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Tsuji flame

Tsuji, Ft. and Yamaoka, 1., Structure and extinction of near-limit flames in a stagnation flow, Proc. Combust. Inst., 19,1533,1982. [Pg.44]

Nagayama J, Takasuga T, Tsuji H. 2001. Contamination levels of brominated flame retardants, dioxins and organochlorine compounds in the blood of Japanese adults. BFR 113-116. [Pg.443]

Beginning with the innovative work of Tsuji and Yamaoka [409,411], various counter-flow diffusion flames have been used experimentally both to determine extinction limits and flame structure [409]. In the Tsuji burner (see Fig. 17.5) fuel issues from a porous cylinder into an oncoming air stream. Along the stagnation streamline the flow may be modeled as a one-dimensional boundary-value problem with the strain rate specified as a parameter [104], In this formulation complex chemistry and transport is easily incorporated into the model. The chemistry largely takes place within a thin flame zone around the location of the stoichiometric mixture, within the boundary layer that forms around the cylinder. [Pg.575]

In 1967 Tsuji and Yamaoka introduced the notion of using stagnation flow as an ideal way to study the structure of nonpremixed (diffusion) flames [410,411], The essential features of their experiment are illustrated in Fig. 17.5. Gaseous fuel issued radially outward from... [Pg.702]

Fig. 17.5 Illustration of the Tsuji and Yamaoka diffusion flame in the forward stagnation region of a porous cylinder [410,411]. Fig. 17.5 Illustration of the Tsuji and Yamaoka diffusion flame in the forward stagnation region of a porous cylinder [410,411].
A number of investigators have modeled the Tsuji and Yamaoka data [104]. In these investigations the flame was modeled as a semi-infinite stagnation flow, with the outer potential flow characterized by the velocity-gradient parameter a (see Section 6.3.1). For the cylindrical geometry, this characterization is correct in the neighborhood of the center stagnation-flow streamline. [Pg.703]

An alternative to the Tsuji and Yamaoka configuration is the planar opposed-flow configuration. In 1981 Hahn and Wendt [161,162] used parallel porous-metal plates to create an opposed-jet diffusion flame of methane and air in which they studied NO formation. They also developed a computational model that included complex chemical kinetics. The model used outer potential flows to characterize the strain field. [Pg.703]

H. Tsuji. Counterflow Diffusion Flames. Prog. Energy Combust. Sci., 8 93-119, 1982. [Pg.838]

H. Tsuji and I. Yamaoka. The Structure of Counterflow Diffusion Flames in the Forward Stagnation Region of a Porous Cylinder. Proc. Combust. Inst., 12 997-1005,1969. [Pg.838]

H. Tsuji and I. Yamaoka, An Experimental Study of Extinction of Near-Limit Flames in a Stagnation Flow, Colloque International Berthe lot-Vieille-Mallard-le Chatelier, First Specialists Meeting International) of The Combustion Institute, Pittsburgh The Combustion Institute, 1981, 111-116. [Pg.444]

Yamaoka, I., and H. Tsuji. 1991. The effect of back diffusion of intermediate hydrogen on methane-air and propane-air flames diluted with nitrogen in a stagnating flow. Combustion Flame 86 135-46. [Pg.63]

Tsuji T, Korematsu M (1975) Highly flame-retardant shaped articles and method for preparing the same. In Google Patents... [Pg.340]


See other pages where Tsuji flame is mentioned: [Pg.35]    [Pg.35]    [Pg.147]    [Pg.703]    [Pg.704]    [Pg.318]    [Pg.97]    [Pg.98]   
See also in sourсe #XX -- [ Pg.703 ]




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