Zero-cross detection circuit

1. Field of the Invention

The present invention relates to a zero-cross detection circuit for detecting a point at which an input alternating-current (AC) voltage crosses a predetermined voltage (0 V). More particularly, the present invention relates to a zero-cross detection circuit which is connected to a full-wave rectifying and smoothing circuit powered from a commercial AC power supply for full-wave rectification and smoothing, and which is also connected to a switching regulator for separating and stepping down the output from the full-wave rectifying and smoothing circuit to output a desired DC voltage.

2. Description of the Related Art

FIG. 10 is a circuit diagram of a power supply circuit using a commercial AC power input, in particular, showing a zero-cross detection circuit in the related art for detecting a point at which an input AC voltage crosses zero volts, and a rectifying and smoothing circuit and a switching regulator which are connected to the zero-cross detection circuit.

In FIG. 10, lines Line 1 and Line 2 are connected to a commercial AC power supply through a filter circuit (not shown). The full-wave rectifying and smoothing circuit is formed of diodes D 11 , D 12 , D 13 , and D 14 , and a smoothing capacitor C 11 .

In FIG. 10, the switching regulator which is the self-excitation type is formed of components indicated by Q 21 , Q 22 , C 21 , C 22 , C 31 , C 32 , D 31 , IC 31 , R 21 to R 27 , R 31 to R 35 , and PC 21 . The switching regulator is insulated by a transformer T 21 , and generates a constant voltage of +24 V.

The zero-cross detection circuit is formed of components indicated by Q 41 , C 41 , C 42 , D 41 , R 41 , R 43 , R 44 , R 45 , and PC 41 . In the zero-cross detection circuit, a low-voltage output terminal of the full-wave rectifying and smoothing circuit is connected to the emitter of the n-p-n transistor Q 41 , and the resistor R 43 is connected between the base and emitter of the transistor Q 41 . The resistor R 43 and the capacitor C 41 are connected in parallel with each other, and the resistor R 41 is connected between the capacitor C 41 and the line Line 1 .

A half-wave rectifying circuit is formed of the resistors R 41 and R 43 in the zero-cross detection circuit, and the diode D 13 , and the output of the half-wave rectifying circuit is applied between the base and emitter of the transistor Q 41 . If the potential of the line Line 1 is higher than the potential of the line Line 2 , a current flows in the resistor R 41 ; otherwise, no current flows in the resistor R 41 . The resistances of the resistors R 41 and R 43 are set to suitable values so that the collector potential in the transistor Q 41 can substantially change according to the potential magnitude of the lines Line 1 and Line 2 . The high/low edges of the collector potential in the transistor Q 41 correspond to zero crossings, and a zero-cross signal ZEROX is transmitted to the secondary of the transformer T 21 via the photocoupler PC 41 . The capacitor C 41 is a capacitor for removing noise, and is not essential to the zero-cross detection circuit.

FIGS. 11A to 11 C and 12 A to 12 C are signal waveforms of the components in the zero-cross detection circuit.

In FIGS. 11A to 11 C and 12 A to 12 C, the x-axis represents time. FIG. 11A shows the potential of the line Line 1 with respect to a ground GND, FIG. 11B shows the potential of the line Line 2 with respect to the ground GND, and FIG. 11C shows the difference in potential between the lines Line 1 and Line 2 . FIG. 12A shows a current flowing in the resistor R 41 , FIG. 12B shows an enlarged version of the y-axis in FIG. 12A, and FIG. 12C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX. In the secondary of the transformer T 21 , the voltage is stepped down from the output (+24 V) of the switching regulator to +3.3 V.

FIG. 13 shows another zero-cross detection circuit in the related art. The zero-cross detection circuits shown in FIGS. 10 and 13 are different from each other in that the zero-cross detection circuit shown in FIG. 13 further includes capacitors C 12 and C 13 . Specifically, in FIG. 13, the capacitors C 12 and C 13 are connected to the high-voltage output terminal and the low-voltage output terminal of the full-wave rectifying and smoothing circuit, respectively, and the node between the capacitors C 12 and C 13 is grounded.

In general, for the terminal noise suppression purpose, a capacitor (a so-called Y-capacitor) of approximately several thousand picofarads is connected between a commercial AC power supply line and a ground GND. The capacitors C 12 and C 13 are Y-capacitors. Although a Y-capacitor may be connected to an input terminal of a full-wave rectifying circuit, it is more effective for the terminal noise suppression purpose to connect a Y-capacitor to an output terminal of a full-wave rectifying circuit. The configuration shown in FIG. 13 is often used.

In the circuit configuration shown in FIG. 13, if Y-capacitors (the capacitors C 12 and C 13 ) have a small capacitance or if the commercial AC power supply exhibits a normal waveform, no problem occurs. However, if the Y-capacitors have a large capacitance or if the commercial AC power supply exhibits an undesirable waveform which is not normal, a problem occurs.

FIGS. 14A to 14 C are signal waveforms of the components in the zero-cross detection circuit when the Y-capacitors in the circuit shown in FIG. 13 have a relatively small capacitance. Since the waveforms indicating the potential of the line Line 1 with respect to the ground GND, the potential of the line Line 2 with respect to the ground GND, and the difference in potential between the lines Line 1 and Line 2 are the same as those shown in FIGS. 11A to 11 C, a description thereof is omitted.

FIG. 14A shows a current flowing in the resistor R 41 , FIG. 14B shows an enlarged version of the y-axis in FIG. 14A, and FIG. 14C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX.

As is apparent from FIGS. 14A to 14 C, if the Y-capacitors have a relatively small capacitance, a zero-cross signal ZEROX can be successfully generated.

FIGS. 15A to 15 C are signal waveforms of the components in the zero-cross detection circuit when the Y-capacitors in the circuit shown in FIG. 13 have a relatively large capacitance. Since the waveforms indicating the potential of the line Line 1 with respect to the ground GND, the potential of the line Line 2 with respect to the ground GND, and the difference in potential between the lines Line 1 and Line 2 are the same as those shown in FIGS. 11A to 11 C, a description thereof is omitted.

FIG. 15A shows a current flowing in the resistor R 41 , FIG. 15B shows an enlarged version of the y-axis in FIG. 15A, and FIG. 15C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX.

As is apparent from FIGS. 15A to 15 C, if the Y-capacitors have a large capacitance, the zero-cross signal ZEROX shown in FIG. 15C does not indicate a correct zero-cross point.

In FIG. 15B, the current flowing in the resistor R 41 rises in a sine-wave fashion at about 15 msec, thus causing a zero-cross point to be unsuccessfully detected.

This current flows in the Y-capacitors C 12 and C 13 towards the ground GND.

The potential of either the line Line 1 or Line 2 , whichever is lower, is used as the low-voltage output potential of the full-wave rectifying and smoothing circuit with respect to the ground GND. This exhibits a half-wave rectified waveform. The high-voltage output potential of the full-wave rectifying and smoothing circuit with respect to the ground GND is produced by adding the capacitance potential stored in the capacitor C 11 to the low-voltage output potential, and, if a DC component is removed, the output would be equal to the half-wave rectified waveform. A current flowing in the Y-capacitors C 12 and C 13 is therefore produced by differentiating the voltage of the half-wave rectified waveform.

This current flows in the rectifier diodes D 11 to D 14 when those diodes are conducting, and otherwise flows in the resistor R 41 . Since the full-wave rectifying and smoothing circuit is capacitor-input, the rectifier diodes D 11 to D 14 have a small conduction angle and do not conduct most of the time.

Therefore, a current shown as the waveform between about 15 and 20 msec in FIG. 15B flows in the resistor R 41 .

FIGS. 16A to 16 C and 17 A to 17 C are signal waveforms of the components in the zero-cross detection circuit when the commercial AC power supply on which the third harmonic is superposed exhibits an undesirable waveform in the circuit shown in FIG. 13 .

FIG. 16A shows the potential of the line Line 1 with respect to the ground GND, FIG. 16B shows the potential of the line Line 2 with respect to the ground GND, and FIG. 16C shows the difference in potential between the lines Line 1 and Line 2 . FIG. 17A shows a current flowing in the resistor R 41 , FIG. 17B shows an enlarged version of the y-axis in FIG. 17A, and FIG. 17C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX.

FIGS. 18A to 18 C and 19 A to 19 C are signal waveforms of the components in the zero-cross detection circuit when the commercial AC power supply which has a 60° phase difference rather than a 180° phase difference exhibits an undesirable waveform in the circuit shown in FIG. 13 .

FIG. 18A shows the potential of the line Line 1 with respect to the ground GND, FIG. 18B shows the potential of the line Line 2 with respect to the ground GND, and FIG. 18C shows the difference in potential between the lines Line 1 and Line 2 . FIG. 19A shows a current flowing in the resistor R 41 , FIG. 19B shows an enlarged version of the y-axis in FIG. 19A, and FIG. 19C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX.

As is apparent from FIGS. 16A to 19 C, if the commercial AC power supply exhibits an undesirable waveform, a correct zero-cross signal ZEROX is not generated.

These phenomena are also caused by a current flowing in the Y-capacitors C 12 and C 13 towards the ground GND.

If the harmonic is superposed on the commercial AC power supply, the harmonic component is also superposed on the output potential of the full-wave rectifying and smoothing circuit with respect to the ground GND. The harmonic distortion causes a current shown as the waveform between 15 and 20 msec in FIG. 17B to flow in the resistor R 41 .

If the line Line 1 is 180° out of phase with respect to the line Line 2 of the commercial AC power supply, the difference in potential between the lines Line 1 and Line 2 is phase-shifted with respect to the output potential of the full-wave rectifying and smoothing circuit with respect to the ground GND, thus causing a current shown as the waveform between about 15 and 20 msec in FIG. 19B to flow in the resistor R 41 . In FIG. 19B, the current flowing in the resistor R 41 is zero at about 18 msec because the rectifier diodes D 11 and D 14 are conducting, and the current at this time is supplied to the Y-capacitors C 11 and C 12 via the diode D 14 .

Accordingly, it is an object of the present invention to provide a zero-cross detection circuit of the half-wave rectifier type, which is correctly operated when a Y-capacitor is provided after a full-wave rectifying and smoothing circuit for the terminal noise suppression purpose and which reliably generates a zero-cross signal when a commercial AC power supply exhibits an undesirable waveform.

A zero-cross detection circuit according to the present invention is connected to a power supply device which includes a full-wave rectifying and smoothing circuit, two capacitors, and a switching regulator. The full-wave rectifying and smoothing circuit is powered via first and second lines from a commercial AC power supply for full-wave rectification and smoothing. The two capacitors have first ends connected to high-voltage and low-voltage output terminals of the full-wave rectifying and smoothing circuit, respectively, and second ends connected to a ground. The switching regulator separates and steps down the output from the full-wave rectifying and smoothing circuit to output a desired DC voltage. The zero-cross detection circuit according to the present invention includes a transistor of which the emitter is connected to the low-voltage output terminal of the full-wave rectifying and smoothing circuit for outputting a zero-cross detection signal from the collector; a first resistor connected between the base and emitter of the transistor; a second resistor connected between the first line and the base of the transistor; and a third resistor connected between the second line and the emitter of the transistor.

Preferably, the third resistor has substantially the same resistance as that of the second resistor.

Therefore, the zero-cross detection circuit according to the present invention can be correctly operated when the above-noted Y-capacitors are provided after a full-wave rectifying and smoothing circuit for the terminal noise suppression purpose. Furthermore, if the commercial AC power supply exhibits an undesirable waveform, the zero-cross detection circuit can reliably generate a zero-cross signal.

Preferably, the zero-cross detection circuit includes a diode connected between the base and emitter of the transistor in such a manner that the anode of the diode is connected to the emitter of the transistor.

Also, a diode may be connected between the first line and the second resistor in such a manner that the anode of the diode is connected to the first line. The second resistor and the diode may be replaced.

This arrangement prevents a reverse bias from being applied between the base and emitter of the transistor if noise is present in the commercial AC power supply. Additionally, another diode may be connected between the second line and the third resistor in such a manner that the anode of the second diode is connected to the second line.

Further objects, features and advantages of the present invention will become apparent from the following description of the preferred embodiments with reference to the attached drawings.

FIG. 1 is a circuit diagram of a power supply device using a commercial AC power supply, showing a zero-cross circuit according to a first embodiment of the present invention, and a rectifying and smoothing circuit and a switching regulator which are connected to the zero-cross detection circuit.

FIGS. 2A to 2 C are waveforms of a normal commercial AC power supply.

FIGS. 3A to 3 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the Y-capacitors have a large capacitance.

FIGS. 4A to 4 C are waveforms of an undesired commercial AC power supply which involves a third harmonic component.

FIGS. 5A to 5 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the third harmonic is superposed on the commercial AC power supply.

FIGS. 6A to 6 C are waveforms of an undesired commercial AC power supply which has a 60° phase difference.

FIGS. 7A to 7 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the commercial AC power supply has a 60° phase difference.

FIG. 8 is a circuit diagram of a power supply device including a zero-cross detection circuit according to a second embodiment of the present invention.

FIG. 9 is a circuit diagram of a power supply device including a zero-cross detection circuit according to a third embodiment of the present invention.

FIG. 10 is a circuit diagram of a power supply device using a commercial AC power input, showing a zero-cross detection circuit in the related art, and a rectifying and smoothing circuit and a switching regulator which are connected to the zero-cross detection circuit.

FIGS. 11A to 11 C are waveforms of a normal AC power supply.

FIGS. 12A to 12 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 10 .

FIG. 13 is a circuit diagram of another zero-cross detection circuit in the related art.

FIGS. 14A to 14 C are signal waveforms of components in the zero-cross detection circuit shown in FIG. 13 when Y-capacitors have a relatively small capacitance.

FIGS. 15A to 15 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 13 when the Y-capacitors have a relatively large capacitance.

FIGS. 16A to- 16 C are waveforms of an undesired commercial AC power supply which involves a third harmonic component.

FIGS. 17A to 17 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 13 when the commercial AC power supply on which the third harmonic is superposed exhibits an undesirable waveform.

FIGS. 18A to 18 C are waveforms of an undesired commercial AC power supply which has a 60° phase difference.

FIGS. 19A to 19 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 13 when the commercial AC power supply which has a 60° phase difference exhibits an undesirable waveform.

Embodiments of the present invention are described below with reference to the drawings.

First Embodiment

FIG. 1 is a circuit diagram of a power supply device including a zero-cross detection circuit according to a first embodiment of the present invention.

In FIG. 13, the same reference numerals are given to substantially the same components in FIG. 1 .

In FIG. 1, the power supply device includes a zero-cross detection circuit, a rectifying and smoothing circuit, and a switching regulator, as in the circuit configuration shown in FIG. 13 . The switching regulator of the self-excitation type is formed of components indicated by Q 21 , Q 22 , C 21 , C 22 , C 31 , C 32 , D 31 , IC 31 , R 21 to R 27 , R 31 to R 35 , and PC 21 . The zero-cross detection circuit is formed of components indicated by Q 41 , C 41 , C 42 , D 41 , R 41 to R 45 , and PC 41 . The switching regulator includes a transformer T 21 for separating and stepping down the DC output from the full-wave rectifying and smoothing circuit to output a desired DC voltage. Although the switching regulator in the power supply device shown in FIG. 1 is implemented as a self-excitation type flyback converter, the zero-cross detection circuit has the same configuration regardless of the type of the switching regulator.

The zero-cross detection circuit according to the present invention is different from that shown in FIG. 13 in that a resistor R 42 is connected between the line Line 2 and the low-voltage output terminal of the full-wave rectifying and smoothing circuit, i.e., the emitter of the transistor Q 41 .

When the potential of the line Line 2 is higher than the potential of the line Line 1 , the resistor R 42 allows a current to flow, and therefore allows a current flowing in the Y-capacitors (capacitors C 12 and C 13 ) to flow to the resistor R 42 . This hinders an unwanted current caused by the Y-capacitors from flowing to the resistor R 41 . Therefore, when the Y-capacitors have a large capacitance or when the commercial AC power supply exhibits an undesirable waveform, a zero-cross signal can be reliably generated.

The resistor R 42 is provided in a circuit portion which is an input to the zero-cross detection circuit from the line Line 2 . This allows an unwanted current caused by the Y-capacitors to bypass the zero-cross detection circuit, thereby reliably generating a zero-cross signal in the zero-cross detection circuit.

Preferably, the resistors R 41 and R 42 have substantially the same resistance in view of the following two points:

1. Desirably, the impedances with respect to the ground GND are a match between the line Line 1 and the line Line 2 because common-mode noise caused in the lines Line 1 and Line 2 , which is impulse noise, would be prevented from diverting into normal-mode noise due to a lack of impedance matching, thereby less possibly reducing the property of the lines Line 1 and Line 2 which is resistant to the common-mode noise; and

2. Noise radiation due to a lack of impedance matching between the lines Line 1 and Line 2 with respect to the output terminal of the full-wave rectifying and smoothing circuit would increase.

Reliable generation of a zero-cross signal in the zero-cross detection circuit is described with reference to FIGS. 2A to 7 C, taken in conjunction with an example.

FIGS. 2A to 2 C and 3 A to 3 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the Y-capacitors have a large capacitance.

In FIGS. 2A to 2 C and 3 A to 3 C, the x-axis represents time. FIG. 2A shows the potential of the line Line 1 with respect to a ground GND, FIG. 2B shows the potential of the line Line 2 with respect to the ground GND, and FIG. 2C shows the difference in potential between the lines Line 1 and Line 2 . FIG. 3A shows a current flowing in the resistor R 41 , FIG. 3B shows an enlarged version of the y-axis in FIG. 3A, and FIG. 3C shows the phototransistor collector potential in the secondary of the photocoupler PC 41 , that is, the zero-cross signal ZEROX.

FIGS. 4A to 4 C and 5 A to 5 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the third harmonic is superposed on the commercial AC power supply.

FIGS. 6A to 6 C and 7 A to 7 C are signal waveforms of the components in the zero-cross detection circuit shown in FIG. 1 when the commercial AC power supply has a 60° phase difference.

As is apparent from FIGS. 3B, 5 B, and 7 B, a current flowing in the resistor R 41 does not exhibit an undesirable waveform, thus allowing a correct zero-cross signal ZEROX to be generated, as shown in FIGS. 3C, 5 C, and 7 C.

Second Embodiment

FIG. 8 is a circuit diagram of a power supply device including a zero-cross detection circuit according to a second embodiment of the present invention. The second embodiment has substantially the same basic structure as the first embodiment, but includes a diode D 42 connected between the base and emitter of the transistor Q 41 in such a manner that the anode of the diode D 42 is connected to the emitter of the transistor Q 41 .

The diode D 42 prevents a reverse bias from being applied between the base and emitter of the transistor Q 41 if noise is present in the commercial AC power supply.

Third Embodiment

FIG. 9 is a circuit diagram of a power supply device including a zero-cross detection circuit according to a third embodiment of the present invention. The third embodiment has substantially the same basic structure as the first embodiment, but includes a diode D 43 connected in series with the resistor R 41 in such a manner that the anode of the diode D 43 is connected to the line Line 1 .

As in the second embodiment, the diode D 43 also prevents a reverse bias from being applied between the base and emitter of the transistor Q 41 if noise is caused in the commercial AC power supply.

In the circuit shown in FIG. 9, a diode which is the same as the diode D 43 may be further connected between the line Line 2 and the resistor R 42 in such a manner that the anode of the additional diode is connected to the line Line 2 , thus making the resistors R 41 and R 42 symmetric.

While the present invention has been described with reference to what are presently considered to be the preferred embodiments, it is to be understood that the invention is not limited to the disclosed embodiments. On the contrary, the invention is intended to cover various modifications and equivalent arrangements included within the spirit and scope of the appended claims. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.