Abstract:
Electric lamps wherein material inside a bulb is excited using capacitive coupling through the bulb wall to external electrodes, forming plasma which emits light. Methods described include use of light-emitting material including sulfur and/or selenium, and a circuit for driving the external electrodes.

Description:
FIELD 
       [0001]    The field relates to systems and methods for converting electricity to light, and more particularly to lamps wherein light is emitted primarily by plasma inside a bulb which is electrically excited using dielectric barrier discharge. 
       BACKGROUND 
       [0002]    Gas-discharge lamps, such as fluorescent lights, use light-emitting plasma in a bulb. The spectrum of light emitted depends on plasma composition. Sulfur can provide a good spectrum for lighting with good efficiency, and it also gives relatively fast startup time, but it cannot be used in a gas-discharge lamp because it reacts with the electrodes used to excite the plasma. For this reason, work on lights using sulfur has largely focused on electrodeless lamps with plasma excited by microwaves generated by a cavity magnetron. However, magnetrons are the limiting factor for the light lifetime, have mediocre efficiency, and are difficult to scale down to power levels appropriate for most lighting fixtures. 
         [0003]    “External electrode fluorescent lamps” (EEFLs) are fluorescent lights which use dielectric barrier discharge to excite the mercury plasma. EEFLs have been used for some specialty applications, but have not been competitive with conventional hot-cathode fluorescent lights for general-purpose lighting. The plasma of sulfur lamps has significantly lower conductivity than the plasma of fluorescent lights, leading to increased resistive energy transfer and increased light output. At the same time, using dielectric barrier discharge solves the problem of electrode corrosion in sulfur lamps. 
         [0004]    Design of driver circuits for EEFLs has been one issue limiting their adoption. A driver circuit for dielectric barrier discharge lamps is also presented. 
       BRIEF SUMMARY OF THE INVENTION 
       [0005]    The technical problem which the present invention relates to is conversion of electricity to light by means of electrically exciting material inside a bulb to form and maintain plasma which emits light, and more specifically to such lamps wherein dielectric barrier discharge is the means of excitation. The present invention solves this problem by means of using a relatively high-density plasma including sulfur as the light-emitting material, and by means of a driver circuit for driving capacitive couplings, and by the other means described in the claims. 
         [0006]    Advantageous effects of the present invention include making possible the manufacturing of electric lamps with improved combinations of efficiency, light quality, cost, lifespan, startup time, and environmental safety. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0007]      FIG. 1  illustrates an electric circuit diagram. 
           [0008]      FIG. 2  illustrates a bulb with a resistive heating system in top view. 
       
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       [0009]    The present invention is not limited to the construction details or component arrangements described in the following description or illustrated in the drawings. Other embodiments of the present invention are possible. The terminology used within is for the purpose of the description and should not be regarded as limiting except to the extent set forth in the claims. 
         [0010]    Turning to  FIG. 1 , a DC power source  1  is switched by power MOSFETs  2  and  3 . This power passes through a transformer winding  4  to the center point of capacitors  5  and  6 . The capacitors  5  and  6  can also act to smooth input power. A small optional capacitor  7  may be used to reduce switching losses. Optional fast diodes  7  and  8  may be placed in parallel with the MOSFETs to reduce switching losses. The diodes  7  and  8  may be silicon carbide Schottky diodes. 
         [0011]    Electrical energy is transferred from transformer winding  4  to transformer winding  9  through a magnetic core  10 . The transformer winding  9  is placed in series with an inductor  11 . The inductor  11  and transformer winding  9  may be combined by use of a transformer designed such that transformer winding  9  has high leakage inductance. This electrical energy is now transferred through the bulb  12  via capacitive couplings  13  and  14 . The capacitors  13  and  14  are formed by: external electrodes on the bulb wall, the bulb wall, and plasma inside the bulb. Electricity travels between the external electrodes through a plasma arc inside the bulb. The external electrodes may be: wire bent into a pattern, metal film, or metal foil. Possible electrode materials include tungsten and chromium. 
         [0012]    The plasma conductivity may decrease significantly once sulfur and/or other materials inside the bulb vaporize. The higher plasma conductivity before this point may make it difficult to vaporize those materials with only heat from the electrical arc. Turning to  FIG. 2 , a resistive heating element  18 , shown on a bulb  15  with electrodes  16  and  17 , is used to heat the bulb during startup. A power source  19  is connected to the heating element  18  through a switch  20 . The switch  20  may be a bimetallic strip which is on or near the bulb surface. The resistive heating element  18  may be a thin wire or metal film bonded to the bulb surface. The resistive heating element  18  may wind around the bulb in a spiral pattern. 
         [0013]    The resistive heating element  18  can also act as a capacitive coupling to the material inside the bulb, affecting the plasma arc shape during startup. Instead of a resistive heating element, the bulb may have a “guide electrode” consisting of a spiral of conductive material wound around the bulb, which may be electrically isolated or connected to an element with relatively constant voltage. Capacitive coupling to this guide electrode causes the initial electrical arc to follow the guide electrode along the inner surface of the bulb, which may vaporize sufficient material on the bulb&#39;s inner surface to facilitate startup of the lamp. 
         [0014]    For general-purpose lighting, the partial pressures in the bulb plasma at an average temperature of 3000K preferably include 1 to 40 bar of sulfur. An inert filler, such as argon, is needed to allow creation of an initial arc. Other components or compositions may be used depending on the desired spectrum of light emitted, especially metal halides used in metal halide lamps.