# IESNA: LM-63-1995 # [TEST] 766063 # [DATE] 6/14/91 # [MANUFAC] COOPER LIGHTING # [LUMCAT] HMX40SXXCM # [LUMINAIRE] 400W HIGH PRESSURE SODIUM TYPE V HIGH MAST # [LAMP] 400W HPS CL E-18 # [_REFLECTOR] ANODIZED SPUN ALUMINUM # [_REFRACTOR] FLAT GLASS # [_SOCKET POSITION] VERTICAL BASE UP # [_LAMP LUMENS] 50000 # TILT=NONE # Bulbs: 1, 50000 lm each # Number of measured angles: 31 vertical, 1 horizontal ones # Photometric type: 1, Units type: 1 # Luminous openig diameter (and height?): 2.330 ( 2.000 ) # Ballast factor: 1, Input power: 400 W # Source file: hmx4scm.ies # Luminaire flux = 31796 lx, # 63.6 % of the bulb flux # between 75 and 90: 9.6 % of the luminaire flux # - this part causes just GLARE in case of road lighting and similar purposes # 80deg and above: max 47.2 cd/1000lm , 2.6 % 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: 19.9 # for a unit case (glass at 1 m height, 1000 lm bulb) its illumination: # Maximum: 40.0 lx # Average: 25.3 lx # Minimum: 13.0 lx # Average/Minimum: 1.9 # 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): 0.0 36.9 5.0 40.5 15.0 30.5 25.0 41.4 35.0 55.7 45.0 81.4 50.0 105.5 55.0 143.9 60.0 194.6 62.5 222.1 65.0 235.8 67.5 231.3 70.0 205.1 72.5 166.3 75.0 124.5 77.5 82.4 80.0 47.2 82.5 25.0 85.0 9.8 87.5 1.7 90.0 0.0 95.0 0.0 105.0 0.0 115.0 0.0 125.0 0.0 135.0 0.0 145.0 0.0 155.0 0.0 165.0 0.0 175.0 0.0 180.0 0.0