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102   Cha p te r  F o u r


                     maximum shaft power) and to part-load performance; the shaft
                     power is modeled as a function of the steam mass flow that is known
                     as the Willan line. This model was extended to condensing steam
                     turbines by Shang (2000). All these works follow the same model
                     structure and employ the same equations; however, they use different
                     values for the turbine regression coefficients.
                        The intercept of the Willan line was mapped by Mavromatis and
                     Kokossis (1998) and by Shang (2000) as identical to the turbine energy
                     losses, also assuming a fixed loss rate. Varbanov, Doyle, and Smith
                     (2004) introduced improvements to those models by (1) recognizing
                     that the Willan line intercept has no direct physical meaning and is
                     simply the intercept of a linearization, and (2) accounting for both
                     inlet and outlet pressures of the steam turbines. These improved
                     steam turbine models have been incorporated into methodologies for
                     simulating and optimizing steam networks; they have also been
                     used to target heat and power cogeneration by assuming a single
                     large steam turbine for each expansion zone between two consecutive
                     steam headers.

                     4.6.5  Advanced Total Site Optimization and Analysis
                     A model for optimizing the utility system serves as a tool for reducing
                     site operating costs related to energy and for analyzing the
                     thermodynamic limitations of energy conversions. An advanced
                     approach to these concepts, known as top-level analysis, is one that
                     allows “scoping” which site processes to target for Heat Integration
                     improvement (Varbanov, Doyle, and Smith, 2004). Consider the utility
                     system shown in Figure 4.69 (Smith and Varbanov, 2005), whose
                     operating properties have been optimized for the given steam and
                     power demands.
                        Suppose it were possible to reduce the HP steam demand—for
                     example, by improving the energy efficiency within the processes
                     that use HP steam. What, then, would such a saving in steam actually
                     be worth? Reducing HP steam demand means that less steam needs
                     to be expanded from the VHP level, which could lead in turn to less
                     power cogeneration and increased import of power. As a support
                     tool for deciding how best to utilize the potential steam excess and
                     estimate the value of potential steam savings, Varbanov, Doyle, and
                     Smith (2004) introduced the concept of  marginal steam price. This
                     characteristic captures the change in a utility system’s energy cost
                     per unit change in steam demand, and it is specific to a given
                     combination of steam header and operating conditions. By
                     optimizing the utility system at gradual successive reductions of
                     potential steam demand on the headers, it is possible to obtain a
                     curve of the marginal steam price versus the savings that could be
                     obtained. The marginal price curve for the utility system in
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