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A User's Manual for DELSOL3 - prod.sandia.gov - Sandia National ...

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J1.D. Heliostats<br />

Either rectangular (IROUND=O) or circular (IROUND=l) mirror shapes<br />

(Figure II-ll(A) and (B)) can be accommodated by the code. The overall dimen-<br />

sions of the heliostat, WM and HM, enclose the mirrored surface, the edge sup-<br />

ports, and cutouts or slots, if any. The fraction of the area defined by WM and<br />

HM which actually reflects sunlight is specified by the parameter DENSMR. The<br />

user has the option of generating more accurate images from canted heliostats by<br />

specifying the size and location of the cant panels (ICPANL=l, namelist HSTAT)<br />

rather than letting DELSOL specify based on NCANTX, NCANTY, HM, and<br />

WM. This option is highly recommended in small systems. The width and height<br />

of the reflective surface of each cant panel are WPANL and HPANL meters, re-<br />

spectively (Figure 11-ll(C)). The center of the Ith cant panel is displaced from<br />

the pivot point (center of the heliostat) by HXCANT(1) meters parallel to the<br />

horizontal edge of the heliostat and HYCANT(1) meters parallel to the vertical<br />

edge of the heliostat.<br />

The reflectivity, given by the value of RMIRL, represents the time averaged<br />

value and the value just after washing. RMIRL should also include transmission<br />

losses due to any enclosure surrounding the heliostat. (See also Section<br />

111. G-2.)<br />

The heliostats are assumed to have altitude-azimuth drive systems pivoted at<br />

the center of the mirrored surface. There<strong>for</strong>e, the geometrical center of a heliostat<br />

is also the center of rotation of the mirrored surface.<br />

11.D-I. Heliostat Error Sources-The per<strong>for</strong>mance of heliostats is degraded<br />

by several error sources. Care must be taken with the input of these terms be-<br />

cause different reports often use different descriptions <strong>for</strong> the same errors. Specif-<br />

ically, a distinction must be made between an error source (e.g., backlash in the<br />

azimuthal motor drive) and the effect of the error source (i.e., the magnitude of<br />

the displacement and/or distortion of the heliostat image on the receivers). The<br />

latter, the effect of the error source, depends on the geometry between the sun,<br />

heliostat, and receiver. Thus, a heliostat with a constant error source will pro-<br />

vide variable effects on the image at different times of the year <strong>for</strong> the same field<br />

position, or at different field positions <strong>for</strong> the same time of the year, due to the<br />

changing relative positions of the sun and receiver.<br />

Consider the example of the effect of a constant backlash error in the az-<br />

imuthal drive in otherwise perfect heliostats. At noon on any given day of the<br />

year, a heliostat located due north of the tower will <strong>prod</strong>uce a larger displacement<br />

of the image on the receiver than its counterpart at the same distance due south.<br />

In fact, as heliostats in the south field approach a horizontal orientation (Le., mir-<br />

ror normal ii vertical), errors in the azimuthal drive <strong>prod</strong>uce no displacement in<br />

the image on the receiver.<br />

44

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