| 1 | .\" RCSid "$Id: rfluxmtx.1,v 1.15 2025/03/27 01:26:55 greg Exp $" | 
| 2 | .TH RFLUXMTX 1 07/22/14 RADIANCE | 
| 3 | .SH NAME | 
| 4 | rfluxmtx - compute flux transfer matrix(es) for RADIANCE scene | 
| 5 | .SH SYNOPSIS | 
| 6 | .B rfluxmtx | 
| 7 | [ | 
| 8 | .B \-v | 
| 9 | ][ | 
| 10 | .B "rcontrib options" | 
| 11 | ] | 
| 12 | .B "{ sender.rad | - }" | 
| 13 | .B receivers.rad | 
| 14 | .B "[ -i system.oct ]" | 
| 15 | .B "[ system.rad .. ]" | 
| 16 | .SH DESCRIPTION | 
| 17 | .I Rfluxmtx | 
| 18 | samples rays uniformly over the surface given in | 
| 19 | .I sender.rad | 
| 20 | and records rays arriving at surfaces in the file | 
| 21 | .I receivers.rad, | 
| 22 | producing a flux transfer matrix per receiver. | 
| 23 | A system octree to which the receivers will be appended may be given with a | 
| 24 | .I \-i | 
| 25 | option following the receiver file. | 
| 26 | Additional system surfaces may be given in one or more | 
| 27 | .I system.rad | 
| 28 | files, which are compiled before the receiver file into an octree sent to the | 
| 29 | .I rcontrib(1) | 
| 30 | program to do the actual work. | 
| 31 | If a single hyphen ('-') is given in place of the sender file, then | 
| 32 | .I rfluxmtx | 
| 33 | passes ray samples from its standard input directly to | 
| 34 | .I rcontrib | 
| 35 | without interpretation. | 
| 36 | By default, all resulting matrix data are interleaved and sent to the standard output | 
| 37 | in ASCII format, but this behavior is typically overridden using inline options | 
| 38 | as described below. | 
| 39 | .PP | 
| 40 | The | 
| 41 | .I \-v | 
| 42 | option turns on verbose reporting for the number of samples and the executed | 
| 43 | .I rcontrib | 
| 44 | command. | 
| 45 | All other supported options are passed on to | 
| 46 | .I rcontrib(1). | 
| 47 | However, the | 
| 48 | .I \-fo, | 
| 49 | .I \-p, | 
| 50 | .I \-b, | 
| 51 | .I \-bn, | 
| 52 | .I \-m, | 
| 53 | and | 
| 54 | .I \-M | 
| 55 | options are controlled by | 
| 56 | .I rfluxmtx | 
| 57 | and may not be set by the user. | 
| 58 | (Recovery mode is not supported, and existing output is always overwritten.)\0 | 
| 59 | Further, the | 
| 60 | .I \-x, | 
| 61 | .I \-y, | 
| 62 | and | 
| 63 | .I \-ld | 
| 64 | options are ignored unless | 
| 65 | .I rfluxmtx | 
| 66 | is invoked in the pass-through mode, | 
| 67 | in which case they may be needed to generate RADIANCE views from | 
| 68 | .I vwrays(1). | 
| 69 | The sample count, unless set by the | 
| 70 | .I \-c | 
| 71 | option, defaults to 10000 when a sender file is given, or to 1 for pass-through mode. | 
| 72 | .SH VARIABLES | 
| 73 | The sender and receiver scene files given to | 
| 74 | .I rfluxmtx | 
| 75 | contain controlling parameters in special comments of the form: | 
| 76 | .nf | 
| 77 |  | 
| 78 | #@rfluxmtx variable=value .. | 
| 79 |  | 
| 80 | .fi | 
| 81 | At minimum, both sender and receiver must specify one of the | 
| 82 | hemisphere sampling types, and there must be at least | 
| 83 | one surface in each file. | 
| 84 | .TP 10n | 
| 85 | .BI h =u | 
| 86 | Set hemisphere sampling to "uniform," meaning a single bin | 
| 87 | of (cosine-distributed) samples. | 
| 88 | In the case of distant "source" primitives, this is the only | 
| 89 | sampling method that supports arbitrary receiver sizes. | 
| 90 | The other methods below require a full hemispherical source. | 
| 91 | .TP | 
| 92 | .BI h =kf | 
| 93 | Divide the hemisphere using the LBNL/Klems "full" sampling basis. | 
| 94 | (Use "h=-kf" for left-handed coordinates.) | 
| 95 | .TP | 
| 96 | .BI h =kh | 
| 97 | Divide the hemisphere using the LBNL/Klems "half" sampling basis. | 
| 98 | (Use "h=-kh" for left-handed coordinates.) | 
| 99 | .TP | 
| 100 | .BI h =kq | 
| 101 | Divide the hemisphere using the LBNL/Klems "quarter" sampling basis. | 
| 102 | (Use "h=-kq" for left-handed coordinates.) | 
| 103 | .TP | 
| 104 | .BI h =rN | 
| 105 | Divide the hemisphere using Reinhart's substructuring of the Tregenza | 
| 106 | sky pattern with | 
| 107 | .I N | 
| 108 | divisions in each dimension. | 
| 109 | If it is not given, | 
| 110 | .I N | 
| 111 | defaults to 1, which is just the Tregenza sky. | 
| 112 | (Use "h=-rN" for left-handed coordinates.) | 
| 113 | .TP | 
| 114 | .BI h =cie | 
| 115 | Divide the hemisphere into CIE sky scanner directions, which is | 
| 116 | similar to Tregenza but with different starting azimuths and | 
| 117 | reversing row direction at each new altitude. | 
| 118 | (Use "h=-cie" for left-handed coordinates.) | 
| 119 | .TP | 
| 120 | .BI h =scN | 
| 121 | Subdivide the hemisphere using the Shirley-Chiu square-to-disk mapping with an | 
| 122 | .I NxN | 
| 123 | grid over the square. | 
| 124 | (Use "h=-scN" for left-handed coordinates.) | 
| 125 | .TP | 
| 126 | .BI u =[-]{X|Y|Z|ux,uy,uz} | 
| 127 | Orient the "up" direction for the hemisphere using the indicated axis or direction | 
| 128 | vector. | 
| 129 | .TP | 
| 130 | .BI o =output_spec | 
| 131 | Send the matrix data for this receiver to the indicated file or command. | 
| 132 | Single or double quotes may be used to contain strings with spaces, and | 
| 133 | commands must begin with an exclamation mark ('!'). | 
| 134 | The file format will be determined by the command-line | 
| 135 | .I \-fio | 
| 136 | option and will include an information header unless the | 
| 137 | .I \-h | 
| 138 | option was used to turn headers off. | 
| 139 | (The input format specification is ignored for senders.)\0 | 
| 140 | .PP | 
| 141 | In normal execution, only a single sender surface is sampled, but it may be | 
| 142 | comprised of any number of subsurfaces, as in a triangle mesh or similar. | 
| 143 | The surface normal will be computed as the average of all the constituent | 
| 144 | subsurfaces. | 
| 145 | The subsurfaces themselves must be planar, thus only | 
| 146 | .I polygon | 
| 147 | and | 
| 148 | .I ring | 
| 149 | surface primitives are supported. | 
| 150 | Other primitives will be silently ignored and will have no effect on the calculation. | 
| 151 | .PP | 
| 152 | In the receiver file, the | 
| 153 | .I source | 
| 154 | primitive is supported as well, and multiple receivers (and multiple output | 
| 155 | matrices) may be identified by different modifier names. | 
| 156 | (Make sure that surfaces using the same modifier are grouped together, | 
| 157 | and that the modifiers are unique and not used elsewhere in the | 
| 158 | scene description.)\0 | 
| 159 | Though it may be counter-intuitive, receivers are often light sources, | 
| 160 | since samples end up there in a backwards ray-tracing system such as RADIANCE. | 
| 161 | When using local geometry, the overall aperture shape should be close to flat. | 
| 162 | Large displacements may give rise to errors due to a convex receiver's | 
| 163 | larger profile at low angles of incidence. | 
| 164 | .PP | 
| 165 | Rays always emanate from the back side of the sender surface and arrive at the | 
| 166 | front side of receiver surfaces. | 
| 167 | In this way, a receiver surface may be reused as a sender in a subsequent | 
| 168 | .I rfluxmtx | 
| 169 | calculation and the resulting matrices will concatenate properly. | 
| 170 | (Note that it is important to keep receiver surfaces together, otherwise a | 
| 171 | "duplicate modifier" error will result.)\0 | 
| 172 | .SH EXAMPLES | 
| 173 | To generate a flux transfer matrix connecting input and output apertures | 
| 174 | on a light pipe: | 
| 175 | .IP "" .2i | 
| 176 | rfluxmtx int_aperture.rad ext_aperture.rad lpipe.rad > lpipe.mtx | 
| 177 | .SH AUTHOR | 
| 178 | Greg Ward | 
| 179 | .SH "SEE ALSO" | 
| 180 | genBSDF(1), getinfo(1), pvsum(1), rcalc(1), rcollate(1), rcomb(1), rcontrib(1), | 
| 181 | rcrop(1), rmtxop(1), rxfluxmtx(1), vwrays(1), wrapBSDF(1) |