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| In the left half of the left plot, specific illuminance by a continuous row of luminaires spaced 5 heights is shown (right half is for a single luminaire). | The right plot is for a single luminaire, unrotated. |
Values below the scale are illuminance / 1 lx. This is for (unrealistic) “unit” case that luminaires would have lamps producing 1 klm only, would be point-like and just 1 m over the terrain.
# IESNA:LM-63-1995
# [TEST] 36332
# [MANUFAC] SiTECO
# [LUMCAT] 5CX622E1MS0408
# [LUMINAIRE] CX 100 COMFORT, streetlight
# [MORE] "", "", "", "", "", "", "", ""
# [LAMPCAT] Osram: NAV-T 50W SUPER
# [LAMP] HST 50W
# TILT=NONE
# Bulbs: 1, 4400 lm each
# Number of measured angles: 37 vertical, 37 horizontal ones
# Photometric type: 1, Units type: 2
# Luminous openig width, length and height: 0.300 0.575 0.000
# Ballast factor: 1, Input power: 66 W
# Source file: ies/36332.ies
# Luminaire flux = 3512 lm,
# 79.8 % of the bulb flux
# between 75 and 90: 1.1 % of the luminaire flux
# - this part causes just GLARE in case of road lighting and similar purposes
# 80deg and above: max 8.2 cd / 1000 lm , 0.3 % of the luminaire flux
# 90deg and above: max 3.5 cd / 1000 lm , 0.1 % of the luminaire flux
# CutOff Type: CIE_CutOff
# Increase of Sky Luminance due to light going
# from the luminaire difectly above horizon, as compared with the
# luminance produced by the light dispersed from the ground: 2 %
# Increase of Sky Luminance in Distant Places by light below 15.0 degrees
# due to light going from the luminaire directly above horizon: 12 %
# (for the zenith luminance such an angle suits places up to 19 km distance)
# The increases concern the following situation:
# Albedo = 0.10
# Zenith Extinction = 0.30 mag (i.e., direct light remaining 76 %)
# Indicatrix type =0 (0: acc. to P.Cinzano, 4..6: CIE sky types)
# (the downward-scattered part of lambertian uplight is 0.1108 then)
# 62.5 deg to <67.5 deg: max 710 cd / 1000 lm,
# 67.5 deg to < 76 deg: max 631 cd / 1000 lm,
# maximum spec. lum. intensity 710 cd / 1000 lm
# The following table gives luminous intensities which would be produced
# using a hypothetic bulb giving a luminous flux of 1000 lm (i.e., cd/klm):
# H: 0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0 90.0 100.0 110.0 120.0 130.0 140.0 150.0 160.0 170.0 180.0 190.0 200.0 210.0 220.0 230.0 240.0 250.0 260.0 270.0 280.0 290.0 300.0 310.0 320.0 330.0 340.0 350.0
#V:
0.0 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153 153
5.0 145 144 146 147 152 158 158 164 165 170 172 176 177 179 182 183 181 183 182 183 181 183 182 179 177 176 172 170 165 164 158 158 152 147 146 144
10.0 141 141 144 145 148 155 158 162 167 175 184 198 202 210 213 219 221 222 225 222 221 219 213 210 202 198 184 175 167 162 158 155 148 145 144 141
15.0 135 137 141 139 143 144 153 157 169 180 195 209 225 232 244 248 246 251 260 251 246 248 244 232 225 209 195 180 169 157 153 144 143 139 141 137
20.0 125 128 133 136 144 138 148 150 167 180 210 234 257 266 283 281 278 267 271 267 278 281 283 266 257 234 210 180 167 150 148 138 144 136 133 128
25.0 121 120 124 134 137 136 143 146 155 172 209 251 279 302 309 299 290 271 272 271 290 299 309 302 279 251 209 172 155 146 143 136 137 134 124 120
30.0 119 117 122 128 127 135 136 146 149 167 207 269 313 322 310 298 294 278 267 278 294 298 310 322 313 269 207 167 149 146 136 135 127 128 122 117
35.0 114 127 140 129 126 126 132 145 150 175 220 293 337 347 317 289 280 271 243 271 280 289 317 347 337 293 220 175 150 145 132 126 126 129 140 127
40.0 104 117 125 126 130 129 130 140 152 180 236 325 363 352 327 278 253 235 200 235 253 278 327 352 363 325 236 180 152 140 130 129 130 126 125 117
45.0 95.4 101 107 118 137 137 139 136 145 173 262 378 399 353 302 245 209 191 161 191 209 245 302 353 399 378 262 173 145 136 139 137 137 118 107 101
50.0 90.4 92.2 100 112 134 138 138 136 142 183 328 458 415 339 257 196 151 138 119 138 151 196 257 339 415 458 328 183 142 136 138 138 134 112 100 92.2
55.0 73.9 74.5 82.3 95.2 119 115 126 130 136 179 366 522 406 274 200 142 107 97.4 88.9 97.4 107 142 200 274 406 522 366 179 136 130 126 115 119 95.2 82.3 74.5
60.0 54.5 56.8 65.9 75.5 93.6 95.8 108 123 141 219 542 567 335 184 142 96.9 71.4 59.2 52.8 59.2 71.4 96.9 142 184 335 567 542 219 141 123 108 95.8 93.6 75.5 65.9 56.8
65.0 43.4 46.8 57.6 80.2 101 114 126 110 86.2 216 710 532 197 167 103 68.9 49.5 30.4 26.6 30.4 49.5 68.9 103 167 197 532 710 216 86.2 110 126 114 101 80.2 57.6 46.8
70.0 22.5 27.9 39.9 42.8 43.2 42.6 38.5 34.1 48.2 228 631 247 58.7 47.7 52.4 81.9 37.7 17.3 15.5 17.3 37.7 81.9 52.4 47.7 58.7 247 631 228 48.2 34.1 38.5 42.6 43.2 42.8 39.9 27.9
75.0 3.9 10.8 13.3 11.2 14.1 16.8 13.9 13.5 15.4 28.4 76.2 37.6 21.3 26.7 13.9 8.4 5.7 3.9 2.4 3.9 5.7 8.4 13.9 26.7 21.3 37.6 76.2 28.4 15.4 13.5 13.9 16.8 14.1 11.2 13.3 10.8
80.0 8.2 6.9 8.0 6.0 7.3 7.8 5.9 6.0 4.9 1.1 7.7 4.7 2.9 6.1 3.7 2.7 1.2 0.6 1.6 0.6 1.2 2.7 3.7 6.1 2.9 4.7 7.7 1.1 4.9 6.0 5.9 7.8 7.3 6.0 8.0 6.9
85.0 0.0 0.4 2.2 2.9 7.4 5.7 1.5 0.1 0.0 0.2 0.5 0.2 0.9 0.0 0.0 0.6 0.1 0.0 0.0 0.0 0.1 0.6 0.0 0.0 0.9 0.2 0.5 0.2 0.0 0.1 1.5 5.7 7.4 2.9 2.2 0.4
90.0 0.0 0.0 0.2 0.8 2.5 3.5 0.4 0.0 0.0 0.0 0.0 0.8 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.5 0.8 0.0 0.0 0.0 0.0 0.4 3.5 2.5 0.8 0.2 0.0
95.0 0.0 0.0 0.1 0.5 1.4 1.4 0.3 0.0 0.0 0.0 0.2 2.1 0.5 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.2 0.5 2.1 0.2 0.0 0.0 0.0 0.3 1.4 1.4 0.5 0.1 0.0
100.0 0.0 0.0 0.1 0.2 1.8 2.0 0.7 0.0 0.0 0.0 0.4 1.7 0.1 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.1 0.1 1.7 0.4 0.0 0.0 0.0 0.7 2.0 1.8 0.2 0.1 0.0
105.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
110.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
115.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
120.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
125.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
130.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
135.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
140.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
145.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
150.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
155.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
160.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
165.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
170.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
175.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0
180.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0