System and method for LLC converter design
09906136 ยท 2018-02-27
Assignee
Inventors
Cpc classification
Y02B70/10
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
International classification
Abstract
An embodiment method for designing a power converter system includes receiving, by a processor, power converter design parameters. The design parameters include a minimum DC input voltage V.sub.min and a maximum DC input voltage V.sub.max, a minimum switching frequency f.sub.min and a maximum switching frequency f.sub.max of a switching bridge of the power converter, and a target output voltage and a target output power. The method also includes calculating, by the processor, a first power converter configuration. The first power converter configuration includes a calculated magnetizing inductance L.sub.mc equal to R.sub.e tan()(2f.sub.min).sup.1, where is a load angle complement equal to a sin(V.sub.minV.sub.max.sup.1), and R.sub.e is an equivalent reflected load resistance of the power converter. The first power converter configuration also includes a calculated resonant inductance L.sub.rc equal to L.sub.mc cos.sup.2()(f.sub.max.sup.2f.sub.min.sup.21).sup.1 and a calculated resonant capacitance C.sub.rc equal to L.sub.rc.sup.1(2f.sub.max).sup.2.
Claims
1. A method for designing an inductance-inductance-capacitance (LLC) power converter, the method comprising: receiving, by a processor, power converter design parameters of the LLC power converter, wherein the LLC power converter comprises a switching bridge coupled to a primary winding of a transformer, a resonant inductor and a resonant capacitor coupled in series between the switching bridge and the primary winding of the transformer, and a secondary side circuit coupled to a secondary winding of the transformer, the power converter design parameters comprising: a minimum DC input voltage V.sub.min and a maximum DC input voltage V.sub.max to be received by the switching bridge, a minimum switching frequency f.sub.min and a maximum switching frequency f.sub.max of the switching bridge, and a target output voltage V.sub.o and a target output power P.sub.o to be output by the secondary side circuit; calculating, by the processor, a first power converter configuration comprising: a calculated magnetizing inductance L.sub.mc of the primary winding equal to R.sub.etan()(2f.sub.min).sup.1, wherein is a load angle complement equal to asin(V.sub.minV.sub.max.sup.1), and R.sub.e is an equivalent reflected load resistance of the power converter, a calculated resonant inductance L.sub.rc of the resonant inductor equal to L.sub.mccos.sup.2()(f.sub.max.sup.2f.sub.min .sup.21).sup.1, and a calculated resonant capacitance C.sub.rc of the resonant capacitor equal to L.sub.rc .sup.1(2f.sub.max).sup.2; writing, by the processor, the first power converter configuration to a non-transitory computer readable medium; determining layout component values based on the first power configuration; and physically implementing the LLC power converter using the layout component values.
2. The method of claim 1, wherein the power converter design parameters further comprise a switching factor s that is equal to 2 when the switching bridge has a half-bridge configuration and that is equal to 1 when the switching bridge has a full-bridge configuration; and the first power converter configuration further comprises a calculated turns ratio n.sub.c of the primary winding relative to the secondary winding of the transformer comprised in the power converter, wherein n.sub.c is not less than 0.99V.sub.max(sV.sub.o).sup.1 and is not greater than V.sub.max(sV.sub.o).sup.1; and the equivalent reflected load resistance R.sub.e equals 8.sup.2n.sub.c.sup.2V.sub.o.sup.2P.sub.o.sup.1.
3. The method of claim 1, further comprising graphically displaying the first power converter configuration at a user terminal.
4. The method of claim 3, wherein the receiving the power converter design parameters comprises: receiving a first set of cells in a spreadsheet, wherein values of the first set of cells comprise the power converter design parameters; and the graphically displaying the first power converter configuration comprises: displaying a second set of cells in the spreadsheet, wherein values of the second set of cells comprise the first power converter configuration.
5. The method of claim 1, wherein the non-transitory computer readable medium is a file.
6. The method of claim 5, further comprising: receiving, by the processor, a list of available components; and determining the layout component values comprises selecting, by the processor, layout component values in accordance with the list of available components and the first power converter configuration, the layout component values comprising: an actual turns ratio n.sub.a of the transformer greater than c.sub.1n.sub.c and less than c.sub.2n.sub.c, wherein c.sub.1 is not less than 0.75 and c.sub.2 is not greater than 1.25, an actual magnetizing inductance L.sub.m.sub._.sub.a of the primary winding of the transformer greater than c.sub.1L.sub.m.sub._.sub.c and less than c.sub.2L.sub.m.sub._.sub.c; an actual resonant inductance L.sub.r.sub._.sub.a of the resonant inductor greater than c.sub.1L.sub.r.sub._.sub.c and less than c.sub.2L.sub.r.sub._.sub.c; and an actual resonant capacitance C.sub.r.sub._.sub.a of the resonant capacitor greater than c.sub.1C.sub.r.sub._.sub.c and less than c.sub.2C.sub.r.sub._.sub.c.
7. The method of claim 6, wherein the selecting the layout component values comprises at least one of: selecting layout components from the list of available components such that the layout component values are closest to component values in the first power converter configuration; and selecting layout components from the list of available components such that the layout component values jointly maximize a figure of merit in accordance with the first power converter configuration.
8. A power converter design system comprising a non-transitory computer-readable medium storing programming, wherein the programming comprises instructions to: receive power converter design parameters of an inductance-inductance-capacitance (LLC) power converter, wherein the LLC power converter comprises a switching bridge coupled to a primary winding of a transformer, a resonant inductor and a resonant capacitor coupled in series between the switching bridge and the primary winding of the transformer, and a secondary side circuit coupled to a secondary winding of the transformer, the power converter design parameters comprising: a minimum DC input voltage V.sub.min and a maximum DC input voltage V.sub.max to be received by the switching bridge, a minimum switching frequency f.sub.min and a maximum switching frequency f.sub.max of the switching bridge, and a target output voltage V.sub.o and a target output power P.sub.o to be output by the secondary side circuit; calculate a first power converter configuration comprising: a calculated magnetizing inductance L.sub.mcof the primary winding equal to R.sub.etan()(2f.sub.min).sup.1, wherein is a load angle complement equal to asin(V.sub.minV.sub.max.sup.1), and R.sub.e is an equivalent reflected load resistance of the power converter, a calculated resonant inductance L.sub.rc of the resonant inductor equal to L.sub.mccos.sup.2()(f.sub.max.sup.2f.sub.min.sup.21).sup.1, and a calculated resonant capacitance C.sub.rc of the resonant capacitor equal to L.sub.rc.sup.1(2f.sub.max).sup.2; write the first power converter configuration to a non-transitory computer readable medium; determine layout component values based on the first power configuration; and physically implement the LLC power converter using the layout component values.
9. The system of claim 8, wherein the power converter design parameters further comprise a switching factor s that is equal to 2 when the switching bridge has a half-bridge configuration and that is equal to 1 when the switching bridge has a full-bridge configuration; and the first power converter configuration further comprises a calculated turns ratio n.sub.c of the primary winding relative to the secondary winding of a transformer comprised in the power converter, wherein n.sub.c is not less than 0.99V.sub.max(sV.sub.o).sup.1 and is not greater than V.sub.max(sV.sub.o).sup.1; and the equivalent reflected load resistance R.sub.e equals 8.sup.2n.sub.c.sup.2V.sub.o.sup.2P.sub.o.sup.1.
10. The system of claim 8, wherein the programming further comprises instructions to graphically display the first power converter configuration at a user terminal.
11. The system of claim 10, wherein the instructions to receive the power converter design parameters comprise instructions to receive a first set of cells in a spreadsheet, wherein values of the first set of cells comprise the power converter design parameters; and the instructions to graphically display the first power converter configuration comprise instructions to display a second set of cells in the spreadsheet, wherein values of the second set of cells comprise the first power converter configuration.
12. The system of claim 8, wherein the non-transitory computer readable medium is a file.
13. The system of claim 12, wherein the programming further comprises instructions to: receive a list of available components; and determine the layout component values by selecting the layout component values in accordance with the list of available components and the first power converter configuration, the layout component values comprising: an actual turns ratio n.sub.a of the transformer greater than c.sub.1n.sub.c and less than c.sub.2n.sub.c, wherein c.sub.1 is not less than 0.75 and c.sub.2 is not greater than 1.25, an actual magnetizing inductance L.sub.m of the primary winding of the transformer greater than c.sub.1L.sub.mc and less than c.sub.2L.sub.mc; an actual resonant inductance L.sub.r of the resonant inductor greater than c.sub.1L.sub.rc and less than c.sub.2L.sub.rc; and an actual resonant capacitance C.sub.r of the resonant capacitor greater than c.sub.1C.sub.cr and less than c.sub.2C.sub.rc.
14. The system of claim 13, wherein the instructions to select the layout component values comprise at least one of: instructions to select the layout component values from the list of available components such that the layout component values are closest to component values in the first power converter configuration; and instructions to select the layout component values from the list of available components such that the layout component values jointly maximize a figure of merit in accordance with the first power converter configuration.
15. The system of claim 13, wherein the programming further comprises instructions to: apply the layout component values to the file, wherein the file is a layout representing a physical circuit for the power converter.
16. The system of claim 15, wherein the programming further comprises instructions to synthesize the physical circuit in accordance with the layout.
17. A power conversion system comprising: a switching bridge comprising a plurality of switches coupled to a DC power source having a minimum input voltage V.sub.min and a maximum input voltage V.sub.max, wherein the switching bridge is configured to switch at a frequency that is not less than a minimum frequency f.sub.min and that is not greater than a maximum frequency f.sub.max; a primary side circuit coupled to the switching bridge, the primary side circuit comprising a primary winding of a transformer; and a secondary winding magnetically coupled to the primary winding through a core of the transformer, and an output terminal coupled to the secondary winding and configured to supply an output voltage that is not greater than a maximum output voltage V.sub.o and an output power that is not greater than a maximum output power P.sub.o; wherein the transformer has a magnetizing inductance L.sub.m such that L.sub.m is greater than c.sub.1R.sub.e(2f.sub.min).sup.1tan() and less than c.sub.2R.sub.e(2f.sub.min).sup.1tan(), wherein c.sub.1 is not less than 0.75 and c.sub.2 is not greater than 1.25, is a load angle complement equal to asin(V.sub.minV.sub.max.sup.1), and R.sub.e is an equivalent reflected load resistance; wherein the primary side circuit has a resonant inductance L.sub.r such that L.sub.r is greater than c.sub.1Lm(f.sub.max.sup.2f.sub.min.sup.21).sup.1cos.sup.2() and L.sub.r is less than c.sub.2L.sub.m(f.sub.max.sup.2f.sub.min.sup.21).sup.1cos.sup.2(); and wherein the primary side circuit has a resonant capacitance C.sub.r in series with the resonant inductance such that C.sub.r is greater than c.sub.1L.sub.r.sup.1(2f.sub.max).sup.2 and less than c.sub.2L.sub.r.sup.1(2f.sub.max).sup.2.
18. The system of claim 17, wherein the switching bridge comprises two switches; and the primary winding has a number of turns that is a multiple n times a number of turns of the secondary winding, wherein n is greater than c.sub.1V.sub.max(2V.sub.o).sup.1 and less than c.sub.2V.sub.max(2V.sub.o).sup.1; and R.sub.e is not less than 8(s).sup.2(0.99V.sub.max).sup.2P.sub.o.sup.1 and not greater than 8(s).sup.2V.sub.max.sup.2P.sub.o.sup.1, wherein s is a switching factor equal to 2.
19. The system of claim 17, wherein the switching bridge comprises four switches; the primary winding has a number of turns that is a multiple n times a number of turns of the secondary winding, wherein n is greater than c.sub.1V.sub.maxV.sub.o.sup.1 and less than c.sub.2V.sub.maxV.sub.o.sup.1; and R.sub.e is not less than 8.sup.2(0.99V.sub.max).sup.2P.sub.o.sup.1 and not greater than 8.sup.2V.sub.max.sup.2P.sub.o.sup.1.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) For a more complete understanding of the present invention, and the advantages thereof, reference is now made to the following descriptions taken in conjunction with the accompanying drawings, in which
(2)
(3)
(4)
(5)
(6)
DETAILED DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS
(7) The making and using of the presently preferred embodiments are discussed in detail below. It should be appreciated, however, that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed are merely illustrative of specific ways to make and use the invention, and do not limit the scope of the invention.
(8) The present invention will be described with respect to preferred embodiments in a specific context, a system and method for LLC converter design for use in EDA and other automated design systems. Further embodiments may be applied to other switched LLC converter design systems that require specifying a range of switching frequencies.
(9)
(10)
(11) The minimum switching frequency f.sub.min is chosen to be high enough for example, at least 30 to 40 kilohertz (kHz) or higher, to reduce interference from audio signals. The maximum switching frequency f.sub.max is chosen to be approximately equal to a resonant switching frequency f.sub.r of the resonant tank inductor 124 and the resonant tank capacitor 126. The inductance and capacitance of these components are in turn chosen so that the resonant switching frequency f.sub.r is both low enough to reduce switching losses and high enough to reduce the required size of the resonant tank inductor 124 and the resonant tank capacitor 126. In an embodiment, component values are selected to provide a resonant switching frequency/maximum switching frequency in the range of 80 to 200 kHz.
(12) The combined required size of the resonant tank inductor 124 and the resonant tank capacitor 126 is proportional to the combined average peak energy E(f.sub.xo) that is contained in each of these components at the minimum switching frequency, where f.sub.xo is a normalized minimum switching frequency equal to f.sub.min/f.sub.r. In turn, the average peak energy E(f.sub.xo) is proportional to a function (f.sub.xo), which has a derivative d(f.sub.xo)/df.sub.xo, such that:
(f.sub.xo)=(1+f.sub.xo.sup.2)[(f.sub.xo)(1+f.sub.xo.sup.2)].sup.1 (Eq. 1A)
d(f.sub.xo)/df.sub.xo=f.sub.xo.sup.4+4f.sub.xo.sup.21 (Eq. 1B)
(13) E(f.sub.xo) reaches a minimum energy level, and the combined required size of the resonant components is minimized, when the derivative d(f.sub.xo)/df.sub.xo is equal to zero, which occurs when f.sub.xo=0.485. In an embodiment, f.sub.min and f.sub.r are selected so that the required size of the resonant components is not very sensitive to changes in f.sub.xo. For example, if f.sub.xo is limited to vary within a range of (0.34, 0.63), which is centered on 0.485, (f.sub.xo) varies by around only ten percent (from 3.71 to 3.68), and therefore the required size of the resonant components varies by around only ten percent.
(14) Referring again to
(15) The primary winding 106 has a number of turns n times greater than or less than a number of turns y of the secondary winding 110. In embodiments of the present invention, the transformer is selected so that this turns ratio n is within plus or minus 25% of a calculated turns ratio n.sub.c. In an embodiment, the calculated turns ratio n.sub.c is in a range from [99%V.sub.max(sV.sub.o).sup.1]n.sub.c[V.sub.max(sV.sub.o).sup.1], where s is a switching factor of the switching bridge. This range of allowable values for n.sub.c takes into account voltage losses that may occur.
(16) In a first embodiment, the power converter is a half-bridge converter in which the switching bridge 102 includes two switches and the switching factor s is equal to 2. In a second embodiment, the power converter is a full-bridge converter in which the switching bridge 102 includes four switches and the switching factor s is equal to 1. In embodiments of the present invention, the rectifier 116 may also be either a half-bridge rectifier made up of two diodes or a full-bridge rectifier made up of four diodes. In other embodiments, the rectifier is a synchronous rectifier.
(17)
(18) The equivalent AC circuit has a load impedance that is the product over the sum of the impedances of the reflected load resistance R.sub.e and the magnetizing inductance L.sub.m such that:
Z.sub.1()=jL.sub.mR.sub.e(R.sub.e+jL.sub.m).sup.1=[L.sub.m+jR.sub.e][.sub.oL.sub.mR.sub.e.sup.1+R.sub.e(.sub.oL.sub.m).sup.1].sup.1 (Eq. 2)
(19) The equivalent AC circuit also has a resonant impedance Z.sub.r() that is the sum of the impedances of the resonant capacitance C.sub.r and the resonant inductance L.sub.r:
Z.sub.r()=jL.sub.r+(jC.sub.r).sup.1=jL.sub.r(1L.sub.r.sup.1C.sub.r.sup.1.sup.2) (Eq. 3)
(20) By substituting an angular resonant frequency .sub.r that is equal to (L.sub.rC.sub.r).sup.0.5, Equation 3 may be rewritten as:
Z.sub.r()=jL.sub.r[(.sub.r/).sup.21](Eq. 4)
(21) This angular resonant frequency .sub.r corresponds to a resonant switching frequency f.sub.r that is equal to 2(L.sub.rC.sub.r).sup.0.5. When the angular operating frequency w is equal to this angular resonant frequency .sub.r, a resonance occurs such that the resonant impedance Z.sub.r is equal to zero and maximum current flows through the series resonant capacitance C.sub.r and series resonant inductance L.sub.r.
(22) The equivalent AC circuit also has an input impedance that is equal to the sum of the resonant impedance and the load impedance such that Z.sub.i()=Z.sub.1()+Z.sub.r(). Because the real component of the input impedance is always positive, the sign of the angle of the input impedance is the same as the sign of the imaginary component of the input impedance Im(Z.sub.i), such that when the angle of the input impedance is less than 0 the LLC converter operates in capacitive mode and the input voltage lags behind the input current. The MOSFET body diodes in the switching bridge will then be exposed to hard commutation which dramatically increases switching losses.
(23) To avoid these switching losses and to allow for MOSFET soft-switching during startup, the LLC converter is instead operated in inductive mode such that input current lags behind the input voltage. This LLC operates in this inductive mode at frequencies that are high enough that the angle of the input impedance and accordingly the imaginary component of the input impedance are greater than or equal to zero.
(24) The equivalent AC circuit also has a transfer function having a gain G() equal to V.sub.o.sub._.sub.acV.sub.in.sub._.sub.ac.sup.1. As will be explained in connection with
(25) Referring to both
(26) The selected components of the LLC converter also support a maximum gain G.sub.max corresponding to the minimum and maximum input voltage parameters such that G.sub.maxV.sub.maxV.sub.min.sup.1, so that the gain may be increased from a minimum gain when V.sub.in is equal to V.sub.max up to a gain of V.sub.maxV.sub.min.sup.1 when V.sub.in is equal to V.sub.min. The gain is increased by decreasing the switching frequency of the switching bridge 102 when the input voltage drops. The selected components also support an equivalent reflected load resistance R.sub.e, which as described earlier is a function of the calculated turns ratio n.sub.c. Thus, R.sub.e corresponds to the target output voltage and maximum input power such that [8(s).sup.2(99%V.sub.max).sup.2P.sub.o.sup.1]R.sub.e[8(s).sup.2V.sub.max.sup.2P.sub.o.sup.1].
(27) In particular, the LLC converter components are selected so that actual values of the turns ratio n, magnetizing inductance L.sub.m, resonant capacitance C.sub.r, and resonant inductance L.sub.r are each within plus or minus 25% of respective calculated values n.sub.c, L.sub.mc, C.sub.rc, and L.sub.rc, which are calculated based on the power converter's design parameters. An expression for the calculated turns ratio n.sub.c is previously described. The calculated magnetizing inductance L.sub.mc is equal to R.sub.e(2f.sub.min).sup.1tan(), where is a load angle complement equal to a sin(V.sub.minV.sub.max.sup.1). The calculated resonant inductance L.sub.rc is equal to L.sub.mc(f.sub.max.sup.2f.sub.min.sup.21).sup.1cos.sup.2(). The calculated resonant capacitance C.sub.rc is equal to L.sub.r.sub._.sub.c.sup.1(2f.sub.max).sup.2.
(28) TABLE-US-00001 TABLE 1 Calculated Vs. Actual Component Values Bridge V.sub.min V.sub.max V.sub.o P.sub.o f.sub.min f.sub.max L.sub.r C.sub.r L.sub.m Type (V) (V) (V) (W) (kHz) (kHz) (H) (nF) (H) n Half 350 384 12 600 90 157 Calc. 15.9 64.6 192 15.9 (s = 2) Actual 15.5 66 195 16 Actual/ 97.5% 102.2% 101.6% 110.6% Calc. Full 16 33 400 125 50 110 Calc. 2.48 843 12.5 12.1.sup.1 (s = 1) Actual 2.3 940 12.2 12.sup.1 Actual/ 92.7% 111.5% 97.6% 100.8% Calc.
(29) Referring now to
G()=Z.sub.1()Z.sub.i().sup.1=Z.sub.1()[Z.sub.1()+Z.sub.r()].sup.1 (Eq. 5)
(30) Using Equations 2 and 3, Equation 5 may be inverted to obtain G().sup.1, the reciprocal of the gain, in terms of the resonant inductance L.sub.r and the angular resonant frequency .sub.r:
G().sup.1=1+Z.sub.r()/Z.sub.1()=1jL.sub.r[(.sub.r/).sup.21]Z.sub.1().sup.1 (Eq. 6)
(31) In these calculations, when the angular operating frequency is less than or equal to the angular resonant frequency .sub.r, the term [(.sub.r/).sup.21] is greater than or equal to zero so that the converter operates with a gain greater than or equal to one. As the angular operating frequency drops further below the angular resonant frequency, the converter operates in boost mode such that the term [(.sub.r/).sup.21] increases and the gain of the converter increases. Maximum gain is thus achieved at a lowest angular operating frequency that is still above the capacitive operating range (i.e., Im(Z.sub.i)0). This condition is fulfilled at the zero-angle operating frequency .sub.o where the angle and the imaginary component of the input impedance are equal to zero.
(32) At this zero-angle operating frequency, the magnitude of the gain |G(.sub.o)| is maximized and the converter operates in resistive mode with the input current in phase with the input voltage. Using the properties of the gain G(.sub.o) at this frequency .sub.o, an expression for .sub.o, the gain angle at .sub.o, can be derived. First, the input impedance of the converter can be written as the product of the load impedance and the reciprocal of the gain such that Z.sub.1()G().sup.1=|Z.sub.i|exp[j()], where is the angle of the input impedance in terms of the angle of the load impedance and the angle of the gain. When the angle of the input impedance is equal to zero, the difference between the load impedance angle and the gain angle .sub.o.sub.o is also equal to zero. Thus, the gain angle .sub.o=.sub.o, where .sub.o is the load impedance angle when the angular operating frequency equals .sub.o.
(33) Referring now to
=.sub.oc+/2=.sub.oc+/2 (Eq. 7)
(34) Using this change of variables, the calculated load impedance at .sub.o may then be expressed as:
Z.sub.lc(.sub.o)=|Z.sub.lc(.sub.o)|exp[j(/2)]=[L.sub.mc+jR.sub.e][.sub.oL.sub.mcR.sub.e.sup.1+R.sub.e(.sub.oL.sub.mc).sup.1].sup.1 (Eq. 8)
(35) This expression for the calculated load impedance is illustrated in the dashed triangle, inspection of which shows that L.sub.mc=R.sub.e.sub.o.sup.1 tan . To derive an expression for the calculated gain, an expression is first derived for the calculated impedance ratio Z.sub.rc(.sub.o)/Z.sub.lc(.sub.o) in terms of , .sub.o, and the calculated resonant angular frequency .sub.rc:
Z.sub.rc(.sub.o)Z.sub.lc(.sub.o).sup.1=jL.sub.rc[(.sub.rc/.sub.o).sup.21](R.sub.e+j.sub.oL.sub.mc)(j.sub.oL.sub.mcR.sub.e).sup.1=jL.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21](1+j tan )=1L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21](cos +j sin )(cos ).sup.1=L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21](cos ).sup.1exp(j) (Eq. 9)
(36) Since the LLC converter is being designed to operate in boost mode in that the calculated angular resonant frequency .sub.rc corresponds to the design parameter for the maximum switching frequency, the zero-angle operating frequency .sub.o will be less than the calculated angular resonant frequency .sub.rc and the term [(.sub.rc/.sub.o).sup.21] will be greater than zero. Using exp(j)=1 and taking /2/2, Equation 9 may be rewritten as:
Z.sub.rc(.sub.o)/Z.sub.lc(.sub.o)=|L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21](cos ).sup.1|exp[j(+)], /2/2 (Eq. 10)
(37) Thus, the angle of the calculated impedance ratio is + when /2/2. Because the gain is maximized at .sub.o, therefore the calculated gain G.sub.c(.sub.o)=G.sub.max[exp(j.sub.oc)], where G.sub.max is a scalar representing the maximum magnitude of the calculated gain. Since the angle of the calculated gain .sub.oc=+/2, therefore the reciprocal of the calculated gain may be expressed as:
G.sub.c(.sub.o).sup.1=G.sub.max.sup.1exp[j(+/2)]=1+|Z.sub.rc(.sub.o)/Z.sub.lc(.sub.o)|exp[j(+)], /2/2 (Eq. 11)
(38) This expression for the gain in Equation 11 is illustrated in the dotted triangle of
=a sin(G.sub.max.sup.1) (Eq. 12)
|Z.sub.rc(.sub.o)/Z.sub.lc(.sub.o)|=|L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21]|(cos ).sup.1=cos() (Eq. 13)
(39) Therefore, the following equation for the calculated resonant inductance is also true:
L.sub.rc=L.sub.mc cos.sup.2()[(.sub.rc/.sub.o).sup.21].sup.1 (Eq. 14)
(40) As an alternative to this graphical demonstration, a complex-variable expression for the reciprocal maximum gain G.sub.max.sup.1 can be derived directly:
G.sub.max.sup.1=exp[j(/2)]G.sub.c(.sub.o).sup.1=exp[j(/2)](1+Z.sub.rc(.sub.o)Z.sub.lc(.sub.o).sup.1)=exp[j(/2)][1+exp[j(+)]|L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21]|(cos ).sup.1]=[exp[j(/2)]+exp[j(3/2)]|L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21]|(cos ).sup.1=sin(.sub.c)+j[cos()|L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21]|(cos ).sup.1]](Eq. 15)
(41) Since G.sub.max.sup.1 is a scalar with no imaginary component, it follows that the imaginary component of the right-hand expression of Equation 15 must be equal to zero:
cos()L.sub.rcL.sub.mc.sup.1[(.sub.rc/.sub.o).sup.21]cos .sup.1=0 (Eq. 16)
(42) By noting that .sub.o is chosen to be approximately equal to 2f.sub.min and the maximum switching frequency is chosen such that .sub.rc2f.sub.max, the following expressions may be derived:
L.sub.rc=L.sub.mc cos.sup.2()[(.sub.rc/.sub.o).sup.21].sup.1L.sub.mc cos.sup.2()[(f.sub.max/f.sub.min).sup.21].sup.1 (Eq. 17)
C.sub.rc=L.sub.rc.sup.1.sub.rc.sup.2L.sub.rc.sup.1(2f.sub.max).sup.2 (Eq. 18)
(43) Recalling Equations 7 and 8, the calculated magnetizing inductance may also be expressed as:
L.sub.mc=R.sub.e.sub.o.sup.1 tan R.sub.e(2f.sub.min).sup.1tan () (Eq. 19)
(44) With the imaginary component of the right-hand expression of Equation 15 set to zero, it then follows that G.sub.max.sup.1=sin(). Since G.sub.maxV.sub.maxV.sub.min.sup.1 and n.sub.cV.sub.max(sV.sub.o).sup.1, therefore:
=a sin(G.sub.max.sup.1)a sin(V.sub.minV.sub.max.sup.1)a sin(V.sub.min(n.sub.csV.sub.o).sup.1) (Eq. 20)
(45)
(46) At step 406, the design system graphically displays the calculated power converter configuration at a user terminal. For example, the system may display a second set of cells in the spreadsheet, where the values of the second set of cells include the calculated power converter configuration. At 408, the design system writes the calculated power converter configuration to a data file, which may be a spreadsheet or any form of data file.
(47) At step 410, the design system selects actual components based on the list of available components as well as the calculated power converter configuration, and applies these actual component values to a layout of a physical circuit for the power converter. The layout component values include an actual turns ratio n, an actual magnetizing inductance L.sub.m, an actual resonant inductance L.sub.r, and an actual resonant capacitance C.sub.r that are each within plus or minus 25% of their respective calculated values n.sub.c, L.sub.mc, L.sub.rc, and C.sub.rc.
(48) In a first embodiment, the layout components are selected from the list of available components such that the layout component values are each as close as possible to the calculated component values of the calculated power converter configuration. In a second embodiment, the layout components are selected from the list such that the layout component values jointly maximize a figure of merit when compared to the calculated values of the calculated power converter configuration. This figure of merit could be, for example, an absolute difference between f.sub.max and a resonant frequency of the selected components, a maximum likelihood, an average percent error, or a weighted metric based on the dollar, space, or power requirements of components.
(49) Referring again to
(50) Referring now to
(51) The bus may be one or more of any type of several bus architectures including a memory bus or memory controller, a peripheral bus, video bus, or the like. The CPU may include any type of electronic data processor. The memory may include any type of system memory such as random access memory (RAM), static RAM (SRAM), dynamic RAM (DRAM), synchronous DRAM (SDRAM), read-only memory (ROM), a combination thereof, or the like. In an embodiment, the memory may include ROM for use at boot-up, and DRAM for program and data storage for use while executing programs.
(52) The mass storage device may include any type of storage device configured to store data, programs, and other information and to make the data, programs, and other information accessible via the bus. The mass storage device may include, for example, one or more of a solid state drive, hard disk drive, a magnetic disk drive, an optical disk drive, or the like.
(53) The video adapter and the I/O interface provide interfaces to couple external input and output devices to the processing unit. As illustrated, examples of input and output devices include the display coupled to the video adapter and the mouse/keyboard/printer coupled to the I/O interface. Other devices may be coupled to the processing unit, and additional or fewer interface cards may be utilized. For example, a serial interface such as Universal Serial Bus (USB) (not shown) may be used to provide an interface for a printer.
(54) The processing unit also includes one or more network interfaces, which may include wired links, such as an Ethernet cable or the like, and/or wireless links to access nodes or different networks. The network interface allows the processing unit to communicate with remote units via the networks. For example, the network interface may provide wireless communication via one or more transmitters/transmit antennas and one or more receivers/receive antennas. In an embodiment, the processing unit is coupled to a local-area network or a wide-area network for data processing and communications with remote devices, such as other processing units, the Internet, remote storage facilities, or the like. The network interface may be configured to have various connection-specific virtual or physical ports communicatively coupled to one or more of these remote devices.
(55) Illustrative embodiments of the present invention have the advantage of providing techniques for designing LLC converters that operate within a specific range of switching frequencies in order to reduce interference from electromagnetic signals and to switching losses and component size. In some embodiments, the use of spreadsheet software tools allow LLC converter designers to rapidly calculate appropriate inductance, capacitance, and turns ratio values. Other embodiment systems may use, for example, EDA software tools that allow designers of electronic systems to design and analyze LLC power converters as an integral part of the design flow for an entire semiconductor chip.
(56) While this invention has been described with reference to illustrative embodiments, this description is not intended to be construed in a limiting sense. Various modifications and combinations of the illustrative embodiments, as well as other embodiments of the invention, will be apparent to persons skilled in the art upon reference to the description. It is therefore intended that the appended claims encompass any such modifications or embodiments.