A User's Manual for DELSOL3 - prod.sandia.gov - Sandia National ...
A User's Manual for DELSOL3 - prod.sandia.gov - Sandia National ...
A User's Manual for DELSOL3 - prod.sandia.gov - Sandia National ...
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epresentation of heliostat errors and to incorporate analytical scaling of the im-<br />
ages as the tower height is varied (Reference 5). DELSOL also employs a method<br />
<strong>for</strong> optimizing heliostat densities similar to the Houston approach (Reference 4).<br />
The primary difference in the two codes is in their design/optimization capabili-<br />
ties. The Houston approach considers only one tower height and receiver size at<br />
a time. These variables must be optimized by manually rerunning the Houston<br />
codes until an optimum is located. In contrast, DELSOL automatically optimizes<br />
the tower height and receiver dimension(s), saving considerable user and com-<br />
puter time. (The user is cautioned, however, to provide his own values <strong>for</strong> the<br />
appropriate input variables if his system of interest differs significantly in size or<br />
cost/per<strong>for</strong>mance from the default system description in the code. See Appendix<br />
Am)<br />
DELSOL is a FORTRAN IV code, developed on <strong>Sandia</strong>’s CDC6600 and<br />
CDC7600, and adapted to execute on a CRAY-1. Typical execution times <strong>for</strong><br />
per<strong>for</strong>mance calculations on the CRAY-1 are 45-60 seconds, while design and op-<br />
timization calculations may take 5-300 seconds. Execution times on a VAX 11-<br />
780 will typically be about ten times as long as on the CRAY-1. This manual de-<br />
scribes the status of DELSOL as of January 1986. The code is intended to evolve<br />
with the development of central receiver technology and revised versions of the<br />
code and manual will be released as needed.<br />
LA. Differences from Earlier Versions of DELSOL<br />
Several corrections and additions have been made in DELSOLS which dis-<br />
tinguish it from its predecessors. Known errors which were fixed included cor-<br />
recting the logic <strong>for</strong> scaling flux point positions during the optimization of cavity<br />
receivers, correcting the flux calculation <strong>for</strong> cavity receivers and extending the<br />
calculation to allow general flux maps in front of the aperture, and correcting the<br />
logic when operating from storage and receiver power simultaneously. Also, the<br />
operating parasitic loss calculation was fixed and modified, and numerous typo-<br />
graphical errors in the code and in the outputs were corrected.<br />
At least four major enhancements were added to <strong>DELSOL3</strong>. First, receiver<br />
loss algorithms were modified based on References 6 and 7 to more closely model<br />
experimental and test facility data of receiver losses, including measured losses<br />
at the Solar One facility near Barstow, Cali<strong>for</strong>nia. Next, algorithms <strong>for</strong> non-<br />
operating parasitic losses were added to the code, thus accounting <strong>for</strong> the en-<br />
ergy which is consumed by a power plant at the times when power is not being<br />
<strong>prod</strong>uced. Third, the sizing algorithm <strong>for</strong> a cavity heat absorber area, which de-<br />
termines receiver cost, was modified so that the new area is based on aperture<br />
height rather than on minimum and maximum field dimensions. The previous<br />
algorithm resulted in an extremely large cavity which had very low incident flux<br />
levels on the upper portion of the heat absorber area. This modification assumes<br />
that some internal spillage is acceptable, and is intended to be an empirical model<br />
based on present and past detailed cavity designs.<br />
22