1996
DOI: 10.1175/1520-0469(1996)053<1123:gafppw>2.0.co;2
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Generalized Adjoint for Physical Processes with Parameterized Discontinuities. Part I: Basic Issues and Heuristic Examples

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Cited by 95 publications
(48 citation statements)
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“…(9) and (12), time evolution of both variables takes the following unified form: (15) where dF (LS is the rate of large-scale advective change, and Ph is compensation due to physical processes. Xu (1996) pointed out quasiequilibrium (F=0, d=0) in a time-averaged sense when dF LS>0, This means that Fl (Fc) satisfies the following 2 quasiequilibrium condition: 1) Fl(Fc) is close to 0 in model stratiform (convective) precipitation areas.…”
Section: Jo Approximationmentioning
confidence: 99%
“…(9) and (12), time evolution of both variables takes the following unified form: (15) where dF (LS is the rate of large-scale advective change, and Ph is compensation due to physical processes. Xu (1996) pointed out quasiequilibrium (F=0, d=0) in a time-averaged sense when dF LS>0, This means that Fl (Fc) satisfies the following 2 quasiequilibrium condition: 1) Fl(Fc) is close to 0 in model stratiform (convective) precipitation areas.…”
Section: Jo Approximationmentioning
confidence: 99%
“…Unfortunately, due to its strong dependence on the adjoint model of the forecast model (Bormann and Thepaut, 2004;Park and Zou, 2004;Caya et al, 2005;Bauer et al, 2006;Rosmond and Xu, 2006;Gauthier et al, 2007), computer implementation of 4DVar is often expensive and not easy to program because of the need to maintain and update the adjoint model of the forecast model. The situation is even worse when the forecast model is highly non-linear and/or the model physics involves discontinuous parameters (Xu, 1996). Furthermore, the applications of the static, thus flowindependent, background-error covariance in the traditional 4DVar often causes its poor assimilation performance (Beck and Ehrendorfer, 2005;Zhang et al, 2009;Cheng et al, 2010).…”
Section: Introductionmentioning
confidence: 99%
“…But whether discontinuous "on-off" switches impact the existence of the CF gradient has been investigated only in the case of single grid point model characterized by an ordinary differential equation (Xu, 1996(Xu, , 1997Zou, 1997;Mu and Wang, 2003). In the case of partial differential equations, the numerical experiments performed by Mu and Zheng (2005) show that traditional numerical treatment at the switches would result in terrible CF zigzags (see Fig.…”
Section: The Existence Of the Gradient Of The Cf With Respect To Icmentioning
confidence: 99%
“…Zou et al, 1993;Verlinde and Cotton, 1993;Zupanski, 1993;Bao and Warner, 1993;Zupanski and Mesinger, 1995;Zou, 1997;Xu, 1996Xu, , 1997Xu, , 1998Xu, , 1999Mu and Wang, 2003;Mu and Zheng, 2005). Due to the difficulties of the involved problems, attentions are mostly paid to simplified theoretical "on-off" models: from an ordinary differential equation describing the evolution of specific humidity on one grid point to a partial differential equation describing the evolution of specific humidity on a vertical or horizontal interval (Xu, 1996(Xu, , 1997(Xu, , 1998Zou, 1997;Mu and Wang, 2003;Mu and Zheng, 2005). The researches on the idealized simple models demonstrate that when discontinuous "on-off" switches occur in the governing equation, the effects of the VDA depend upon two facts: one is the simple discretization at the switches of the forward model, which usually induces the associated discrete cost function (CF) to depend discontinuously on the initial condition (IC) and the numerical solution of the forward model to contain the zigzag oscillations (Xu, 1997;Mu and Zheng, 2005).…”
Section: Introductionmentioning
confidence: 99%