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Secondary plant is generally taken to mean equipment at room and, in some cases, distribution level. Room emitters, chilled ceiling and beams, coils, pumps and fans, conduits are examples of equipment in this category. Primary plant is associated with centralised equipment for the generation (or dissipation) of energy. Examples include boilers, chillers and combined heat and power plant. Probably the most comprehensive treatments to date of models for equipment in both categories (including recommended Fortran code listings) can be found in Brandemeuhl (1993) (secondary systems) and LeBrun et al. (1999) (primary plant). Afurther classi cation related to modelling concerns the extent to which detail is attached to the description of plant. Fundamentally, there are three possibilities as far as plant descriptions integrated within building energy models are concerned as summarised in Table 6.4. Areview and examples of some the recent progress in plant modelling, with particular reference to steady-state applications, now follows. Section 6.5 then concentrates on some of the recent developments in dynamic-state applications with particular reference to control problems.



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Two items are of interest here. First, notice how the Library demarcation surrounds not just the text ( Copyright (c) 2000 ) but all of its formatting attributes. Library items can do far more than just cut and paste raw text. The second thing to note is that the Library markers are placed discreetly within HTML comments. Web browsers ignore the Library markers and render the code in between them. The value in the opening Library code, /Library/title.lbi , is the source file for the Library entry. This file is located in the Library folder, inside of the current site root folder. Library source (.lbi) files can be opened with a text editor or in Dreamweaver; they consist of plain HTML code without the <html> and <body> tags.





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50 mm a 1 Intriguingly, this corresponds with a period of major reorganization of global plate motions (Rona and Richardson, 1978), the age of the major bend in the Hawaiian Emperor seamount chain, and a period in which the rate of true polar wander (Section 56) was much greater than during the period 10 50 Ma ago, when it was virtually at a standstill (Besse & Courtillot, 2002) If hotspots remain xed, and provide a framework for absolute plate motions, then paleomagnetic studies should be able to provide a test of their unchanging latitude Paleomagnetic data for the oceanic plates of the Paci c are sparse, and subject to greater uncertainties than those obtained for continental areas Nevertheless preliminary results (Tarduno & Cottrell, 1997) suggest that the Hawaiian hotspot may have migrated south through as much as 15 20 of latitude during the period 80 43 Ma.

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Paleomagnetic results obtained from Ocean Drilling Program drill core, from which any latitudinal change in of the Reunion hotspot could be deduced (Vandamme & Courtillot, 1990), suggest that this hotspot may have moved northwards through approximately 5 of latitude between 65 and 43 Ma These latitudinal shifts are compatible with the discrepancy between the two hotspot reference frames prior to 43 Ma ago, and support the assumptions regarding Cenozoic late Mesozoic plate boundaries within and around the Antarctic plate These results also imply that the major bend in the Hawaiian Emperor seamount chain at approximately 43 Ma does not re ect a major change in the absolute motion of the Paci c plate, as originally thought, but can be accounted for almost entirely by the southward motion of the Hawaiian hotspot (Norton, 1995) Predicted hotspot traces in the Atlantic and Indian Ocean (M ller et al.

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