could be isolated from the output.
The circuit configuration using an insulation transformer in the output circuit is
shown in Fig. 2. The circuit configuration of connecting an insulation transformer
in the input circuit, or inserting a DC-DC converter between the input and output,
has the same result, but insulation transformers are large, heavy and expensive. Use
of the DC-DC converter makes the circuit configuration complicated, and
manufacturing an insulation transformer for a large capacity inverter is difficult and
limits application of this circuit configuration to small capacity inverters.
A circuit configuration using a voltage-doubler rectifier + half-bridge inverter is
shown in
Fig. 3.
The rectifier circuit that is used in Fig. 3, is a high power factor converter circuit.
The DC voltage in the middle of this circuit becomes as follows when taking
fluctuation of the input voltage into consideration:
100V
1.15 2 = 325V
When this circuit is used for 200 V, double the voltage of the above figure becomes
necessary. This means that the semiconductors used in the latter stage of the
inverter must have a high withstand voltage, which reduces the efficiency.
Furthermore, it requires a larger air clearance and a longer creepage distance, which
hinder the design of a compact unit.
In addition, the mid-point voltage of capacity fluctuates in the half-bridge inverter
when an unbalanced load such as a half-wave rectifier load is connected.
Fluctuation of the mid-point voltage of capacity can create deviations of magnetism
and insufficient withstand voltage of the capacitor.
Each circuit system has its own merits and demerits as we have examined. We
have developed a floating output DC-DC converter (FCON) in order to solve these
problems for a UPS that operates on 200 V input and delivers output voltages of 3
kVA or more.
3. FCON Circuit
3.1 Operation of FCON
The FCON circuit that provides a floating output with respect to the input is shown
in
Fig. 4 (A).
The input energy is stored in the reactor L through the two semiconductor switches
Q1 and Q2. The stored energy is discharged through the two diodes D1 and D2. This
circuit operation is the same as that of a flyback converter or of a polarity-inverting
chopper circuit except that an insulating transformer is not necessary. The spike
voltage that is created normally in the polarity-inverting chopper circuit due to its
leakage inductance, is absorbed by Cdc and is suppressed.
The principle of obtaining a floating output using FCON is described below.
Fig. 4 (B) shows the energy storage mode in the reactor L.
When Q1 and Q2 are turned on, current flows into reactor L from the DC power
supply, and stores electromagnetic energy in L.
The capacity of the reactor that is required here is about 4% of the input
impedance, and is fairly small compared with the transformer.
During storage mode, the diodes D1 and D2 are reverse-biased by the reactor L
and the capacitor Cdc voltages, so that any current does not flow into the output
side that is separated from the input side.
When Q1 and Q2 are turned off, the system enters energy discharge mode as
shown in Fig. 4 (C). Energy that was stored in L during the storage mode is now
discharged into capacitor Cdc and the load side circuit through D1 and D2.
Because Q1 and Q2 are turned off during the discharge mode, the output side is
separated from the input side. This separation of the output from the input is
obtained by repeating the two modes of (B) and (C).
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