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International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
42
BESS at Point of Common Coupling for Wind Farm
Sandeep Tapre, Prof.K.Venkata Ramamohan
M.E (student), Professor
MSS’s College of Engg. Jalna
sandeep.tapre85@rediffmail.com, ram.mohan822@gmail.com
Abstract- A computational procedure to determine the Battery energy storage system capacity and the evaluation of the
voltage .This paper presents the results of a wind data and provide effectively continuous power for the consumers or
grid without any disturbance. It also examined for the purpose of attenuating the effects of unsteady input power from
wind farms. A novel 2 wind generating plants at Point of common coupling, Battery storage-based power allocation
method also is proposed. The effectiveness of these methods was verified using MATLAB/SIMULINK software.
1. INTRODUCTION
Wind power is the fastest-growing renewable energy
source, but one of the typical problems of wind energy
converters (WECs) is the variation in their delivered
power, which is the main cause of the relationship
between the random nature of wind and the power. The
purpose of the present investigation is to fill in the gap in
the aforementioned daily load-tracking application. It
addresses the design of a BESS, incorporated into a
power buffer for the wind farm. While the BESS
possesses higher energy capacity than several other
energy storage media, and hence, it is suitable for the
long-term load-tracking operation [1], BESS is also
shown to be cost-effective for use in power systems [2].
However, nowadays it is common to find wind
converters where an electronic converter is used to
connect the generator to the network, so the delivered
power can be smoothed [3].
The purpose of this paper is to investigate the periodic
power pulsations that have been measured during the day
and give continuous power. The loads on an electricity
supply system, which are reflected in the spot price of
electricity, vary according to the time of day, day of the
week, season, and also other, unpredictable factors. For
the wind farm application, for example, a flow battery
system has been described in [4], although the authors
have yet to provide a method by which the battery
capacity can be determined. Thus, the present
investigation proposes a methodology to determine the
required BESS capacity for the purpose of daily load
tracking or load leveling. The method is based on a given
wind power profile and the optimization of an objective
function through which the Optimal dispatched power
level from the wind farm will be obtained.
2. MODEL DESCRIPTION
This paper is organized as follows. PMSG is
interconnected with the grid through a fully rated
converter so that the variable ac frequency at the
generator terminal is converted to steady grid frequency
at the output. Here two plants are to be considering which
are join at PCC through the PWM Generator as shown in
Fig 1. Also it shows that the wind energy captured by the
turbine blades is converted through the PMSG into
electrical power, denoted by Pw. From previous
references, it is clear that Pw tends to be highly
stochastic, and an effective way to describe Pw could be
through statistical means [5], [6]. Alternatively, as part of
the wind farm planning, site selection, and design
process, wind data are often collected at site if such data
of (say) past few years are unavailable. As the main focus
of this paper is on the design of the BESS, it is now
assume that sufficient wind data are available and the
profile of Pw is known over a period of T h. Fig. 2 shows
a typical profile of Pw, derived from the wind speed data
.In the figure, Pw has been normalized, and hence is
within the range [0, 1] per unit (p.u.).
All wind speed distributions were corrected to a long-
term mean wind speed of 12 m/s. At short time scales. As
per Fig. 1 the system configuration of a direct drive
PMSG based grid interfaced WECS. A horizontal axis
wind turbine is used to drive the PMSG. A surface
mounted non salient pole type PMSG is used. The kinetic
energy presents in the wind is converted into the
mechanical torque using a wind turbine. Mechanical
energy is converted into electrical energy using a PMSG.
To facilitate variable speed operation for achieving
MPPT, the PMSG cannot be interfaced with the grid
directly. Therefore, two VSCs are used in back to back
configuration with common DC link known as a MSC
and a GSC. These VSC’s are controlled independently.
42
International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
Figure 1. Variable speed wind turbine with
interconnection to the mains grid through BESS.
Figure 1. Typical wind power profile based on data taken:
constant Pd is shown.
One can assume that the power loss in the two converters
is negligible. The dc-link capacitor C functions as
harmonics filter, and in some designs, it can also take the
role of the energy-storage system [7]. However, typical
energy storage capacity of the capacitor tends to be small
compared to the BESS considered in the study. Hence, in
terms of initial power flow analysis, the capacitor power
may be neglected. It is further assumed that the
dispatched power Pd from CON2 to the mains grid is to
be kept constant over the interval T. Although this
assumption tends to facilitate analysis, it also has a
desirable effect from a practical viewpoint: it prevents
the fluctuating Pw from impacting negatively on the grid,
in terms of network voltage and frequency profiles. To
realize the constant power feature, the mismatch power
between Pw and Pd has to be compensated for by the
BESS, which has the output Pb (t), shown in Fig. 1.
3. CONTROL ALGORITHM
The block diagram of the proposed control scheme as
in Fig. 1, The MSC controls the active power of the
PMSG to achieve MPPT and the GSC regulates the DC
link voltage under change in active power output from
the PMSG. The control scheme for the MSC and the
GSC are as follows:
A. Machine Side Converter (MSC) Control
The MSC is controlled in rotor reference frame and the
phasor diagram. The stator resistance of a PMSG is
negligible which is practically valid in MW size of
generators. The rotor flux linkage is aligned with the d-
axis of the synchronous reference frame. All vectors
along with dqaxis frame rotate in space at synchronous
speed ωs which is also the rotor speed of the generator
ωr. The stator current vector is is perpendicular to the
rotor flux vector λr.
B. Mathematical model
The following table shows the definition of various
variables used in this model:
E = Kinetic Energy (J)
Ρ = Density (kg/m3)
M = Mass (kg) A = Swept Area (m2)
V = Wind Speed (m/s)
Cp = Power Coefficient
P = Power (W)
r = Radius (m)
Under constant acceleration, the kinetic energy of an
object having mass m and velocity v is equal to the work
done W in displacing that object from rest to a distance s
under a force F i.e.
E =W = Fs
According to Newton’s Law, we have:
F = ma
Hence,
E = mass … (1)
Using the third equation of motion:
PWM CvAP 3
2
1
ρ=
(1)
v 2 = u2 + 2as and as per paper [10].
A German physicist Albert Betz concluded in 1919
that no wind turbine can convert more than 16/27
(59.3%) of the kinetic energy of the wind into
mechanical energy turning a rotor. To this day, this is
known as the Betz Limit or Betz'Law. The theoretical
maximum power efficiency of any design of wind turbine
is 0.59 (i.e. no more than 59% of the energy carried by
the wind can be extracted by a wind turbine). This is
called the “power coefficient” and is defined as:
C pmax = 0.59
Also, wind turbines cannot operate at this maximum
limit. The Cp value is unique to each turbine type and is a
function of wind speed that the turbine is operating in.
Once we incorporate various engineering requirements of
a wind turbine - strength and durability in particular – the
real world limit is well below the Betz Limit with values
of 0.35-0.45 common even in the best designed wind
43
International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
turbines. By the time we take into account the other
factors in a complete wind turbine system - e.g. the
gearbox, bearings, and generator and so on - only 10-
30% of the power of the wind is ever actually converted
into usable electricity. Hence, the power coefficient
needs to be factored in equation (4) and the extractable
power from the wind is given by:
PWavail CvAP 3
2
1
ρ=
(2)
Where ρ is the air density which is approximately
equal to 1.2 kg/m3 this study; where Cp is the power
coefficient considered 0.48 for this wind turbine; A is the
sweep area of turbine blades in m2 and υw is the wind
velocity in m/s. In direct drive system, due to the absence
of a gear box, the mechanical torque (TM) and the shaft
speed of the wind turbine are directly transferred to the
shaft of the generator. The mechanical torque developed
by the wind turbine is as,
Tm = Pm/wm
(3)
C. Grid Side Converter (GSC) Control
The DC link voltage is selected such that it should be
more than peak of the line voltage for satisfactory
operation of GSC for controlled active power transfer to
the grid.
4. BESS CAPACITY
The battery capacity is normally specified in terms of
power and energy capacity [9]. The energy capacity
describes the energy that can be drawn from or stored in
the battery. The power rating determines the power that
can be supplied or stored by the battery under rated
discharge/charge time interval. The capital cost of the
battery can also be determined, based on the power and
energy capacities [8]. Consequently, the design problem
in hand is to determine the BESS capacity based on a
cost-benefit consideration, as shown later.
Figure 2. Simulink model for BESS at point of common
coupling at wind farm with interconnection to
the Loads.
Determination of BESS Power and Energy
Capacities
In the buffer system, the BESS power Pb (t) can be
written in terms of Pw and Pd as
Pb (t) = Pw − Pd .
(4)
From (1), for a given constant Pd , Pb (t) will vary in
the same manner as Pw. By setting Pd to another
constant value will only result in the Pb (t) curve being
shifted up or down, but Pb (t) will remain as the same
shape as Pw. For example, for the Pw profile given in
Fig. 2, the Pb (t) profile given in Fig. 3(a) corresponds to
Pd = 0.6 p.u. From Fig. 3(a), one finds that the maximum
battery power Pb ,max occurs at T1 when Pb ,max =−0.5
p.u. over the interval T. The negative sign indicates that,
at this precise moment, the BESS is discharging. It is
quite conceivable for a different value of Pd, the
corresponding Pb,max may be positive.
It then indicates that the BESS is being charged at the
maximum value at that instance. Integration of Pb (t)
with respect to time yields the net energy (Eb) injected
into or discharged from the BESS, up to time t.
Corresponding to the changes in Pb (t), the Eb (t) profile
will also vary for different Pd. For instance, Eb (t)
profiles corresponding
to Pd = 0.55, 0.6, and 0.65 p.u., respectively, have
been given in Fig. 3(b). Positive values in Fig. 3(b) show
net gain/loss in stored energy in the BESS, as compared
to the battery initial stored energy level. For specific
value of Pd, the corresponding value of Pb, max
determines the BESS power capacity. To achieve the
goal of dispatching the constant Pd over the designed
period T, the BESS capacity has to be specified to be at
least as large as the
corresponding Pb,max. once the BESS capacity is
designed to be at least as large as Pb,max, the BESS
could absorb/supply the surplus/shortfall in power for the
corresponding constant dispatched level Pd . As
described earlier, besides the power capacity, the battery
energy capacity should also be considered. For the study
undertaken in this paper, the BESS energy capacity is
specified in a similar manner as in the case of BESS
power capacity: the energy capacity of the BESS has to
be as large as that it could absorb/supply the maximum
amount of the charged/discharged energy. Hence, the
BESS energy capacity should be at least as large as
Eb,max for the corresponding Pd value.
44
International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
Figure 3. Simulink model for PMSG
Figure 4. Simulink model for BESS
Figure 5. Simulink model for Convertor
5. SYSTEM CONFIGURATION
Battery Model
Several equivalent battery circuit models have been
reported in the literature. The models are applicable to
study the battery behavior over short- or long-term
intervals during its charge/discharge process [16]. For the
present study, the consideration is for the
charging/discharging processes of the battery for
relatively long-term operations, e.g., over hours/days.
The lead–acid battery model proposed by Ceraolo [17] is
suitable for such an application.
Capacitor used
Characteristics
1. Rated capacitance 100-2000 µF
2. Capacitance tolerance = 10%
3. Rated DC Voltage (Un) max1800 V DC
4. Self-inductance max. 70 nH
5. Typical tan. d (50 Hz) <5.0E−4
6. Series resistance <3 m /1 kHz
7. Filling Resin Dry, UL94, V0
8. Dielectric Self healing MPP aluminium case
without overpressure device
9. Terminals M6, M8 internal threads M8 screw
type’s bolds
10. Maximum rating :- Overvoltage 1.1 x Un
(8h/day)
11. Max. (dV/dt) 25 V/us
Application
I. Hybrid vehicles
II. Wind plants
III. Solar power plants
IV. Electric energy generation from sea waves
V. Medical equipment
VI. Industrial equipment
VII.Car electronics
VIII. Railway and turbines (generator)
IX. Frequency transducer
X. Elevators
6. SYSTEM OUTPUTS
Figure 6. Graph for Capacitor charging (Voltage v/s
Time)
45
International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
Figure 7. Graph for SOC for Battery charging &
discharging
Figure 8. Graph for Power generating in MW
Figure 9. Graph for Convertor output (voltage & curren)
7. CONCLUSION
This research has established that key aspects of the
use of Energy storage can be captured by a simplified
probabilistic approach, which requires only limited input
data. Specific conclusions based on the modeling indicate
the following:
A method to determine the BESS capacity has been
developed with the purpose of not only keeping the
injected power from the wind farm constant, but also to
achieve maximum economic benefit.
The proposed BESS and capacitor sizing procedure
has been demonstrated through simulation studies and
using the wind data obtained from a theoretically wind
farm
Energy storage up to one day cannot exclude energy
curtailment in a weak grid connection.
Energy management incorporating energy storage over
24 hrs and energy curtailment can allow up to three times
the amount of wind energy to be absorbed by a weak grid
compared to conventional grid connection of wind farms.
The impact of energy capacity has been sidestepped in
this study through the assumption of a storage capacity
that is large enough for the time scale considered.
Nevertheless, the conclusions should be valid provided
reasonably generous storage capacities are used of the
orders of magnitude estimated.
REFERENCES
[1] J. P. Barton and D. G. Infield, “Energy storage and
its use with intermittent renewable energy,” IEEE
Trans. Energy Convers., vol. 19, no. 2, pp. 441– 448,
Jun. 2004.
[2] P. F. Ribeiro, B. K. Johnson, M. L. Crow, A. Arsoy,
and Y. L. Liu, “Energy storage systems for advanced
power application,” in Proc. IEEE, vol. 89, no. 12,
pp. 1744–756, Dec. 2001.
[3] C. Carrillo, “Análisis y simulación de
sistemaseólicosaislados,” Ph.D. dissertation (in
Spanish), Universidade de Vigo, Spain, 2001.
[4] T. Hennessy and M. Kuntz, “Flow battery storage
application with wind power,” in Proc. IEEE PES
Transmiss. Distrib. Conf. Expo., Dallas, May 2006,
pp. 937–939.
[5] R. Karki, P. Hu, and R. Billinton, “A simplified
wind power generation model for reliability
evaluatuin,” IEEE Trans. Energy Convers., vol. 21,
no. 2, pp. 533–540, Jun. 2006.
[6] G. Sideratos and N. D. Hatziargyriou, “An advanced
statistical method for wind power forecasting,” IEEE
Trans. Power Syst., vol. 22, no. 1, pp. 258–265, Feb.
2007
[7] W. Li, G. Joos, and C. Abbey, “Attenuation of wind
power fluctuations in wind turbine generators using
a dc bus capacitor based filtering control scheme,” in
46
International Journal of Research in Advent Technology, Vol.4, No.2, February 2016
E-ISSN: 2321-9637
Available online at www.ijrat.org
Proc. IEEE 41st IAS Annu. Meet., Florida, Oct.2006,
pp. 216–220.
[8] T.-Y. Lee and N. Chen, “Optimal capacity of the
battery energy storage system in a power system,”
IEEE Trans. Energy Convers., vol. 8, no. 4, pp. 667–
673, Dec. 1993.
[9] J. N. Baker and A. Collinson, “Electrical energy
storage at the turn of the millennium,” Inst. Elect.
Eng. Power Eng. J., vol. 13, no. 3, pp. 107–112, Jun.
1999.
[10]S. Mathew, Wind Energy, Fundamentals, Resource
Analysis and Economics. Berlin, Germany: Springer-
Verlag, 2006.
[11]S. Heier and R.Waddington, Grid Integration of
Wind Energy Conversion Systems, 2nd ed. Hoboken,
NJ: Wiley, 2006.
[12]C. Luo and B.-T.Ooi, “Frequency deviation of
thermal power plants dueto wind farms,” IEEE
Trans. Energy Convers., vol. 21, no. 3, pp. 708–
716,Sep. 2006.
[13]C. Carrillo, A. E. Feijoo, J. Cidras, and J. Gonzalez,
“Power fluctuationsin an isolated wind plant,” IEEE
Trans. Energy Convers., vol. 19, no. 1,pp. 217–221,
Mar. 2004.
[14]S. Nomura, Y. Ohata, T. Hagita, H. Tsutsui, S. Tsuji-
Iio, and R. Shimada,“Wind farms linked by SMES
systems,” IEEE Trans. Appl. Supercond.,vol. 15, no.
2, pp. 1951–1954, Jun. 2005.
BIOGRAPHIES
1) Sandeep Tapre received the B.E. degree in electrical
engineering from the P.E.S College of Engineering,
Aurangabad (M. S.), India.Presently; he is an M E (EPS)
student at MSS’S College of Engineering & Technology
Jalna (M.S.), India.
2) K.Venkata Rama Mohan received the B.Tech.
degree in electrical and Electronics Engineering from
S.K.T.R.M.C.E College . (M.S.), India, the M.TECH.
(EPS) degree from S.P.R.C.E.T, India, & Presently, he is
working as Asst. Professor , at MSS’S College of
Engineering & Technology Jalna (M.S.), India.
47

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Paper id 42201607

  • 1. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org 42 BESS at Point of Common Coupling for Wind Farm Sandeep Tapre, Prof.K.Venkata Ramamohan M.E (student), Professor MSS’s College of Engg. Jalna sandeep.tapre85@rediffmail.com, ram.mohan822@gmail.com Abstract- A computational procedure to determine the Battery energy storage system capacity and the evaluation of the voltage .This paper presents the results of a wind data and provide effectively continuous power for the consumers or grid without any disturbance. It also examined for the purpose of attenuating the effects of unsteady input power from wind farms. A novel 2 wind generating plants at Point of common coupling, Battery storage-based power allocation method also is proposed. The effectiveness of these methods was verified using MATLAB/SIMULINK software. 1. INTRODUCTION Wind power is the fastest-growing renewable energy source, but one of the typical problems of wind energy converters (WECs) is the variation in their delivered power, which is the main cause of the relationship between the random nature of wind and the power. The purpose of the present investigation is to fill in the gap in the aforementioned daily load-tracking application. It addresses the design of a BESS, incorporated into a power buffer for the wind farm. While the BESS possesses higher energy capacity than several other energy storage media, and hence, it is suitable for the long-term load-tracking operation [1], BESS is also shown to be cost-effective for use in power systems [2]. However, nowadays it is common to find wind converters where an electronic converter is used to connect the generator to the network, so the delivered power can be smoothed [3]. The purpose of this paper is to investigate the periodic power pulsations that have been measured during the day and give continuous power. The loads on an electricity supply system, which are reflected in the spot price of electricity, vary according to the time of day, day of the week, season, and also other, unpredictable factors. For the wind farm application, for example, a flow battery system has been described in [4], although the authors have yet to provide a method by which the battery capacity can be determined. Thus, the present investigation proposes a methodology to determine the required BESS capacity for the purpose of daily load tracking or load leveling. The method is based on a given wind power profile and the optimization of an objective function through which the Optimal dispatched power level from the wind farm will be obtained. 2. MODEL DESCRIPTION This paper is organized as follows. PMSG is interconnected with the grid through a fully rated converter so that the variable ac frequency at the generator terminal is converted to steady grid frequency at the output. Here two plants are to be considering which are join at PCC through the PWM Generator as shown in Fig 1. Also it shows that the wind energy captured by the turbine blades is converted through the PMSG into electrical power, denoted by Pw. From previous references, it is clear that Pw tends to be highly stochastic, and an effective way to describe Pw could be through statistical means [5], [6]. Alternatively, as part of the wind farm planning, site selection, and design process, wind data are often collected at site if such data of (say) past few years are unavailable. As the main focus of this paper is on the design of the BESS, it is now assume that sufficient wind data are available and the profile of Pw is known over a period of T h. Fig. 2 shows a typical profile of Pw, derived from the wind speed data .In the figure, Pw has been normalized, and hence is within the range [0, 1] per unit (p.u.). All wind speed distributions were corrected to a long- term mean wind speed of 12 m/s. At short time scales. As per Fig. 1 the system configuration of a direct drive PMSG based grid interfaced WECS. A horizontal axis wind turbine is used to drive the PMSG. A surface mounted non salient pole type PMSG is used. The kinetic energy presents in the wind is converted into the mechanical torque using a wind turbine. Mechanical energy is converted into electrical energy using a PMSG. To facilitate variable speed operation for achieving MPPT, the PMSG cannot be interfaced with the grid directly. Therefore, two VSCs are used in back to back configuration with common DC link known as a MSC and a GSC. These VSC’s are controlled independently. 42
  • 2. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org Figure 1. Variable speed wind turbine with interconnection to the mains grid through BESS. Figure 1. Typical wind power profile based on data taken: constant Pd is shown. One can assume that the power loss in the two converters is negligible. The dc-link capacitor C functions as harmonics filter, and in some designs, it can also take the role of the energy-storage system [7]. However, typical energy storage capacity of the capacitor tends to be small compared to the BESS considered in the study. Hence, in terms of initial power flow analysis, the capacitor power may be neglected. It is further assumed that the dispatched power Pd from CON2 to the mains grid is to be kept constant over the interval T. Although this assumption tends to facilitate analysis, it also has a desirable effect from a practical viewpoint: it prevents the fluctuating Pw from impacting negatively on the grid, in terms of network voltage and frequency profiles. To realize the constant power feature, the mismatch power between Pw and Pd has to be compensated for by the BESS, which has the output Pb (t), shown in Fig. 1. 3. CONTROL ALGORITHM The block diagram of the proposed control scheme as in Fig. 1, The MSC controls the active power of the PMSG to achieve MPPT and the GSC regulates the DC link voltage under change in active power output from the PMSG. The control scheme for the MSC and the GSC are as follows: A. Machine Side Converter (MSC) Control The MSC is controlled in rotor reference frame and the phasor diagram. The stator resistance of a PMSG is negligible which is practically valid in MW size of generators. The rotor flux linkage is aligned with the d- axis of the synchronous reference frame. All vectors along with dqaxis frame rotate in space at synchronous speed ωs which is also the rotor speed of the generator ωr. The stator current vector is is perpendicular to the rotor flux vector λr. B. Mathematical model The following table shows the definition of various variables used in this model: E = Kinetic Energy (J) Ρ = Density (kg/m3) M = Mass (kg) A = Swept Area (m2) V = Wind Speed (m/s) Cp = Power Coefficient P = Power (W) r = Radius (m) Under constant acceleration, the kinetic energy of an object having mass m and velocity v is equal to the work done W in displacing that object from rest to a distance s under a force F i.e. E =W = Fs According to Newton’s Law, we have: F = ma Hence, E = mass … (1) Using the third equation of motion: PWM CvAP 3 2 1 ρ= (1) v 2 = u2 + 2as and as per paper [10]. A German physicist Albert Betz concluded in 1919 that no wind turbine can convert more than 16/27 (59.3%) of the kinetic energy of the wind into mechanical energy turning a rotor. To this day, this is known as the Betz Limit or Betz'Law. The theoretical maximum power efficiency of any design of wind turbine is 0.59 (i.e. no more than 59% of the energy carried by the wind can be extracted by a wind turbine). This is called the “power coefficient” and is defined as: C pmax = 0.59 Also, wind turbines cannot operate at this maximum limit. The Cp value is unique to each turbine type and is a function of wind speed that the turbine is operating in. Once we incorporate various engineering requirements of a wind turbine - strength and durability in particular – the real world limit is well below the Betz Limit with values of 0.35-0.45 common even in the best designed wind 43
  • 3. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org turbines. By the time we take into account the other factors in a complete wind turbine system - e.g. the gearbox, bearings, and generator and so on - only 10- 30% of the power of the wind is ever actually converted into usable electricity. Hence, the power coefficient needs to be factored in equation (4) and the extractable power from the wind is given by: PWavail CvAP 3 2 1 ρ= (2) Where ρ is the air density which is approximately equal to 1.2 kg/m3 this study; where Cp is the power coefficient considered 0.48 for this wind turbine; A is the sweep area of turbine blades in m2 and υw is the wind velocity in m/s. In direct drive system, due to the absence of a gear box, the mechanical torque (TM) and the shaft speed of the wind turbine are directly transferred to the shaft of the generator. The mechanical torque developed by the wind turbine is as, Tm = Pm/wm (3) C. Grid Side Converter (GSC) Control The DC link voltage is selected such that it should be more than peak of the line voltage for satisfactory operation of GSC for controlled active power transfer to the grid. 4. BESS CAPACITY The battery capacity is normally specified in terms of power and energy capacity [9]. The energy capacity describes the energy that can be drawn from or stored in the battery. The power rating determines the power that can be supplied or stored by the battery under rated discharge/charge time interval. The capital cost of the battery can also be determined, based on the power and energy capacities [8]. Consequently, the design problem in hand is to determine the BESS capacity based on a cost-benefit consideration, as shown later. Figure 2. Simulink model for BESS at point of common coupling at wind farm with interconnection to the Loads. Determination of BESS Power and Energy Capacities In the buffer system, the BESS power Pb (t) can be written in terms of Pw and Pd as Pb (t) = Pw − Pd . (4) From (1), for a given constant Pd , Pb (t) will vary in the same manner as Pw. By setting Pd to another constant value will only result in the Pb (t) curve being shifted up or down, but Pb (t) will remain as the same shape as Pw. For example, for the Pw profile given in Fig. 2, the Pb (t) profile given in Fig. 3(a) corresponds to Pd = 0.6 p.u. From Fig. 3(a), one finds that the maximum battery power Pb ,max occurs at T1 when Pb ,max =−0.5 p.u. over the interval T. The negative sign indicates that, at this precise moment, the BESS is discharging. It is quite conceivable for a different value of Pd, the corresponding Pb,max may be positive. It then indicates that the BESS is being charged at the maximum value at that instance. Integration of Pb (t) with respect to time yields the net energy (Eb) injected into or discharged from the BESS, up to time t. Corresponding to the changes in Pb (t), the Eb (t) profile will also vary for different Pd. For instance, Eb (t) profiles corresponding to Pd = 0.55, 0.6, and 0.65 p.u., respectively, have been given in Fig. 3(b). Positive values in Fig. 3(b) show net gain/loss in stored energy in the BESS, as compared to the battery initial stored energy level. For specific value of Pd, the corresponding value of Pb, max determines the BESS power capacity. To achieve the goal of dispatching the constant Pd over the designed period T, the BESS capacity has to be specified to be at least as large as the corresponding Pb,max. once the BESS capacity is designed to be at least as large as Pb,max, the BESS could absorb/supply the surplus/shortfall in power for the corresponding constant dispatched level Pd . As described earlier, besides the power capacity, the battery energy capacity should also be considered. For the study undertaken in this paper, the BESS energy capacity is specified in a similar manner as in the case of BESS power capacity: the energy capacity of the BESS has to be as large as that it could absorb/supply the maximum amount of the charged/discharged energy. Hence, the BESS energy capacity should be at least as large as Eb,max for the corresponding Pd value. 44
  • 4. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org Figure 3. Simulink model for PMSG Figure 4. Simulink model for BESS Figure 5. Simulink model for Convertor 5. SYSTEM CONFIGURATION Battery Model Several equivalent battery circuit models have been reported in the literature. The models are applicable to study the battery behavior over short- or long-term intervals during its charge/discharge process [16]. For the present study, the consideration is for the charging/discharging processes of the battery for relatively long-term operations, e.g., over hours/days. The lead–acid battery model proposed by Ceraolo [17] is suitable for such an application. Capacitor used Characteristics 1. Rated capacitance 100-2000 µF 2. Capacitance tolerance = 10% 3. Rated DC Voltage (Un) max1800 V DC 4. Self-inductance max. 70 nH 5. Typical tan. d (50 Hz) <5.0E−4 6. Series resistance <3 m /1 kHz 7. Filling Resin Dry, UL94, V0 8. Dielectric Self healing MPP aluminium case without overpressure device 9. Terminals M6, M8 internal threads M8 screw type’s bolds 10. Maximum rating :- Overvoltage 1.1 x Un (8h/day) 11. Max. (dV/dt) 25 V/us Application I. Hybrid vehicles II. Wind plants III. Solar power plants IV. Electric energy generation from sea waves V. Medical equipment VI. Industrial equipment VII.Car electronics VIII. Railway and turbines (generator) IX. Frequency transducer X. Elevators 6. SYSTEM OUTPUTS Figure 6. Graph for Capacitor charging (Voltage v/s Time) 45
  • 5. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org Figure 7. Graph for SOC for Battery charging & discharging Figure 8. Graph for Power generating in MW Figure 9. Graph for Convertor output (voltage & curren) 7. CONCLUSION This research has established that key aspects of the use of Energy storage can be captured by a simplified probabilistic approach, which requires only limited input data. Specific conclusions based on the modeling indicate the following: A method to determine the BESS capacity has been developed with the purpose of not only keeping the injected power from the wind farm constant, but also to achieve maximum economic benefit. The proposed BESS and capacitor sizing procedure has been demonstrated through simulation studies and using the wind data obtained from a theoretically wind farm Energy storage up to one day cannot exclude energy curtailment in a weak grid connection. Energy management incorporating energy storage over 24 hrs and energy curtailment can allow up to three times the amount of wind energy to be absorbed by a weak grid compared to conventional grid connection of wind farms. The impact of energy capacity has been sidestepped in this study through the assumption of a storage capacity that is large enough for the time scale considered. Nevertheless, the conclusions should be valid provided reasonably generous storage capacities are used of the orders of magnitude estimated. REFERENCES [1] J. P. Barton and D. G. Infield, “Energy storage and its use with intermittent renewable energy,” IEEE Trans. Energy Convers., vol. 19, no. 2, pp. 441– 448, Jun. 2004. [2] P. F. Ribeiro, B. K. Johnson, M. L. Crow, A. Arsoy, and Y. L. Liu, “Energy storage systems for advanced power application,” in Proc. IEEE, vol. 89, no. 12, pp. 1744–756, Dec. 2001. [3] C. Carrillo, “Análisis y simulación de sistemaseólicosaislados,” Ph.D. dissertation (in Spanish), Universidade de Vigo, Spain, 2001. [4] T. Hennessy and M. Kuntz, “Flow battery storage application with wind power,” in Proc. IEEE PES Transmiss. Distrib. Conf. Expo., Dallas, May 2006, pp. 937–939. [5] R. Karki, P. Hu, and R. Billinton, “A simplified wind power generation model for reliability evaluatuin,” IEEE Trans. Energy Convers., vol. 21, no. 2, pp. 533–540, Jun. 2006. [6] G. Sideratos and N. D. Hatziargyriou, “An advanced statistical method for wind power forecasting,” IEEE Trans. Power Syst., vol. 22, no. 1, pp. 258–265, Feb. 2007 [7] W. Li, G. Joos, and C. Abbey, “Attenuation of wind power fluctuations in wind turbine generators using a dc bus capacitor based filtering control scheme,” in 46
  • 6. International Journal of Research in Advent Technology, Vol.4, No.2, February 2016 E-ISSN: 2321-9637 Available online at www.ijrat.org Proc. IEEE 41st IAS Annu. Meet., Florida, Oct.2006, pp. 216–220. [8] T.-Y. Lee and N. Chen, “Optimal capacity of the battery energy storage system in a power system,” IEEE Trans. Energy Convers., vol. 8, no. 4, pp. 667– 673, Dec. 1993. [9] J. N. Baker and A. Collinson, “Electrical energy storage at the turn of the millennium,” Inst. Elect. Eng. Power Eng. J., vol. 13, no. 3, pp. 107–112, Jun. 1999. [10]S. Mathew, Wind Energy, Fundamentals, Resource Analysis and Economics. Berlin, Germany: Springer- Verlag, 2006. [11]S. Heier and R.Waddington, Grid Integration of Wind Energy Conversion Systems, 2nd ed. Hoboken, NJ: Wiley, 2006. [12]C. Luo and B.-T.Ooi, “Frequency deviation of thermal power plants dueto wind farms,” IEEE Trans. Energy Convers., vol. 21, no. 3, pp. 708– 716,Sep. 2006. [13]C. Carrillo, A. E. Feijoo, J. Cidras, and J. Gonzalez, “Power fluctuationsin an isolated wind plant,” IEEE Trans. Energy Convers., vol. 19, no. 1,pp. 217–221, Mar. 2004. [14]S. Nomura, Y. Ohata, T. Hagita, H. Tsutsui, S. Tsuji- Iio, and R. Shimada,“Wind farms linked by SMES systems,” IEEE Trans. Appl. Supercond.,vol. 15, no. 2, pp. 1951–1954, Jun. 2005. BIOGRAPHIES 1) Sandeep Tapre received the B.E. degree in electrical engineering from the P.E.S College of Engineering, Aurangabad (M. S.), India.Presently; he is an M E (EPS) student at MSS’S College of Engineering & Technology Jalna (M.S.), India. 2) K.Venkata Rama Mohan received the B.Tech. degree in electrical and Electronics Engineering from S.K.T.R.M.C.E College . (M.S.), India, the M.TECH. (EPS) degree from S.P.R.C.E.T, India, & Presently, he is working as Asst. Professor , at MSS’S College of Engineering & Technology Jalna (M.S.), India. 47