reactor cross section
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2009 ◽  
Vol 36 (8) ◽  
pp. 1138-1150 ◽  
Author(s):  
Nathanael H. Hudson ◽  
Abderrafi. M. Ougouag ◽  
Farzad Rahnema ◽  
Hans Gougar

2003 ◽  
Vol 48 (2) ◽  
pp. 197-204 ◽  
Author(s):  
H. Jupsin ◽  
E. Praet ◽  
J.-L. Vasel

This article presents a mathematical model to describe High-Rate Algal Ponds (HRAPs). The hydrodynamic behavior of the reactor is described as completely mixed tanks in series with recirculation. The hydrodynamic pattern is combined with a subset of River Water Quality Model 1 (RWQM1), including the main processes in liquid phase. Our aim is to develop models for WSPs and aerated lagoons, too, but we focused on HRAPs first for several reasons:• Sediments are usually less abundant in HRAP and can be neglected• Stratification is not observed and state variables are constant in a reactor cross section• Due to the system's geometry, the reactor is quite similar to a plugflow type reactor with recirculation, with a simple advection term. The model is based on mass balances and includes the following processes:Phytoplankton growth with NO3-, NO2- and death• Aerobic growth of heterotrophs with NO3-, NH4+ and respiration• Anoxic growth of heterotrophs with NO3-, NO2- and anoxic respiration• Growth of nitrifiers (two stages) and respiration. The differences with regard to RWQM1 are that we included a limiting term associated with inorganic carbon on the growth rate of algae and nitrifiers, gas transfers are taken into account by the familiar Adeney equation, and a subroutine calculates light intensity at the water surface. This article presents our first simulations.


Author(s):  
C.R. Weisbin ◽  
N.M. Greene ◽  
H. Henryson ◽  
R.J. LaBauve ◽  
C. Durston ◽  
...  

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