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.\" RCSid "$Id: rfluxmtx.1,v 1.14 2024/02/08 02:26:01 greg Exp $"
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.TH RFLUXMTX 1 07/22/14 RADIANCE
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.SH NAME
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rfluxmtx - compute flux transfer matrix(es) for RADIANCE scene
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.SH SYNOPSIS
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.B rfluxmtx
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[
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.B \-v
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][
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.B "rcontrib options"
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]
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.B "{ sender.rad | - }"
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.B receivers.rad
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.B "[ -i system.oct ]"
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.B "[ system.rad .. ]"
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.SH DESCRIPTION
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.I Rfluxmtx
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samples rays uniformly over the surface given in
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.I sender.rad
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and records rays arriving at surfaces in the file
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.I receivers.rad,
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producing a flux transfer matrix per receiver.
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A system octree to which the receivers will be appended may be given with a
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.I \-i
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option following the receiver file.
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Additional system surfaces may be given in one or more
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.I system.rad
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files, which are compiled before the receiver file into an octree sent to the
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.I rcontrib(1)
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program to do the actual work.
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If a single hyphen ('-') is given in place of the sender file, then
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.I rfluxmtx
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passes ray samples from its standard input directly to
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.I rcontrib
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without interpretation.
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By default, all resulting matrix data are interleaved and sent to the standard output
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in ASCII format, but this behavior is typically overridden using inline options
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as described below.
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.PP
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The
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.I \-v
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option turns on verbose reporting for the number of samples and the executed
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.I rcontrib
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command.
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All other supported options are passed on to
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.I rcontrib(1).
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However, the
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.I \-f,
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.I \-e,
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.I \-p,
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.I \-b,
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.I \-bn,
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.I \-m,
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and
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.I \-M
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options are controlled by
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.I rfluxmtx
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and may not be set by the user.
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Also, the
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.I \-x,
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.I \-y,
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and
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.I \-ld
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options are ignored unless
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.I rfluxmtx
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is invoked in the pass-through mode,
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in which case they may be needed to generate RADIANCE views from
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.I vwrays(1).
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The sample count, unless set by the
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.I \-c
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option, defaults to 10000 when a sender file is given, or to 1 for pass-through mode.
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.SH VARIABLES
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The sender and receiver scene files given to
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.I rfluxmtx
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contain controlling parameters in special comments of the form:
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.nf
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#@rfluxmtx variable=value ..
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.fi
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At minimum, both sender and receiver must specify one of the
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hemisphere sampling types, and there must be at least
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one surface in each file.
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.TP 10n
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.BI h =u
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Set hemisphere sampling to "uniform," meaning a single bin
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of (cosine-distributed) samples.
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In the case of distant "source" primitives, this is the only
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sampling method that supports arbitrary receiver sizes.
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The other methods below require a full hemispherical source.
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.TP
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.BI h =kf
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Divide the hemisphere using the LBNL/Klems "full" sampling basis.
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(Use "h=-kf" for left-handed coordinates.)
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.TP
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.BI h =kh
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Divide the hemisphere using the LBNL/Klems "half" sampling basis.
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(Use "h=-kh" for left-handed coordinates.)
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.TP
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.BI h =kq
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Divide the hemisphere using the LBNL/Klems "quarter" sampling basis.
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(Use "h=-kq" for left-handed coordinates.)
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.TP
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.BI h =rN
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Divide the hemisphere using Reinhart's substructuring of the Tregenza
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sky pattern with
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.I N
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divisions in each dimension.
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If it is not given,
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.I N
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defaults to 1, which is just the Tregenza sky.
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(Use "h=-rN" for left-handed coordinates.)
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.TP
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.BI h =cie
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Divide the hemisphere into CIE sky scanner directions, which is
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similar to Tregenza but with different starting azimuths and
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reversing row direction at each new altitude.
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(Use "h=-cie" for left-handed coordinates.)
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.TP
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.BI h =scN
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Subdivide the hemisphere using the Shirley-Chiu square-to-disk mapping with an
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.I NxN
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grid over the square.
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(Use "h=-scN" for left-handed coordinates.)
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.TP
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.BI u =[-]{X|Y|Z|ux,uy,uz}
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Orient the "up" direction for the hemisphere using the indicated axis or direction
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vector.
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.TP
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.BI o =output_spec
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Send the matrix data for this receiver to the indicated file or command.
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Single or double quotes may be used to contain strings with spaces, and
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commands must begin with an exclamation mark ('!').
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The file format will be determined by the command-line
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.I \-fio
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option and will include an information header unless the
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.I \-h
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option was used to turn headers off.
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(The output file specification is ignored for senders.)\0
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.PP
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In normal execution, only a single sender surface is sampled, but it may be
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comprised of any number of subsurfaces, as in a triangle mesh or similar.
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The surface normal will be computed as the average of all the constituent
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subsurfaces.
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The subsurfaces themselves must be planar, thus only
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.I polygon
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and
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.I ring
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surface primitives are supported.
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Other primitives will be silently ignored and will have no effect on the calculation.
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.PP
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In the receiver file, the
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.I source
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primitive is supported as well, and multiple receivers (and multiple output
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matrices) may be identified by different modifier names.
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(Make sure that surfaces using the same modifier are grouped together,
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and that the modifiers are unique and not used elsewhere in the
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scene description.)\0
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Though it may be counter-intuitive, receivers are often light sources,
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since samples end up there in a backwards ray-tracing system such as RADIANCE.
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When using local geometry, the overall aperture shape should be close to flat.
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Large displacements may give rise to errors due to a convex receiver's
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larger profile at low angles of incidence.
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.PP
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Rays always emanate from the back side of the sender surface and arrive at the
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front side of receiver surfaces.
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In this way, a receiver surface may be reused as a sender in a subsequent
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.I rfluxmtx
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calculation and the resulting matrices will concatenate properly.
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(Note that it is important to keep receiver surfaces together, otherwise a
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"duplicate modifier" error will result.)\0
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.SH EXAMPLES
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To generate a flux transfer matrix connecting input and output apertures
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on a light pipe:
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.IP "" .3i
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rfluxmtx int_aperture.rad ext_aperture.rad lpipe.rad > lpipe.mtx
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.SH AUTHOR
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Greg Ward
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.SH "SEE ALSO"
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genBSDF(1), getinfo(1), pvsum(1), rcalc(1), rcollate(1), rcomb(1), rcontrib(1),
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rcrop(1), rmtxop(1), vwrays(1), wrapBSDF(1)
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