Electric power conversion systems – Current conversion – With means to introduce or eliminate frequency components
Reexamination Certificate
2000-05-16
2001-03-06
Han, Jessica (Department: 2838)
Electric power conversion systems
Current conversion
With means to introduce or eliminate frequency components
C363S017000, C363S126000
Reexamination Certificate
active
06198644
ABSTRACT:
TECHNICAL FIELD
This invention relates to a rectifying and smoothing circuit based on a current doubler rectification method, and a double-ended (bipolar) converter using the rectifying and smoothing circuit, such as a push-pull converter, a half-bridge converter, an asymmetric half-bridge converter, a full-bridge converter, and an active clamp converter.
BACKGROUND ART
Conventionally, as a power supply including a rectifying and smoothing circuit based on the current doubler rectification method of the above-mentioned kind, a power supply 
81
 shown in 
FIG. 17
 is known. This power supply 
81
 includes a switching transformer 
2
, and a current doubler rectifying and smoothing circuit 
82
. In this case, the current doubler rectifying and smoothing circuit 
82
 is comprised of a smoothing choke coil 
14
 connected between one end 
2
b
1
 of a secondary winding 
2
b 
of the transformer 
2
 and an output terminal 
16
b 
on a low-potential side, a smoothing choke coil 
15
 connected between the other end 
2
b
2
 of the secondary winding 
2
b 
and an output terminal 
16
b 
on a high-potential side and having the same inductance value as that of the choke coil 
14
, a diode 
11
 as a rectifying element, connected between the one end 
2
b
1
 of the secondary winding 
2
b 
and an output terminal 
16
a
, and a diode 
12
 as a rectifying element, connected between the other end 
2
b
2
 of the secondary winding 
2
b 
and the output terminal 
16
a
. The current doubler rectifying and smoothing circuit 
82
 outputs a DC voltage V0 generated by rectifying and smoothing a bipolar voltage induced between the opposite ends of the secondary winding 
2
b 
to a load 
4
.
In this power supply 
81
, push-pull FET circuits, not shown, connected to one end 
2
a
1
 of a primary winding 
2
a 
of the transformer 
2
 and the other end 
2
a
2
 thereof, respectively, are driven at 180 degrees out of phase with respect to each other, whereby as shown in 
FIG. 18
, a bipolar voltage VS having a voltage value±VS is induced between the opposite ends of the secondary winding 
2
b 
of the transformer 
2
. In this case, in a period T1 during which one of the FET circuits is controlled to an ON state at a duty ratio D of 25%, a high voltage is induced on the side of the one end 
2
b
1
 of the secondary winding 
2
b 
during the ON time period TON of the FET, and this induced voltage causes a current I
31
 shown in 
FIG. 17
 to flow through a current path of the one end 
2
b
1
 of the secondary winding 
2
b
, the diode 
11
, the load 
4
, the choke coil 
15
, and the other end 
2
b
2
 of the secondary winding 
2
b
. In this state, as shown in 
FIG. 18
, a voltage VL
15
 having a voltage value (VS−V0=(1−D)/D−V0/f, where f represents a frequency of the bipolar voltage VS) and directed as shown in 
FIG. 17
 is generated between opposite ends of the choke coil 
15
, whereby energy is accumulated in the choke coil 
15
.
Further, during an OFF time period TOFF of the period T1, the energy accumulated in the choke coil 
15
 causes a current I
32
 to flow in a direction shown in the same figure through a current path of one end of the choke coil 
15
, the diode 
12
, the load 
4
, and the other end of the choke coil 
15
. Consequently, the voltage VL
15
 between the opposite ends of the choke coil 
15
 is caused to have a voltage (−V0), and at the same time, as shown in 
FIG. 18
, a current IL
15
 varying within a range of a current variation width ((VS−V0)•TON/Lo=(1−D)•V0/f, where Lo represents an inductance value of the choke coils 
14
 and 
15
) flows through the choke coil 
15
.
Further, in the period T2 (the same time period as the period T1) during which the other FET is controlled to an ON state at a duty ratio D of 25%, a high voltage is induced on the side of the other end 
2
b
2
 of the secondary winding 
2
b 
during the ON time period TON of the FET, and this induced voltage causes a current I
33
 shown in 
FIG. 17
 to flow through a current path of the other end 
2
b
2
 of the secondary winding 
2
b
, the diode 
12
, the load 
4
, the choke coil 
14
, and the one end 
2
b
1
 of the secondary winding 
2
b
. In this state, as shown in 
FIG. 18
, between the opposite ends of the choke coil 
14
 is generated a voltage VL
14
 having a voltage value (VS−V0) and directed as shown in 
FIG. 17
, whereby energy is accumulated in the choke coil 
14
.
Further, during an OFF time period TOFF of the period T2, the energy accumulated in the choke coil 
14
 causes a current I
34
 to flow in a direction shown in 
FIG. 17 through a
 current path of one end of the choke coil 
14
, the diode 
11
, the load 
4
, and the other end of the choke coil 
14
. Consequently, the voltage VL
14
 between the opposite ends of the choke coil 
14
 become equal to a voltage value (−V0), and as shown in 
FIG. 18
, a current IL
14
 varying within a range of a current variation width ((VS−V0)•TON/Lo=(1−D)•V0/f) flows through the choke coil 
14
. In the above process of operation, each of average current values of the currents IL
15
 and IL
14
 becomes equal to one half of an output current I0, since a sum total of the current values of the currents becomes equal to the output current I0, shown in 
FIGS. 17 and 18
, and at the same time the current values thereof are equal to each other. It should be noted that as shown in 
FIGS. 17 and 18
, a ripple current IC flowing through the capacitor 
13
 varies within a range of a current variation width ((1−2D)•V0/f=(1−TON/(T−TON))•(VS−V0)•TON/Lo, where D represents a duty ratio, and f represents the reciprocal of the period T).
As described above, smoothing operations are carried out by the choke coils 
14
 and 
15
 during a time period of each of the periods T1 and T2, so that as shown in 
FIG. 18
, an output current Io from which a ripple component is substantially eliminated is output to the load 
4
.
DISCLOSURE OF THE INVENTION
The inventor studies the above prior art and found out the following problems:
Firstly, the conventional current doubler rectifying and smoothing circuit 
82
 uses the choke coils 
14
 and 
15
 constructed as separate component parts independent of each other. Therefore, the current doubler rectifying and smoothing circuit 
82
 has a large number of component parts and suffers from the problem of increased manufacturing costs caused by the mounting of component parts.
Secondly, a DC current having a predetermined current value constantly flows through the choke coils 
14
 and 
15
, as shown in 
FIG. 18
, respectively. In this case, as shown by the characteristics of the DC current with respect to the excitation inductance (LX) in 
FIG. 16
, there is a predetermined relationship between the excitation inductance (LX) of smoothing coils (choke coils 
14
 and 
15
 in the above current doubler rectifying and smoothing circuit 
82
) and a DC current allowed to pass through the smoothing coils. That is, to enhance the effect of the smoothing coils as smoothing filters, it is preferred that the smoothing coils have a large excitation inductance, whereas the value of a saturation DC current is reduced as the excitation inductance is increased. More specifically, when the effective volume of a smoothing choke coil as a magnetic material is small, if the excitation inductance is set to a small value (L
2
), as shown by a characteristic CH
1
, the smoothing choke coil can be used without magnetic saturation thereof until a current having a rather large current value (I
22
) flows therethrough, whereas if the excitation inductance is set to a large value (L
1
), there is a fear that the magnetic material undergoes magnetic saturation, since the limit value of a current below which the smoothing coil can be used without magnetic saturation thereof is lowered to a very small value (I
21
). Further, as shown by a characteristic CH
2
, when the effective volume of the coil as a magnetic material is made sufficiently large, if the excitation 
Greenblum & Bernstein P.L.C.
Han Jessica
Nagano Japan Radio Co. Ltd.
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