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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] 35617
# [MANUFAC] SiTECO
# [LUMCAT] 5NA551E1MR01
# [LUMINAIRE] SR 50, Street light
# [MORE] upper housing and gear tray made of glas fibre reinforced polyester
# [MORE] diffuser, acryl
# [LAMPCAT] Osram: NAV-T 70W SUPER
# [LAMP] HST 70W
# TILT=NONE
# Bulbs: 1, 6500 lm each
# Number of measured angles: 37 vertical, 37 horizontal ones
# Photometric type: 1, Units type: 2
# Luminous openig width, length and height: 0.290 0.603 0.000
# Ballast factor: 1, Input power: 83 W
# Source file: ies/35617.ies
# Luminaire flux = 5371 lm,
# 82.6 % of the bulb flux
# between 75 and 90: 9.7 % of the luminaire flux
# - this part causes just GLARE in case of road lighting and similar purposes
# 80deg and above: max 370.0 cd / 1000 lm , 3.1 % of the luminaire flux
# 90deg and above: max 3.0 cd / 1000 lm , 0.5 % of the luminaire flux
# CutOff Type: Non-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: 49 %
# (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 398 cd / 1000 lm,
# 67.5 deg to < 76 deg: max 997 cd / 1000 lm,
# maximum spec. lum. intensity 997 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:
0.0 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207 207
5.0 206 207 211 216 219 219 218 217 217 217 217 217 218 219 219 216 211 207 206 207 211 216 219 219 218 217 217 217 217 217 218 219 219 216 211 207
10.0 206 209 213 212 212 212 213 214 214 215 214 214 213 212 212 212 213 209 206 209 213 212 212 212 213 214 214 215 214 214 213 212 212 212 213 209
15.0 202 202 202 202 205 207 211 214 216 217 216 214 211 207 205 202 202 202 202 202 202 202 205 207 211 214 216 217 216 214 211 207 205 202 202 202
20.0 191 191 193 194 197 203 211 217 222 225 222 217 211 203 197 194 193 191 191 191 193 194 197 203 211 217 222 225 222 217 211 203 197 194 193 191
25.0 182 182 185 187 190 198 212 228 238 241 238 228 212 198 190 187 185 182 182 182 185 187 190 198 212 228 238 241 238 228 212 198 190 187 185 182
30.0 173 172 173 176 184 191 205 223 233 237 233 223 205 191 184 176 173 172 173 172 173 176 184 191 205 223 233 237 233 223 205 191 184 176 173 172
35.0 161 161 162 167 175 182 193 216 235 241 235 216 193 182 175 167 162 161 161 161 162 167 175 182 193 216 235 241 235 216 193 182 175 167 162 161
40.0 147 145 147 155 164 170 181 205 237 247 237 205 181 170 164 155 147 145 147 145 147 155 164 170 181 205 237 247 237 205 181 170 164 155 147 145
45.0 130 129 133 141 146 156 185 198 243 261 243 198 185 156 146 141 133 129 130 129 133 141 146 156 185 198 243 261 243 198 185 156 146 141 133 129
50.0 112 111 115 120 130 136 155 190 244 270 244 190 155 136 130 120 115 111 112 111 115 120 130 136 155 190 244 270 244 190 155 136 130 120 115 111
55.0 90.0 90.0 94.0 100 108 119 139 175 267 318 267 175 139 119 108 100 94.0 90.0 90.0 90.0 94.0 100 108 119 139 175 267 318 267 175 139 119 108 100 94.0 90.0
60.0 59.0 65.0 70.0 88.0 93.0 100 156 110 294 400 294 110 156 100 93.0 88.0 70.0 65.0 59.0 65.0 70.0 88.0 93.0 100 156 110 294 400 294 110 156 100 93.0 88.0 70.0 65.0
65.0 38.0 47.0 56.0 63.0 72.0 49.0 34.0 51.0 303 398 303 51.0 34.0 49.0 72.0 63.0 56.0 47.0 38.0 47.0 56.0 63.0 72.0 49.0 34.0 51.0 303 398 303 51.0 34.0 49.0 72.0 63.0 56.0 47.0
70.0 17.0 24.0 29.0 24.0 18.0 12.0 22.0 48.0 626 820 626 48.0 22.0 12.0 18.0 24.0 29.0 24.0 17.0 24.0 29.0 24.0 18.0 12.0 22.0 48.0 626 820 626 48.0 22.0 12.0 18.0 24.0 29.0 24.0
75.0 9.0 12.0 12.0 16.0 20.0 20.0 17.0 35.0 828 997 828 35.0 17.0 20.0 20.0 16.0 12.0 12.0 9.0 12.0 12.0 16.0 20.0 20.0 17.0 35.0 828 997 828 35.0 17.0 20.0 20.0 16.0 12.0 12.0
80.0 2.0 3.0 5.0 7.0 18.0 23.0 14.0 20.0 213 370 213 20.0 14.0 23.0 18.0 7.0 5.0 3.0 2.0 3.0 5.0 7.0 18.0 23.0 14.0 20.0 213 370 213 20.0 14.0 23.0 18.0 7.0 5.0 3.0
85.0 1.0 2.0 3.0 4.0 8.0 10.0 7.0 10.0 30.0 39.0 30.0 10.0 7.0 10.0 8.0 4.0 3.0 2.0 1.0 2.0 3.0 4.0 8.0 10.0 7.0 10.0 30.0 39.0 30.0 10.0 7.0 10.0 8.0 4.0 3.0 2.0
90.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 3.0 3.0 3.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 3.0 3.0 3.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0
95.0 0.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0 0.0 1.0 1.0 1.0 1.0 1.0 1.0 2.0 2.0 2.0 2.0 2.0 1.0 1.0 1.0 1.0 1.0 1.0
100.0 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 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 1.0 1.0 1.0 1.0 1.0
105.0 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 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 1.0 1.0 1.0 1.0 1.0
110.0 0.0 0.0 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 0.0 0.0 0.0 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 0.0
115.0 0.0 0.0 0.0 1.0 1.0 1.0 2.0 3.0 3.0 2.0 3.0 3.0 2.0 1.0 1.0 1.0 0.0 0.0 0.0 0.0 0.0 1.0 1.0 1.0 2.0 3.0 3.0 2.0 3.0 3.0 2.0 1.0 1.0 1.0 0.0 0.0
120.0 0.0 0.0 0.0 1.0 1.0 1.0 2.0 3.0 3.0 3.0 3.0 3.0 2.0 1.0 1.0 1.0 0.0 0.0 0.0 0.0 0.0 1.0 1.0 1.0 2.0 3.0 3.0 3.0 3.0 3.0 2.0 1.0 1.0 1.0 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