Solid state RF light driver for electrodeless lighting
AssigneeNorthrop Grumman Corporation
InventorAlfred W. Morse
Life of this patent
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AssigneeNorthrop Grumman Corporation
InventorAlfred W. Morse
Estimating the term…
A transformerless power oscillator for driving a high intensity electrodeless light bulb. The driver uses a silicon carbide static induction transistor (SIT) operating as a power oscillator powered by an unregulated power supply potential generated by a full wave rectifier bridge connected to an AC power line. A CW output signal is generated at S-band and is coupled to the excitation coil of an electrodeless lamp by means of a matching network.
A solid state RF power oscillator connected to an AC power source for powering a high intensity electrodeless light bulb, comprising:
A solid state RF power oscillator connected to an AC power source for generating CW power for driving a high intensity electrodeless light bulb, comprising:
Dependencies are inferred from the claim text.
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No related US applications are recorded in the indexed filing history.
Circuit arrangements: in which the lamp is fed by high frequency AC , or with separate oscillator frequency
Active element in amplifier being semiconductor device: the amplifier being a single transistor
Active element in amplifier being semiconductor device: the amplifier comprising one or more field effect transistors
Comprising means for varying the frequency of the generator: the means comprising a voltage dependent capacitance
Term ended 19 May 2017 (estimated)
USPTO file history isn’t available for this patent, so only indexed dates are shown.
1. Field of the Invention
This invention relates generally to apparatus for exciting a light source and more particularly to solid state driver circuitry for exciting a high intensity electrodeless light bulb.
2. Description of Related Art
The present invention will become more fully understood from the detailed description provided hereinafter and the accompanying drawings which are provided by way of illustration only, and thus are not meant to be limitative of the present invention, and wherein:
FIG. 1 is an electrical schematic diagram illustrative of the preferred embodiment of the invention; and
FIG. 2 is an exploded diagram illustrative of means used for cooling the embodiment shown in FIG. 1.
Referring now to the drawings and more particularly to FIG. 1, reference numeral 10 denotes a field effect transistor having gate (g), source (s), and drain (d) electrodes, and more particularly a silicon carbide static induction transistor (SIT) which is capable of operating at S-band frequencies. Such a device has been developed by the present assignee and comprises a transistor which is significantly superior to prior art devices fabricated, for example, on silicon or gallium arsenide, particularly as it pertains to power, gain, operating voltage, efficiency and temperature tolerance. The details of a silicon carbide static induction transistor are furthermore disclosed in the above cross referenced related applications as well as U.S. Pat. No. 5,612,547.
The SIT 10 is powered by a DC supply voltage generated by a full wave rectifier bridge 12 which is connected to an AC power line voltage (120 VAC) shown in FIG. 1 applied across a pair of AC terminals 14 and 16. The DC output voltage from the bridge 12 is filtered by means of an L-C filter consisting of a series inductor 18 and a parallel capacitor 20 connected across a pair of output terminals 19 and 21. A pair of supply voltage leads 22 and 24 are connected across the capacitor 20, lead 22 being a positive (+) potential lead, while supply lead 24 is a reference or ground lead. The DC voltage which appears across leads 22 and 24 is from about 170 VDC at no load but drops down to about 108 VDC when loaded by the circuitry shown in FIG. 1. A SIT 10 used in connection with this invention has a nominal operating voltage of 108 V DC but has the capability to withstand transient voltages above 170 V DC. This occurs because silicon carbide S-band SITs can typically operate in the 80-100 V range, while having a breakdown voltage up to 350 V DC. This voltage capability can be increased as required for use with a transformerless power supply.
The SIT 10 as shown in FIG. 1 operates as a power oscillator by virtue of having its gate electrode (g) connected to the ground side lead 24 by means of an inductance reactance element 26, while the source (s) electrode is coupled to the ground side lead 24 by means of a length of stripline microwave transmission line 28, which acts as an impedance matching element, and a series connected frequency determining element 30, shown comprising a variable capacitive reactance. However, when desirable, the frequency determining element may be comprised of a resonator structure or crystal, not shown. The drain (d) electrode is connected to the power supply lead 22 by means of another length of stripline 32, which also acts as an impedance matching element, and a choke coil 34. The oscillator 35 configuration shown in FIG. 1 preferably operates at a frequency of 2450 MHz and can output, for example, at between 50 and 100 Watts of continuous (CW) power. A frequency of 900 MHz can also be implemented simply by changing component values in a well known manner.