01.03.2013 Views

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 ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

DELSOL will examine NUMHTW (520) equally spaced discrete values of<br />

RY(l)/RX(l) from a minimum of HTWST to a maximum of HTWEND.<br />

If NUMREC or NUMHTW is set to 1, the value of the receiver vari-<br />

able will be fixed to be the last defined value of the appropriate variable<br />

(RX(1) or RY(1)) in Namelist REC.<br />

In the case of multiple flat plate receivers, all receiver dimensions are<br />

assumed proportional to the first receiver’s dimensions. RX2TRX,<br />

RX3TRX, and RX4TRX are the ratios of the second, third, and fourth<br />

plate’s horizontal dimension to the first plate’s horizontal dimension. The<br />

vertical/horizontal ratio, RYTRX, is assumed the same <strong>for</strong> all plates.<br />

c) Cavity Receiver Dimensions and Optimization-DELSOL assumes during<br />

optimization that a cavity receiver has an aperture which can be treated<br />

like a flat plate receiver as described above. It also assumes that the cav-<br />

ity is shaped as a semicircular right cylinder centered horizontally on the<br />

aperture, so that the heat absorbing surface depth needs to be deter-<br />

mined. Further, the optimum height of the heat absorbing surface should<br />

be determined, in order to find an optimum system based on levelized en-<br />

ergy cost (LEC). These are more design parameters than DELSOL can<br />

vary at one time, thus making cavity receivers more complicated to design<br />

than other receiver types. However, because varying some of these vari-<br />

ables does not affect the optimum choice (based on LEC) of other of the<br />

variables, it is possible to run a series of optimization and per<strong>for</strong>mance<br />

runs that will lead to a “good” cavity design. This is especially true be-<br />

cause almost all power calculations <strong>for</strong> cavities are done at the aperture<br />

(all except convective losses), so that power and energy are nearly inde-<br />

pendent of the configuration of the interior of the cavity. Thus, cavity<br />

depth and heat absorber height, which depend on flux levels and cost, can<br />

be optimized separately from aperture dimensions without affecting the<br />

optimum choice of those variables.<br />

Different pairs of receiver variables are selected in sequence <strong>for</strong> optimiza-<br />

tion. First, the width of the aperture and depth of the cavity should be<br />

optimized by specifying IOPTUM=2. Second, the aspect ratio of the<br />

aperture can be optimized separately (IOPTUM= 1). Finally, per<strong>for</strong>mance<br />

runs can be used to generate flux maps within the cavity so that the user<br />

can trim or adjust the shape of the heat absorbing surface, if desired or<br />

required.<br />

The first step in optimizing a cavity is to determine the aperture width<br />

and cavity depth by specifying the variable IOPTUM=2. DELSOL<br />

searches NUMREC equally spaced discrete values of the width of the first<br />

(north) aperture, RX(l), from a minimum value of WST meters to a max-<br />

imum value of WEND meters. The relative aperture height, RY(l), will<br />

remain fixed as specified by the value of RYTRX, and the dimensions of

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!