[an error occurred while processing this directive] next up previous contents
Next: Semi-Theoretical Models Up: POST-CHF HEAT TRANSFER Previous: Empirical Correlations

8.4. Non-Equilibrium Empirical Models

As mentioned previously our goal is to predict the heat transfer coefficient after the critical heat flux has been exceeded. If one used the empirical correlations of the past section, it is clear these are applicable between the axial location of CHF, tex2html_wrap_inline5402 (Figure 8.1), and the location where the equilibrium quality, equals one ( tex2html_wrap_inline5524 1, tex2html_wrap_inline5526 ). Remember, these past correlations are based on the assumptions that thermodynamic equilibrium exists between the vapor and liquid, and one temperature, tex2html_wrap_inline5528 , with quality, tex2html_wrap_inline5130 , determines the thermodynamic state of the fluid. However, if one considers the more realistic situation where the liquid droplets are at a different temperature, tex2html_wrap_inline4283 , than the vapor tex2html_wrap_inline4926 , one must again determine the "true" quality variation in difference to tex2html_wrap_inline5536 to then determine the wall temperature given the heat flux. This situation is analogous to our discussion in subcooled boiling when tex2html_wrap_inline5536 = 0 but actually X'(z) > 0 now in the post-CHF region, tex2html_wrap_inline5542 but X' (z < 1) (Figure 8.1). Therefore, our first objective is to determine the axial variation of this "true" quality, and the point where tex2html_wrap_inline5552 1 (i.e., tex2html_wrap_inline5554).

Consider the case of a constant heat flux. Now in this non-equilibrium approach we assume that the heat flux can be divided into two portions; one directly heating the vapor, q"g , and one directly into the liquid, q"f , causing it to evaporate.


where we define e as


and it is assumed for simplicity that e = f(Z). If we realistically consider the temperature difference of tex2html_wrap_inline4926 and tex2html_wrap_inline4283 , then one must realize that e is actually a function of position; for a constant e we get


Now from a one-dimensional energy balance on the channel the thermodynamic quality is given by


where for tex2html_wrap_inline5130 = 1 we can find the location of tex2html_wrap_inline5526


Now we can use the same energy balance method to find X'(z)


where once again we only use the portion of the total heat flux which goes into evaporation. The location where X'(Z) = 1 is defined as tex2html_wrap_inline5276 and is given by


so that we can solve for this fraction of the total flux, e, as


where we can correlate e based on measurements of these quantities. Once we have a correlation for e we can derive an expression for the heat transfer coefficient from it definition. Note that the heat transfer coefficient would be different between the wall-vapor and wall-liquid. Groeneveld has suggested such a correlation for e given by



This approach is not necessarily recommended compared to others, because although it includes some degree of realism it still remains quite empirical for the key variable.

next up previous contents
Next: Semi-Theoretical Models Up: POST-CHF HEAT TRANSFER Previous: Empirical Correlations

All contents © Michael L. Corradini
Last Modified: Tue Sep 2 15:06:55 CDT 1997