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] 36272 # [MANUFAC] SiTECO # [LUMCAT] 5CX63321TS01 # [LUMINAIRE] CX 200 BASIC, streetlight # [MORE] "", "", "", "", "", "", "", "" # [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: 0.390 0.825 0.000 # Ballast factor: 1, Input power: 440 W # Source file: ies/36272.ies # Luminaire flux = 48583 lm, # 87.5 % of the bulb flux # between 75 and 90: 1.7 % of the luminaire flux # - this part causes just GLARE in case of road lighting and similar purposes # 80deg and above: max 32.4 cd / 1000 lm , 1.4 % of the luminaire flux # 90deg and above: max 32.4 cd / 1000 lm , 0.8 % of the luminaire flux # CutOff Type: CIE_Semi-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: 29 % # Increase of Sky Luminance in Distant Places by light below 15.0 degrees # due to light going from the luminaire directly above horizon: 146 % # (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 462 cd / 1000 lm, # 67.5 deg to < 76 deg: max 197 cd / 1000 lm, # maximum spec. lum. intensity 462 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: 0.0 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 200 5.0 171 172 172 173 177 182 187 190 195 200 204 210 213 214 219 222 224 228 230 228 224 222 219 214 213 210 204 200 195 190 187 182 177 173 172 172 10.0 146 146 149 157 163 170 180 191 201 211 221 232 241 246 246 249 249 253 256 253 249 249 246 246 241 232 221 211 201 191 180 170 163 157 149 146 15.0 132 134 138 143 149 157 169 185 200 217 231 243 250 263 277 279 273 275 281 275 273 279 277 263 250 243 231 217 200 185 169 157 149 143 138 134 20.0 122 126 132 131 137 149 160 181 207 232 252 272 284 296 297 308 304 302 303 302 304 308 297 296 284 272 252 232 207 181 160 149 137 131 132 126 25.0 118 123 125 125 131 134 143 167 214 257 281 293 307 318 331 335 340 332 332 332 340 335 331 318 307 293 281 257 214 167 143 134 131 125 125 123 30.0 112 114 116 122 123 126 136 159 216 270 311 330 342 350 352 359 358 354 367 354 358 359 352 350 342 330 311 270 216 159 136 126 123 122 116 114 35.0 101 102 104 108 114 118 128 153 206 279 325 350 365 381 377 384 382 396 405 396 382 384 377 381 365 350 325 279 206 153 128 118 114 108 104 102 40.0 93.1 93.5 95.1 99.0 105 112 128 144 207 306 365 390 394 405 409 399 391 384 384 384 391 399 409 405 394 390 365 306 207 144 128 112 105 99.0 95.1 93.5 45.0 85.0 87.6 87.7 96.9 105 116 118 134 208 319 385 399 398 396 382 335 301 296 296 296 301 335 382 396 398 399 385 319 208 134 118 116 105 96.9 87.7 87.6 50.0 77.6 78.5 82.3 93.2 97.9 104 116 132 196 314 387 396 392 339 290 242 206 200 203 200 206 242 290 339 392 396 387 314 196 132 116 104 97.9 93.2 82.3 78.5 55.0 71.9 69.5 77.5 87.3 87.7 93.4 113 144 194 316 404 411 379 280 182 147 135 110 94.1 110 135 147 182 280 379 411 404 316 194 144 113 93.4 87.7 87.3 77.5 69.5 60.0 60.9 59.1 71.0 78.3 84.2 90.3 118 129 196 388 451 411 329 218 122 85.0 74.4 63.0 53.2 63.0 74.4 85.0 122 218 329 411 451 388 196 129 118 90.3 84.2 78.3 71.0 59.1 65.0 40.6 44.4 56.4 71.3 80.0 101 122 136 223 435 462 391 274 159 89.4 68.7 40.4 42.1 35.8 42.1 40.4 68.7 89.4 159 274 391 462 435 223 136 122 101 80.0 71.3 56.4 44.4 70.0 16.3 20.7 26.5 41.5 53.1 74.0 35.1 37.6 86.8 193 197 161 92.0 56.5 94.3 63.3 27.7 31.1 23.8 31.1 27.7 63.3 94.3 56.5 92.0 161 197 193 86.8 37.6 35.1 74.0 53.1 41.5 26.5 20.7 75.0 3.2 3.7 4.0 6.1 4.1 4.5 6.3 11.1 26.7 39.5 43.2 40.2 26.0 9.6 7.6 12.7 25.3 20.5 13.4 20.5 25.3 12.7 7.6 9.6 26.0 40.2 43.2 39.5 26.7 11.1 6.3 4.5 4.1 6.1 4.0 3.7 80.0 0.3 0.8 1.0 1.1 0.2 1.4 1.3 1.5 6.2 8.5 7.1 3.7 3.2 1.6 2.2 1.2 0.3 1.5 2.2 1.5 0.3 1.2 2.2 1.6 3.2 3.7 7.1 8.5 6.2 1.5 1.3 1.4 0.2 1.1 1.0 0.8 85.0 0.5 0.0 0.0 0.2 0.1 0.1 1.0 8.2 19.3 17.2 17.4 12.8 1.8 0.1 0.2 0.8 1.0 3.5 3.8 3.5 1.0 0.8 0.2 0.1 1.8 12.8 17.4 17.2 19.3 8.2 1.0 0.1 0.1 0.2 0.0 0.0 90.0 1.4 0.1 0.0 0.0 0.0 0.1 7.1 19.2 32.4 28.0 20.2 19.1 6.2 0.0 0.0 0.0 2.5 8.0 7.8 8.0 2.5 0.0 0.0 0.0 6.2 19.1 20.2 28.0 32.4 19.2 7.1 0.1 0.0 0.0 0.0 0.1 95.0 0.1 0.1 0.0 0.0 0.0 0.6 3.5 8.2 25.8 24.6 13.7 4.5 1.7 0.0 0.0 0.0 1.0 4.0 5.0 4.0 1.0 0.0 0.0 0.0 1.7 4.5 13.7 24.6 25.8 8.2 3.5 0.6 0.0 0.0 0.0 0.1 100.0 0.4 0.0 0.0 0.0 0.0 0.3 3.0 5.0 16.9 19.2 10.5 5.4 1.8 0.0 0.0 0.3 0.1 3.6 0.5 3.6 0.1 0.3 0.0 0.0 1.8 5.4 10.5 19.2 16.9 5.0 3.0 0.3 0.0 0.0 0.0 0.0 105.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.1 0.1 1.2 1.1 0.1 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.1 0.0 0.1 1.1 1.2 0.1 0.1 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