The present application is the U.S. National Phase of PCT/EP2017/071770, filed on Aug. 30, 2017, which claims priority to German Patent Application No. 10 2016 217 040.6, filed on Sep. 7, 2016, the entire contents of which are incorporated herein by reference.
The invention relates to DC-DC converters. More specifically, the invention is directed to a charge pump for high power applications, in particular, including inductive elements combined with capacitors which allow zero current switching processes and consequently a minimization of the losses.
Efficient and lightweight DC to DC voltage conversion is required in a widespread range of applications which involve the most disparate power levels from small supplies with output powers in the mW order to large MW plants.
To obtain an efficient DC to DC conversion there are several possible topologies. However, the basic principle behind DC-DC conversion is always the same. Any topology presents an input DC link, an output DC link, and one (or more) storage element. In a first step, some energy is transferred from the input DC Link to the storage element. In a second step, energy is transferred from the storage element to the output DC link. The sequence is then repeated.
The quasi-totality of high power converters employs inductive elements as storage elements. In very low power applications it is also common to employ capacitors as storage elements, often with circuits known as charge pumps.
For high power applications, charge pumps (e.g., capacitors as storage elements) are practically never used.
Charge pumps allow extremely poor control possibilities concerning the current flow and/or the output voltage. However, the utilization of capacitors as storage elements involves significant benefits in terms of costs, weight, and manufacturing process.
A specific type of DC to DC power converter and a method of conversion is disclosed in U.S. Pat. No. 6,429,632 B1, provided using high-frequency switched capacitors where the switches are implemented by CMOS transistors or diodes on an integrated-circuit chip and using inductors to limit charging current. High efficiency is achieved using inductors to reduce energy losses in circuit capacitors by high frequency switching when inductor current is zero and capacitor voltage is maximized. The high-frequency (100 MHz or greater) operation of the converter circuit permits the use of inductors with a low inductance value on the order of 100 nH (100×10−9 Henrys) capable of fabrication directly on an integrated-circuit (IC) chip. The use of CMOS integrated components allows the entire converter to be formed on a single IC chip, saving significant space within the portable system. Output voltage and current is high enough to permit EEPROM programming. In addition, fluctuations in the output voltage (ripple voltage) are substantially eliminated when several of the converter circuits are used in parallel. While this type of converter is adapted for the use inside integrated circuits and operating with high currents, it is not suitable for high voltages and high power applications as for instance in hybrid or electric vehicles.
The object of the present invention is a charge pump topology suited for high power applications which does not require an accurate output voltage control.
This object is achieved by the features of independent claim 1. Further embodiments and advantageous variants of the inventive concept are given in the dependent claims, the following specification, and the accompanying drawings.
Compared to classical and widespread charge pump topologies (designed for low power applications) the design proposed herein includes inductive elements which allow a zero current switch and a resonant operation of the converter, with the special resonant waveform generated with only one coil and one capacitor. In addition, the necessary winding goods can be reduced considerably, thereby making the new converter design more cost-effective and more lightweight.
The working frequency is typically below 500 kHz, preferably spans the range from about 20 kHz to about 200 kHz. The rated input voltage is typically in the range of about 400 V and can be boosted up to 800 V, allowing for instance to charge 800 V batteries at 400 V stations or allowing the supply of 400 V systems by such 800 V batteries. Typical power values are between 20 kW up to 200 kW, but can even be lower or higher.
The list of reference numerals is part of the disclosure. The drawing figures are described in correlation and jointly. The same reference numerals are used for the same parts. Reference numerals with different indices are used for functionally identical or similar parts.
Again, after a short “dead time” the charging switch 9 is turned on and the whole process is repeated. Each of the described switching processes can be considered as zero current transitions, and therefore the switching losses of the described system are very low. The switches are all activated and deactivated, respectively, for about 50% of the duty cycle.
For a correct operation, it is important that the resonance frequency between the components 3 and 2 is equal to or larger than the switching frequency. Nevertheless, to minimize the dead time, and thus reduce the peak current in the components, the switching frequency should possibly equal the resonance frequency.
In addition, to avoid oscillations on the output voltage, the DC-link capacitors 4 and 5 must be significantly larger than the storage capacitor 2.
The whole process described above can be summarized as follows: In a first step, energy is transferred from the bottom DC link capacitor 4 (which is connected to the input DC-Link) to the storage capacitor 2. In a second step, energy is transmitted to the top DC-link capacitor 5.
An embodiment which allows to halve the input voltage is shown in
The combination of the two principles described above results in a bidirectional embodiment which is shown in
With a bidirectional configuration it is also possible to implement the so-called active rectification, e.g., activate the switch parallel to the conducting diode to reduce losses. However, it is very important that the switch is turned off before the end of the half period oscillation. If the switch is not deactivated, the diode cannot stop the oscillation after a half of the period and the operation of the circuit is significantly degraded.
Alternatively to charging resistors, it is also possible to place highly resistive switches 16 parallel to one or more of the main switches. In this way, during the first switching events only the highly resistive paths are activated, thus avoiding high currents to charge the capacitors 2, 4, and 5. Once the capacitors are charged, the system can operate normally and the main switches 8, 9, 14, and 15 can be activated.
Another option to avoid inrush currents is to operate one or more of the main switches 8, 9, 14, and 15 with very short on pulses until the capacitances of the system 4, 5, and 2 are charged.
With a bidirectional topology, as for example the one shown in
A two-step “cascading” charge pump embodiment is disclosed in
A fractional voltage ratio can also be obtained with a single step. An embodiment which boosts the voltage by a factor 1.5 is shown in
The serially connected circuit 20, which is in
It is important to notice that the embodiment of
Another fractional voltage ratio can be obtained with the embodiment shown in
The serially connected circuit 20, which is in
As shown in
To obtain a lower voltage ripple on the DC-link capacitors, it is convenient to design circuits composed of two or more charge pumps (phases) which operate preferably at the same frequency. To minimize the voltage ripple, it is wiser to set the phase delay at 360°/n where n is the number of the operating phases.
The circuit in a preferred embodiment relies on the principle of balancing the top and bottom capacitors 4 and 5 and alternating buck and boost operation, and comprises two DC link capacitors 4 and 5, the sum voltage of both capacitors being the sum of both capacitor voltages. The top and the bottom capacitors 4 and 5 have about the same voltage. During the boost mode, the top capacitor 5 is lightly charged and the bottom capacitor 4 is lightly discharged, while in buck mode, the top capacitor 5 is lightly discharged and the bottom capacitor 4 is lightly charged. By alternating the two modes of operation, the equality of both capacitor voltages can be assured.
According to a further preferred embodiment, two or more DC capacitors can be switched on each other in the DC link.
Number | Date | Country | Kind |
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10 2016 217 040 | Sep 2016 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2017/071770 | 8/30/2017 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2018/046370 | 3/15/2018 | WO | A |
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International Search Report and Written Opinion issued in International Application No. PCT/EP2017/071770 dated Nov. 27, 2017. |
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