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Code Manual for CONTAIN 2.0 - Federation of American Scientists

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output after a run is completed, this keyword may be specified on a restart. A restart at a given<br />

restart time will automatically include energy accounting in<strong>for</strong>mation up to that time.<br />

Aerosol materials can be either a nongaseous thermodynamic material or a dedicated aerosol material<br />

defined by the user in the AERNAMES and global AEROSOL input blocks. (If an aerosol material<br />

is declared to be the H20V material, a usage that is now considered obsolete, the material will be<br />

treated as the liquid H20L.) Only the aerosol components that are thermodynamic materials are<br />

included in the mass and energy accounting. Both suspended and deposited aerosol masses are<br />

considered. It should be noted that fission products, by convention, cannot be comprised <strong>of</strong><br />

thermodynamic materials and are, there<strong>for</strong>e, excluded from the scheme.<br />

The details <strong>of</strong> the accounting scheme are described in Appendix A. The strategy used in the mass<br />

and energy accounting is discussed in Section A.2. The repositories considered and the mass and<br />

energy contributions reported in the accounting scheme are discussed in Section A.3.<br />

As discussed in Appendix A, the present mass and energy accounting scheme is repository-oriented.<br />

The mass and energy output is organized so that the mass and energy balance <strong>for</strong> each repository may<br />

be obtained by inspection, without having to refer to other repositories. An example <strong>of</strong> the mass and<br />

energy accounting output (enabled by the PRENACCT keyword) is given in Figure 3-2. As shown<br />

in this figure, a number <strong>of</strong> repositories and their mass and energy balances are reported. The mass<br />

reporting in this case includes only the coolant mass, given in kilograms, since “nmtrac” and<br />

TRACKMAT were not specified. In Figure 3-1, the present energy EP <strong>for</strong> each repository should be<br />

compared with the second column labeled “i+e+r+i- c,” which is a combination <strong>of</strong> the first letters<br />

<strong>of</strong> the labels <strong>of</strong> the next five columns. This column contains the sum EO+ E. + E, + E~- EC,which ~<br />

according to Equation (A-11) should be equal to EP, plus any work done by the repository against<br />

its geometric constraints (see Section A.3), if no energy accounting errors have occurred.<br />

The <strong>for</strong>mat shown is that obtained when the implicit flow solver is used. If the explicit flow solver<br />

is used, the atmosphere mass and energy balances <strong>for</strong> each cell are replaced by a single mass and<br />

energy balance representing the sum over all cell atmospheres. The reason <strong>for</strong> reporting this sum<br />

is that the explicit solver has not been upgraded to track the change in audit energies resulting from<br />

intercell flow.<br />

Note that because all internal interfaces are conservative with respect to audit energies, the sum <strong>of</strong><br />

the influx energies E~over all repositories should be zero. The user can check this if desired.<br />

It should be noted that a sizeable relative error in the energy balance, based on repository contents,<br />

does not necessarily imply that the error is significant in terms <strong>of</strong> the calculated thermodynamic state.<br />

For example, a repository may have a great deal <strong>of</strong> mass and energy cycled through it but contain<br />

only a small fraction <strong>of</strong> the total cycled mass and energy at any given time. A relatively small error<br />

in the calculation <strong>of</strong> the thermodynamic state may buildup overtime to a relatively large error, based<br />

on the repository contents. The error may actually be tolerable if the measure <strong>of</strong> significance is the<br />

error relative to the total mass and energy cycled through the repository.<br />

Rev O 6/30/97

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