The present invention relates to a switching power supply circuit capable of reducing switching loss of a switching element.
A boost-type switching power supply circuit has been known heretofore.
A parallel circuit including a diode Da and a capacitor Ca is connected to a drain and a source of the switching element Q1. The diode Da may be formed of a parasitic diode of the switching element Q1, and the capacitor Ca may be formed of a parasitic capacitor of the switching element Q1.
A series circuit including a rectifying diode D1 and a smoothing capacitor C1 is connected to a series circuit including the switching element Q1 and the current detection resistor R1. The control circuit 100 turns on and off the switching element Q1 based on a voltage from a criticality detection winding 1b of the reactor L1, a voltage from the smoothing capacitor C1, and a voltage from the current detection resistor R1, and thus makes control to output an output voltage Vo which is a constant voltage higher than an input voltage (voltage of the DC power supply Vin).
Next, operations of parts of the conventional boost-type switching power supply circuit will be described with reference to
In a period T4, once the switching element Q1 is turned off, a voltage Q1v between the drain and the source of the switching element Q1 increases, and the current L1i of the reactor L1 decreases. Next, in a period T5, a current D1i of the rectifying diode D1 and the current L1i of the reactor L1 gradually decrease while flowing in a path from the positive electrode to the negative electrode of the DC power supply Vin via the reactor L1, the rectifying diode D1 and the smoothing capacitor C1.
In periods T6 to T2, after excitation energy of the reactor L1 is released, voltage quasi resonance is generated by the reactor L1 and the capacitor Ca connected to the switching element Q1 in parallel. Accordingly, after the voltage Q1v of the switching element Q1 decreases to zero volts, the switching element Q1 is turned on, and thus zero-voltage switching (ZVS) can be achieved.
However, when a load is light, or when the input voltage (voltage of the DC power supply Vin) is high, as shown in a period T6 of
A conventional switching power supply circuit described in Japanese Patent Application Publication No. 2004-327152 includes, in addition to the configuration of the conventional switching power supply circuit shown in
This switching power supply circuit reduces switching loss in the turning-on and turning-off of the switching elements Q1, Q2, because the switching power supply circuit performs zero-voltage switching when turning on the switching elements Q1, Q2, and gradually raises the voltage when turning off the switching elements Q1, Q2.
However, the conventional switching power supply circuit described in Japanese Patent Application Publication No. 2004-327152 allows a voltage between a drain and a source of the switching element Q2 to become larger than the voltage of the smoothing capacitor C1, and, in some cases, to exceed a breakdown voltage of the switching element Q2, because the switching power supply circuit is provided with the resonance reactor L2 in parallel with the switching element Q2.
An object of the present invention is to provide a highly efficient switching power supply circuit by achieving a resonance operation in a wider input voltage range and load region by using a conventional reactor without provision of a resonance reactor.
The switching power supply circuit of the present invention includes: a first series circuit which is connected between one end and the other end of a DC power supply, and in which a reactor, a first diode, and a first capacitor are connected in series; a first switching element connected between the one end of the DC power supply and a connection point between the reactor and the first diode; a second series circuit which is connected to the first diode in parallel, and in which a second switching element and a second capacitor are connected in series; and a control circuit configured to control on and off of the second switching element in order that turn on of the first switching element becomes to zero-voltage switching.
A switching power supply circuit of an embodiment of the present invention will be described below in detail with reference to the drawings.
A parallel circuit including a diode Db and a capacitor Cb is connected between a drain and a source of the switching element Q2. A parasitic diode of the switching element Q2 may be substituted for the diode Db, and a parasitic capacitor of the switching element Q2 may be substituted for the capacitor Cb.
A control circuit 10 generates a gate signal Q1g based on a voltage from a criticality detection winding 1b of the reactor L1, a voltage from a smoothing capacitor C1, and a voltage from a current detection resistor R1. The control circuit 10 then outputs the gate signal Q1g to a gate of the switching element Q1 (first switching element), and thus turns on and off the switching element Q1.
The control circuit 10 generates a gate signal Q2g by inverting the gate signal Q1g used to turn on and off the switching element Q1. The control circuit 10 outputs the gate signal Q2g to a gate of the switching element Q2 (second switching element), and thus turns on and off the switching element Q2.
Next, descriptions will be given of operations of the parts of the switching power supply circuit of critical type of Example 1 with reference to
First, in a period T1 of
Next, in a period T2 of
Thereafter, in a period T3 of
Then, in a period T4 of
Next, after the capacitor Ca is charged, in a period T5 of
Thereafter, in a period T6 of
Then, in a period T7 of
Next, in a period T8 of
Thereafter, in a period T9 of
Then, in a period T10 of
Note that processes performed in the periods T1, T2 . . . are repeated after the period T10. In the period T2, the switching element Q1 is turned on as described above, and at this time, zero-voltage switching of the switching element Q1 is achieved.
The switching power supply circuit of Example 1 is capable of achieving the zero-voltage switching when the switching element Q1 is turned on, because: the additionally-provided series circuit (active clamp circuit) including the switching element Q2 and the capacitor C2 creates a time period for returning the energy from the load (the smoothing capacitor C1) side to the input (the DC power supply Vin) side, and thereby increases the energy which excites the reactor L1 to the input side, i.e., the circulating energy to flow to the input side; and thus the electric charges of the capacitor Ca are extracted by the circulating energy to thereby reduce the voltage of the switching element Q1 to zero volts.
Accordingly, the resonance operation can be achieved in a wider input voltage range and load region can be achieved using a conventional reactor without provision of a resonance reactor. Thus, a highly efficient switching power supply circuit can be provided.
Moreover, an on-period of the switching element Q1 becomes longer, and a time length in which the increased portion of the excitation energy is released through the rectifying diode D1 (off-period of the switching element Q1) also becomes longer. In other words, a switching frequency of the switching element Q1 decreases.
Next, a description is given of an operation of turning on and off the switching element Q2 in accordance with a load state (load amount).
The control circuit 10 includes an error amplifier 11, a comparator 13, an one-shot multivibrator 14, a flip-flop circuit 15, a comparator 16, a dead time generation circuit 17, an inverter 18, a driver 19, a comparator 20, and an AND circuit 21.
The comparator 13 compares a voltage of the criticality detection winding 1b inputted via a resistor R2 with a reference voltage Vref2. Upon receiving an L-level signal from the comparator 13, the one-shot multivibrator 14 outputs one pulse, as a set signal, to a set terminal of the flip-flop circuit 15.
The flip-flop circuit 15 is set in response to the set signal, and outputs an H-level signal from a Q output terminal. The flip-flop circuit 15 thus turns on the switching element Q1 via the dead time generation circuit 17, the driver 19, and a resistor R4. Once the switching element Q1 is turned on, a current flows in the path from the positive electrode to the negative electrode of the DC power supply Vin via the reactor L1, the switching element Q1 and the current detection resistor R1, as well as the reactor L1 is charged with energy. The current detection resistor R1 converts the current flowing through the switching element Q1 to a voltage, and outputs the converted voltage to a non-inverting input terminal of the comparator 16 via a resistor R3.
The error amplifier 11 amplifies an error voltage between a reference voltage Vref3 and a divided voltage obtained by dividing a voltage of the smoothing capacitor C1 between a resistor R53 and a resistor R54, as well as outputs this error voltage to the comparators 16, 20 and a capacitor C3.
The comparator 16 compares a current target value Vm outputted from the error amplifier 11 with a voltage to occur at the current detection resistor R1. Once the current Q1i of the switching element Q1 reaches the current target value Vm, the comparator 16 outputs an H-level reset signal to the flip-flop circuit 15. The flip-flop circuit 15 is reset in response to the reset signal from the comparator 16, and switches the H-level signal, which has been outputted from the Q output terminal, to an L-level signal. Thus, the switching element Q1 is turned off.
Once the switching element Q1 is turned off, the energy with which the reactor L1 is charged is released. Once this energy release is completed, the voltage of the criticality detection winding 1b is inverted. The comparator 13 compares the inverted voltage with the reference voltage Vref2, and outputs an L-level signal to the one-shot multivibrator 14. Because the one-shot multi-vibrator 14 outputs one pulse to the set terminal of the flip-flop circuit 15, the switching element Q1 is thus turned on again.
The switching element Q1 repeats the on and off operations described above, and a switching waveform Q1E shown in
Next, an operation of the switching element Q2 is described. The capacitor C3 is charged by the voltage obtained by dividing the voltage of the smoothing capacitor C1 between the resistor R53 and the resistor R54, i.e. a voltage corresponding to a state of a load (not illustrated) connected to the smoothing capacitor C1, which is outputted from the error amplifier 11.
While a voltage VG of the capacitor C3 is equal to or larger than a reference voltage Vref1 (from time t1 through time t2 in
On the other hand, while the voltage VG of the capacitor C3 is smaller than the reference voltage Vref1 (before time t1 and after time t2 in
Like the conventional switching power supply circuit, as described above, the switching power supply circuit of Example 1 is capable of operating the switching element Q1 in the zero-voltage switching operation by operating only the switching element Q1 without operating the switching element Q2 (an OFF state), when the load is a heavy load.
Moreover, the conventional switching power supply circuits deteriorates the efficiency since the conventional switching power supply circuit has an increases in the switching frequency and fails to perform the zero-voltage switching operation when the load is a light load. On the other hand, the switching power supply circuit of Example 1 is capable of enhancing the efficiency since, when the load is a light load, the switching power supply circuit of Example 1 operates the active clamp circuit including the switching element Q2 and the capacitor C2 to fully operate the switching elements Q1, Q2 in the zero-voltage switching operations and to make the switching frequency lower than the switching frequency of the conventional switching power supply circuit.
Furthermore, the switching power supply circuit described in Japanese Patent Application Publication No. 2004-327152 achieves the zero-voltage switching by making the current flow to the load side in the path starting and ending at the switching element Q1 via the resonance reactor, the rectifying diode D1, the smoothing capacitor C1 and the current detection resistor R1, when the switching element Q2 is turned off.
On the other hand, the switching power supply circuit of Example 1 regenerates an output into an input (DC power supply Vin), and makes a current flow to the input side in the path starting and ending at the reactor L1 after passing the DC power supply Vin, the current detection resistor R1 and the switching element Q1 when the switching element Q2 is turned off. Thus, the configuration and operation of the switching power supply circuit of Example 1 are completely different from those of Japanese Patent Application Publication No. 2004-327152.
Furthermore, the switching frequency cannot be decreased in the switching power supply circuit described in Japanese Patent Application Publication No. 2004-327152. On the other hand, the switching power supply circuit of Example 1 has an advantage that the switching frequency can be decreased.
The switching power supply circuit of Example 2 shown in
While the divided voltage VH is less than a reference voltage Vref1 (from time t1 through time t2 in
On the other hand, while the divided voltage VH is equal to or more than the reference voltage Vref 1 (before time t1 and after time t2 in
As described above, the switching power supply circuit of Example 2 is capable of enhancing the efficiency since, when the voltage of the DC power supply Vin is high, the switching power supply circuit of Example 2 operates the active clamp circuit including the switching element Q2 and the capacitor C2 to fully operate the switching elements Q1, Q2 in the zero-voltage switching operations and also to make the switching frequency lower than the switching frequency of the conventional switching power supply circuit.
The AC power supply Vac supplies an AC voltage to the rectifying circuit RC1. The rectifying circuit RC1 rectifies the AC voltage from the AC power supply Vac. The capacitor C4 constitutes a path of energy which excites a reactor L1 to an input side, i.e. circulating energy to flow to the input side.
The multiplier 12 multiplies a rectified voltage divided by the resistor R51 and the resistor R52 by a voltage from an error amplifier 11, and outputs the obtained voltage to a inverting input terminal of a comparator 16.
The switching power supply circuit of Example 3 is capable of enhancing the efficiency since the switching power supply circuit of Example 3 enhances the power factor, and operates in the same manner as does the switching power supply circuit of Example 1, as well as since, when the load is a light load, the switching power supply circuit of Example 3 operates the active clamp circuit including the switching element Q2 and the capacitor C2 to fully operate the switching elements Q1, Q2 in the zero-voltage switching operations, and also to make the switching frequency lower than the switching frequency of the conventional switching power supply circuit.
Compared to the control circuit 10a shown in
The multiplier 12 multiplies a rectified voltage divided by the resistor R51 and the resistor R52 by a voltage from an error amplifier 11, and outputs the obtained voltage to a inverting input terminal of a comparator 16.
The switching power supply circuit of Example 4 is capable of enhancing the efficiency since the switching power supply circuit of Example 4 enhances the power factor, and operates in the same manner as does the switching power supply circuit of Example 2, as well as since, when the AC voltage of the AC power supply Vac is high, the switching power supply circuit of Example 4 operates the active clamp circuit including the switching element Q2 and the capacitor C2 to fully operate the switching elements Q1, Q2 in the zero-voltage switching operations, and also to make the switching frequency lower than the switching frequency of the conventional switching power supply circuit.
Note that the present invention is not limited to the switching power supply circuits of Examples 1 to 4. For example, the control circuit 10 of the switching power supply circuit of Example 1 shown in
The present invention can achieve the zero-voltage switching when the first switching element is turned on, because: the additionally-provided second switching element and second capacitor creates a time period for returning the energy from the load side to the input side, and thereby increases the energy which excites the reactor to the input side, i.e., the circulating energy to flow to the input side; and thus, this energy reduces the voltage of the first switching element to zero volts.
Accordingly, the present invention can achieve the resonance operation in a wider input voltage range and load region by using a conventional reactor without provision of a resonance reactor. Thus, the present invention can provide a highly efficient switching power supply circuit.
The present invention is applicable to a DC-DC converter, a power factor correction circuit, and an AC-DC converter.
Number | Date | Country | Kind |
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2010-138282 | Jun 2010 | JP | national |