The field of the invention refers to high efficiency electrical power conditioning equipment which is used to power a variety of loads and it may be considered to be an AC:DC converter or a DC:DC converter.
High voltage power supplies (voltages >100 V) are essential to such technologies as Radar, X-ray inspection, Cancer therapy, Corona processing, Semiconductor Fabrication, and a variety of other important fields. In creating a high voltage power supply using existing inverter topologies such as the Cuk converter, there are problems due to the energy in the stray capacitance, and due to insulation in the presence of a magnetic core. The core distances in a DC power supply—particularly at high voltage—are all constrained because the leakage inductance of the system must be small, and distance increases inductance since the field energy between windings depends on the distance between windings.
An ideal system would allow for increased insulation, reductions in the core material used, and improved handing of the capacitive energy stored between the primary and the secondary. Operation with reduced coupling coefficient has been described by Abramyan in the unique case of pulse charging of output capacitances. Details of such transformer designs have been proposed—for example by Crewson. Adler showed how to use loosely coupled transformers in a very specific application. A general method of creating improved high voltage power supplies would be desirable.
In our new topology, we use the series inductance of the transformer as part of the current limiting means. This allows us to separate windings to a greater degree than in existing transformers. The total inductance of the secondary is part of the secondary parallel resonant circuit which allows us to have very low total inductances—even air core secondary windings. Such windings allow us to design air core transformers without the constraint of a conductive core, and with much improved high voltage properties. Magnetic material can be eliminated, used only to shape fields, or used to make transformers in our topology.
The capacitive energy in the secondary of a high voltage transformer is highly problematic. It causes ringing in conventional circuits and excess voltages in the windings. By using a parallel resonant system on the secondary winding, the capacitive energy is used in the circuit design. In general, capacitance is added to the secondary stray capacitance, but it may not necessarily be added depending on the specific design.
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The transformer consists of a primary (20), secondary (21), and possibly a ground shield (17). The secondary (21) and the resonant capacitance (23) make up a resonant circuit which is somewhat separate from the primary due to the imperfect coupling of the transformer. The secondary current is limited by the voltage multipliers 22, 24,25,26 (positive side) and 30,28, 31,29 (negative side). The output is applied to the load 40 and rectifier/multiplier capacitors 26 and 29. In an alternative embodiment, a “buck” regulator 71 can be added to the power supply.
The arrangement of outputs can be used to create either a unipolar or bipolar charge with respect to ground. The ground shield is used prevent transient capacitive coupling between primary and secondary.
The circuit is “phased” by controlling the applied frequency of the gate drive pulses to 9,10, 11, and 12 relative to the resonant frequency of the secondary f=½p(L2C2)1/2. In our topology when the drive and secondary resonant frequencies are within 10%, and when the coupling is >0.6, the secondary circuit “back EMF” or induced flux reduces the current in the primary, which in turn reduces the current to be switched. In some cases the current to be switched can be arranged to be zero. The reduction in current past the peak of the waveform is shown in FIG. 5. The current is turned off before the peak in the secondary waveform
In the “Half-H” circuit of
A challenge of our topology is that the secondary must carry an RMS current V/(2L2/C2)1/2 which increases the amount of wire which must be used on the secondary to reduce losses. Such wire is inexpensive and easy to wind.
The simplest transformer geometry for the loosely coupled resonant transformer topology consists of solenoidal coils such as are shown in FIG. 3. The wire is wound in a spiral on a circular form as shown in a plan view in FIG. 3. The coupling is equal to the area ratio of the inner over the outer coil if there are inner and outer coils only. In the configuration of
Combination of our topology with a preconverter such as a buck converter or power factor correction circuit is shown in
We can use two separate secondaries with two separate functions as shown in FIG. 6. In
Number | Name | Date | Kind |
---|---|---|---|
3450996 | Abramvan et al. | Jul 1969 | A |
4184197 | Cuk et al. | Jan 1980 | A |
5124658 | Adler | Jun 1992 | A |
5157593 | Jain | Oct 1992 | A |
5555494 | Morris | Sep 1996 | A |
5909362 | Adams | Jun 1999 | A |
6163242 | Crewson et al. | Dec 2000 | A |
6246599 | Jang et al. | Jun 2001 | B1 |
6418038 | Takahama et al. | Jul 2002 | B2 |
Number | Date | Country | |
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20040208025 A1 | Oct 2004 | US |