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Purely Inductive Ripple Power Storage for Improved Lifetime in
Solar Photovoltaic Micro-inverter Topology Ramprakash Kathiresan1,2, Pritam Das1,2, Thomas Reindl1 and Sanjib Kumar Panda1,2
1Solar Energy Research Institute of Singapore, Singapore - 117574 2Electrical and Computer Engineering Department, National University of Singapore, Singapore - 117583
Abstract — In a solar photovoltaic (PV) system, decoupling of power ripple is necessary in order to maximize the energy harvest because the power flowing to the grid is time varying while the power extracted from the photovoltaic panel needs to be maintained constant. This necessitates the requirement of energy storage elements between the input and output to decouple the unbalance of power. The location of the decoupling element can be either at the PV-side or the AC-side. The traditionally used energy storage element is the electrolytic capacitor. Due to its fast degradation, it is often replaced by film capacitors with active decoupling schemes that perform better at higher temperatures with less degradation, however at significantly higher cost. From an economic perspective, both electrolytic and film capacitors have similar lifetimes, which are substantially lower than the typical warranty of the solar module (20-25 years) though. An inductor, in contrast, is an energy storage element with aging of less than 0.5 percentage over a 20-year lifecycle. Further, the reduced temperature drift compared to a capacitor makes it a highly suitable candidate for storage of power ripple in solar photovoltaic power converters. This paper demonstrates a proof-of-concept decoupling scheme using an inductor as the energy storage element at the PV-side of a DC-AC single stage power converter.
Index Terms — Power decoupling, Inductive ripple storage, Micro-inverter, Lifetime.
I. INTRODUCTION
The numbers of solar photovoltaic (PV) system installations
are growing exponentially and are adding GWs of renewable
power to the global energy mix [1]. The main reason for the
tremendous growth is due to the so-called "grid-parity" being
achieved in several countries. Also, the drastic reduction in PV
module prices (partially also due to over-capacity in the
market), has led to a wide-spread use of PV for a variety of
applications. The most common form of installation is grid-
connected PV systems, which require an inverter to convert
the available DC output of the PV generator into a grid-
compatible AC form. PV inverters are available in different
forms depending on the capacity and functionalities.
Generally, there are: central inverters (typically > 100 kWp),
string inverters (typically 1- 100 kWp) and micro-inverters
(typically < 1 kWp).
This work is related to micro-inverters. Like in other
inverter types, the power flow to the grid is time-varying while
the power extracted from the solar-PV panel needs to be
maintained constant for maximizing the harvested energy. This
requires an energy storage element to store the power ripple
and hence decouple the unbalance of power.
Fig.1. Description of decoupling of DC and AC power [2]
Mathematically, the instantaneous output power ‘po’ (see
Fig. 1) of the inverter in a single phase grid connected system
consists of:
an average output power ‘Pdc’ and
a time varying pulsating power ‘pac’ which oscillates
at twice the line frequency.
(1)
(2)
where ‘U’ and ‘I’ are the amplitudes of the grid voltage and
grid current respectively. When Pdc > pac, the surplus energy is
stored into the energy storage element; and is later released
when pac > Pdc.
To serve the purpose of decoupling, a capacitor is
commonly used as the energy storage element. Presently,
electrolytic capacitors are the most widely used means of
decoupling and are placed across the PV panel terminals. This
will result in a very large capacitance so as to restrict the
voltage ripple to low values. Also, they have a lifetime of
around 7000 hours only at a temperature of 105°C [3].
Alternatively used film capacitors have less degradation and
higher ripple current density and are employs a power
decoupling circuit. Several topologies employing a power
decoupling circuit with capacitive energy storage elements are
suggested as in [4]-[6]. However, film capacitors have an
increased cost of nearly 3 to 4 times that of electrolytic
capacitors [7]. Batarseh et.al. have extensively reviewed the
decoupling techniques for micro-inverters [2] with different
capacitive methods presently available, which showcases that
the lifetime of the capacitor is the limiting factor. Hence, a
means of decoupling with an increased cycle life while still
UIPdc2
1
1cos(2 )
2acp UI wt
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being easily available and cost-effective would be desirable.
The solution proposed in this work addresses this lifetime
issue for PV inverters by using an inductor to eliminate the
second harmonic ripple power. It is to note that the inductor
has an aging factor of less than 0.5% over a 20-year life cycle
and hence the lifetime is significantly higher than both
electrolytic and film capacitors.
In this paper, an inductive means of ripple power storage is
proposed and implemented at the DC side of the DC-AC
converter. While compared to capacitive means of decoupling,
inductive method shall be economical and also practical at
high temperature range due to its reduced temperature drift.
Also, there will be significant cost savings as elucidated in
Table I.
TABLE I
COMPARISON OF COST AND LIFE OF DECOUPLING ELEMENTS
Decoupling
component (for
250W)
Cost
(USD)
Lifetime
(operation hrs @ 85°C)
Electrolytic
capacitor 4 10,000
Film capacitor 12 30,000
Proposed
inductor 4.5
0.5% degradation over
20 years
The following sections describe the system description and
proof-of-concept demonstration of the proposed decoupling
technique.
II. SYSTEM DESCRIPTION
The proposed purely inductive decoupling scheme can be
applied to any DC to AC converter including those with high
frequency galvanic isolation and require ripple mitigation at
the DC side. Typically all micro-inverters have galvanic
isolation between input and output for safety purposes.
A micro-inverter based on a simple fly-back type DC-AC
converter with galvanic isolation and output unfolding circuit
and related filter is demonstrated here as shown in Fig. 2(a).
The micro-inverter output is connected to the utility grid.
Now, the DC link between the solar panel and the inverter
experiences a second harmonic ripple (i.e, ripple at twice the
frequency of the AC grid), which needs to be eliminated. It is
suggested here to add an inductor and an auxiliary circuit
along with a suitable controller to enable the ripple power
storage mechanism at the PV side. When the ripple mitigation
technique is exercised, high MPP efficiency operation could
be achieved.
The proposed technique could be implemented in all types of
DC to AC converters as generalized in Fig. 2(b) and is
especially applicable for single-stage micro-inverter topologies
with high frequency galvanic isolation. This is because in
single stage micro-inverter, the power converter needs to
accomplish both the tasks namely: Maximum Power Point
Tracking (MPPT) operation along with rectified sine
waveform modulation followed by unfolding; so the simple
means of power ripple decoupling is to place the decoupling
element at the PV or DC side. Decoupling at the AC output
side will require several active switches and additional
complexity in the control method. Also, in the case of AC-side
decoupling, a third phase shall be necessary to implement the
power decoupling and the control complexity is increased
dramatically [2].
Unfolder
circuit
L
C AC utility
grid
Flyback
transformer Output filter
Solar
Panel
Auxiliary
circuit
IPV
IGRID
VGRIDVPV
Sfly
Inductor as energy storage element
Fig. 2 (a). Proposed Inductive ripple storage mechanism implementation in a DC-AC converter employing Flyback topology
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Solar panel
Vaux+
DC/ACAC
utility
grid
Iref
Vaux-
Fig. 2 (b). Block diagram representation of the generalised system.
A. Auxiliary circuit description
The proposed auxiliary circuit schematic as shown in Fig. 3
consists of two switches S1 & S2, two diodes D1 & D2 and an
inductor as the energy storage element. The inductor is
represented with a series resistance ‘RL’ and inductive
reactance ‘XL’.
MOSFET switches and diodes are connected in an H-bridge
fashion where one phase is controlled by the switches S1 & S2
and the other phase by the diodes D1 & D2 only. This
auxiliary circuit is connected at the points Vaux+ and Vaux- of the
DC link to handle the second harmonic ripple power. Current
sensors are used for measuring the currents ‘Iref’ and ‘Iaux’ as
shown in Fig. 2 and Fig. 3 respectively.
Fig.3. Schematic representation of the auxiliary circuit.
The operation of the auxiliary circuit (see Fig. 4) can be
divided into the following zones when ripple energy has to be
stored inside the inductor, denoted in the paper as BUCK
mode, in which S2 will remain ON:
1) Zone-1 (t0< t <t1): At time t0, the auxiliary switch S1 is
turned ON and switch S2 remains ON during the energy
storage mode. By doing so, a positive voltage of ‘VDC’ at
the output of the PV panel is reflected across the inductor
so that the current through the inductor will rise, thus
“pumping” energy into the inductor.
2) Zone-2 (t1< t <t2): At time t1, the auxiliary switch S1 is
turned OFF but switch S2 remains ON. The current in the
inductor freewheels through D1 and S2 with ideally zero
volt across the inductor. The current through the inductor
will remain constant in this zone. This mode ends with
turning switch S1 ON again, which signifies the completion
of one switching cycle in the buck mode.
By controlling the duration of zone-1 and zone-2 of Buck
mode, the net energy stored in the inductor can be controlled.
Again, the operation of the auxiliary circuit can be divided
into the following zones when ripple energy has to be
extracted from the inductor, denoted in the paper as BOOST
mode, in which S2 will always remain OFF:
1) Zone-1 (t’0< t <t’1): At time t’0, the auxiliary switch S1 is
turned ON and switch S2 always remains OFF. The current
in the inductor will freewheel through D2 and S1. By doing
so, zero volt is incident across the inductor.
2) Zone-2 (t’1< t <t’2): At time t’1, the auxiliary switch S1 is
turned OFF. The current in the inductor flows through D2
and D1 so that a voltage of ‘-VDC’ is incident across the
inductor so that the current through the inductor will ramp
down in this zone and the stored energy in the inductor is
released. End of this mode signifies the completion of one
switching cycle in the boost mode.
By controlling the duration of zone-1 and zone-2 of Boost
mode, the net energy released from the inductor can be
controlled.
Fig.4. Ideal waveforms of both BUCK and BOOST modes of
operation.
B. Control method
The control method for the proposed inductive energy
storage scheme is explained in Fig. 5 and Fig. 6. The control
system has to ensure that the second harmonic current required
by the DC-AC converter is completely provided by the
discharging and charging of the auxiliary inductor.
To do so, band-pass filters with center frequency ‘fc’
matching the 2nd harmonic frequency of the utility AC grid are
used to extract the second harmonic components ‘Iaux2’ and
‘Iref2’ of currents ‘Iaux’ and ‘Iref’ respectively from the DC-AC
converter and from the positive rail of the auxiliary circuit. A
RLXL
D1
D2
VGS1
S1
VGS2
S2
Vau
x+
Vau
x-
Iaux
Inductor
current, IL
Inductor
voltage, VL
Gate VGS1
Gate VGS2
t
BUCK mode BOOST mode
t0 t1 t2
S1
S2
D1
S2
D2
S1
D2
D1
t'0 t'1 t'2
VDC
-VDC
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proportional-integral (PI) controller is used to minimize the
error between the peak values ‘Iaux2p’ and ‘Iref
2p’ of currents
‘Iaux2’ and ‘Iref
2’ that are already obtained. The signal from the
PI controller is multiplied with the modulus of the grid voltage
‘Vgrid’ phase shifted through ‘-45°’ to obtain the control signal
‘Ctrl’ for modulation of the auxiliary circuit as shown in Fig.5.
Fig.5. PI controller implementation for proposed auxiliary circuit
Fig.6. Modulation logic (ST: saw-tooth carrier)
The detection of the afore-mentioned boost and buck modes
are done using a phase detector circuit. When pac > Pdc, i.e. the
AC load requires more energy than what is provided by the
DC source, the inductor is discharged and helps in meeting the
load demand – hence the term ‘BOOST’. When pac < Pdc, i.e.
the AC load requires less energy than what is provided by the
DC source, the inductor is charged from this excess amount of
energy - hence the term ‘BUCK’.
C. Inductor Design
The 3-dimensional design of the proposed inductor used as
the energy storage element in this paper is as shown in Fig. 7.
The inductor core consists of a lamination stack made up of
0.35mm cold-rolled grain-oriented electrical (Fe-Si) steel as in
[8]. The winding consists of several turns of copper foil. A
planar geometry of the core is considered for improved
packaging of the inductor. The fundamental considerations and
calculations are followed as described in [9].
Fig.7. 3-D representation of the proposed Inductor.
III. SIMULATION & EXPERIMENTAL RESULTS
The proposed technique is simulated on a 250W micro-
inverter powered by a PV panel with 45V, 6.0A as shown in
Fig.8, at the MPPT voltage and current, using the simulation
software PSIM Ver.9.3.1. The value of the inductor used is
6mH.
Fig.8. Simulated Output Current and Voltage of PV Panel (V: Volts,
I: Amps)
Both the buck and boost mode respectively are dependent
on the status of the ripple. According to the status of ripple
inherited by the ‘Ctrl’ signal, the switch S1 is modulated with a
saw-tooth carrier for controlled charging and discharging of
the inductor. The inductor current and related waveforms in
the buck and boost mode of operation are shown in Fig. 9.
The magnetic flux density of the proposed inductor design is
investigated using COMSOL Multiphysics Ver.4.4. The core
parameters from [8] are incorporated. The magnetic flux
density norm attains 1.89 T at the maximum while injected
with a DC current of 15A. The distribution of the magnetic
flux density in the inductor core is as shown in Fig. 10 which
proves the sufficient and appropriate sizing of the inductor.
Fig. 10. Magnetic flux density of the proposed inductor design
validated in multi-physics tool.
Iref2
Iaux2
Ctrl
+-
|Vgrid Ð-45°|
K + ʃ Peak current conversion
Peak current conversion
Iref2p
Iaux2p
ST
Ctrl
Ctrl>ST
Ctrl<ST
Buck
Boost
VGS1
+
-
+
-
VGS2Buck
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For experimental purpose, a modular solar array simulator -
Agilent E4360 is used to mimic a solar panel input. The
voltage and current values at MPPT were maintained at 45V
and 6.0A respectively, same as in simulation condition. The
auxiliary circuit is introduced at the DC side of the fly-back
type DC to AC converter. The charging and discharging action
is observed in the current in the ripple energy storage inductor
is as shown in Fig. 11. The output current of the flyback
transformer at the secondary side is as shown in Fig. 12. The
MPPT voltage, grid current and grid voltage respectively are
shown in Fig. 13.
Fig. 11. Auxiliary inductor current waveform
From the simulation and experimental results, it is proven
that the proposed power ripple decoupling circuit is able to
store the ripple power effectively which leads to operation of
the micro-inverter with MPPT. Moreover the output current
and voltage of the micro-inverter are in phase with minimal
harmonic distortion which can only be realized by proper
MPPT operation of the overall converter wherein the output
voltage of the emulated PV panel is always stabilized at its
MPPT value with negligible amount of low frequency ripple.
Fig. 12. Flyback transformer output current waveform
Fig.13. Experimental waveforms showing MPPT voltage, grid
voltage and grid current respectively.
Fig. 9. Simulated Auxiliary Inductor Current, 2nd harmonic ac current of dc-ac converter, boost, buck mode detection (I: Amps)
978-1-4799-4398-2/14/$31.00 ©2014 IEEE 0984
IV. CONCLUSION
Long lifetime of the power electronics is the primary
concern in any solar PV installation that is supposed to last for
20-25 years. By implementing a purely inductive decoupling
scheme, the reliability of the DC-AC inverter which is the key
electronic component of a PV system is improved without
significant cost and complexity compared to other means of
active power decoupling schemes provided in the literature.
Based on the successful simulation results, a patented
hardware prototype is developed to implement this scheme in
an “AC module” (i.e. PV module with a micro-inverter) rated
at 250W and the proof-of-concept results are discussed.
REFERENCES
[1] International Energy Agency, “Energy technology
perspectives2008- scenarios and strategies to 2050” [Online]. Available: http://www.eia.org
[2] Haibing Hu; Harb, S.; Kutkut, N.; Batarseh, I.; Shen, Z.J., "A Review of Power Decoupling Techniques for Microinverters With Three Different Decoupling Capacitor Locations in PV Systems," Power Electronics, IEEE Transactions on , vol.28, no.6, pp.2711,2726, June 2013
[3] C. C. Dubilier, “Type 381EL 105 ◦C ultra-long life snap-in, aluminum.”
[4] T. Shimizu,K.Wada, andN.Nakamura, “Flyback-type single-phase utility interactive inverter with power pulsation decoupling on the dc input for an ac photovoltaic module system,” IEEE Trans. Power Electron., vol. 21, no. 5, pp. 1264–1272, Sep. 2006.
[5] S. B. Kjaer and F. Blaabjerg, “Design optimization of a single phase inverter for photovoltaic applications,” in Proc. IEEE 34th Annu. Power Electron. Spec. Conf., Jun. 2003, vol. 3, pp. 1183–1190.
[6] H. Hu, S. Harb, X. Fang, D. Zhang, Q. Zhang, Z. J. Shen, and I. Batarseh, “A three-port flyback for PV micro-inverter applications with power pulsation decoupling capability,” IEEE Trans. Power Electron., vol. 27, no. 9, pp. 3953–3964, Sep. 2012.
[7] “Advances in Capacitors and Ultracapacitor for power electronics”, IEEE Applied Power Electronics Conference, Industrial Session 1.3, March 2013.
[8] Material specification of electrical steel : TEMPEL International grade GS0140 066 C02.
[9] Colonel Wm. T. McLyman, “Transformer and Inductor Design Handbook,” Kg Magnetics, Inc.
978-1-4799-4398-2/14/$31.00 ©2014 IEEE 0985