1. Field of the Invention
The present invention relates to power conversion. More specifically, the present invention relates to isolated DC/DC converters.
2. Description of the Related Art
Known techniques for power conversion include a zero voltage switching (ZVS) technique and/or a resonant conversion technique. One conventional topology uses a ZVS bridge that requires an additional resonant inductor. Another known technique uses an LLC resonant converter that requires a relatively low magnetizing inductance for ZVS, resulting in excessive losses at light- and no-load conditions. The drawbacks of conventional approaches are added complexity and/or light load efficiency reduction.
To overcome the problems described above, preferred embodiments of the present invention provide a converter that solves the switching loss problem, allowing for a higher frequency operation and for a greater power density.
According to preferred embodiments of the present invention, a converter includes a transformer including a primary winding and a secondary winding, a primary-side circuit connected to first and second input terminals and to the primary winding and including a switching circuit connected to the primary winding and a parallel resonant tank circuit including the primary winding and a resonant capacitor connected in parallel with the primary winding, a secondary-side circuit connected to the secondary winding and to first and second output terminals and including a rectifier circuit connected to the secondary winding, and an inductor including a primary inductor winding connected to the first input terminal and the primary winding and a secondary inductor winding connected to the secondary winding and the first output terminal.
The primary-side circuit further preferably includes a clamp circuit connected to the first input terminal. The clamp circuit is also preferably connected to either the switching circuit or the primary winding.
The primary inductor winding is preferably connected to the primary winding through the switching circuit. The secondary inductor winding is preferably connected to the secondary winding through the rectifier circuit. The inductor further preferably includes an auxiliary inductor winding connected between the second input terminal and the clamp circuit.
The following ratio is preferably satisfied: NpT/NsT=NpI/NsI, where NpT is a number of turns in the primary winding, NsT is a number of turns in the secondary winding, NpI is a number of turns in the primary inductor winding, and NsI is a number of turns in the secondary inductor winding.
The primary inductor winding and the secondary inductor winding are preferably coupled together by a magnetic core. The primary inductor winding, the secondary inductor winding, and the primary auxiliary inductor winding are preferably coupled together by a magnetic core.
The switches of the switching circuit are preferably switched at a frequency equal to a resonant frequency of the parallel resonant tank.
The primary-side circuit further preferably includes additional resonant capacitors connected across corresponding switches of the switching circuit. The primary-side circuit further preferably includes a capacitor connected across the first and second input terminals. The secondary-side circuit further preferably includes an additional resonant capacitor connected across the secondary winding.
The secondary-side circuit further preferably includes an output capacitor connected in parallel across the first and second output terminals. The output capacitor and the secondary inductor winding are preferably connected together to define an output filter.
The switching circuit preferably includes at least two MOSFETs. The rectifier circuit preferably includes at least two rectifiers. The at least two rectifiers are preferably MOSFETs. The at least two rectifiers are preferably diodes. The switching circuit preferably has either a full-bridge or a push-pull topology. The rectifier circuit preferably has either a full bridge or a center-tap scheme.
The above and other features, elements, characteristics and advantages of the present invention will become more apparent from the following detailed description of preferred embodiments of the present invention with reference to the attached drawings.
Preferred embodiments of the present invention are shown in
The preferred embodiments of the present invention preferably use full-bridge (FB) and push-pull (PP) converter topologies with FB and center-tap (CT) output rectifier schemes. FB and PP converter topologies are current-fed double-ended topologies. It is also possible to use current-fed single-ended topologies that include a parallel resonant tank.
The converter according the first preferred embodiment of the present invention is shown in
The principle of operation of the converter shown in
In one mode of operation, the switching frequency Fsw is equal to the resonant frequency of the parallel resonant tank, i.e., Fsw=1/(2π*√(Lr*Cr), where Cr is the capacitance of the equivalent resonant capacitor defined by Crp and the optional capacitors Cr1, Cr2, Cr3, Cr4, and Crs and where Lr is the inductance of the resonant inductor Lr. As long as the switching frequency of the primary switches S1, S2, S3, and S4is set to the resonant tank frequency, a ZVS mode of operation is maintained under all operational conditions, including from no load to full load. Inductance L of the primary power winding NpI of inductor LI is selected to be large enough so that the input current does not change significantly during the switching period Tsw and so that the parallel resonant tank is driven by square wave current pulses of fixed magnitude defined by the load current. The quality factor of the parallel resonant tank is selected to be large enough so that the voltages across the resonant inductor Lr, which is the primary winding of the transformer T, across the diagonal of the primary full-bridge circuit, and across the secondary winding NsT of the transformer T are of the sinusoidal type and so that the corresponding voltages across the primary switches S1, S2, S3, and S4 and the secondary rectifiers S5, S6, S7, and S8 are of the half-sine-wave type. Because the average voltage across the primary full-bridge circuit is equal to the input voltage Vin, the sine wave magnitude Vbm across the transformer primary and across each of the primary switches S1, S2, S3, and S4 is equal to:
V
bm
=V
in*π/2. (1)
The secondary transformer voltage and the voltages across each of the secondary rectifiers S5, S6, S7, and S8 is defined by the input voltage Vin and by the transformer turns ratio NpT/NsT. The magnitude of the secondary transformer voltage is (Vin*π/2)/(NpT/NsT). An output filter circuit is provided by the secondary power winding NsI and the output capacitor C3. This output filter circuit averages the voltage rectified by the secondary full-bridge circuit so that the output voltage Vo is essentially of a DC type:
V
o=(Vin*π/2)/(NpT/NsT)*(2/π)=Vin*NsT/NpT. (2)
According to equation (2), the output voltage Vo is directly proportional to the input voltage Vin with a slope factor defined by the transformer turns ratio NsT/NpT. The dotted ends of the primary power winding NpI and the secondary power winding NsI are connected to the input terminal Vin and the output terminal Vo, respectively; the non-dotted ends of the primary power winding NpI and the secondary power winding NsI are connected to the top terminals of the primary full-bridge circuit and the secondary full-bridge circuit, respectively. The inductor's LI turns ratio is set to be equal to the transformer turns ratio: NpI/NsI=NpT/NsT-r. This ensures that the secondary voltages created by the transformer T and inductor LI are matched.
The DC current in the primary power winding NpI is flying from the input terminal Vin return to the dotted end of the primary power winding NpI, and the DC current in the secondary power winding NsI is flying from the top terminal of the secondary full-bridge circuit to the non-dotted end of the secondary power winding NsI, resulting in the DC flux cancellation in the magnetic core of the inductor LI. In turn, this DC flux cancellation results in a relatively small inductor size for the inductor LI. If the primary power winding NpI and the secondary power winding NsI are not coupled, the converter can operate in the same way, but the inductors corresponding to the primary power winding NpI and the secondary power winding NsI are subjected to input and output DC bias currents, respectively, resulting in the need for inductors with larger magnetic core sizes.
The clamp circuit including capacitor C2 and diode D1 connected to the auxiliary primary winding NpaI works in the following manner. The capacitor C2 is selected to be large enough to ensure that the DC voltage \Opplied across the capacitor C2 has small ripples. That DC voltage Vc is equal to the input voltage Vin because the capacitor C2 is connected to the input terminal Vin through the primary power winding NpI and to the input terminal Vin return through the auxiliary primary winding NpaI. The forward voltage VF applied to diode D1 is equal to Vb−Vc−Vin, where Vb is the voltage across the primary full-bridge circuit at the non-dotted end of the primary power winding NpI with respect to Vin return and Vc is the voltage across the capacitor C2. Because Vc=Vin,
VF=V
b−2*Vin. (3)
Under steady state conditions, Vb≦Vin*π/2<2*Vin according to equation (1), the forward voltage VF is negative according to equation (3), the diode D1 is reverse biased, and the clamp circuit is not activated. Under transient conditions, for example, when the load current goes to zero with a high slew rate, the input inductor energy is released, resulting in a voltage spike across the primary full-bridge circuit. At the instant that voltage Vb exceeds twice the voltage level of the input terminal Vin, the diode D1 is forward biased (see equation (3)), and the inductor energy is recovered to the input capacitor C1 and to the input source connected to the input terminals Vin and Vin return. As a result, the voltage Vb and the corresponding voltages across the primary switches S1, S2, S3, and S4 are clamped at twice the voltage level of the input terminal Vin plus the voltage drop across the diode D1. The capacitors C1 and C2 connect the dotted and non-dotted terminals of the coupled primary power winding NpI and the auxiliary primary winding NpaI, respectively. Because the inductances of the primary power winding NpI and the auxiliary primary winding NpaI are connected in parallel at AC voltages, the numbers of turns of the primary power winding NpI and the auxiliary primary winding NpaI are selected to be equal. If the primary power winding NpI connected to the clamp circuit is not coupled to the auxiliary power winding NpaI, the clamp circuit works the same way at the expense of an additional magnetic component, an auxiliary inductor equivalent to NpaI.
The secondary rectifiers S5, S6, S7, and S8 can be uncontrolled diodes D2, D3, D4 and D5 as shown with dashed lines in
The converter of the second preferred embodiment of the present invention is shown in
The capacitor C2 is selected to be large enough to ensure that the DC voltage Vc applied across the capacitor C2 has small ripples. Accordingly, the DC voltage Vc is equal to the input voltage Vin because the capacitor C2 is connected to the input terminal Vin through the primary power winding NpI and to the input terminal Vin return through the auxiliary primary winding NpaI. The forward voltage VF applied to diode D1 is equal to Vct−Vc−Vin, where Vct is the voltage at the center tap of the primary winding of the power transformer T with respect to Vin return and Vc is the voltage across the capacitor C2. Because Vc=Vin,
VF=V
ct−2*Vin. (4)
Under steady state conditions, the peak voltage Vctm at the center tap of the primary winding of the power transformer T with respect to Vin return, similar to equation (1), is Vctm=Vin*π/2, Vct≦Vin*π/2<2*Vin, and according to equation (4) the forward voltage VF is negative, the diode D1 is reverse biased, and the clamp circuit is not activated. Under transient conditions, for example, when the load current goes to zero with a high slew rate, the input inductor energy is released, resulting in a voltage spike at the center tap of the primary winding of the power transformer T. At the instant that voltage Vct exceeds twice the voltage level of the input terminal Vin, the diode D1 is forward biased (see equation (4)), and the inductor energy is recovered to the input capacitor C1 and to the input source connected to the input terminals Vin and Vin return. As a result, the voltage Vct is clamped at twice the voltage level of the input terminal Vin plus the voltage drop across the diode D1 and the corresponding voltages across the primary switches S1 and S2 are clamped at twice the center tap voltage level. The capacitors C1 and C2 connect the dotted and non-dotted terminals of the coupled primary power winding NpI and the auxiliary primary winding NpaI, respectively. Because the inductances of the primary power winding NpI and the auxiliary primary winding NpaI are connected in parallel at AC voltages, the numbers of turns of the primary power winding NpI and the auxiliary primary winding NpaI are selected to be equal. If the primary power winding NpI connected to the clamp circuit is not coupled to the auxiliary power winding NpaI, the clamp circuit works the same way at the expense of an additional magnetic component, such as an auxiliary inductor equivalent to NpaI.
The converters shown in
It should be understood that the foregoing description is only illustrative of the present invention. Various alternatives and modifications can be devised by those skilled in the art without departing from the present invention. Accordingly, the present invention is intended to embrace all such alternatives, modifications, and variances that fall within the scope of the appended claims.
Number | Date | Country | |
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61532663 | Sep 2011 | US |
Number | Date | Country | |
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Parent | PCT/US2012/054109 | Sep 2012 | US |
Child | 14159544 | US |