and develop upward, but intense updrafts exist only around the cloud top; they do not extend to the bottom of the condensation layer. The cloud layer is rapidly warmed by latent heat during the cloud events, and then the layer is slowly cooled by the specified thermal forcing, and supersaturation gradually develops leading to the next cloud event. The periodic appearance of cloud events does not occur when number mixing ratio of condensed particles is large.


Fuel ◽  
2008 ◽  
Vol 87 (6) ◽  
pp. 905-914 ◽  
Author(s):  
Vasilije Manovic ◽  
Mirko Komatina ◽  
Simeon Oka

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