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    • 51. 发明授权
    • Cold cathode lamp with snap fitted specular reflector
    • 冷阴极灯带扣式镜面反射器
    • US5394314A
    • 1995-02-28
    • US139941
    • 1993-10-20
    • Jim Evanisko
    • Jim Evanisko
    • F21V7/22F21V17/06F21V7/14F21V7/16
    • F21V7/22F21V17/06
    • A cold cathode fluorescent tube reflector comprises an extruded ABS thermoplastic support subtending an arc of about 317 degrees and dimensioned to snap fit to the tubular body of fluorescent glass tube. The support has bonded thereto a metallized Mylar film which comprises vapor deposited aluminum which forms a specular second surface mirror. The aluminum coating is next to the support and protected from the ambient atmosphere by the clear Mylar film. The reflector is preferably for 7/8 inch diameter tubes and has a film thickness of about 0.8 mils. In one embodiment, the metallized film is attached during extruding of the support. In the alternative, the film is secured to the support during injection molding of the support.
    • 冷阴极荧光管反射器包括对着约317度的弧形的挤出的ABS热塑性支撑件,其尺寸被设计成与荧光玻璃管的管状体卡扣配合。 支撑体已经结合到金属化的聚酯薄膜上,该薄膜包括形成镜面反射镜的气相沉积铝。 铝涂层靠近支撑,并通过清除的聚酯薄膜保护环境。 反射器优选地用于直径为7/8英寸的管,并具有约0.8密耳的膜厚度。 在一个实施例中,金属化膜在支撑件的挤出期间被连接。 在替代方案中,在支撑件的注射成型期间将膜固定到支撑件。
    • 59. 发明专利
    • FR2721688B1
    • 1996-09-06
    • FR9407809
    • 1994-06-24
    • ARMINES
    • RABL ARI
    • F21V7/04F21V7/14F21V7/12
    • The present invention relates to a process for the production of the profile of reflective elements of a light as well as the lights obtained by this process, the light comprising at least two cylindrical reflective elements (5, 5'). This process is characterized in that it comprises the steps consisting of: defining the position of one end (Ro) of the profile of each reflective element (5, 5') defining an illumination function E( theta ) corresponding to a desired illumination curve, connected to a luminance function L( theta ) by the formula: E( theta )=L( theta )xcos2 theta =k[sxcos theta + rho rxsin ( phi - theta )- rho rosin ( phi o- theta )] cos2 theta if said end (Ro) of the profile of the reflective element (5, 5') is the downstream end of this latter, and an illumination function: E( theta )=L( theta )xcos2 theta =k[sxcos theta - rho rxsin ( phi - theta )+ rho roxsin ( phi o- theta )] cos2 theta if said end (Ro) is the upstream end of said profile determining, from said end (Ro), the coordinates of each of the points (R) of said profile of each reflective element (5, 5') satisfying the differential equation: d alpha /d theta =sin alpha xcos alpha [d log p( theta )/d theta ]-sin2 alpha , in which the function p( theta ) is equal to rho rxsin( phi - theta ) and the value of the angle alpha is equal to ( phi - theta )/r.
    • 60. 发明专利
    • FR2721688A1
    • 1995-12-29
    • FR9407809
    • 1994-06-24
    • ARMINES
    • RABL ARI
    • F21V7/04F21V7/14F21V7/12
    • The present invention relates to a process for the production of the profile of reflective elements of a light as well as the lights obtained by this process, the light comprising at least two cylindrical reflective elements (5, 5'). This process is characterized in that it comprises the steps consisting of: defining the position of one end (Ro) of the profile of each reflective element (5, 5') defining an illumination function E( theta ) corresponding to a desired illumination curve, connected to a luminance function L( theta ) by the formula: E( theta )=L( theta )xcos2 theta =k[sxcos theta + rho rxsin ( phi - theta )- rho rosin ( phi o- theta )] cos2 theta if said end (Ro) of the profile of the reflective element (5, 5') is the downstream end of this latter, and an illumination function: E( theta )=L( theta )xcos2 theta =k[sxcos theta - rho rxsin ( phi - theta )+ rho roxsin ( phi o- theta )] cos2 theta if said end (Ro) is the upstream end of said profile determining, from said end (Ro), the coordinates of each of the points (R) of said profile of each reflective element (5, 5') satisfying the differential equation: d alpha /d theta =sin alpha xcos alpha [d log p( theta )/d theta ]-sin2 alpha , in which the function p( theta ) is equal to rho rxsin( phi - theta ) and the value of the angle alpha is equal to ( phi - theta )/r.