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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] 35721
# [MANUFAC] SiTECO
# [LUMCAT] 5NA553E1TT13
# [LUMINAIRE] SR 200, Street light
# [MORE] upper housing and gear tray made of glas fibre reinforced polyester,
# [MORE] with power reduction relay "ECO"
# [MORE] radial facetted reflector, diffuser, PC
# [MORE] default position, LP 40, RP 4
# [LAMPCAT] Osram: NAV-T 400W SUPER
# [LAMP] HST 400W
# TILT=NONE
# Bulbs: 1, 55500 lm each
# Number of measured angles: 37 vertical, 37 horizontal ones
# Photometric type: 1, Units type: 2
# Luminous openig width, length and height: 0.358 0.870 0.000
# Ballast factor: 1, Input power: 440 W
# Source file: ies/35721_D.ies
# Luminaire flux = 45551 lm,
# 82.1 % of the bulb flux
# between 75 and 90: 2.8 % of the luminaire flux
# - this part causes just GLARE in case of road lighting and similar purposes
# 80deg and above: max 17.0 cd / 1000 lm , 1.1 % of the luminaire flux
# 90deg and above: max 4.0 cd / 1000 lm , 0.5 % 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: 14 %
# Increase of Sky Luminance in Distant Places by light below 15.0 degrees
# due to light going from the luminaire directly above horizon: 56 %
# (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 402 cd / 1000 lm,
# 67.5 deg to < 76 deg: max 399 cd / 1000 lm,
# maximum spec. lum. intensity 426 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:
0.0 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166 166
5.0 151 151 154 157 158 159 160 163 164 167 170 173 176 178 180 179 178 177 179 177 178 179 180 178 176 173 170 167 164 163 160 159 158 157 154 151
10.0 141 143 146 145 149 154 158 164 170 176 183 188 193 197 196 196 198 196 195 196 198 196 196 197 193 188 183 176 170 164 158 154 149 145 146 143
15.0 135 139 137 143 147 149 151 154 163 171 182 194 209 222 229 225 215 213 217 213 215 225 229 222 209 194 182 171 163 154 151 149 147 143 137 139
20.0 137 132 136 141 141 140 143 148 152 164 182 199 218 232 248 255 241 232 233 232 241 255 248 232 218 199 182 164 152 148 143 140 141 141 136 132
25.0 131 126 133 133 130 131 133 138 145 157 181 199 220 241 257 267 267 258 253 258 267 267 257 241 220 199 181 157 145 138 133 131 130 133 133 126
30.0 124 121 124 119 121 124 126 131 133 147 178 209 235 250 264 266 272 270 256 270 272 266 264 250 235 209 178 147 133 131 126 124 121 119 124 121
35.0 117 114 112 112 112 115 119 125 126 138 175 222 246 265 281 268 263 278 249 278 263 268 281 265 246 222 175 138 126 125 119 115 112 112 112 114
40.0 112 110 109 116 115 115 115 119 120 130 170 232 262 266 289 283 262 292 260 292 262 283 289 266 262 232 170 130 120 119 115 115 115 116 109 110
45.0 100 98.0 99.0 111 121 118 114 119 118 126 173 245 266 278 303 320 293 323 305 323 293 320 303 278 266 245 173 126 118 119 114 118 121 111 99.0 98.0
50.0 91.0 93.0 88.0 102 117 118 112 106 116 126 205 275 298 311 348 369 388 401 422 401 388 369 348 311 298 275 205 126 116 106 112 118 117 102 88.0 93.0
55.0 76.0 75.0 77.0 92.0 106 105 113 109 110 133 259 319 344 362 375 363 380 409 426 409 380 363 375 362 344 319 259 133 110 109 113 105 106 92.0 77.0 75.0
60.0 61.0 60.0 66.0 78.0 94.0 94.0 106 115 112 155 328 403 386 347 281 205 188 268 280 268 188 205 281 347 386 403 328 155 112 115 106 94.0 94.0 78.0 66.0 60.0
65.0 38.0 43.0 48.0 60.0 69.0 82.0 84.0 101 111 190 396 402 319 221 134 90.0 84.0 129 147 129 84.0 90.0 134 221 319 402 396 190 111 101 84.0 82.0 69.0 60.0 48.0 43.0
70.0 17.0 27.0 26.0 36.0 41.0 55.0 69.0 65.0 104 240 399 271 183 105 81.0 59.0 54.0 47.0 46.0 47.0 54.0 59.0 81.0 105 183 271 399 240 104 65.0 69.0 55.0 41.0 36.0 26.0 27.0
75.0 12.0 27.0 12.0 10.0 18.0 19.0 30.0 32.0 39.0 93.0 173 150 122 67.0 54.0 56.0 46.0 27.0 19.0 27.0 46.0 56.0 54.0 67.0 122 150 173 93.0 39.0 32.0 30.0 19.0 18.0 10.0 12.0 27.0
80.0 4.0 8.0 7.0 3.0 8.0 3.0 5.0 7.0 9.0 11.0 13.0 13.0 11.0 6.0 12.0 14.0 17.0 13.0 7.0 13.0 17.0 14.0 12.0 6.0 11.0 13.0 13.0 11.0 9.0 7.0 5.0 3.0 8.0 3.0 7.0 8.0
85.0 1.0 2.0 2.0 2.0 2.0 2.0 3.0 4.0 5.0 5.0 5.0 6.0 5.0 3.0 3.0 3.0 3.0 3.0 3.0 3.0 3.0 3.0 3.0 3.0 5.0 6.0 5.0 5.0 5.0 4.0 3.0 2.0 2.0 2.0 2.0 2.0
90.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 4.0 3.0 3.0 3.0 3.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 3.0 3.0 3.0 3.0 4.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0
95.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0
100.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0
105.0 1.0 1.0 1.0 2.0 4.0 2.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 4.0 2.0 1.0 1.0
110.0 1.0 1.0 1.0 1.0 2.0 1.0 1.0 2.0 1.0 1.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 0.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 1.0 1.0 2.0 1.0 1.0 2.0 1.0 1.0 1.0
115.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 0.0 0.0 0.0 0.0 0.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0
120.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0
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