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Stability of adiabatic reactors

We have already considered the stability of the adiabatic stirred tank (Sec. 7.5) and have observed that since M = 1, the slope condition L N suffices to ensure stability. Now recalling the definitions of L and N this is [Pg.252]

This is the equation of a stirred tank with feed concentration a, temperature F, and composition d. The quantity 6 is a holding time for the particle. [Pg.253]

If the heat of reaction is A// and is negative, then heat will be generated at a rate (—In the steady state this balances the rate of heat transfer where U is the heat transfer coefficient (notation [Pg.254]

The pseudo-homogeneous reaction rate for the packed reactor is [Pg.254]

The right-hand side is the familiar sigmoidal function of t shown in Fig. 8.17. The left-hand side is a family of lines pivoting about the point of ordinate I and abscissa Since T is the intersection of one such line with the horizontal axis, the lines corresponding to T(z) will sweep toward the vertical [Pg.254]


Backmixing by axial diffusion, and stability of adiabatic reactors, 344... [Pg.402]


See other pages where Stability of adiabatic reactors is mentioned: [Pg.329]    [Pg.333]    [Pg.335]    [Pg.337]    [Pg.339]    [Pg.341]    [Pg.343]    [Pg.345]    [Pg.347]    [Pg.349]    [Pg.350]    [Pg.351]    [Pg.402]    [Pg.252]    [Pg.253]   


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