A DC to 3-phase series-resonant converter with low harmonic
distortion
Citation for published version (APA):
Huisman, H., & Haan, de, S. W. H. (1985). A DC to 3-phase series-resonant converter with low harmonic distortion. IEEE Transactions on Industrial Electronics, 32(2), 142-149. https://doi.org/10.1109/TIE.1985.350185
DOI:
10.1109/TIE.1985.350185
Document status and date: Published: 01/01/1985 Document Version:
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A DC
to
3-Phase
Series-Resonant
Converter with
Low
Harmonic
Distortion
H. HUISMANANDS. W. H. DE HAAN
Abstract-A type of dc to 3-phase series-resonant converter (s.r.-converter) for potentially submegawatt industrial applications is pre-sented. The converter provides variable-frequency sine-wave currents, with low harmonic distortion at the output terminals, and with the frequency ranging from-200 throughdc to +200 Hz.The converter can transfer power in both forward and reverse power-flow directions to almostany typeof load circuit. Themethods of controlareformulated suchthattheycanbeimplemented easily with high-speed logical circuits. Testresults fora1-kW demonstration converter aresupplied.
I. INTRODUCTION
DURING the last decadethe interest in electrical
wind-en-ergy conversion has increased significantly. Thisattention concerns both the generation of autonomous multiphase ac
grids,as well as the delivery of power toexistingutilitygrids.
To carryoutthe electricalconversionprocess,oneoftenuses a
cycloconverter or a cascaded ac-dc and dc-ac converter. The dc to3-phaseconverterpresentedinthispaper isconsideredas an intermediate step in the development of a novel type of 3-phase-to 3-phasecycloconverter.Apart fromwind-energy con-version this converter canbe appliedtootherareasof
technol-ogyincludingpowergenerationandvariablefrequency-machine driving.
Fundamentals of dc to 3-phase ac power conversion have been known for many decades. Because of the simplicity of control and the clarity of insight into the method of opera-tion, some of these systems, such as the load-commutated bridge inverter, the square-wave inverter, and the
high-fre-quency pulsewidth-modulated inverter,arewelldeveloped [1]
andwidelyspread. The advantages of these systemsare,
how-ever,countered byoneor more of thefollowing disadvantages:
1)the stress on electronic switches is high due to forced
commutationtechniques,
2)heavy and costly filters are required to remove the
low-frequency harmoniccontentof the electricalwaveforms,and
3) thepowerfactorispoor and cannotbe controlledfreely. The s.r.dcto3-phaseacconverterpresented,whichisbased
on aconceptpresented by Schwarz [2],doesnotpossessthese
disadvantages. Moreover, the system has thecommonfeatures of series-resonant converters (s.r.-converters) such as, 1) the system isinherently short-circuit proof, 2) the sizeof the
sys-tem is smallduetothehigh internal frequency,and 3) the
sys-tem is capable ofcontrolling and turning off power bya
frac-tion ofa millisecond. The technology of the single-quadrant
Manuscript receivedSeptember, 1984.
The authorsare with the DelftUniversity ofTechnology, Mekelweg4,
2624,CDDelft,TheNetherlands.
ipt
pPI1PIIPIPPII11111 I I I IiIiiil I i ilIIIlI I I P
TTP
t-iqt I ili I I II h Ii i liifi
irt~~P1~~~~PPbP1i||1111|l1PP 'I'i UFPI IF IGwF1w|1
Fig. 1. Example ofthe distributionofthe currentpulses in theresonant
currenti1overthe line currentsip, iq,andi4.
dc-dc s.r.-converter has been well established by now and
manyauthors have discussed thesubject [3] -[6].
Sincethe beginning of theeighties attemptshave been made
to breakthroughtothedevelopment ofacandmultiphase s.r.-converters. Some successful experiments of ac-dc
s.r.-con-verters were reported by Schwarz [7], [8].Recently, a single-phase dc-ac converter has been presented [9]. The
30-dc
(3-phase to dc) s.r.-converters described up to now [7],[8]
do, however, extract currents from the power grid which aresimilar to the currentswhich areextracted by a3-phasediode
rectifier. These square-wave-like currents cause harmonics in the supply lines, while thepowerfactoristheoretically limited
to0.955 [8].
From a fundamental point of view, the s.r.-converter is
capableofdealing withmultiphaseacpowerina more sophisti-cated way [2].A s.r.-converter canbe consideredas anetwork
whichgenerates an array ofcurrentpulsesat ahighfrequency
(5-50 kHz). Byproperly distributing the pulses from this high-frequency carrier over the 3 lines of the grid, it is possible to generate current waveforms, which do contain one single fre-quency in the low-frequency range (<3 kHz).Theprinciple of the process is illustrated in Fig. 1, where resonant current
pulses are represented by impulses. Fig. 1 is obtained from a
simulation program, which operates similarly to the one
de-scribedin
[10]
.Thehigh-frequency contentofthe outputcur-rent is removed by a relatively small filter, with the result
being a low-frequency phase current with low harmonic
dis-tortion. The pulse distribution process can be applied bothto
30-dc
convertersaswell astodc-34
converters.Inthis paper a dc-30converter is described whichisbased
on the above principle. The converter is capableof generating
a 3-phase output waveform with frequencies rangingfrom ca
+200 via 0to-200 Hz(phase reversal).Moreover, the conver-ter can beconnectedtoleadingaswellaslaggingloads(+
1800
to -180°),both linear and nonlinear, inboth the forward and
0278-0046/85/0500-0142$01.00 © 1985 IEEE
i1
t I 11i tI I I I i I I i i I iI k i I I I 11i Ii I I I II I I I iI I i Ireverse power-flow directions. The critical points thatcan be identifiedin the system design of the dc-34 converter are: 1) the pulse-distribution algorithm (line selection), 2) the
algo-rithm for the selection of particular switches in the selected lines (switch selection, and 3) the method of control to guarantee thyristor turnoff and continued oscillation (Vs-control). The method of controlis in accordance with a
con-trolmode, which isdescribed in acompanion paper [11].The
theory is verified ona small-scale (1 kW) demonstration con-verter.
II.PROPERTIES OFTHEGENERALIZED DC-DC
S.R.-CONVERTER
The operationmodesofthe
dc-30
s.r.-converter isbased onthe principles of the dc-dc s.r.-converter, which is treated in
literature [3]-[6],
[11]
, [12]. Toenable greaterinsight, someproperties of the dc-dc s.r.-converter will be reconsideredina
nonorthodox manner. Fig. 2 shows the basic, generalized dc-dc s.r.-converter. The input switch matrix consisting of
switches QA and QB connects the resonant circuit to
+E,
or-E5,
where E is the dc source voltage. The output matrix consisting of switchesQC
and QD connects the resonantcir-cuit to +V0 or -VO. By appropriate control of the switch
matrices a bipolar voltage, compounded of square waves, is
generated across the resonant circuit, thus inducing a
reso-nant current of thewell-knownshape(Fig.3(a)). In thispaper the resonant current is consideredas a seriesofcurrentpulses. The time ofinitiation of theKth current pulse is denoted by
ak, where : is the normalized time defined
by
:=t/<LI
C1.The current gap which is not present in most dc-dc
con-verters is a prerequisite in ac-converters for the purpose of
commutation and control
[11]
.Dependingontheapplication,the switches are implemented as single diodes or as combina-tions of diodes and/or controllable switches suchasthyristors
andMOSFET's.Inmultiphaseconvertersallsymbolicalswitches shouldbe implemented asthyristors. Althoughthemultiphase
converter does not contain diodes, we will stick to the term
"diode current" foreach firstcurrentsegmentfollowinga cur-rent zero crossing; the second current segment will be
desig-nated as "thyristor current". TheKth event betweenthe time
fk and fk±1 willalso be referred toastheKthconverter
cycle.
It is well known that a number ofswitching modes canbe
distinguished for the generalized s.r. dc-dcconverter
[4],
[11].It will be shown that all switching modes have the following
properties in common:
1) the diode current is (at least) opposed by the highest
terminal voltage (this follows from the commutation
condition),
2) the thyristor current at the high-voltage side extracts
power from that source (this follows from the power
balance),and
3) both diode and thyristor currents on the low-voltage
sidetransferpowerinthe desired direction.
Conversely, one may state that if the above rules are obeyed,
one can transfer power in any desired direction in any
com-binationofinputandoutputvoltages.
The statements are based on the
following
considerations.EsQ4
j
j)Vo
aB
Wl04A
Fig.2. Basic schematic and thedefinitionof thevoltagesandcurrents ina
generalizeds.r.dc-dcconverter.
Suppose that in thesymbolic converter from Fig. 2, the source
voltage Es and the outputvoltage V0 are both allowed to be
positive or negative. In either an input or an output line the
current will be prescribed by some reference. The desired
power direction is defined by the sign of thisreference cur-rent and the sign of the actual voltage at the associated port. As stated before, a resonant current phase consists of a diode
current and a thyristor current. QD andQT aredefinedasthe charge transferred bythe diode and the thyristor current,
re-spectively. Both QD and QT are defined such that they are
always positive. The input and output matrices facilitate QD
and QT being routed in any desirable directionon input and
output terminals.
If one bears in mind that the energy transferred by a cur-rent in a certain interval is equal to theproduct of voltage and transferred charge, it follows from considering theenergy bal-ance applied to the input and output port ofthe converter
(Fig. 2)
ES(QDSll
+QTS1 2)
=VO(QDS21
+QTS22)-
(1)Here
SI1
to S22 indicate in which direction the charge flowson input and output, so
Si1
iseither +1 or -1. Note that (1)is valid under nonsteady-state conditions, provided that
v,p(k)
=vcp(k
+ 1) and that both E and V0 are constant duringthecycle considered.From(1)itfollowsthat
QD
S¾2Es-S22Vo
QT
S11Es
-S21 Vo
(2)Because both QD and QT are positive, the sign ofthe left-hand term is negative. To satisfy (2), the coefficients
Si,
and Si2 of the highest voltage, either Es or VO, should be opposite in sign. On the low-voltage side bothSji
and Sj2 areunconstrained, so that they are chosen such that the power is transferred in the desired direction. For a proper commuta-tion from the diode to the thyristorcurrentthe diode current is required to be opposed by the highest voltage. By way of
example Fig. 3(b) shows the resulting current waveforms of
isandio,if
Es
>0,Vo
> 0,Es
<Vo
andioref < 0. The elaboration of the switch selection mechanism in thedc-30 converter presented is primarily based on the previous discussion. The basic diagram of the power network of the
converter is depicted in Fig. 4. The switches symbolize ap-propriate electronic switches such as antiparallel thyristors.
(a)
is!
Pkf:
T
(b)
Fig. 3. (a) Resonantcurrentwaveform forconverterswithacurrent gap.(b) ExampleofsourceandloadcurrentsinaconverterwhenEs>0,V0 >0,
IEst < IV,1 andi,.f < 0.
vc
Fig.4. Basicschematicofthepowernetwork ofadc-3 s.r.-converter.
In essence, the multiphase-converter operation is based ona
selection mechanism which, for any converter cycle, selects twoout of three output linestocarrycurrents. Theparticular implementation of this line-selection mechanism will bU dis-cussed later. For our present considerations it is importart to note that once one ofthe three output lines has been
ex-cluded from current flow, during this particular converter
cycle, the converter can be treated as a generalized dc-dc converter.
A.BasicRequirements
Prior to describing the control and selection mechanisms,
we formulaterequirementswhich the ac-converterhastomeet. Theconverter should be abletoinject currents inanyarbitrary
active or passive output circuit. These currents will often be
sinusoidal ofshape. The size and shape ofthe voltages at the output terminals depend on the character ofthe load and the
shape of the injected currents. The amplitudes of the output
voltages are allowed to be greater as well as smaller than the source voltage. For that reason the converter should be able to transfer power to a lower as well as to a higherterminal
voltage. Moreover, because the load may require reactive
power, the instantaneouspower should be allowed to flow in both directions. The output capacitors of the converter are
sufficiently large
tojustify
the assumption that theoutput
voltage
is constantduring
a converter cycle, althoughtheout-put voltage is essentially a low frequency ac-voltage. One should bear in mind that the output capacitors are intended
to remove the high-frequency content (order 10 kHz) from theoutputwaveform.
Concluding,
it is evident thatduring
each convertercycle
the
multiphase
converter should be able to operate as a gen-eralizeddc-dcconverter.B. The
Principal
Functions and BlockDiagram
To operate as a dc-dc converter during a converter
cycle,
it is necessary to select for each convertercycle two lines on
the ac side. Two out of M lines have to be selected for an
M-phase
converter. This line-selection process and the associ-ated pulse-distribution process is controlled by the actual measured output currents im(m = p, q, r) and by therefer-ences for the output current imref. The selection
circuit,
which is of theintegral-pulse-controller type [11],[13
[14]is symbolicallyindicated in the lower left of the blockdiagram
in
Fig.
5. The line-selection block also generates a signal pwhenever a current pulse should be initiated to bringone of theoutputwaveforms in accordance with the reference.
After twogridlineshave been selected, it is theknownby
measurements, to which actual input and outputvoltagethe
dc-converter will be connected. The appropriate information
is passed via a multiplexer to the switch-selection logic. The
switch-selection logic, in the middle of Fig. 5, determines
from the signs of the passed signal and from the state ofthe
converter (diode cycle, thyristor cycle,orgap)which switches have to be closed during the following converter subcycle.
Four out of20switches have tobe selected.Thisinformation
is passed to the latched thyristor pulse generators whenevera p-signal is issued during a current gap or when a cs (change
state) signalisissuedbytheso-called VJ-peakpredictor. Essentially, thep-signal initiatesthe turnover from the cur-rent gap to the diode current, while the cs-signal initiates the
turnover from the diode currenttothethyristor current. The
vup-predictor
generates a cs-signal whenever this cir-cuit predicts that the resonant capacitor voltage will be at aspecified reference levelatthe end of the convertercycle. C. Switch-Mode Selection
Once a pair of terminalshas been selected, an appropriate andunique setofswitchescanbedesignated.
Explicitly, the switch-selection process for the diode and the thyristor cycle, respectively, will be explained with
refer-ence toFig.2.
1) Diode Cycle: Based on the sign of thecapacitor voltage
vC at time
Ok,
it is known in which direction the resonant cur-rent will flow during the following converter cycle. As statedbefore, the diode current should at least be opposed by the highest terminal voltage (Es or VO)- So, if one measuresE,
V,
and vu, one can straightforwardly designate two switcheson the "high-voltage side" which have to be closed. On the
then sign
(i,)
=-sign(VO)and sign(i5)=sign(. ,)
sign(Es) (6)
Fig. 5. Blockdiagramof the controller for the dc-34 s.r.-converter. The PIC and the
Vp-predictor
doprocess analogsignals. All other circuits process booleans.desired power transfer direction, defined byIoref Uo,is
satis-fied.
So,if
I
VO
I
<Es
then sign
(i,)
=sign(ioref)andsign
(is)
=-sign(Es)andif
I
VO
I>I
then sign
(io)
=sign(VO)
If the signsofE, VC,
'oref,
andv, are determined, the ap-propriate switches can bedesignated easily from (3) to (6). D. Line SelectionIn the following section it isassumed that a s.r.-converter should feed an M-phase network with ac power. For the pur-pose of driving machinery, it is suitable if the converter be-haves like a multiphase current source, although for multi-phase power generation avoltage-source character is more ap-propriate.The line-selection mechanismwill be explained with respect to a current-source character. The multiphase
con-verter should be controlled such that the current im in line
m (m =
1,
2, **, M) is a replica ofa reference current imref(m = 1, , M). The reference current in lines 1, ,M-1
can be chosen freely; the reference current in line Mfollows from
m
Y,
imre6f-°m=l
(7)
The current waveform synthesis is based on the concept of pulse-integral control [11],
[121.
In a dc-dc converter the resonant currentil
is measured, subsequently rectified and compared to areference iref. The errorsignal(li1
-ii'f)
is fed to an integrator. Whenever the integrator outputec
ex-ceeds some threshold eT, the power switches are actuated, thus generating another current pulse. When two successsivethreshold crossings are denoted by ta and tb, the following
holds: sign
(ioref
VO)
andsign
(is)
= sign (Es)
sign(Es)
If the directions of
is
andio, areknown,and if the direction ofil
isknown,
a unique set of fourappropriate thyristors
canbedesignated. Note that sign
(ij)
in the Kth cycle follows fromsign(vc(f3k)).
2)Thyristor Cycle: The current direction on the
low-volt-age side occurs during the
thyristor
cycle
such that thede-sired
power-transfer
direction is satisfied. On the high-volt-age side the direction of thethyristor
currentisopposite
tothat of the diodecurrentonthat side. So, if
VO
<EsI
then sign
(io)
=sign(ioref)andsign
(is)
=sign(Es)
(5)
and, if
VO
I
>I
EsI
Itb
(4)
(io-
iref)dt=0.
ta
(8)
For dc and single-phase converters,ta and tb coincide with the beginningoftwosuccessive convertercycles.
For normal unipolar dc-dc s.r.-converters the
implementa-tion of the pulse-integral controller
(PIC)
for the outputcur-rent io is relatively simple because
i4
= lii In multiphaseconverters only twolines are served during a converter cycle.
For that reason (8) is implemented such that the interval
(ta,
tb) effectively spans several cycles. This implies that during
each cycle alimited error occurs for each line.Moreover, the implementation should be modified such that the PIC can
handle both positiveandnegative
valuies
ofil
andiref.Fig.6(a)gives the implementation of one of the M-1 PIC's and
Fig.
6(b) shows the associated waveforms. Whenever theintegrator output
e.
gets into one of the arced areas, a pulse-requestsignalPm isgenerated.
The gap between the comparator levels is intended to pre-vent the immediate generation of a pulse request whenever
the reference signal changes
polarity.
IfA=0,thisundesirable(a)
imreff
ect
lint
(b)
Fig. 6. BipolarPICforline m. (a)Schematic diagram.(b)Signals that may occuratthetimethat the reference signali7Jrefisreversingpolarity. Note thatattimet4 apulserequest that is issued by another line is served.
be slightly larger than the integrator swing during a current
pulse, although this is not critical. Note that signal P only
in-dicates that line m requests a currentpulse. It does not
indi-cate inwhich direction the currentpulse should flow intothe line.
All lines are equipped with individual PIC's and the
pulse-request signals are logically OR'ed. When a pulse request is
issued, the next converter cycle will be generated. The line that issues the request willtake part inthe oscillationandthe
current will flow inthat line inthe directionof theassociated reference. Next asecond line that will take partinthe
oscilla-tion should be selected. Only those lines whose sign of the
reference current isopposite the reference signofthelinethat
issues the pulse request are considered. Ifmore than one line
satisfies this requirement, a line is selected whose integrator
output is closest to the associated threshold level. Note that the line selectionprocess described above is based fora great part on two-state logic, whichcanbeimplemented easilywith
digitalelectronics.
After two lines on the ac side have been selected, the con-verter can further be considered as a generalized dc-dc con-verter. For this specific dc-dc converter, the voltagebetween the selectedlinewillbedesignatedasoutputvoltage
V',
while the output current inthe linethat issuedthepulserequest will bedenotedbyi,
The further selection ofswitchesiscarriedout asdescribed
intheprecedingsection.
During the servicing ofa pulse-request, i.e., thegeneration
of a current pulse, the pulse-request signal will inherently be cleared duetothe integratoraction.
E.
VJ-Control
One of the most critical pointsin multiphase convertersis
the choice of the firing-angle control module. This control
module should be chosen such that thyristor turn-off
condi-tionsand uninterrupted converter operation areguaranteed.
In a companion paper [11],acontrol module hasbeen
pre-sented which guarantees continuous oscillation, in particular
under dynamic conditions and at abrupt changing source and load voltages as occurring in multiphase converters. This
con-trol module maintains the capacitor peak voltage at a prede-scribed level
Vcpref,
whichshouldbeatleasttwicethehighestterminal voltage.
Duringthe diode interval following
1k,
the circuitcontinu-ously generates a real-time prediction of
vup(k)
accordingtothefollowing formula [11]:
vcp(k)=U1 - U2 + {(U1 -
U2-VC())2
+(Zlil)2
}11
2(9)
where
U1
and U2 correspond to either+E,
or-E,
and+±V
or -VO, depending on the current flow direction through thesourceand loadintheinterval considered.Atatime
(,
thepre-diction wouldbevalidif thecircuit were to turn overfrom the diode to the thyristor cycleatthat time.So wheneverthe
pre-dicted value crosses thereference value Vcpref, the turnover is
actually initiated. The beginning ofaconverter cycle at time
(k isinitiated by thelogically oR'edpulse requestsignals. Asdiscussedin [ 1],thecontrol module providesa method of independent control of the average current and capacitor
peak voltage. Note that the time betweenthe terminationof a
thyristorcycleandtheinitiationofthe nextdiodecycle should be larger than the thyristor turnoff time tq. Protection cir-cuitry is providedto delay the initiation ofa diode cycle ifa
pulse-request signal is issued before the associated thyristors
haveturned off.
Because the charge which is transferred by the resonant circuit ina converter cycle islimited to 2
vcpl,C
thisdoes infact signify that theconverterinherently hasacurrentlimiting character.
III.
VERIFICATIONThe proposed algorithmsandtheassociated electronicswere
tested on a 1-kW demonstration converter whichhad the fol-lowingspecifications (referto Fig.4):
sourcevoltage
maximuminverterfrequency
peak capacitorvoltage
maximumallowable output voltage resonantcapacitor
resonant inductor input filter capacitor
output filter capacitors
power at full load
Es
=120V dcfi
= 10kHz Vcp =350VVomax=
170VC1
= 1.11 pF L1 = 146,uHCs
=50MF
CO
= 50,F
PO
= 1 kWThe electronic switches are implemented with 10 pairs of
Fig. 7. Pulse-distributionprocess at a lowoutput frequency. Uppertrace:
resonant currentca, 40 A/div. Lower traces: unfilteredlinecurrents, 50 A/div, 100 ps/div.
The converter was primarily intended to demonstrate the
most important features of the
dc-30
s.r.-converter such asharmonic distortion, power factor regulation and load
inde-pendence. Optimizing the performance with respect to
ef-ficiency and size was not a goal,
although
a maximumef-ficiency of 85 percent was established. The relatively high
losses are due to the low source voltage in combination with the oversized power network.
Fig. 7 shows the resonant current and the unfiltered output currents at a relatively low linefrequency. Note the difference
in shape of the current pulse inthelinesp andq, whichis due
tothe fact that Vpr< Eswhile Vqr>
E,
Fig. 8 gives an impression of the pulse-distribution
mecha-nism. Simultaneously, it isshown that the capacitor peak
volt-age ismaintained within 10 percent at a constantlevel.
The filtered and unfiltered currents in line p are shown in
Fig. 9. The frequency of the reference current isapproximately 60 Hz. From the
frequency
spectrum ofFig.10(a)
it can be concluded that theharmonic distortion of the filteredline cur-rent is extremely low. The 3rd, 5th, and 7thharmonicsare atleast 40 dB below the 100-Hz fundamental component. For comparative purposes, the harmonics of a line-commutated
converter are indicated in the same graph. The difference is
self-explanatory.
As stated in relation to (7), two reference currents can be chosen independently. For the purpose of examining the cross
distortion between lines, a frequency spectrum (Fig. 10(b))
was recordedforaconditioninwhich line p generated a 100-Hz
sinoid, and line q a 130-Hz sinoidal current. The cross
distor-tion is approximately -25 dB. Notethat the 3rd, 5th, and 7th harmonics have disappeared from the graph. The "grass" at -60 dB between the harmonics is due to the more or less stochastic character of the unfiltered line current, which is
rooted in the fact that the inverter cycle is not synchronized withthe ac-cycle. From the lastgraphitmay beconcluded that the converter presented canbeconsideredas a
multiphase
cur-rent amplifier. Any arbitrary current
iref
can be reproducedin theoutputline.
To investigate the ability of the converter to feed currents
in nonlinear and active loads, two test circuits were set up. In the firstcircuit theconverterwasconnectedto anasynchronous machine. The converter was able to accelerate and decelerate
the machine in both rotation directions. When the axis of the machine was connected to a mechanical drive, it was possible
Fig. 8. Sinusoidal (200 Hz) modulated output currents. Upper traces: unfiltered line currents 50 A/div. Lowertrace: resonant capacitor voltage ca, 700V/div.
Fig. 9 Sinusoidal (60 Hz) modulated currents in line p. Upper trace: unfilteredcurrentinlinep, 50 A/div. Middle trace:filtered current in line
p, 10A/div. Lowertrace: reference for line p, 2ms/div.
to use the machine as a generator, thus transferring power to
the dc "source"
E,
The reactive power for the machine was inboth casessuppliedby theconverter.In the second-setup theconverter wasconnected via a
trans-former to the 3-phaseutility grid. In order to test the ability of the converter to supply current independent of the actual output voltage, a 33 1/3-Hz
30
reference was phase lockedtothe 50 Hz grid, forcing the converter to supply a 33 1/3-Hz current. The filtered output currents, shown in Fig. 11, arise
from a superposition of the 33 1/3-Hz converter current anda
50-Hzcurrent, which iscaused by the connection of the con-verter filtercapacitors to the grid.
IV.CONCLUSIONS
A
dc-30
s.r.-converter is presented which has a combination offavorable properties comparedto other types ofmultiphaseconverters.
Thesepropertiesinclude:
low sizeand weight ofthe converter;
lowharmonic distortion ofthe generatedcurrents;
ability to generate low-frequency ac currents(up to several hundredsofHz) of any arbitrary shape;
abilityto feedcurrents to almostany typeofloadincluding existingutility grids,machinery and passive loads;
potential abilitytoprocesshundreds of kW of power with an
efficiency ofmorethan 90 percent;
high speed of reaction;
inherently short-circuit proof; and bothforward and reverse power flows.
_ 3-phase AC 105 Hz spectrumof i p 1 - 1 = p q pq- qr r = 12.5 A r u = 75 V rp fifth harmonic of a LCC
---
--_I- -
iffiLIILIIIIL_-100 200 seventh harmonic of a LCC 300 400 500 600 700 800 900 Hz (a) OdE - - - -.~~~~~~~~~~~~~~~~spectrum
of dBdd
t~~~~~~~~~~~~~~~~~~~
A;
100qHz
S -10 5 A; 130 Hz -20 -30 -40 --f---- -. --80 -100 200 300 400 500 600 700 800 900 (b)Fig. 10 Frequency spectra of the line currents. (a) Spectrum of i,; the reference for linepisa 100-Hz sinoid. (b)Spectrum ofi,;thereferences for thelines p and qare100- and 130-Hz sinoids, respectively.
Fig. 11 Filtered load currents in lines p and q when the converter is
connectedtoa50-Hz3-phasegrid andwhilethe current referenceis set to 33 1/3 Hz. Uppertrace: i, , 10 A/div. Middle trace: Vpq, 100 V/div.
Lowertrace: if, 10A/div; 10 ms/div.
a dB -10 -20 -30 -40 -50 -60 -70 -80 0 F 0 Hz
The properties of the converter are rooted in
combining
a well-known s.r. power networktopology
withanovel method of preserving the energycontent of theconverter(vp
-control),and ofdistributing currentpulsesovertheoutput lines.
REFERENCES
[1] J. M. D. Murphy, ThyristorcontrolofACmotors. New York: Pergamon, 1973.
[2] F. C. Schwarz, "A doublesided cycloconverter,"IEEE Trans. Ind. Electron. Instrum.,vol. IECI-28,pp.282-291,Nov. 1981. [3] ,"Animprovedmethod ofresonant currentpulsemodulation for
powerconverters," IEEE Trans. Ind. Electron. ControlInstrum., vol.IECI-23, pp. 133-141, May1976.
[4] F. C. Schwarz and J. B. Klaassens, "Acontrollable 45-kW current sourcefor DCmachines,"IEEETrans.Ind.Appl.,vol.IA-15,pp. 437-444,July/Aug. 1979.
[5] R. J.Kingand T.A.Stuart, "Modellingthefull-bridgeseries-resonant converter," IEEE Trans. Aerosp. Electron. Syst., vol. AES-18, pp.449-459,July 1982.
[6] V. Vorperian and S. Cuck, "Acomplete DC analysisof the series-resonantconverter,"presentedattheIEEEPowerElectronics Special-istsConf.,(Cambridge, MA),June1982.
[71 F. C. Schwarz and W. L. Moize de Chateleux, "A multikilowatt
polyphaseAC/DCconverterwithreversible power flow andwithout
passivelowfrequencyfilters,"presented atthe10thIEEEElectronics
SpecialistsConf. (SanDiego,CA), June1979.
[8] F. C. Schwarz and J. B. Klaassens, "A controllable secondary
multikilowatt DCcurrent source with maximum power factor in its three phase supply line," IEEE Trans. Ind. Electron. Control
Instrum. vol.IECI23,pp. 142-150, 1976.
[9] J.B.Klaassens,"DCtoAC series-resonant converter system withhigh internalfrequencygeneratingsynthesised waveforms formultikilowatt powerlevels," presented at the IEEEPower Electronics Specialists
Conf., (Gaithersburg, MD),June1984.
[10] R.J.Kingand T. A.Stuart,"Alarge-signaldynamic simulation for the series-resonant converter," IEEE Trans. Aerosp. Electron. Syst.,
vol.AES-19,pp. 820-829, Nov. 1983.
[11] S. W. H. de Haan and H. Huisman, "Novel operation and control modes forseries-resonant converters," IEEE Trans. Ind. Electron.,
pp. 150-157,thisissue.
[12] F. C. Schwarz and J. B. Klaassens, "A reversible smooth current sourcewith momentaryinternalresponse fornon-dissipative control of multikilowattDC-machines,"presentedatthe IEEE SummerMeeting PowerConf., (MN), 1980.
[131 F. C. Schwarz, "Engineering information on an analog signal to discrete time intervalconverter,"NASACR-134544, 1973.
[141 S. W. H. de Haan, "A new integral pulse module for the
series-resonantconverter,"IEEE Trans. Id.Electron., vol. IE-8, pp.