A ZVS PWM Inverter With Active Voltage Clamping Using the Reverse Recovery Energy of the Diodes.pdf

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IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS—I: REGULAR PAPERS, VOL. 52, NO. 10, OCTOBER 2005
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A ZVS PWM Inverter With Active Voltage Clamping
Using the Reverse Recovery Energy of the Diodes
Marcello Mezaroba, Denizar Cruz Martins, and Ivo Barbi
Abstract— This paper presents a zero-voltage-switching (ZVS)
pulsewidth modulated inverter with active voltage clamping using
only a single auxiliary switch. The structure is particularly simple
and robust. It is very attractive for single-phase high-power appli-
cations. Switching losses are reduced due to implementation of the
simple active snubber circuit that provides ZVS conditions for all
switches, including the auxiliary one. Its main features are: simple
modulation strategy, robustness, low weight and volume, low har-
monic distortion of the output current and high efficiency. The
principle of operation for steady-state conditions, mathematical
analysis and experimental results from a laboratory prototype are
presented.
Index Terms— Active clamping, inverters, soft commutation.
Fig. 1.
Proposed circuit.
I. I NTRODUCTION
M UCH effort has been exerted by researchers all over
widely known is the Undeland snubber [1]. This snubber pro-
vides good performance in the majority of its applications, but
is not capable of regenerating the energy lost in switching. To
try to minimize these losses, some works have considered mod-
ifications to the Undeland snubber, aiming at the regeneration
of the energy lost in switching [2]–[4] and [5]. The active solu-
tions are already distinguished by the use of controlled switches
to obtain soft commutation. The main ones are those that use
conventional pulsewidth modulation (PWM), without the need
for special control circuits. One of these works is the auxiliary
resonant auxiliary resonant diode pole inverter (ARDPI) [6].
This topology matches the use of PWM modulation, with the
soft switching attained through a relatively simple circuit. On
the other hand, it needs a high current circulating in the circuit,
about 2.5 times the load current, raising the current stress in
the switches. A topology very similar to the previous one is the
auxiliary resonant pole inverter (ARPI) [7]. Theoretically, this
circuit reduces the current levels necessary for switching, but
it involves a complex control strategy. Another circuit found
in literature is the auxiliary resonant commutated pole inverter
(ARCPI) [8], [9], and [10]. This inverter has auxiliary switches
that are only turned on when the load current is not sufficient to
effect the soft switching, causing the control circuit to become
very complex and dependent on the sensors.
Recently, some research was carried out using the reverse re-
covery energy from the diodes to obtain soft commutation in the
switches of the pre-regulated rectifiers with high power factor
[11] and [12].
In this paper, a zero-voltage-switching (ZVS) PWM inverter
with voltage clamping across the switches, using only a single
auxiliary switch, is presented. The proposed structure uses the
diode reverse recovery energy technique to obtain soft commu-
tation in all switches, such as the rectifier shown in [12].
the world in an attempt to reduce harmonic distortion
and audible noise in the output of inverters. Their objectives
have been attained through an increase in inverter commutation
frequencies and an appropriate modulation strategy. These
measures have provided some benefits, such as a reduction in
the weight and volume of the magnetic elements. However,
they have caused some difficulties due to the high commutation
losses in the switches and the appearance of electromagnetic
interference. These factors occur mainly in inverter topologies
that use the bridge inverter configuration. At the moment that
the main switch turns on, the anti-parallel diode of the bridge
complementary switch begins its reverse recovery phase.
During this stage, the switches are submitted to a high current
ramp rate and a high peak-reverse recovery current .
Both contribute significantly to increasing the commutation
losses and produce electromagnetic interference.
To solve this problem, diverse works have been developed
by the scientific community in recent years and can be divided
into two groups: passive techniques and active techniques.
The passive techniques are characterized by the absence of
controlled switches in the switching aid circuit, while the active
techniques are characterized by circuits that use controlled
switches.
Among
the
passive
solutions,
perhaps
the
most
Manuscript received May 28, 2004; revised September 15, 2004. This paper
was recommended by Associate Editor A. Ioinovici.
M. Mezaroba is with the Power Electronics Laboratory (LEPO), the State
University of Santa Catarina (UDES), 89223-100 Joinville, SC, Brazil (e-mail:
mezaroba@joinville.udesc.br).
D. C. Martins and I. Barbi are with the Power Electronics Institute (INEP),
the Federal University of Santa Catarina (UFSC), 88040-970 Florianópolis, SC,
Brazil (e-mail: denizar@inep.ufsc.br; ivobarbi@inep.ufsc.br).
Digital Object Identifier 10.1109/TCSI.2005.852914
1057-7122/$20.00 © 2005 IEEE
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IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS—I: REGULAR PAPERS, VOL. 52, NO. 10, OCTOBER 2005
Fig. 2. Operation stages. (a) First state (t0-t1). (b) (b) Second stage (t1-t2). (c) Third stage (t2-t3). (d) Fourth stage (t3-t4). (e) Fifth stage (t4-t5). (f) Sixth stage
(t5-t6). (g) Seventh stage (t6-t7). (h) Eighth stage (t7-t8). (i) Ninth stage (t8-t0).
II. P ROPOSED C IRCUIT
. At the end of this stage, the current through inductor
reaches its maximum value,
(Fig. 3)
The proposed circuit is shown in Fig. 1. It presents a
half-bridge inverter configuration, where are the main
switches. The snubber circuit is formed by one switch ,
one small center-tapped inductor and one capacitor
. , and are the commutation capacitors. Capacitor
is responsible for the storage of the diode reverse recovery
energy and for the clamping of the voltage across the switches.
Inductors and are responsible for the control of the
during the diode reverse recovery time.
(1)
(2)
(3)
(4)
(5)
This stage was chosen to initiate the converter analysis because
it precedes the commutation process of the main switch,
,
during the half-cycle of operation. At time t0 current
becomes positive and increases linearly. At the end of the
first stage this current is responsible for the soft commutation
process of .
Second Stage (t1-t2): This stage starts when auxiliary switch
is blocked. Current
III. O PERATION S TAGES ( FOR F IRST H ALF -C YCLE )
To simplify the analysis, the following assumptions are
made: the circuit operates in steady state; the components are
considered ideal; the voltage across capacitor
and the cur-
charges capacitor
from zero
rent through the output inductor
are considered constant
to
, and discharges
from
to zero .
during the switching period.
In the following paragraphs, the operation stage (Fig. 2) of
the first positive half-cycle of the output current is described in
detail.
First Stage (t0–t1): At t0, switch is turned on. During
this interval, the output current, , is delivering energy to
source via diode . At the same time, additional current
circulates through the mesh, formed by
. During this stage the current,
, circulates through
the intrinsic capacitor of switch
(6)
where
is the maximum current through
. Thus
, and
(7)
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MEZAROBA et al. : ZVS PWM INVERTER WITH ACTIVE VOLTAGE CLAMPING
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Fig. 3.
Main waveforms.
(8)
of diode
. The auxiliary inductors limit the reverse recovery
(9)
(16)
(17)
(18)
(10)
Third Stage (t2-t3): At t2, the voltage across reaches zero
and is clamped by diode . At this moment, the voltage
is applied across inductors
(19)
and
and currents
and
decrease linearly. In this stage, switch
must
(20)
be turned on
Fifth Stage (t4-t5): This stage starts when diode
stops
(11)
(12)
(13)
conducting. Current
begins charging capacitor
from
zero to
and discharging
from
to zero
(21)
(14)
(22)
where
.
where
is the maximum negative current through
. So,
(15)
Fourth Stage (t3-t4): This stage begins when current
inverts its direction and flows through switch . The turn-on
occurs at zero voltage. Current continues to decrease until
inverting its direction, which begins the reverse recovery phase
(23)
(24)
(25)
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IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS—I: REGULAR PAPERS, VOL. 52, NO. 10, OCTOBER 2005
Sixth Stage (t5-t6): At t5, the voltage across capacitor
reaches zero and is clamped by diode . Currents and
increase, due to the application of voltage across in-
ductors and . In this stage, switch must be turned
on. It is important to emphasize that the drive time of switch
is estimated previously and kept constant during the en-
tire inverter operation range. So, the use of current sensor is not
necessary
(46)
For the second half-cycle, the operation stage is analogous and
can be described in an identical way.
The main operation stages are shown in Fig. 2. Fig. 3 shows
the main waveforms.
IV. M ATHEMATICAL A NALYSIS OF C OMMUTATION
To guarantee the ZVS conditions, it is necessary, in the second
stage, that the stored energy in inductor be
sufficient to discharge capacitor and to charge . Thus, by
inspection of Fig. 3 (Interval t1–t2), the following condition can
be formulated:
(26)
(27)
(28)
(29)
(47)
(30)
where is the maximum current in and is maintained
constant during the switching period. The current must be
sufficient to promote the charge and discharge of the commuta-
tion capacitors.
Assuming that
Seventh Stage (t6-t7): This stage begins when current
changes its direction and flows through switch
. Current
continues to increase linearly
,wehave
(31)
(32)
(33)
(48)
It is necessary to know the clamping voltage behavior for the
design of the switches and capacitor .
In steady-state conditions, the clamping capacitor average
current must be zero . Thus
(34)
(35)
Eighth
Stage
(t7-t8): During
this
stage,
switch
is
blocked and the current through
inverts its direction and
flows through diode
. Capacitor
charges itself from zero
to
and capacitor
discharges from
to zero
(49)
(36)
where is the switching period.
In relation to the switching period, the commutation time
is very short. Therefore, the following simplifications can be
made:
(37)
(38)
(39)
(50)
(51)
(40)
From (50) and (51), (49) can be re-written as follows:
(41)
Ninth Stage (t8-t0): This stage begins when the voltage
across capacitor reaches zero and is clamped by diode .
Current continues to increase. This stage finishes when
inverts its direction and flows through auxiliary switch
, restarting the first operation stage
(52)
Solving the integral equation, and considering
(42)
(43)
(44)
(53)
we have
(45)
(54)
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MEZAROBA et al. : ZVS PWM INVERTER WITH ACTIVE VOLTAGE CLAMPING
2223
Fig. 4.
Modulation strategy.
Considering that the load current is a sinusoidal function and is
in phase with the output voltage, then
Equation (63) shows the inverter duty cycle obtained from (58),
(59), and (62)
(63)
(55)
Combining (54), (55), and (63), we obtain the expression of the
snubber capacitor voltage,
where is the load impedance.
Fig. 4 shows some signals of the modulation strategy used to
drive the main switches.
The sawtooth waveform is lined on the left edge. This facili-
tates the synchronism between the auxiliary switch and the main
switches.
The converter output voltage is controlled by the amplitude
modulation factor , which is obtained through the relation
between the peak value of the sinusoidal reference signal and
the peak value of the sawtooth waveform
, given by
(64)
where is the peak reverse recovery current of the anti-parallel
diode, which can be given by [16]
(65)
(56)
represents the reverse recovery charge of the diode.
From the analysis of the current behavior in capacitor
, the
The inverter output voltage for a switching period can be ex-
pressed by
expression of current
can be obtained
(66)
(57)
Combining (64) with (66), and making some simplifications, we
obtain the expression that represents the evolution of current
From (57) we can obtain the duty cycle
, that is
(58)
(67)
The inverter output voltage for an output period is given by
To guarantee the ZVS condition in all load ranges, the minimum
value of current obtained from (67) must be greater than the
value obtained from (48).
(59)
where
is expressed by
V.
D ESIGN E XAMPLE
(60)
A. Input Data
V
bus voltage;
V RMS output voltage;
VA output power;
A
Output Frequency
The maximum output voltage is given by
output current;
(61)
fs
kHz
switching frequency;
Hz
output frequency;
The RMS output voltage is obtained from
mH
load inductance;
load resistance;
modulation factor.
(62)
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Zgłoś jeśli naruszono regulamin