# IESNA: LM-63-1995 # [TEST] E418-14 # [DATE] # [MANUFAC] COOPER LIGHTING # [LUMCAT] CFB40SXX65 # [LUMINAIRE] 400W HPS 6H X 5V FLOODLIGHT # [LAMP] 400W HPS CL E-18 # [_REFLECTOR] SEMI-SPECULAR ALUMINUM # [_REFRACTOR] CLEAR FLAT GLASS # [_SOCKET POSITION] HORIZONTAL # [_LAMP LUMENS] 50000 # TILT=NONE # Bulbs: 1, 50000 lm each # (luminous intensites divided by 2.00 in the original ies file) # Number of measured angles: 25 vertical, 13 horizontal ones # Photometric type: 2, Units type: 1 # Luminous openig width, length and height: 0.580 1.100 0.000 # Ballast factor: 1, Input power: 465 W # Source file: cfb4s65.ies # Luminaire flux = 12960 raw, for the given bulb(s) it would be 25921 lx, # 51.8 % of the bulb flux # between 75 and 90: 48.9 % of the luminaire flux # - this part causes just GLARE in case of road lighting and similar purposes # 80deg and above: max 737.8 cd/1000lm , 51.0 % of the luminaire flux # 90deg and above: max 737.8 cd/1000lm , 31.6 % of the luminaire flux # CutOff Type: Unknown # 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:1568 % # Increase of Sky Luminance in Distant Places by light below 30.0 degrees # due to light going from the luminaire directly above horizon:3267 % # (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) # 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 4.0 12.0 20.0 28.0 36.0 44.0 52.0 60.0 68.0 76.0 84.0 90.0 #V: 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 6.0 19.0 20.0 19.2 17.6 11.0 5.7 4.0 9.2 15.3 20.8 26.1 31.4 0.0 14.0 25.0 31.3 47.4 36.2 29.4 30.4 8.3 9.7 3.5 4.6 15.6 26.8 0.0 22.0 114.8 114.2 110.6 99.4 86.4 72.2 53.6 23.7 4.6 2.8 5.5 22.4 0.0 30.0 119.9 119.4 118.2 107.6 98.4 83.6 66.2 40.9 12.3 3.2 2.1 18.2 0.0 38.0 135.7 135.3 137.5 130.3 112.8 93.9 75.3 51.1 22.2 3.6 2.3 14.3 0.0 46.0 176.9 175.5 171.7 161.8 136.2 107.6 82.9 60.6 28.3 7.8 2.5 10.8 0.0 54.0 206.2 205.2 203.6 193.9 162.8 121.3 94.2 67.8 34.5 10.0 2.6 7.8 0.0 62.0 282.1 279.4 264.0 236.1 193.5 144.4 110.2 72.1 38.6 10.4 2.6 5.2 0.0 70.0 252.9 251.0 255.6 247.1 208.5 144.2 103.9 72.5 40.4 9.5 2.6 3.3 0.0 78.0 263.7 262.7 262.2 259.1 228.7 162.0 112.6 71.8 39.5 7.5 2.5 2.0 0.0 86.0 463.2 468.4 480.2 450.3 383.6 268.5 145.4 70.3 38.2 7.7 2.2 1.3 0.0 90.0 737.8 732.2 705.9 660.6 577.6 428.6 180.9 69.8 37.7 8.0 2.0 1.2 0.0 94.0 562.5 559.9 554.5 533.8 465.2 304.4 135.0 64.0 32.2 7.3 2.0 1.3 0.0 102.0 205.3 201.3 190.2 167.6 131.5 99.6 59.1 37.8 20.7 5.8 1.8 2.0 0.0 110.0 50.5 50.7 54.0 51.6 35.3 22.5 15.0 8.8 10.0 4.4 1.7 3.3 0.0 118.0 16.2 16.5 17.8 17.5 14.4 11.0 7.7 5.5 4.2 3.1 1.6 5.2 0.0 126.0 8.5 8.8 9.2 8.1 5.9 4.3 4.2 3.3 3.0 2.2 1.5 7.7 0.0 134.0 2.9 2.9 3.6 4.3 3.3 3.0 2.7 2.4 2.1 1.8 1.4 10.8 0.0 142.0 3.2 3.0 2.6 2.6 2.3 2.3 2.2 2.0 1.8 1.5 1.3 14.4 0.0 150.0 1.3 1.4 1.6 1.8 1.8 1.8 1.8 1.7 1.6 1.4 1.2 18.4 0.0 158.0 0.5 0.6 1.0 1.3 1.4 1.5 1.5 1.4 1.4 1.3 5.0 22.7 0.0 166.0 0.4 0.6 1.1 1.4 1.4 1.4 1.4 1.4 1.3 3.6 15.9 27.3 0.0 174.0 0.6 1.0 1.4 1.5 1.4 1.4 1.4 9.2 16.2 22.0 27.2 32.0 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