FIELD OF INVENTION

The present invention relates to an AC/DC boost converter that has a high power factor and that can be connected to different network or mains voltages.

BACKGROUND OF THE INVENTION

Traditional rectifier circuits in which energy is first stored in a capacitor that is charged to a peak voltage from a rectifier bridge have low power factors. These circuits also usually generate markedly distorted sinusoidal currents that are liable to cause disturbances in a connected public switched network. Various solutions to this problem have been proposed.

US-A 5,383,109 teaches a rectifier circuit that has a high power factor. The circuit is constructed as a full-wave rectifier bridge for high mains voltages and as a voltage doubler for low mains voltages . Output voltage control and power factor correction are achieved with the aid of a high frequency booster circuit that includes two coils which are parallel-coupled at low mains voltages and series-coupled at high mains voltages. The circuit also includes two series- coupled transistors which function as pulse wave modulators.

One drawback with the aforedescribed circuit is that it includes double transistors and double switches, causing the circuit to be unnecessarily complicated.

SUMMARY OF THE INVENTION

The present invention solves, on the one hand, the problem of how the power and efficiency of a load coupled to an electric rectifying circuit shall be held constant irrespective of whether the alternating mains voltage takes one of two different values, e.g. either a value of 220V or a value of 110V, and, on the other hand, the problem of how an input current shall be able to assume a predetermined current curve.

Another problem is that in order to maintain constant load power values when the mains voltage assumes the aforesaid typical values for instance, certain circuit components must be dimensioned for very high energies and therewith become unnecessarily large and expensive.

The aforesaid problems are solved by means of the present invention with the aid of an improved electric rectifying circuit that includes a plurality of diodes, at least one coil, at least two capacitors, at least one selector switch, and at least one high frequency switch.

In one embodiment, two pairs of series-coupled diodes are arranged to form a full-wave rectifier. A DC voltage is applied to the full-wave rectifier at a connection point located in the connection line between the diodes of the one diode pair, and the other connection point is located between the diodes of the other diode pair. Two coils and the high frequency switch are coupled in parallel with the full-wave rectifier. One terminal of the first coil is connected to one DC-side of the full-wave rectifier that has the highest

potential, the so-called positive side. One terminal of the other coil is connected to the other DC-side of the full-wave rectifier that has the lowest potential, the so-called negative side. The high frequency switch is coupled between the two coils such that a first terminal of the high frequency switch will be coupled to a second terminal of the first coil and a second terminal of the high frequency switch will be coupled to the other terminal of the second coil.

A fifth and a sixth diode and two capacitors are coupled in parallel with the high frequency switch. The anode of the fifth diode is coupled to the first coil, so that said first coil will sit between the positive side in the full-wave rectifier and said fifth diode. The cathode of a sixth diode is coupled to the second coil, so that the second coil will sit between the negative side in the full-wave rectifier and the cathode on the sixth diode.

Two series-coupled capacitors are disposed between the first and the second diode. One terminal or side of a switch is connected to the connecting line between the one diode-pair in the full-wave rectifier. The other terminal or side of the switch is disposed on the connecting line between the two capacitors.

In the case of a relatively high AC voltage, for instance 220V, the switch is open and the circuit operates in a so- called low boost mode. In the case of a relatively low AC voltage, for instance 110V, the switch is closed and the circuit operates in a so-called high boost mode or voltage doubling mode. The switch will preferably change mode, or

state, automatically depending on the voltage to which the circuit is connected.

When the high frequency switch is conductive and the circuit operates in its high boost mode, current is taken from the mains voltage and stored in the two coils. When the high frequency switch is turned off, the magnetic energy in the coils is discharged and charges the capacitors . The pulse width of the high frequency switch is adapted so that the input current will assume a predetermined curve shape, for instance a sinusoidal shape.

When the high frequency switch conducts and the circuit operates in its low boost mode, the circuit functions as when in its high boost mode. When the high frequency switch is turned off, the magnetic energy is discharged from the first coil in one-half cycle period and charges the first capacitor. The magnetic energy is discharged from the other coil in the second-half cycle period and charges the second capacitor.

The described couplings enable the same energy to be converted in the high boost mode as in the low boost mode when the mains voltage in the high boost mode is twice as high as in the low boost mode.

When the same energy is converted in the low boost load, 220V, and the high boost mode, 110V, the current in the low boost mode must be twice as high as that in the high boost mode. This is achieved by increasing the conduction time of the high frequency switch to an appropriate value in the low boost mode.

The aim of the invention is to reduce the number of components and the size of the components required of an electric circuit for rectifying alternating voltages and capable of functioning between at least two different mains voltages, for instance 110V and 220V, and also to maintain constant circuit efficiency irrespective of which of the aforesaid mains voltages is used.

One advantage afforded by the present invention is that only one transistor is included in the circuit.

Another advantage afforded by the present invention is that the power factor is high.

The invention will now be described in more detail with reference to preferred embodiments thereof and also with reference to the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

Figure 1 illustrates a first embodiment of an inventive electric circuit .

Figure 2 illustrates a second embodiment of an inventive electric circuit.

Figure 3 shows a voltage curve for the circuit illustrated in Figure 1.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Shown in Figure 1 is a first embodiment of a voltage doubler rectifier circuit which can switch between variable mains voltages. The electric circuit includes two pairs of series- coupled diodes Dl, D2 and D2, D4 respectively, which are combined to form a full-wave rectifier. The full-wave rectifier has a negative side 11 and a positive side 12 and is connected to a network alternating voltage U such that one contact point 21 on said mains voltage U is located on the connection line between the diodes of the first diode pair, and the second contact point 22 on the mains alternating voltage U is located on the connection line between the diodes of the second diode pair.

Two coils LI, L2 and a high frequency switch Tl are connected in parallel with the diode pairs of the full-wave rectifier. A first terminal of the first coil LI is connected to the positive side 12 of the full-wave rectifier and a second terminal of said coil is connected to the high frequency switch Tl, which is comprised of a transistor in the illustrated case. The high frequency switch Tl may alternatively comprise a component that has properties similar to those of a transistor. The second terminal of the first coil is connected to the transistor drain. The transistor gate and transistor source are connected to control means not shown in the Figure. The first terminal of the second coil L2 is connected to the negative side 11 of the full-wave rectifier, while the second terminal of said coil L2 is connected to the transistor source. The coils may either be separate from one another or mounted on one and the same core.

Two diodes D5, D6 and two capacitors Cl, C2 are connected in parallel with the high frequency switch Tl. The anode of the fifth diode D5 is coupled to the second terminal of the coil LI. The cathode of the sixth diode D6 is connected to the second terminal of the coil L2. Two series-coupled capacitors Cl and C2 are disposed between the cathode of the diode D5 and the anode of the diode Dβ .

One side of a switch S is connected to the connecting line between the diodes of one of the diode pairs Dl, D3 or D2, D4. The other side of the switch is connected on the connecting line between the capacitors Cl and C2. The switch S of this embodiment alternates between two different states, the state of the switch being dependent on the mains or network alternating voltage to which the circuit is connected, and will preferably switch automatically between its two different states in accordance with methods well known in this field.

When the circuit is connected to relatively high mains voltages, for instance 220V, the selector switch S is open and the circuit operates in a so-called low boost mode. The diodes Dl, D2, D3 and D4 coact mutually to form a conventional full-wave rectifier. In its low boost mode or 220V mode, the inventive circuit functions as a so-called pump in accordance with known practice. When Tl is conductive, current is taken from the network or mains alternating voltage U via D1/D4 or D2/D3 and is stored in Ll and L2, which are then charged with magnetic energy. When Tl is switched off, the magnetic energy in Ll is discharged to Cl via D5, while the magnetic energy in Ll is discharged to Cl via D6. The pulse width on Tl is adapted at each point so

that the input current can be shaped according to a desired curve form over one period. Assume that the input current is sinusoidal, the amount of energy transferred from L1/L2 to C1/C2 at the top of the sinusoidal curve will be small but the current at its highest . Both current and energy are low at the zero crossing of the sinusoidal curve. The highest power is transferred between these points.

Figure 2 illustrates a second embodiment of an inventive voltage doubler rectification circuit which is able to switch states in dependence of a variable mains voltage. The electric circuit includes two pairs of series-coupled diodes

Dl, D3 and D2, D4 respectively, which are mutually connected to form a full-wave rectifier. The full-wave rectifier has a negative side 11 and a positive side 12. The full-wave rectifier is connected to a alternating mains voltage U such that one contact point 21 on the mains alternating voltage U is located on the connection line between the diodes of the first diode pair and the other contact point on the mains alternating voltage U is located on the connection line between the diodes of the second diode pair.

A coil Ll and a high frequency switch Tl are connected in parallel with the diode pairs of the full-wave rectifier. The first terminal of the coil Ll is connected to the positive side 12 of the full-wave rectifier, whereas the second terminal of said coil is connected to the high frequency switch Tl. In the illustrated embodiment the high frequency switch is comprised of a transistor, although it will be understood that a component having corresponding properties may alternatively be used. In the illustrated case, the second terminal of the coil is connected to the transistor

drain. The transistor is connected to the negative side ll of the full-wave rectifier. The transistor gate and transistor source are connected to a control means, not shown in the Figure. Two diodes D5, D6 and two capacitors Cl, C2 are connected in parallel with the transistor Tl. The anode of the fifth diode D5 is connected to the second terminal of the coil Ll. The cathode of the sixth diode OS is connected to the negative side of the full-wave rectifier and also to the transistor source. Two series-coupled capacitors Cl and C2 are connected between the cathode of diode D5 and the anode of diode D6.

One side of a switch S is connected to the connecting line between the diodes of one of the diode pairs Dl, D3 or D2, D4 of the full-wave rectifier. The other side of the switch is connected between the connecting line to the capacitors Cl and C2. The switch S of this embodiment switches between two different states, depending on the network alternating voltage to which the circuit is connected, said switch preferably switching automatically between said two states in accordance with methods well known in this field.

A pump of this kind will normally be dimensioned to charge a capacitor (Cl + C2) to the same voltage as at 220V even when the input voltage is 110V. The disadvantage with a pump of this kind is that it is necessary to convert a large amount of energy and that the pump is co mensurably large and expensive. Such pumps also have a low efficiency. The most energy is transferred at the top of the sinusoidal curve.

The inventive switchable pump converts the same amount of energy in the case of 110V as in the case of 220V. Only a

small amount of energy is transferred at the top of the sinusoidal curve, as in the case of 220V, but since this energy is taken from 110V via D2/D3 or D1/D4, the current must be twice as high, which is achieved by increasing the conducting time of Tl to an appropriate value.

The electric circuit illustrated in Figure 1 will also operate without the coil L2, although this will somewhat impair the performance of the circuit. The electric circuit may also include at least one current restricting resistor. The resistor may be placed with its one connection end between the cathode of the diode D6 and the second terminal of the coil L2. The other connection end of the resistor may be connected to the transistor Tl.

Figure 3 illustrates an example of the modus operandi of the pump and shows the configuration of the rectified voltage in the low boost mode of the circuit in Figure 1.

It will be understood that the invention is not restricted to the aforedescribed and illustrated embodiments thereof and that modifications can be made within the scope of the following Claims.