The disclosure relates to a DC/DC (Direct-Current to Direct-Current) converter including a single ended primary inductor converter (SEPIC).
A step-up/down converter is used as a method of generating a stable output voltage from an unstable input source, such as an automobile battery. Multiple power supplies are required to power sensors for safe operations of automobiles. CN109450252A (Patent Document 1) discloses, for example, a three-channel output DC/DC converter configured with a SEPIC circuit, as illustrated in
The two step-up/down output voltages, the positive output voltage +Vout, and the negative output voltage −Vout in
Vin·D=(VCo1+Vc1−Vin)·(1−D)
D/(1−D)=(VCo1+Vc1−Vin)/Vin EQ(1)
Since the charge and the discharge of the positive side reactor L1 are equal as well,
Vc1·D=VCo1·(1−D)
D/(1−D)=VCo1/Vc1 EQ(2)
From equations EQ(1) and EQ(2),
(Vout+Vc1−Vin)/Vin=VCo1/Vc1
Vc1·(Vout+Vc1−Vin)−VCo1·Vin=0
Vc1·(Vout+Vc1)−Vc1·Vin−VCo1·Vin=0
Vc1·(Vout+Vc1)−(Vc1+VCo1)·Vin=0
(Vc1−Vin)·(Vc1+VCo1)=0
∴Vc1=Vin
(However, Vc1=−VCo1 is not valid because of a breakdown of the diode D1.)
Therefore, the voltage of the decoupling capacitor C1 is Vin.
Also, from equation EQ(1),
Since Vc1=Vin,
VCo1=Vin−D/(1−D)
Similarly, on a side of the negative output voltage −Vout, since the charge and the discharge of the input side reactor Lin are equal in the steady state, the following relationship is established.
Vin·D=(Vc2−Vin)·(1−D)
D/(1−D)=(Vc2−Vin)/Vin EQ(3)
Since the charge and the discharge are equal for the negative output reactor L2 as well,
(Vc2−VCo2)·D=VCo2·(1−D)
D/(1−D)=VCo2/(Vc2−VCo2) EQ(4)
From equations EQ(3) and EQ(4),
(Vc2−Vin)/Vin=VCo2/(Vc2−VCo2)
(Vc2−Vin)·(Vc2−VCo2)=Vin·VCo2
Vc22−Vc2·VCo2−Vin·Vc2+Vin·VCo2−Vin·VCo2=0
Vc22−Vc2·VCo2−Vin·Vc2=0
Vc2(Vc2−VCo2−Vin)=0
Vc2=Vin+VCo2
The voltage of the decoupling capacitor C2 is the input voltage Vin+the negative output voltage VCo2.
Also, from equation EQ(3),
D/(1−D)=(Vc2−Vin)/Vin
Vin·D/(1−D)=Vc2−Vin
Vin·D/(1−D)+Vin=Vc2
(Vin·D+Vin−Vin·D)/(1−D)=Vc2
Vin/(1−D)=Vc2 EQ(5)
From equation EQ(4),
D/(1−D)=VCo2/(Vc2−VCo2)
D·(Vc2−VCo2)=VCo2(1−D)
D·Vc2−D·VCo2=VCo2−D·VCo2
D·Vc2=VCo2
Vc2=VCo2/D EQ(6)
From equations EQ(5) and EQ(6),
Vin/(1−D)=VCo2/D
VCo2=Vin·D/(1−D)
Therefore, the same voltage is output for the positive output voltage +Vout (=VCo1) and the negative output voltage −Vout (=VCo2).
However, in the SEPIC circuit illustrated in
The discharge path of the negative side reactor L2 is not only a discharge path g, which is the negative side reactor L2→the diode D2→the capacitor Co2→the negative side reactor L2, but also a discharge path i, which is the negative side reactor L2→the decoupling capacitor C2→the decoupling capacitor C1→the diode D1→the capacitor Co1→the capacitor Co2→the negative side reactor L2.
Therefore, a relationship equation of the following is established.
VCo1=Vc2−Vc1
VCo2=VCo1+VCo2+Vc1−Vc2
When capacitances of the decoupling capacitor C1 and the decoupling capacitor C2 are large enough for an output current, the voltage Vc1 of the decoupling capacitor C1 becomes the input voltage Vin and the voltage Vc2 of the decoupling capacitor C2 becomes Vin+VCo2; therefore, VCo1=Vin+VCo2−Vin=VCo2.
However, when the capacitances of the decoupling capacitor C1 and the decoupling capacitor C2 are increased, time for the voltage of the decoupling capacitor C1 being equal to the input voltage Vin and the voltage of the decoupling capacitor C2 being equal to Vin+VCo2 may be long or a transient response speed may be slow as initial voltages of the decoupling capacitor C1 and the decoupling capacitor C2 are zero volts before a power supply operation. Therefore, selecting a small capacitance may be preferable for the decoupling capacitor C1 and the decoupling capacitor C2.
However, when the capacitances of the decoupling capacitor C1 and the decoupling capacitor C2 are reduced, a ripple voltage ΔVc1 and a ripple voltage ΔVc2 of the decoupling capacitor C1 and the decoupling capacitor C2, respectively, become larger. As a result, the voltage of the decoupling capacitor C1 is Vin+ΔVc1, and the voltage of the decoupling capacitor C2 is Vin+VCo2+ΔVc2.
Therefore, when a load current of the decoupling capacitor C1 is high and the load current of the decoupling capacitor C2 is low, or vice versa, the ripple voltage ΔVc1 of the decoupling capacitor C1 and the ripple voltage ΔVc2 of the decoupling capacitor C2 are added to the one with the lower load current. Therefore, an issue occurs that cross regulation between the positive output voltage VCo1 and the negative output voltage VCo2 deteriorates.
In other words, as illustrated in a cross regulation characteristic diagram in
A DC/DC converter providing positive and negative output voltages according to one or more embodiment may include an input side reactor; a first coupling capacitor; a positive rectifier diode; a positive output side reactor; a first smoothing capacitor; a second coupling capacitor; a negative rectifier diode; a negative output side reactor; and a second smoothing capacitor. In one or more embodiments, a positive output of the DC/DC converter may be electrically connected via the input side reactor, the first coupling capacitor, and the positive rectifier diode. The first smoothing capacitor may be electrically connected between the positive output and a ground potential. The positive output side reactor may be electrically connected between a connecting point of the first coupling capacitor and the positive rectifier diode and the ground potential. A negative output of the DC/DC converter may be electrically connected to a connecting point of the first coupling capacitor, the positive rectifier diode, and the positive output side reactor via the second coupling capacitor and the negative output side reactor. The second smoothing capacitor may be electrically connected between the negative output and the ground potential. The negative rectifier diode may be connected between a connecting point of the second coupling capacitor and the negative output side reactor and the ground potential.
A DC/DC converter providing positive and negative output voltages according to one or more embodiments may include an input side reactor; a first coupling capacitor that is electrically connected in series with the input side reactor; a positive rectifier diode that is electrically connected in series with the first coupling capacitor and outputs a positive output voltage; a positive output side reactor that is electrically connected to a connecting point of the first coupling capacitor and the positive rectifier diode and a ground potential; a first smoothing capacitor that is electrically connected to the positive rectifier diode and a ground potential; a second coupling capacitor that is electrically connected in series with the first coupling capacitor; a negative rectifier diode that is electrically connected to the positive output side reactor and the second coupling capacitor and outputs a negative output voltage; a negative output side reactor that is electrically connected to a connecting point of the second coupling capacitor and the negative rectifier diode; and a second smoothing capacitor that is electrically connected to the negative rectifier diode, the ground potential, and the negative output side reactor.
A DC/DC converter according to one or more embodiments is described in detail with reference to drawings.
The DC/DC converter 1 outputs a positive output voltage +Vout, which is an output potential of the positive rectifier diode D1, and the first smoothing capacitor Co1. The DC/DC converter 1 outputs a negative output voltage −Vout, which is an output potential of the negative rectifier diode D2, and a second smoothing capacitor Co2. The PWM signal controller Cont1 generates an on/off drive signal of the switch Q1. The PWM signal controller Cont1 conducts a feedback control by calculating an error signal between a reference voltage Vref and the positive output voltage +Vout.
Compared to a DC/DC converter illustrated in
In the DC/DC converter illustrated in
Vin·D=(Vco1+Vc1−Vin)·(1−D)
D/(1−D)=(Vco1+Vc1−Vin)/Vin EQ(7)
Since the positive side reactor L1 is equal to the charge and the discharged as well,
Vc1·D=VCo1·(1−D)
D/(1−D)=VCo1/Vc1 EQ(8)
From equations EQ(7) and EQ(8),
(Vco1+Vc1−Vin)/Vin=VCo1/Vc1
Vc1·(Vco1+Vc1−Vin)−VCo1·Vin=0
Vc1·(Vco1+Vc1)−Vc1·Vin−VCo1·Vin=0
Vc1·(Vco1+Vc1)−(Vc1+VCo1)·Vin=0
(Vc1−Vin)·(Vc1+VCo1)=0
∴Vc1=Vin
(Vc1=−VCo1 is not valid because of the breakdown of the diode D1.)
Therefore, the voltage of the decoupling capacitor C1 is the input voltage Vin.
Also, from equation EQ(7),
From Vc1=Vin,
the positive output voltage +Vout may be expressed as
Vco1=Vin·D/(1−D)
Since the charge and the discharge of the input side reactor Lin are equal in the steady state on the negative output voltage −Vout side as well,
Vin·D=(Vc1+Vc2−Vin)·(D−1)
D/(D−1)=(Vc1+Vc2−Vin)/Vin EQ(9)
Since the charge and the discharge of the negative side reactor L2 are equal as well,
(Vc1+Vc2−VCo2)·D=VCo2·(D−1)
D/(D−1)=VCo2/(Vc1+Vc2−VCo2) EQ(10)
From equations EQ(9) and EQ(10),
(Vc1+Vc2−Vin)/Vin=VCo2/(Vc1+Vc2−VCo2)
(Vc1+Vc2−Vin)·(Vc1+Vc2−VCo2)=Vin·VCo2
Vc1+Vc2=Vin+VCo2
The voltages of the decoupling capacitor C1 and the decoupling capacitor C2 are expressed as (the input voltage+the output voltage). The voltage Vc1 of the decoupling capacitor C1 is found to be the input voltage and the voltage Vc2 of the decoupling capacitor C2 is VCo2 since the voltage Vc1=Vin from the SEPIC operation described above.
From equation EQ(7),
D/(1−D)=(Vc1+Vc2−Vin)/Vin
Vin·D/(1−D)=Vc1−Vc1+Vin
Vin·D/(1−D)+Vin=Vc1+Vc2
(Vin·D+Vin−Vin·D)/(1−D)=Vc2
Vin/(1−D)=Vc2 EQ(11)
From equation EQ(8),
D/(1−D)=Vco2/(Vc1+Vc2−VCo2)
D(Vc1+Vc2−Vco2)=Vco2(1−D)
D·Vc1+D·Vc2−D·Vco2=VCo2−D·Vco2
D·Vc1+D·Vc2=Vco2
Vc1+Vc2=VCo2/D EQ(12)
From equations EQ(11) and EQ(12),
Vin/(1−D)=VCo2/D
VCo2=Vin·D/(1−D)
VCo1 and VCo2 output the same voltage.
Therefore, the same voltage is output for the positive output voltage +Vout (=VCo1) and the negative output voltage −Vout (=VCo2).
The discharge path of the negative side reactor L2 is not only a discharge path g, which is the negative side reactor L2→the diode D2→the capacitor Co2→the negative side reactor L2, but also a discharge path i, which is the negative side reactor L2→the decoupling capacitor C2→the diode D1→the capacitor Co1→the capacitor Co2→the negative side reactor L2.
The DC/DC converter illustrated in
Hence,
VCo1=Vc2
VCo2=VCo1+VCo2−Vc2
When the capacitance of the decoupling capacitor C2 is large enough for the output current, the voltage Vc2 of the decoupling capacitor C2 becomes VCo2; therefore,
VCo1=VCo2=Vc2
Therefore, by making the capacitance of the decoupling capacitor C1 small and the decoupling capacitor C2 large, the cross regulation is improved. In other words, since the capacitance of the decoupling capacitor is only C1, there is an advantage that improvements in start-up time and load response may be achieved simultaneously.
The DC/DC converter according to one or more embodiments may provide a multi-output SEPIC circuit with good cross regulation accuracy regardless of the cross load current.
In the related arts, as shown in the cross regulation characteristic diagrams in
Although one or more embodiments are described above, the above-mentioned embodiments are examples to embody the technical concept, and individual configurations, combinations, etc. are not specific to those described above. A various change may be made to one or more embodiments described to the extent that the gist is not departed from.
For example, as illustrated in
As described above, the DC/DC converter according to one or more embodiments is suitable for obtaining the multi-output of positive and negative poles. Thus, the DC/DC converter may be used as a power supply for an in-car device, etc.
This application claims priority based on 35 USC 119 from prior International Patent Application No. PCT/JP2021/019537 filed on May 24, 2021, the entire contents of which are incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2021/019537 | May 2021 | US |
Child | 18505298 | US |