WO1991009455A1

WO1991009455A1 - Dc/dc-converter

Info

Publication number: WO1991009455A1
Application number: PCT/DK1990/000331
Authority: WO
Inventors: Ole Steen Seiersen
Original assignee: Ole Steen Seiersen
Priority date: 1989-12-19
Filing date: 1990-12-18
Publication date: 1991-06-27
Also published as: DK646589D0; DE69023250T2; US5317496A; EP0571372B1; DE69023250D1; DK646589A; ATE129601T1; EP0571372A1; AU7048591A

Abstract

A voltage converter which has a primary circuit and which, with an input voltage, is connected through at least one primary winding to respective secondary windings of at least one secondary circuit. The primary circuit and each of the secondary circuits are tuned individually so that each of them comprises an oscillatory circuit with coinciding resonance frequencies.

Description

DC/DC converter

The invention concerns a voltage converter comprising a transformer through which a primary circuit is connected to at least one secondary circuit, wherein a voltage applied to the input of the primary circuit is converted to output voltages on respective secondary circuits.

A. H. einberg and L. Ghislanzoni: "A new Zero Voltage and Zero Current Power Switching Technique." PESC 89 provides a DC voltage converter with a constant ratio of conver¬ sion. The converter uses a transformer through which a primary circuit is coupled to one or more secondary cir- cuits. The primary circuit has two electrical switches which periodically reverse the voltage across the primary windings wound around the core of the transformer. When the first switch is switched off, double voltage will be present across the second switch. The parallel inductance of the transformer now forms a resonance circuit with the parasitic capacities across the switches. The magnetizing current in the transformer resonantly recharges these ca¬ pacities so that there will be no voltage across the se¬ cond switch after a period of time. The second switch can then be switched on without instantaneous great voltage changes and with a greatly reduced loss. When the second switch is switched off again, a corresponding process takes place. This art is also described in the European Patent Specification EP 0 077 958.

When one of the switches is switched on, a series reso¬ nance circuit will be formed, consisting of an inductance in series with the transformer (the inductance may e.g. consist of the parasitic series inductance of the trans- former) as well as a capacity on either the primary side or on each of the outputs on the secondary side, and reso- nant energy transfer takes place from the primary side to the secondary side. When the current in the resonance cir¬ cuit is zero, the on-switch can be switched off without instantaneous great current changes and with a greatly re- duced loss.

The prior art operates satisfactorily as long as the loads on the respective secondary circuits are of the same order and are fairly constant. When the load distribution is very skew, e.g. a 90% load on one tap and a 10% load on another tap, the output voltage drops in relation to the nominal value on the tap most loaded. Correspondingly, the voltage rises with respect to the nominal value on the tap least loaded. These deviations from the nominal voltage values (cross-regulation) entail that the voltage conver¬ ters of the prior art are not useful where precise feed voltages are required, and where extreme load distribu¬ tions may occur.

Further, it is necessary that the employed transformer is optimized with respect to the parasitic series inductance such that in case of capacitive tuning on the primary side the parasitic series inductance on the secondary side must be insignificant and reverse. If this requirement is not satisfied, the tuning frequency varies with the load dis¬ tribution, and the switches can no longer be expected to be switched off with low losses. It may be difficult to fully satisfy this requirement in practice, and even par¬ tial satisfaction of the requirement may be inconsistent with the requirement of low power losses in the trans¬ former.

The object of the invention is to provide a voltage con¬ verter which is optimized with respect to cross-regula- tion, and which has a constant tuning frequency irrespec¬ tive of the load distribution. As stated in the characterizing portion of claim 1, these optimum conditions may be realized with a simple tuning technique where both the primary side and each of the out¬ put circuits on the secondary side are individually tuned to form oscillatory circuits with like resonance fre¬ quency.

As stated in the characterizing portion of claim 3, the voltage converter may moreover comprise a switching cir- cuit adapted to reverse the current in one or more primary windings with a constant switching frequency. The reso¬ nance frequency of the respective oscillatory circuits may advantageously be of the same order as the switching fre¬ quency. The voltage converter of the invention has a plu- rality of advantages, and there will e.g. not be any interaction (cross-regulation) between the outputs on the secondary side. The tuning frequency will be independent upon the load distribution and will continue to be con¬ stant even if the load distribution is changed.. The power transformer may be optimized exclusively with a view to minimizing losses and without having regard to either pri¬ mary or secondary tuning.

Furthermore, the limits with respect to the physical cir- cuit layout may be eliminated since almost any practically occurring circuit inductance, e.g. connection to and through rectifier diodes and tuning capacities can be com¬ bined in a distributed circuit tuning, without this having a negative impact on the performance of the converter.

An explanation of the above-mentioned effects can be found in the equivalent diagram shown in fig. 4 of the periods in which one contact is made. All the secondary sides are converted to the primary side. The primary side of the converter and each of the secondary sides are equated with a series connection consisting of a coil and a current generator connected in parallel with a capacity. All these series connections are connected to earth and to a common node V . The coils will typically be identical with the parasitic series inductances of the transformer. This equivalent diagram can be applied to both the prior art and to the invention. In the prior art with primary tun¬ ing, the capacities on the secondary side, however, will

* be very great. The voltage in the node V will then depend upon the load on the individual outputs, and considerable cross-regulation will be observed. Furthermore, the effec¬ tive tuning inductance and thereby the tuning frequency depend upon the load distribution.

On the other hand, if the primary side and each of the output circuits on the secondary side are tuned individu¬ ally to the same resonance frequency, a current will run on the primary side at this frequency, said current being distributed to each of the secondary circuits. Since each individual branch is tuned to this frequency, the voltage drop across the coil in a branch is just as great as, but oppositely directed, the voltage drop across the capacity

* in the same branch. The common node V will hereby have the same voltage as earth irrespective of the load distri¬ bution, and there is no longer any interaction between the individual outputs.

The invention will be explained more fully below in con¬ nection with preferred embodiments and with reference to the drawing, in which

fig. 1 shows a preferred embodiment of a voltage converter according to the invention,

fig. 2 shows an alternative embodiment of a voltage con- verter according to the invention, fig. 3 shows two voltage signals applied to the control electrodes on the transistors T.. and T,. shown in figs. 1 and 2, and

fig. 4 is an equivalent diagram for the circuit shown in fig. 1.

Fig. 1 shows a preferred embodiment of a DC voltage con¬ verter according to the invention. The converter is based on a transformer coupling TRA, through which a primary side is coupled to one or more output circuits on the se¬ condary side.

An input terminal V. , is connected to earth through a capacitor C, and is connected through a coil .. to a node

V . The node V is moreover connected to earth through a

P P ^a capacitor C«. The node V is the center of two transformer windings N. , N„ of the same size, where current through these windings N, and N~ generates a flux in the trans- former core, the direction of the flux being dependent upon which of the windings N-, N₂ is conducting. A drive circuit 10 generates two identical, but time-delayed sig¬ nals V..(t) and V₂(t), which are shown in fig. 3. The sig¬ nals V_η (t) and V~(t) are passed to respective control electrodes on FET transistors T.. and T„, which will be conducting with a positive voltage on the control elec¬ trode, i.e. while the signal is high.

Two output circuits are shown on the secondary side, a first output circuit supplying +5 volts, while a second output circuit supplies -15 volts. A first secondary winding N^ and N. has a center V connected to earth, while the extremities of the secondary coil N_, N. are connected to a node V₁ through rectifier couplings. These rectifier couplings are illustrated with two diodes D.. and D~, it being generally known by skilled persons to par- allel connect such rectifier diodes with a series connec¬ tion of a resistor and a capacitor, to protect the diode against instantaneous high voltage values to thereby in¬ crease its life. The AC voltage induced in the secondary windings N„ and N, is rectified through the rectifier coupling D. and D„ so that there will be a DC voltage level in the node V₁ with a superimposed AC voltage. The DC voltage level depends upon the polarity of the diodes D- and D~, and the voltage will be positive with the shown diode configuration. The node V.. is connected to earth through a capacitor C- and to the output terminal with +5 volts through an inductance L„. The output terminal with +5 volts is moreover connected to earth through a capaci¬ tor C.. Corespondingly, the second output circuit has secondary windings N-. and N, whose center V „ is connected to earth. The extremities of the secondary windings N.., N, are connected to a node V₂ through rectifier couplings. The rectifier coupling, like in the first output circuit, is realized by two diodes D„ and D., which can likewise advantageously be connected in parallel with a resistor and a capacitor. It is noted that the polarity of the dio¬ des are oppositely directed to the diodes D. , D„ mentioned in connection with the first output circuit, it being de¬ sired to have a negative voltage of -15 volts on the out- put terminal of the second output circuit. The node V,, is connected to earth through a capacitor C-. and to the out¬ put terminal at -15 volts through an inductance „, the output terminal being moreover connected to earth through a capacitor C,.

A current runs from the input terminal of +42 volts through the inductance L. toward the node V , and then the current alternately runs through the primary windings N- and N_ in dependence upon which of the transistors T. and T~ is conducting. This creates a flux of alternating pola¬ rity in the core in the transformer TRA, the flux direc- tion being controlled by the added signal to the control electrodes on the transistors T- and T„. The flux oscil¬ lator frequency in the transformer core will then corres¬ pond to the pulse repetition frequency in the signals from the drive circuit added to the control electrodes on the transistors T- and T.-,. The drive circuit may e.g. be com¬ posed of an integrated circuit with the number UC1825 from the firm UNITRODE.

The oscillating flux in the transformer core induces cur¬ rents in the secondary windings N~, N., N,-, N_fi between which taps are provided to earth V and V „ or to the previously mentioned node V, and V.-, through rectifier couplings. The mean voltages in the nodes V₁ and V₂ are determined by the ratio of the number of secondary wind¬ ings on the circuit concerned to the number of windings on the primary side. Since the node voltages V.. and V fluc¬ tuate violently, the voltage is smoothed by large smooth¬ ing capacities C . and C_β, respectively. The inductance ₉ and the capacitor C . may be considered to be a current generator with an infinitely great impedance. The same applies to the inductance L₃ and the capacitor C_fi. Accord¬ ing to the invention the primary side and each of the out¬ put circuits on the secondary side are tuned so as to in- dividually comprise an oscillatory circuit with coinciding resonance frequency. It is thus possible to equate the circuit diagram shown in fig. 1 with the equivalent dia¬ gram shown in fig. 4. Since both the input terminals and the output terminals are contained in a current generator formed by a large smoothing capacitor, which is connected to earth and is "concealed" in terms of AC voltage by an inductance - , L-, ,, connected to the terminal, the cur¬ rent generator will have a very great AC voltage impedance and will therefore not be included in the resonance consi- derations. Thus, on the primary side it is the capacitor C_ as well as the dispersion inductances associated with the windings N- , N- which, together with various other dispersion inductances and capacities, constitute the oscillatory circuit. Similar considerations can be made with respect to the output side. The equivalent components marked ' are thus to be dimensioned such that the voltage drop across an inductance ' is numerically just as great as the voltage drop across a capacitor C , but with oppo¬ site polarity.

A balanced bridge will thus be obtained in which:

-L'p = l/(ωCp)' (1)

oL' a = 1/(»C' a) (3)

The voltage on the star node V_A will consequently be iden¬ tical with the voltage in the node which is connected to earth. The current running through the individual oscilla¬ tory circuits creates no error voltage in the star node v*.

The art described here of tuning a voltage converter so that each individual circuit forms a separate tuned oscil¬ latory circuit, thus entails that a zero error node V_A is obtained for a voltage converter with several output cir¬ cuits.

The circuit shown in fig. 1 may be improved additionally, which is shown in fig. 2 where the voltage on the input terminal is controlled by a regulation circuit 20, which scans the flux in the iron core of the transformer with transformer windings N arranged on the primary side, where the regulation provides a stiff primary voltage which thereby improves the stability on the output of the converter. When the regulation circuit 20 is moreover tuned to an oscillatory circuit with the same resonance frequency as the other circuits of the converter, it is achieved that the regulation circuit does not influence the other functions of the converter. The regulation circuit may be based on a regulater LM117 from National.

The invention has been explained in the foregoing with reference to a DC voltage converter, but the principle of distributed tuning so that the primary side and the output circuits on the secondary side are tuned individually to form individual oscillatory circuits with a common reso¬ nance frequency, can also be used in connection with an AC voltage converter. The drive circuit 10 converts precisely the DC voltage on the input to an AC voltage which is transferred through the transformer to the secondary wind¬ ings, the rectifier couplings converting the AC voltage to a DC voltage signal which is additionally smoothed before reaching the output terminal.

As will be seen in fig. 4, it is possible to connect any number of output circuits on the secondary side to the node V .

The smoothing capacities C . _t C, with associated coils „, - are mentioned in the foregoing as having such a great impedance that the individual couplings may be regarded as current generators. This will not be expedient in prac¬ tice, but the principle outlined here will nevertheless be fully applicable even though the "current generators" do not exhibit an infinitely high impedance, and will there¬ fore be included in the oscillatory circuits concerned. However, this contribution is so limited that it is not necessary to pay any regard to this in practice. The voltage converter is shown with just two secondary circuits in figs. 1 and 2, but this number has just been selected for simplicity and may thus be selected as needed from one secondary circuit and upwards.

Claims

P a t e n t C l a i m s :

1. A voltage converter which has a primary circuit and which, with an input voltage, is coupled through at least one primary winding to respective secondary windings of at least one secondary circuit, c h a r a c t e r i z e d in that the primary circuit and each of the secondary cir¬ cuits are tuned individually so that each circuit forms an oscillatory circuit with coinciding resonance frequences.

2. A voltage converter according to claim 1, c h a ¬ r a c t e r i z e d in that a DC voltage is converted to one or more DC voltage levels.

3. A voltage converter according to claim 1 or 2, addi¬ tionally comprising a switching circuit which is adapted to reverse the resulting current in one or more primary windings with a constant switching frequency, c h a - t a c t e r i z e d in that the resonance frequency is of the same order as the switching frequency.

4. A voltage converter according to claims 1-3, moreover including a regulation circuit which comprises means for regulating the input voltage in response to a parameter sensed by the transformer, c h a r a c t e r i z e d in that the regulation circuit is tuned to the resonance frequency.

5. A voltage converter according to claims 1-4, c h a ¬ r a c t e r i z e d in

that the primary circuit has an input terminal to which a DC voltage level is applied and which is connected to the center (V ) of two symmetrical primary windings (N., N_?) through an inductance (L..), the center (V ) being moreover connected to earth, through a capacitor (C~), respective extremities of the primary windings (N.. , N~ ) being con¬ nected to respective transistors (T., T„ ) whose states are controlled by a control circuit (10) connected thereto,

and that each secondary circuit has a plurality of secon¬ dary windings (N , N.; N-. _Nfi) arranged symmetrically around the center (V - ; V _) connected to earth, the ex¬ tremities of said secondary windings being connected to a node (V.; V,- ) through respective rectifier couplings (D- , D ; D„, D. ), to produce a rectifier voltage, said node (V..; V«) being connected partly to earth through a capa¬ citor (C ; C-.), partly to an output terminal through an inductance ( L~; „), said output terminal being connected to earth through a smoothing capacitor (C.; C_fi) .