IMPROVED AC-AC CONVERTER FOR INDUCTION
HEATING APPLICATIONS
Electrical and Electronics Project by Ravi Devani
ABSTRACT
Induction heating applications require high frequency currents which are
obtained using resonant converters viz., Series and Parallel resonant
inverters. The resonance frequency in these converters will be tuned to a high
value. In this paper a single-switch parallel resonant converter for induction
heating is simulated. It is compared with the existing inverter topologies;
half bridge and full bridge. The circuit consists of input LC-filter, bridge
rectifier and one controlled power switch. The switch operates in soft
commutation mode and serves as a high frequency generator. Output power is
controlled via switching frequency.
Keywords —
High frequency, induction heating, Resonant converters
INTRODUCTION
Induction heating is a non-contact heating process. It uses high frequency
electricity to heat materials that are electrically conductive. Since it is
non-contact, the heating process does not contaminate the material being
heated. It is also very efficient since the heat is actually generated inside
the work-piece. This can be contrasted with other heating methods where heat is
generated in a flame or heating element, which is then applied to the
work-piece. For these reasons Induction heating lends itself to some unique applications
in industry. Static frequency converters have been extensively applied in
industry as a medium –frequency power supply for induction heating and melting
installations. They are applied in all branches of the military,
machine-building industries, domestic heating cooking devices and other
purposes. Increasing the frequency of operation of power converters is
desirable, as it allows the size of circuit magnetics and capacitors to be
reduced, leading to cheaper and more compact circuits. However, increasing the
frequency of operation also increases switching losses and hence reduces system
efficiency. One solution to this problem is to replace the "chopper"
switch of a standard SMPS topology (Buck, Boost etc.) with a "resonant"
switch, which uses the resonances of circuit capacitance and inductance to
shape the waveform of either the current or the voltage across the switching
element, such that when switching takes place, there is no current through or
voltage across it, and hence no power dissipation. Because they require a
substantial drive current, bipolar transistors are not generally used in
resonant converters, unless the base drive is provided by the resonant circuit
itself (for example in TV deflection circuits and fluorescent lamp ballasts).
Power MOSFETs and IGBTs, with their effectively capacitive inputs and low drive
energy requirements, are the most frequently used types. The power converter
generally implemented in domestic IH appliances is a resonant inverter due to its
improved efficiency and lower size, which allows developing compact appliances.
Inverter topologies commonly used for IH are the full-bridge and half bridge
operations some deviations of these topologies are used often to achieve
multiple-output converters. The modulation strategies commonly applied to
control output power are based on modifying either switching frequency or duty
cycle to achieve the desired output power. Each power converter topology offers
different performance features with specific requirements in terms of costs, and
hardware and control complexity. The full-bridge topology can offer the higher output
power (up to 5 kW) and control flexibility, and its efficiency can be
significantly optimized through the proper control strategy. However, its
higher cost makes it unfeasible for the mean IH appliance. The half-bridge
series resonant inverter is the most used topology due to its appropriate
balance between performance, complexity, and cost. It is used to design
converters with up to 3.5-kW output power.
The decision has to be made considering the proper balance between cost and
performance. This paper presents circuit of an AC-AC converter for induction
heating .It typically includes a controlled rectifier and a frequency
controlled current source or a voltage source inverter. It is a fact that the input
rectifier does not ensure a sine wave input current, and is characterized by a
low power. Recently many studies of high power factor rectifiers with a single
switch have been made. These schemes are also characterized by a close to sine wave
input current. The input circuit of the converter is constructed similarly to
the input circuit in, which also ensures a high power factor. The present problem
aims to minimize the cost of induction heater system by using an embedded
controller.
IH TECHNOLOGY
The main blocks of an induction cooking appliance are shown in Fig. 1.
Fig 1. Induction cooking appliance block diagram.
The energy taken from the mains is filtered by an electromagnetic
compatibility (EMC) filter, which prevents the device from inserting
interferences and provides immunity to voltage transients. Then it is converted
to DC using a rectifier. Then, connect this DC current to a high frequency
switching circuit to administer high frequency current to the heating coil.
According to Ampere’s Law, a high frequency magnetic field is created around
the heated coil. A low value of filter capacitor is taken to get a high power
factor, and as a consequence, a high-ripple dc bus is obtained. Then, the
resonant inverter supplies variable frequency current (20–100 kHz) to the
induction coil. This current produces an alternating magnetic field, which causes
eddy currents and magnetic hysteresis heating up the pan. The inductor-pan
system is modeled as the series connection of an equivalent resistance Req
and an equivalent inductance Leq. This model shows proper results to
analyze power-converter operation. At the resonance frequency, the inductive
reactance and the capacitive reactance become the same, i.e. the voltage of the
power source and the current in the circuit stay at the same level. The current
in the circuit reaches its peak when the source frequency becomes identical to
the resonance frequency. It decrements when the source frequency gets higher or
lower than the resonance frequency. The current and output energy reaches its
maximum value at resonance frequency.
HALF BRIDGE SERIES RESONANT INVERTER
The main power circuit employs a half-bridge series converter switching at
a high frequency as shown in Fig. 2. The switching circuit consists of an IGBT.
Zero voltage/current turn-on switching is enabled by turning on the IGBT
while the diode is in turn on period. The resonant circuit comprises of
resonant inductance (Lr) and resonant capacitance (Cr). The capacitors, C1 and
C2, are the lossless turn-off snubbers for the switches, S1 and S2. The
resonant frequency fr of the converter is mainly determined by the inductance
Lr and the capacitance Cr of the series capacitor.
The switching frequency of
the system is set higher than the resonance frequency, in order to avoid noise generated
within the audio frequency band. The resonant load consists of the pan, the
induction coil and the resonant capacitor. Induction coil and pan coupling is modeled
as the series connection of an inductor and a resistor, based on its analogy
with respect to a transformer. The basic circuit of a half bridge series
resonant circuit is shown in Fig. 2
Fig 2. Half bridge series resonant inverter
By connecting the IGBT switching circuit, S1 and S2 in parallel to diodes
D1 and D2, current loss is minimized. When S1 is turned-off, D2 helps S2 stay on
zero voltage/current before being turned on, thereby substantially reducing current
loss (the same is the case with S1). There is no reverse- recovery problem as
the voltage on both sides remains zero after the diode is turned off. However,
as the switching circuit is turned off at around the upper limit of voltage and
current, some switching loss results on turn-off. The capacitors C1 and C2,
acting as turn-off snubbers connected in parallel to S1 and S2, keep this loss
to a minimum. Upon turn-on the switching circuit starts from zero
voltage/current, so these turn-off snubbers operate as lossless turn-off snubbers.
This has been simulated using MATLAB/ SIMULINK with the circuit diagram shown
in Fig. 3.
This system does not require a big capacitor to make DC more leveled, as
the primary purpose of the system is to generate heat energy. Rather, the
rugged form of DC helps improve the power factor of the system. In this system,
the leveling capacitor serves as a filter preventing the high frequency current
from flowing toward the inverter and from entering the input part. Input current
becomes the average of the inverter current, and the ripples flow to the
leveling capacitor. The voltage passing the leveling capacitor is turned into a
square wave in the process of high frequency switching in the inverter. The
high frequency harmonics contained in the square wave are eliminated by the Lr,
Cr filter. The square wave enables resonance in the resonant circuit, which in turn,
creates a magnetic field around the resonant inductor affecting the load. Eddy
currents are formed around the surface of the object, generating heat energy.
Fig 3 . SIMULINK model of Half bridge inverter
Electrical and Electronics Project by Ravi Devani
The voltage and current waveforms of the simulated circuit are also shown
below (fig. 4).
Fig. 4. (a) The voltage waveform and
(b) Current waveform
Since it is a voltage- source inverter voltage waveform is having square
pulses and the current waveform is oscillatory as is seen in figure 4(a),(b).
SIMULATION PARAMETERS:
Lr=52.7uH and Cr=0.8uF, resonant
frequency=24.5kHz
FULL BRIDGE HYBRID RESONANT INVERTER
Another commonly used inverter topology with 4 semiconductor switches is
described in this section. This high frequency full bridge hybrid resonant inverter
supplies more power when compared to half bridge series resonant inverter. One
hybrid resonant inverter consists of four semiconductor switches (IGBT’s) for
each heat in grange. The switching frequency lies between 25 to 35 kHz. It can
be considered as a combination of both series and parallel resonant circuits
where the switching is made at zero current cross over (ZCS). An advantage of
the series circuit is that both zero current and zero voltage switching are
possible. Different diameters of induction coils can be chosen for different
diameters of flat bed pans. For getting maximum efficiency (with induction
system, about 88%) of the system, the coil diameter and the diameter of the
utensils must be equal. The full resonant current passes through the switches resulting
in ON losses. Depending on the converter design there will be reactive power consumption
or more complexity. In a parallel load, there would be low ON losses in the
switches but turn-on / turn-off losses would be more as the switching takes
place at high voltage and current. So, a hybrid inverter, (i.e. by using
combined series and parallel circuit) can be used to reduce the losses in the
switches. Fig. 5 shows a resonant inverter system for one cooking zone. Here the
energy is transferred from the series resonant circuit to the parallel resonant
circuit. By turning on one of the switch pairs S1, S4 or S2, S3 a resonant current
starts flowing through L1 to CR and when this current is zero, the switches are
turned off. After that the series resonant circuit is disconnected and the energy
transferred to resonant capacitor is dissipated as heat in RL by the current
flowing through the parallel resonant circuit. RL is the equivalent resistance
for the magnetic loss in the induction heating system.
This is simulated and the SIMULINK block is shown in Fig. 6 and the
corresponding voltage waveform is shown in Fig.7
Fig. 6 SIMULINK model of hybrid resonant inverter using IGBT
Fig. 7 voltage
waveform of hybrid resonant inverter
TABLE1: INPUT PARAMETERS OF SIMULATION
AC TO AC CONVERTER
In the proposed scheme of the AC-AC converter there are two main
advantages: It is having a high power factor and a sine wave input current.
Also the inverter circuit is composed with only a single controlled switch,
which serves as a high-frequency generator for induction heating. Fig.8 shows
the circuit diagram.
Fig. 8 Circuit diagram of AC- AC converter
The operating principles of the circuit are illustrated by Fig. 9
Fig.9a. Mode 1 (to-t1)
Fig.9b. Mode 1I (t1-t2)
Fig.9c. Mode 1II (t2-t3)
Fig.9 Equivalent Circuits
Interval 1: t0<t<t1
The equivalent circuit is shown in Fig.9a. Four diodes D1-D4 and
the switch S are off. In this interval the capacitor C charges up linearly at a
rate and a polarity corresponding to the instantaneous input voltage Vin.
Interval 2: t1<t<t2
The equivalent circuit is shown in Fig.9b. Two diodes D1, D3 and the
switch S are on. In this interval the capacitor C is discharging via the
circuit C-D1-S-Lrload- D3. This interval ends when the
capacitor voltage reduces to zero.
Interval 3: t2<t<t3
The equivalent circuit is shown in Fig.9c. All the diodes and the switch S
are on. In this interval the current through switch S flows via two parallel
bridge branches. This interval ends when this switch current decreases to zero.
At this moment the switch turns off and the process starts from the beginning. The
theoretical waveforms are shown in fig.10
Fig.10 Ideal Switching Waveforms
Before the analysis it is assumed that all the circuit components are
ideal. The analytical calculations are based on two more assumptions: the
switch current can be assumed as semi sinusoidal, and the load power is
determined by the first harmonic of the load voltage. Evaluation of the
relationship between input and output voltages
Mg = Vo/Vin
The AC to AC
converter fed induction heater is simulated using Matlab/Simulink and their
results are presented here. The SIMULINK model of AC-AC converter is shown in
Fig 11 and its corresponding waveform is also shown ( fig. 12)
Fig.11 SIMULINK model of AC-AC converter
Fig.12 Voltage Waveform of AC- AC converter
TABLE 2: SIMULATION PARAMETERS
CONCLUSION
Different inverter topologies are used in induction heating applications.
Of that the basic half- bridge and full bridge inverter topologies have been
compared. A new topology have been proposed. The AC-AC converter circuit for
induction heating has been simulated. Its power factor is close to unity. The circuit
topology is very simple since includes only one power switch. This switch
operates in a soft commutation mode. The converter provides a wide range power
control. This converter has advantages like reduced hardware, reduced stresses
and high power density.
REFERENCES
[1] J.Acero, J. M. Burdio, L.A. Barragan, D. Navarro, R.Alonso, J. R.
Garcia, F. Monterde, P. Hernandez, S. Llorente, and I. Garde, “Domestic
induction appliances,” IEEE Ind. Appl. Mag., vol. 16, no. 2, pp. 39–47,
Mar./Apr. 2010.
[2] I. Mill´an, J. M. Burd´ıo, J. Acero, O. Luc´ıa, and S. Llorente, “Series
resonant inverter with selective harmonic operation applied to all-metal
domestic induction heating,” IET Power Electron., vol. 4, pp. 587–592,
May 2011.
[3] R. L. Steigerwald, “A comparison of half-bridge resonant converter
topologies,” IEEE Trans. Power Electron., vol. 3, no. 2, pp. 174–182,
Apr. 1988
[4] H. W. Koertzen, J. D. van Wyk, and J. A. Ferreira, “Design of the
halfbridge series resonant converters for induction cooking,” Proc. IEEE
Power Electron. Spec. Conf. Records, 1995, pp. 729–735
[5] Nitai Pal, Pradip Kumar Sadhu, Dola Sinha and Atanu Bandyopadhyay,” Selection
of Power Semiconductor Switches – a Tool to Reduce Switching & Conduction
Losses of High Frequency Hybrid Resonant Inverter fed Induction Cooker”, International
Journal of Computer and Electrical Engineering, Vol. 3, No. 2, April,
2011 1793-8163
[6] P. K. Sadhu, N. Jana, R. Chakrabarti, and D. K. Mittra “A Unique
Induction Heated Cooking Appliances Range Using Hybrid Resonant Converter” – Int.
J. of Circuits, Systems and Computers, World Scientific, Volume 14, Number 3,
June
2005, pp. 619-630
[7] Bayindir, N.S.; Kukrer, O.; Yakup, M (May 2003).: “DSP based PLL
controlled 50–100 kHz 20 kW high-frequency induction heating system for surface
hardening and welding applications”. IEE Proc.-Electr. Power Appl., Vol.
150, No.3, pp. 365-371.
[8] Mollov, S.V.; Theodoridis, M.; Forsyth, A.J. (January 2004): “High
frequency voltage-fed inverter with phase-shiftcontrol for induction heating”,
IEE Proc.-Electr. Power Appl., Vol. 151, No. 1, pp. 12-18.
[9] J. M. Burdío, L. A. Barragán, F. Monterde, D. Navarro, and J. Acero,
“Asymmetrical voltage-cancelation control for fullbridge series resonant
inverters,” IEEE Trans. Power Electron., vol. 19, no. 2, pp. 461–469, Mar.
2004.
[10] I. Millán, D. Puyal, J. M. Burdío, C. Bemal, and J. Acero, “Improved
performance of half-bridge series resonant inverter for induction heating with
discontinuous mode control,” in Proc. IEEE Appl. Power Electron. Conf. Expo.,
2007, pp. 1293–1298.
[11] F. P. Dawson and P. Jain, “A comparison of load commutated inverter
systems for induction heating and melting applications,” IEEE Trans. Power
Electron., vol. 6, no. 3, pp. 430–441, Jul. 1991.
[12] O. Lucía, J. M. Burdío, I. Millán, J. Acero, and D. Puyal, “Load-adaptive
control algorithm of half-bridge series resonant inverter for domestic
induction heating,” IEEE Trans. Ind. Electron., vol. 56, no. 8, pp. 3106– 3116,
Aug. 2009.
[13] N. J. Park, D. Y. Lee, and D. S. Hyun, “A power-control scheme with
constant switching frequency in class-D inverter for induction-heating jar
application,” IEEE Trans. Ind. Electron., vol. 54, no. 3, pp. 1252–1260, Jun.
2007.
[14] J. M. Burdío, F. Monterde, J. R. García, L. A. Barragán, and A.
Martínez, “A two-output series-resonant inverter for induction-heating cooking
appliances,” IEEE Trans. Power Electron., vol. 20, no. 4, pp. 815–822, Jul.
2005.
Electrical and Electronics Project by Ravi Devani