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] 35720 # [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] indiv. Position, LP 40, RP 3 # [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/35720.ies # Luminaire flux = 45562 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 16.0 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: 13 % # Increase of Sky Luminance in Distant Places by light below 15.0 degrees # due to light going from the luminaire directly above horizon: 53 % # (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 438 cd / 1000 lm, # 67.5 deg to < 76 deg: max 419 cd / 1000 lm, # maximum spec. lum. intensity 438 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: 0.0 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 172 5.0 154 156 162 166 167 167 169 171 173 176 180 184 187 189 192 193 191 187 185 187 191 193 192 189 187 184 180 176 173 171 169 167 167 166 162 156 10.0 143 148 151 150 154 160 168 174 181 188 196 202 207 212 211 208 210 209 203 209 210 208 211 212 207 202 196 188 181 174 168 160 154 150 151 148 15.0 136 141 140 146 152 155 157 163 171 183 197 209 224 237 243 239 227 227 223 227 227 239 243 237 224 209 197 183 171 163 157 155 152 146 140 141 20.0 138 134 136 143 143 144 147 153 161 174 196 214 231 244 261 268 255 245 239 245 255 268 261 244 231 214 196 174 161 153 147 144 143 143 136 134 25.0 131 127 134 135 131 133 136 141 147 174 195 212 233 254 268 276 277 267 256 267 277 276 268 254 233 212 195 174 147 141 136 133 131 135 134 127 30.0 124 120 125 120 122 125 129 133 138 157 193 223 249 262 273 272 279 274 255 274 279 272 273 262 249 223 193 157 138 133 129 125 122 120 125 120 35.0 116 113 112 112 113 116 121 125 128 146 189 232 256 274 285 269 264 281 244 281 264 269 285 274 256 232 189 146 128 125 121 116 113 112 112 113 40.0 110 110 110 118 116 115 115 118 122 139 184 239 266 266 292 282 259 287 255 287 259 282 292 266 266 239 184 139 122 118 115 115 116 118 110 110 45.0 98.0 96.0 100 114 122 118 115 118 119 135 188 253 271 281 299 314 288 309 292 309 288 314 299 281 271 253 188 135 119 118 115 118 122 114 100 96.0 50.0 88.0 91.0 89.0 104 120 119 111 107 119 151 228 288 308 315 342 349 357 363 371 363 357 349 342 315 308 288 228 151 119 107 111 119 120 104 89.0 91.0 55.0 73.0 73.0 77.0 94.0 107 105 114 110 113 170 292 330 349 356 352 314 309 336 338 336 309 314 352 356 349 330 292 170 113 110 114 105 107 94.0 77.0 73.0 60.0 53.0 55.0 62.0 75.0 90.0 89.0 101 110 109 200 371 402 381 330 246 169 144 181 186 181 144 169 246 330 381 402 371 200 109 110 101 89.0 90.0 75.0 62.0 55.0 65.0 35.0 41.0 47.0 60.0 69.0 78.0 88.0 101 113 257 438 418 310 205 119 82.0 71.0 80.0 85.0 80.0 71.0 82.0 119 205 310 418 438 257 113 101 88.0 78.0 69.0 60.0 47.0 41.0 70.0 16.0 26.0 26.0 38.0 43.0 57.0 70.0 72.0 117 307 419 259 168 99.0 75.0 57.0 51.0 40.0 35.0 40.0 51.0 57.0 75.0 99.0 168 259 419 307 117 72.0 70.0 57.0 43.0 38.0 26.0 26.0 75.0 11.0 26.0 13.0 11.0 21.0 24.0 32.0 34.0 39.0 120 199 138 110 74.0 54.0 52.0 45.0 26.0 17.0 26.0 45.0 52.0 54.0 74.0 110 138 199 120 39.0 34.0 32.0 24.0 21.0 11.0 13.0 26.0 80.0 4.0 7.0 7.0 4.0 9.0 3.0 5.0 7.0 10.0 13.0 13.0 13.0 11.0 6.0 9.0 12.0 16.0 13.0 7.0 13.0 16.0 12.0 9.0 6.0 11.0 13.0 13.0 13.0 10.0 7.0 5.0 3.0 9.0 4.0 7.0 7.0 85.0 1.0 2.0 2.0 2.0 2.0 2.0 2.0 4.0 5.0 5.0 5.0 5.0 5.0 3.0 3.0 3.0 2.0 2.0 2.0 2.0 2.0 3.0 3.0 3.0 5.0 5.0 5.0 5.0 5.0 4.0 2.0 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 1.0 1.0 1.0 1.0 1.0 1.0 1.0 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 1.0 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 1.0 1.0 1.0 1.0 1.0 1.0 100.0 1.0 1.0 1.0 2.0 2.0 2.0 1.0 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 1.0 2.0 2.0 2.0 1.0 1.0 105.0 1.0 1.0 1.0 2.0 3.0 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 3.0 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 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 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 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 1.0 120.0 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