# IESNA: LM-63-1995 # [TEST] 46142 # [DATE] 10/06/75 # [MANUFAC] COOPER LIGHTING # [LUMCAT] GAL91SXXRCN # [LUMINAIRE] 1000W HPS RECTANGULAR CUTOFF FLOODLIGHT # [LAMP] 1000W HPS CL E-25 # [_REFLECTOR] HYDROFORMED ALUMINUM WITH INTERNAL BLADE LOUVERS # [_REFRACTOR] CLEAR FLAT GLASS # [_SOCKET POSITION] HORIZONTAL # [_LAMP LUMENS] 140000 # TILT=NONE # Bulbs: 1, 140000 lm each # Number of measured angles: 19 vertical, 19 horizontal ones # Photometric type: 1, Units type: 1 # Luminous openig width, length and height: 0.000 0.000 0.000 # Ballast factor: 1, Input power: 1000 W # Source file: gal9srcn.ies # Luminaire flux = 33095 lx, # 23.6 % of the bulb flux # between 75 and 90: 0.0 % of the luminaire flux # - this part causes just GLARE in case of road lighting and similar purposes # 80deg and above: max 0.0 cd/1000lm , 0.0 % of the luminaire flux # 90deg and above: max 0.0 cd/1000lm , 0.0 % of the luminaire flux # CutOff Type: Full_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: 0 % # Increase of Sky Luminance in Distant Places by light below 30.0 degrees # due to light going from the luminaire directly above horizon: 0 % # (for the zenith luminance such an angle suits places up to 10 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) # Illumination of a rectangle of 0.0:1.0:-2.5:2.5 pole heights: # Per cent of luminaire output falling there: 53.6 # for a unit case (glass at 1 m height, 1000 lm bulb) its illumination: # Maximum: 286.1 lx # Average: 25.4 lx # Minimum: 0.3 lx # Average/Minimum: 74.0 # The following table gives luminous intensities which would be produced # using a hypotetic 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 #V: 0.0 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 122.1 5.0 186.1 184.2 180.5 175.0 167.9 159.6 150.1 139.9 129.1 118.2 105.0 92.3 80.4 69.6 60.3 52.8 47.3 43.9 43.0 10.0 251.8 247.3 239.0 227.2 210.3 191.4 171.3 151.5 131.7 112.0 86.7 62.4 39.6 48.3 56.7 64.0 69.1 72.5 74.0 15.0 317.5 309.5 295.5 272.4 246.2 215.6 184.8 154.6 128.5 103.8 67.9 34.9 48.6 62.2 75.5 87.0 97.0 102.5 105.0 20.0 273.9 271.4 269.5 268.9 267.6 229.1 186.8 148.1 116.9 93.8 49.4 37.2 54.0 71.9 90.0 109.2 125.0 135.8 139.8 25.0 230.4 229.1 225.3 221.7 219.5 217.3 177.8 134.5 100.4 83.9 33.2 37.6 56.2 77.1 101.7 127.6 151.9 169.1 174.6 30.0 133.2 137.1 149.2 171.4 176.3 170.0 158.0 114.3 81.3 74.1 20.2 37.3 56.4 79.4 107.5 138.7 164.1 183.4 190.5 35.0 36.1 41.4 59.2 91.5 127.2 119.5 111.2 86.2 62.2 67.0 19.3 36.0 55.2 78.9 105.9 133.8 167.0 194.8 206.4 40.0 20.5 17.8 10.5 22.2 59.2 62.7 58.9 54.3 42.7 61.4 18.1 33.5 52.0 75.4 94.8 125.3 144.0 151.9 155.2 45.0 5.0 6.4 5.6 4.0 16.2 22.3 25.7 30.6 29.1 56.8 16.8 31.1 48.3 64.8 80.3 93.4 98.1 102.8 103.9 50.0 0.0 1.0 4.0 4.0 3.8 8.9 12.1 22.3 25.6 47.3 15.9 30.0 46.3 52.6 60.4 59.2 59.8 63.4 64.4 55.0 0.0 0.0 0.0 4.1 3.6 4.6 6.0 24.1 27.5 34.3 15.0 28.4 42.8 39.3 36.9 32.3 32.8 28.7 24.9 60.0 0.0 0.0 0.0 3.8 3.2 3.2 2.7 15.8 21.6 23.2 13.6 24.1 31.9 23.9 19.0 16.4 12.4 5.6 0.0 65.0 0.0 0.0 0.0 0.0 2.6 2.7 2.5 6.4 12.9 12.3 11.2 17.3 17.4 10.8 7.3 7.0 2.5 0.0 0.0 70.0 0.0 0.0 0.0 0.0 1.6 1.9 1.6 2.7 5.3 5.4 7.7 9.8 7.2 4.0 2.9 2.8 0.0 0.0 0.0 75.0 0.0 0.0 0.0 0.0 1.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.3 1.3 0.0 0.0 0.0 80.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 85.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 90.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0