Current-resonant switching power supply

Abstract: In a switching power supply, primary-side MOS transistors are alternately turned on, so that a resonant current flows into the primary winding of a transformer and an alternate power is transferred to the secondary side. The alternate voltage generated at the secondary winding is applied by the voltage generated at the wound-up secondary winding to the gates of secondary-side MOS transistors such that they are turned on respectively in periods when the polarity of the voltage is positive. Rectified currents flow into a capacitor through a choke coil to perform synchronous rectification. If the voltage of a smoothing capacitor becomes higher than the alternate output voltage when the transformer is inverted, reverse currents flow into the secondary-side MOS transistors. With the counterelectromotive force of the choke coil, the reverse currents flowing when the transformer is inverted are suppressed, and the efficiency of the switching power supply is prevented from decreasing.

Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a current-resonant switching power supply in accordance with the precharacterizing part of claim 1. A current-resonant switching power supply of that kind is known from Xiao Li et al.: "Soft switched PWM DC/DC converter with synchronous rectifiers", Intelec. International Telecommunications Energy Conference, US, New York, IEEE, Vol. Conf. 18, 1996, pages 476 - 484, XP000699870 ISBN: 0-7803-3508-2. 2. Description of the Related Art As the use of less energy has been required for earth environmental protection in recent years, higher efficiency and lower noise are further demanded for various types of switching power supplies. As power supply circuits for computers and communication units, DC-DC converters which have low noise and which maintain high efficiency even at a low-voltage output are required. When a low voltage is output, a high output current is generally obtained if a constant power consumption is maintained. In a DC-DC converter, a resistance loss at a rectifying diode in the secondary side becomes a large power loss. Therefore, it is considered that a current-resonant switching power supply having relatively low noise and high efficiency and a transistor which provides a low on-resistance at the secondary-side output are driven in a synchronous rectifying method to obtain a DC output voltage. Fig. 4 shows a switching power supply circuit having such a combination. Switching devices Q1 and Q2 are formed of MOS FETs connected in series, and an insulating transformer T transfers a switching power at the primary side to the secondary side. A power supply control circuit IC alternately opens and closes the switching devices Q1 and Q2, and is usually configured such that a reference voltage is compared with an output voltage V 0 by voltage detection means not shown to adjust the switching frequency of the switching devices in order to obtain a constant output voltage V 0 . The outputs of the switching devices Q1 and Q2 are sent to a primary winding L 1 of the insulating transformer T and a resonant capacitor C 1 . When the switching devices Q1 and Q2 are alternately opened and closed, the primary winding L 1 of the transformer is driven by a current that charges and discharges the resonant capacitor C 1 , which resonates with the leakage inductance of the transformer T. As shown in Fig. 5, a voltage V 1 applied to the primary winding L 1 causes an induced voltage V 2 at the secondary winding L 2 , and full-wave rectification is applied by one set of rectifying diodes in a usual DC-DC converter. Since a loss caused by the rectifying diodes, which have relatively high on-resistances, is rather large when an output voltage is low, there is known a circuit in which N-channel MOS transistors Q3 and Q4 are used instead of the rectifying diodes and full-wave rectification is applied in a synchronous method to output the DC voltage V 0 from a smoothing capacitor C 0 , as shown in Fig. 4. In the circuit shown in Fig. 4, since a full-wave-rectified voltage is accumulated in the smoothing capacitor C 0 through the MOS transistors Q3 and Q4 at a low resistance, a relatively low DC voltage V 0 can be efficiently output. Parasitic diodes D are formed due to the structures of the MOS transistors Q3 and Q4. A current-resonant switching power supply having switching devices half connected features essential low noise with zero-current switching at turning on and current resonance at turning off, and a wide variable output voltage V 0 at the secondary side with a switching frequency being changed. The power supply has in the entire period a rectified current continuous mode in which power is transferred to the secondary side and a secondary-side rectification discontinuous mode in which power is not sent to the secondary side in a period, in order to provide a wide regulation range. When the switching frequency becomes lower than the resonant frequency due to constant-voltage control, the mode is changed to the secondary-side rectification discontinuous mode. In this case, the rectifying capacitor at the secondary side is not charged for periods t1 in one switching cycle as shown in Fig. 5, and the output voltage V 0 is higher than the secondary voltage V 2 of the transformer in the periods t1. Since a reverse current is blocked by diodes even in such a discontinuous mode in a usual rectification with the diodes, there occurs no problem. In rectification with MOS FET transistors, however, since a reverse current flows, when the transistors are controlled such that they are turned on in the periods, negative-direction currents id1 and id2 flow into the synchronous-rectifying MOS transistors Q3 and Q4 in the periods t1 in the reverse direction, respectively, as shown in Fig. 5. With these currents id flowing in the negative direction, the MOS transistors Q3 and Q4 generate heat and a switching loss occurs at the primary side. To solve these problems, it has been considered that control circuits IC1 and IC2 each having a logic circuit for detecting the output voltage and the current of the transformer T to control the MOS transistors Q3 and Q4 are provided such that the MOS FET transistors Q3 and Q4 are turned on at appropriate timing. Since such control circuits IC1 and IC2 need to be prepared separately, however, the cost of a power supply increases and the circuit configuration is made complicated. When a charging period in which the capacitor C0 is charged becomes short, the peak value of the current accumulated in this period becomes large and a continuity angle becomes small to reduce the power factor of the switching power supply. Xiao et al.: "Soft switched PWM DC/CD converter with synchronous rectifiers" Intelec. International Telecommunications Energy Conference, US, New York, IEEE, Vol. Conf. 18, 1996, pages 476-484, XP000699870 ISBN: 0-7803-3508-2, mentioned above, discloses a current-resonant switching power supply in accordance with the pre-characterizing parts of claim 1. This known current-resonant switching power supply has a push-pull driving scheme for the pair of MOS-transistors connected to the secondary winding of the insulating transistors. As it is shown in Fig. 3 of this document, this converter circuit has also the drawbacks described above with reference to the prior art circuit shown in the present Fig. 4, namely that negative direction currents can flow into the synchronous rectifying MOS-transistors in periods where the rectifying capacitor at the secondary side is not charged in a switching cycle. DE 36 05 417 C1 discloses a rectifying circuit which has as a rectifying element a Schottky diode or a diode with a small forward voltage. Reverse voltage loss of this diode is minimized by a field effect transistor coupled in series to said diode and driven by an auxiliary winding on the storage inductivity of a transformer. DE 37 27 170 A discloses a DC-DC converter having an insulating transformer. In Fig. 2 of this document, a practically identical connection of the MOS transistors FT1 and FT2 is provided to extensions L4 and L6 of the secondary winding of the insulating transformer. Column 3, lines 24 to 44 of this document states that with such a connection the turn-on and turn-off instants of both MOS transistors can be precisely determined which implies that a reverse current conduction can be avoided. SUMMARY OF THE INVENTION Accordingly, it is an object of the present invention to provide a switching power supply having an improved efficiency. The above object is solved according to an essential aspect of the present invention by a current-resonant switching power supply which includes a driving circuit that alternately turns on and off switching devices half-bridge-connected against a DC voltage, and in which an alternate voltage is applied from the connection point of the switching devices to the primary side of an insulating transformer through a resonant capacitor and a predetermined alternate voltage is obtained from the secondary winding of the insulating transformer (T), said current-resonant switching power supply comprising: a pair of MOS transistors which are controlled at timing when they are alternately turned on at the secondary side of the insulating transformer, said insulating transformer having a third winding provided at the secondary side of said insulating transformer and insulated from said secondary winding, wherein a current rectified by the pair of MOS transistors charges a smoothing capacitor through a choke coil, characterized in that the pair of MOS transistors is driven by voltages sent from said third winding so that said MOS transistors are turned on according to the polarity of the voltage induced in said third winding against the ground. Since a full-wave-rectified current output from the synchronous-rectifying MOS transistors for charging the smoothing capacitor charges the smoothing capacitor through the choke coil, reverse currents flowing in the reverse direction through the MOS transistors can be prevented from flowing by the counteralectromotive force of the choke coil even in the discontinuous mode, in which the rectified currents are not continuous within one cycle. As described above, since a current-resonant switching power supply according to the present invention is used, especially when a half-bridge current-resonant switching power supply is used with synchronous-rectification rectifying devices, and the peak values of rectified currents are suppressed by an inserted inductor, the distribution angles of the rectified currents become large, and a power factor can be increased. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a circuit diagram of an example of a switching power supply circuit for explaining basic operating features of the present invention. Fig. 2 is a waveform view of a signal at each section shown in Fig. 1 during a switching operation. Fig. 3 is a circuit diagram of a switching power supply circuit according to an embodiment of the present invention. Fig. 4 is a general circuit diagram of a current-resonant switching power supply which employs a synchronous rectification method. Fig. 5 is a waveform view of reverse currents generated during synchronous rectification. DESCRIPTION OF THE PREFERRED EMBODIMENTS Fig. 1 shows an example of a current-resonant switching power supply circuit. As shown in Fig. 4, switching devices Q1 and Q2 constitute a half-bridge-connected switching circuit and are formed of MOS transistors, and a supply power source E is provided. The switching outputs thereof are connected to the ground terminal of the supply power source E through the primary winding L 1 of a drive transformer T and a resonant capacitor C 1 . A full-wave rectification circuit is formed such that the voltage induced at the secondary winding L 2 of the insulating transformer T charges a smoothing capacitor C 0 through synchronous-rectifying MOS transistors Q3 and Q4 and a choke coil Lc. This switching power supply is controlled by a winding-voltage detection method in which both ends of the secondary winding L 2 are wound up to drive the MOS transistors Q3 and Q4 and the MOS transistors Q3 and Q4 are turned on according to the polarity of the voltage induced in the secondary winding against the ground. A control IC circuit IC drives the switching devices Q1 and Q2. This IC circuit usually controls a switching frequency so as to maintain an output voltage V 0 at a constant voltage, and is allowed to have a protection function which detects an unusual temperature increase of the switching power supply to stop a switching operation. Resistors r1 and r2 provide gate capacitors with appropriate time constants to set the on timing of the transistors connected. An operation of the switching power supply will be briefly described below. When the supply power source E is applied, control is performed, for example, such that the MOS transistor Q1 is turned on and the MOS transistor Q2 is turned off. The resonant capacitor C 1 is charged through the supply power source E to the MOS transistor Q1 and the primary winding L 1 of the transformer. Control is next performed according to a resonant cycle at the primary side such that the MOS transistor Q1 is turned off and the MOS transistor Q2 is turned on. A resonant current flows from the resonant capacitor C1 to the primary winding L1 of the transformer, and an alternate power is transferred to the secondary side. The alternate voltage generated at the secondary winding L 2 is applied to the gates of the MOS transistors Q3 and Q4 by the voltage formed by the wound-up secondary winding, for example, while the voltage is positive so that the transistors are turned on, and rectified currents id3 and id4 flow into the capacitor C 0 through the choke coil Lc to perform full-wave rectification. A current can flow through parasitic diodes D of the MOS transistors Q3 and Q4 in a period in which the gate voltage of each transistor does not reach the threshold value. The diodes may be externally connected. If a load changes and the output voltage is changed, for example, the switching frequency is set lower than the resonant frequency by constant voltage control, and a reverse current is generated in the discontinuous rectification mode as shown in Fig. 5. As shown in switching waveforms of Fig. 2, the voltage V 2 induced in the secondary side against the voltage V 1 at the primary side has a waveform shown in Fig. 2, and a current I 1 at the primary side has a waveform in which the peak value is suppressed by the choke coil Lc. In discontinuous periods t 1 shown in Fig. 5, the charging current flowing through the smoothing capacitor at the secondary side disappears irrespective of the condition in which the switching devices in the primary side are not inverted. In these periods, since the MOS transistor Q3 is being driven to be on, the current makes an attempt to flow through the MOS transistor Q3 in the reverse direction. However, as shown in Fig. 2, the transformer is magnetically inverted at a point "a" and the current id4 starts flowing into the MOS transistor Q4. With the counterelectromotive force of the choke coil, the current id3 continues flowing into the MOS transistor Q3. When the current id3 becomes zero at a point "c," only the current id4 flows through the MOS transistor Q4. In other words, within the periods t2, the output voltage of the transformer is balanced with the counterelectromotive force generated by the inductor of the choke coil, and the current flows in the same direction. Therefore, the currents continuously flow into the MOS transistors Q3 and Q4 until they become zero, and the reverse currents caused by the transformer which has been inverted do not flow at the point "c," where a current becomes zero. At a point "b," the relationship between the MOS transistors Q3 and Q4 becomes reverse and the currents flow. The counterelectromotive force is generated in the choke coil Lc, the current id3 which has been flowing through the MOS transistor Q3 starts attenuating gradually, the transformer is driven in the direction in which the current id4 flows through the MOS transistor Q4, the current flowing through the choke coil Lc changes from the current id3 to the current id4 at the end of the discontinuous period t2, and thus a reverse current is not generated. As described above, when the inductance of the choke coil is set appropriately, since the power supply can be configured such that a reverse current does not flow in the present invention, the synchronous-rectifying MOS transistors can be driven in the winding-voltage detection method, which is the most simple method. In addition, since the inductor is inserted into a smoothing section, the distribution angles of the currents flowing through the synchronous-rectifying devices become large and their peak values are suppressed. Therefore, the power factor is improved. The losses caused by the semiconductor, the transformer, and the smoothing capacitor are greatly reduced. Fig. 3 shows an embodiment of the present invention. The functional principals explained above in relation to Figs. 1 and 2 are applied to this embodiment and the same symbols as those in Fig. 1 are assigned to the same portions. In the embodiment, to output voltages used for driving MOS transistors Q3 and Q4, an independent third winding L3 insulated from a secondary winding is provided. The third winding drives the synchronous-rectifying MOS transistors Q3 and Q4. The MOS transistors Q3 and Q4 are connected to the ground at the sources, and thereby gate driving is made easy.

Claims: A current-resonant switching power supply which includes a driving circuit that alternately turns on and off switching devices (Q1, Q2) half-bridge-connected against a DC voltage (E), and in which an alternate voltage is applied from the connection point of the switching devices (Q1, Q2) to the primary side (L 1 ) of an insulating transformer (T) through a resonant capacitor (C 1 ) and a predetermined alternate voltage is obtained from the secondary winding (L 2 ) of the insulating transformer (T), said current-resonant switching power supply comprising: a pair of MOS transistors (Q3, Q4) which are controlled at timing when they are alternately turned on at the secondary side of the insulating transformer (T). said insulating transformer (T) having a third winding (L 3 ) provided at the secondary side of said insulating transformer (T) and insulated from said secondary winding (L 2 ), wherein a current rectified by the pair of MOS transistors (Q3, Q4) charges a smoothing capacitor (C 0 ) through a choke coil (Lc), characterized in that the pair of MOS transistors (Q3, Q4) is driven by voltages sent from said third winding (L 3 ) so that said MOS transistors (Q3, Q4) are turned on according to the polarity of the voltage induced in said third winding (L 3 ) against the ground. The current-resonant switching power supply according to claim 1, wherein the pair of MOS transistors (Q3, Q4) is connected with their sources to ground. The current-resonant switching power supply according to one of the claims 1 and 2, wherein the switching devices (Q1, Q2) are formed of MOS transistors.

Inventors: IMAMURA NORITOSHI, KOBORI KATSUMI, IMAMURA, NORITOSHI, KOBORI, KATSUMI, Imamura, Noritoshi c/o Sony Corporation, Kobori, Katsumi c/o Sony Corporation
Applicants: SONY CORP, SONY CORPORATION
Application year: 1999
Main classification: H02M3
IPC codes: H02M3