Theoretical simulations on pulsed exciplex pumped Rb vapor laser

2021 ◽  
Vol 141 ◽  
pp. 107165
Author(s):  
Jinghua Huang ◽  
Chenyi Su ◽  
Xingqi Xu ◽  
Bailiang Pan
2015 ◽  
Vol 27 (1) ◽  
pp. 11009
Author(s):  
黄伟 Huang Wei ◽  
谭荣清 Tan Rongqing ◽  
李志永 Li Zhiyong ◽  
李琳 Li Lin
Keyword(s):  
3D Model ◽  
Rb Vapor ◽  

2019 ◽  
Vol 27 (1) ◽  
pp. 132
Author(s):  
Jinghua Huang ◽  
Chunsheng Xia ◽  
Xingqi Xu ◽  
Chenyi Su ◽  
Bailiang Pan

2021 ◽  
Vol 133 ◽  
pp. 106529
Author(s):  
Chunsheng Xia ◽  
Jinghua Huang ◽  
Chenyi Su ◽  
Xingqi Xu ◽  
Bailiang Pan

1985 ◽  
Vol 17 (8) ◽  
pp. 1475-1478 ◽  
Author(s):  
A P. C. Warner ◽  
G. A. Ekama ◽  
G v. R. Marais

The laboratory scale experimental investigation comprised a 6 day sludge age activated sludge process, the waste sludge of which was fed to a number of digesters operated as follows: single reactor flow through digesters at 4 or 6 days sludge age, under aerobic and anoxic-aerobic conditions (with 1,5 and 4 h cycle times) and 3-in-series flow through aerobic digesters each at 4 days sludge age; all digesters were fed draw-and-fill wise once per day. The general kinetic model for the aerobic activated sludge process set out by Dold et al., (1980) and extended to the anoxic-aerobic process by van Haandel et al., (1981) simulated accurately all the experimental data (Figs 1 to 4) without the need for adjusting the kinetic constants. Both theoretical simulations and experimental data indicate that (i) the rate of volatile solids destruction is not affected by the incorporation of anoxic cycles and (ii) the specific denitrification rate is independent of sludge age and is K4T = 0,046(l,029)(T-20) mgNO3-N/(mg active VSS. d) i.e. about 2/3 of that in the secondary anoxic of the single sludge activated sludge stystem. An important consequence of (i) and (ii) above is that denitrification can be integrated easily in the steady state digester model of Marais and Ekama (1976) and used for design (Warner et al., 1983).


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