1. Technical Field
The present invention relates to a step-down DC-to-DC converter.
2. Related Art
Patent Document 1: Japanese Patent No. 4784155
Because a switching device having high breakdown voltage has problems that both a size of the device and a conduction loss are large, the step-down DC-to-DC converter in the related art as described above has problems that a size of the step-down DC-to-DC converter is increased and efficiency is deteriorated.
In addition, because a switching loss increases when a switching speed is slowed down, a switching period cannot be shortened. Hence, there arises a need for a large reactor and such a need raises a problem that a size of the DC-to-DC converter is increased.
The invention has an object to make a switching device having low breakdown voltage feasible and shorten a switching period in a step-down DC-to-DC converter by lowering a voltage applied to the switching device when the switching device switches OFF from ON or ON from OFF.
A step-down DC-to-DC converter according to a first aspect of the invention includes: a switching device and a free wheel semiconductor device sequentially connected in series to an input power supply; a reactor connected sequentially in series between a connecting point of the switching device and the free wheel semiconductor device and a ground point; an output smoothing capacitor; a drive circuit controlling the switching device to switch ON and OFF; an inductor inserted in series between the input power supply and the switching device; and an input smoothing capacitor provided between a connecting point of the inductor and the switching device and a ground point. Herein, let L be an inductance value of the inductor, C be an electrostatic capacity of the input smoothing capacitor, and T1 be a time since the switching device is switched from an OFF state to an ON state until the switching device is switched to an OFF state again according to an output signal from the drive circuit, then T1 is set so as to satisfy
0<T1<π√{square root over (L×C)}
Also, a step-down DC-to-DC converter according to a second aspect of the invention includes: a switching device and a free wheel semiconductor device sequentially connected in series to an input power supply; a reactor connected sequentially in series between a connecting point of the switching device and the free wheel semiconductor device and a ground point; an output smoothing capacitor; a drive circuit controlling the switching device to switch ON and OFF; an inductor inserted in series between the input power supply and the switching device; and an input smoothing capacitor provided between a connecting point of the inductor and the switching device and a ground point. Herein, let L be an inductance value of the inductor, C be an electrostatic capacity of the input smoothing capacitor, and T2 be a time since the switching device is switched from an ON state to an OFF state until the switching device is switched to an ON state again according to an output signal from the drive circuit, then T2 is set so as to satisfy
0<T2<π√{square root over (L×C)}
By setting the ON time T1 of the switching device shorter than half the resonance period of the inductor and the input smoothing capacitor provided between the input power supply and the switching device, the step-down DC-to-DC converter can not only lower a voltage across the switching device but also shorten the switching period.
The foregoing and other objects features, aspects, and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken conjunction with the accompanying drawings.
First Embodiment
The reactor L2, the input smoothing capacitor C2, the switching device Q1, and the free wheel diode D1 together form a step-down converter portion whereas the reactor L1 and the output smoothing capacitor C1 together form a step-down output portion.
By allowing the drive circuit DR to output a drive signal to the switching device Q1 so that an ON state of a predetermined time T1 and an OFF state of a predetermined time T2 are repeated alternately, an input voltage is stepped down to a predetermined output voltage and supplied to a load L connected in parallel with the output smoothing capacitor C1.
Herein, let L2 be an inductance value of the inductor L2 and C2 be an electrostatic capacity value of the input smoothing capacitor C2. Then, the predetermined time T1 is set so as to satisfy
0<T1<π√{square root over (L2×C2)}
During an OFF period of the switching device Q1, a current supplied from an input side via the inductor L2 is charged to the input smoothing capacitor C2. Hence, a positive terminal voltage of the switching device Q1 rises. In the meantime, a current flows into the reactor L1 via the free wheel diode D1. Hence, a negative terminal voltage of the switching device Q1 is about 0 V (only a voltage drop across the diode with respect to ground potential).
During an ON period of the switching device Q1, a current flows into the reactor L1 via the switching device Q1. Hence, the input smoothing capacitor C2 is discharged and the positive terminal voltage of the switching device Q1 drops. On the other hand, the negative terminal voltage of the switching device Q1 drops to about 0 V with respect to the positive terminal voltage (only a voltage drop caused by an ON resistance).
When the switching device Q1 again switches OFF from ON, a voltage Vt1, which is a voltage across the input smoothing capacitor C2 superimposed with a surge voltage Vsg generated by parasitic inductance, is applied to the positive terminal of the switching device Q1.
As is shown in the drawing, Vt1 drops to a lowest voltage when T1 substantially coincides with
π√{square root over (L2×C2)}
Thereafter, Vt1 repeats pulsation.
On the other hand, because the switching period T is a sum of T1 and T2, given a same step-down ratio, T2 and T1 have a proportional relation. Hence, the switching period T is proportional to T1.
In other words, by making the ON time T1 of the switching device Q1 shorter than half the resonance period of the inductor L2 and the input smoothing capacitor C2, not only can Vt1 be lowered, but also the switching period T can be shortened.
More specifically, because it becomes possible to use a switching device having low breakdown voltage, the switching device can be smaller in size and the switching period can be shorter. Accordingly, the inductance value L1 of the reactor L1 can be smaller, which can in turn reduce the reactor L1 in size. Further, because the DC-to-DC converter can be reduced in size, a degree of freedom in layout can be enhanced for use in circumstances where an attachment space is limited, for example, in-vehicle use.
In particular, Vt1 can be lowered to the minimum extent possible when T1 substantially coincides with
π√{square root over (L2×C2)}
For example,
π√{square root over (L2×C2)}
In comparison with the configuration in the related art, Vt1 becomes smaller.
In the first embodiment, a MOSFET is shown as the switching device Q1. It should be appreciated, however, that other switching devices, for example, an IGBT and a bipolar transistor, are also available.
Also, a diode is used as the free wheel element. It should be appreciated, however, that other semiconductor devices, such as a MOSFET, are also available.
Second Embodiment
By allowing the drive circuit DR to output a drive signal to the switching device Q1 so that an ON state of a predetermined time T1 and an OFF state of a predetermined time T2 are repeated alternately, an input voltage is stepped down to a predetermined output voltage.
Herein, let L2 be an inductance value of the inductor L2 and C2 be an electrostatic capacity value of the input smoothing capacitor C2. Then, T2 is set so as to satisfy
0<T2<π√{square root over (L2×C2)}
When the switching device Q1 switches OFF from ON, a current supplied from the input side via the inductor L2 is charged to the input smoothing capacitor C2. Hence, a positive terminal voltage of the switching device Q1 rises. In the meantime, because a current flows into the reactor L1 via the free wheel diode D1, a negative terminal voltage of the switching device Q1 is about 0 V (only a voltage drop across the diode with respect to ground potential).
Herein, when the switching device Q1 switches ON from OFF, a voltage across the input smoothing capacitor C2, that is, the positive terminal voltage of the switching device Q1, rises to Vt2, which is lower than a peak voltage Vpk generated by resonance of the inductor L1 and the input smoothing capacitor C2. Hence, it becomes possible to use a low voltage switching device.
For example,
π√{square root over (L2×C2)}
That is, Vt2 can be lower than Vpk when the switching device Q1 is operated in a range within which T2 satisfies
0<T2<π√{square root over (L2×C2)}
Third Embodiment
By allowing the drive circuit DR to output a drive signal to the switching device Q1 so that an ON state of a predetermined time T1 and an OFF state of a predetermined time T2 are repeated alternately, an input voltage is stepped down to a predetermined output voltage.
Herein, let L2 be an inductance value of the inductor L2 and C2 be an electrostatic capacity value of the input smoothing capacitor C2. Then, T1 and T2 are set so as to satisfy
0<T1<π√{square root over (L2×C2)}
0<T2<π√{square root over (L2×C2)}
When the switching device Q1 is switched OFF from ON to stop driving of the step-down DC-to-DC converter, a current supplied from the input end via the inductor L2 is charged to the input smoothing capacitor C2. Accordingly, a positive terminal voltage of the switching device Q1 rises above a positive terminal voltage Vt2 of the switching device Q1 during a driving OFF time T2.
Herein, by setting an operating voltage Vz of the zener diode Z1 for surge absorption at or above Vt2 and at or below a peak voltage Vpk generated by resonance of the inductor L2 and the input smoothing capacitor C2, it becomes possible to use a switching device having low breakdown voltage.
The zener diode Z1 for surge absorption does not operate while the step-down DC-to-DC converter is driven and therefore the zener diode Z1 for surge absorption operates only on one pulse when the step-down DC-to-DC converter is at rest. Hence, not only does it become possible to select a zener diode having a relatively small capacity, but it also becomes possible to avoid deterioration of efficiency during normal driving.
A zener diode is used as the surge absorbing element. It should be appreciated, however, that other surge absorbing elements, for example a varistor, are also available.
Various modifications and alterations of this invention will be apparent to those skilled in the art without departing from the scope and spirit of this invention, and it should be understood that this is not limited to the illustrative embodiments set forth herein.
Number | Date | Country | Kind |
---|---|---|---|
2012-032341 | Feb 2012 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
4916380 | Burroughs | Apr 1990 | A |
6259237 | Fischer | Jul 2001 | B1 |
20030141857 | Nishida et al. | Jul 2003 | A1 |
20070018618 | Endo | Jan 2007 | A1 |
20110156495 | Saligram et al. | Jun 2011 | A1 |
20110241641 | Chen et al. | Oct 2011 | A1 |
Number | Date | Country |
---|---|---|
199 13 464 | Sep 2000 | DE |
H06 292357 | Oct 1994 | JP |
H06 2922357 | Oct 1994 | JP |
2005 295753 | Oct 2005 | JP |
2009 183093 | Aug 2009 | JP |
2011 004557 | Jan 2011 | JP |
4784155 | Oct 2011 | JP |
Entry |
---|
Japanese Office Action issued Aug. 20, 2013, Patent Application No. 2012-032341. |
German Office Action, issued Feb. 20, 2014, Patent Application No. 10 2012 211 829.2. |
Number | Date | Country | |
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20130214758 A1 | Aug 2013 | US |