Upload
others
View
2
Download
0
Embed Size (px)
Citation preview
FUZZY BASED EV CHARGING WITH
REDUCED POWER FLUCTUATION
UNDER RENEWABLE POWER
CONSUMPTION CONSTRAINT
1Kavin.R
2Kesavan.T
3 Dr.Nandagopal.V
4Malini.T
Email: [email protected]
1,2&4 Assistant Professor,
3Professor Department of Electrical and Electronics Engineering, Sri Krishna
College of Engineering & Technology
Abstract
Based on environmental condition we can reduce the power consumption in domestic
load by using light and temperature sensor in the logic of fuzzy and also stabilize the grid power
.In this paper proposes that more number of vehicle can charge at same time in different places.
Our proposed model aims to minimize the total electricity cost considering user comfort, house
occupancy and EV travel patterns, thermal dynamics, EV electricity demand, and other operation
constraints.
I. INTRODUCTION
International Journal of Pure and Applied MathematicsVolume 119 No. 18 2018, 1691-1706ISSN: 1314-3395 (on-line version)url: http://www.acadpubl.eu/hub/Special Issue http://www.acadpubl.eu/hub/
1691
DEMAND SIDE management in the residential sector (i.e., residential buildings) is an
important research topic since buildings contribute a significant fraction of overall electricity
consumption. In fact, it accounted for 72% of total U.S. energy consumption in 2006 out of that
residential buildings accounted for 51% according to the U.S. Environmental Protection Agency
(EPA) [1]. This research topic has received lots of attention from the research community [2]–
[8]. In [2], Shengnan et al. assessed the use of demand response as a load shaping tool to
improve the distribution transformer utilization and avoid overloading for the transformer.
Mohsenian-Rad et al. [3] proposed an optimization framework that aims to minimize electricity
bills considering user comfort. However, the assumption on homogeneous appliances and using
waiting time to represent user comfort in this paper would be too simple to represent different
characteristics of grid appliances and user requirements. In a typical grid, thermostatically
controlled appliances (TCAs) including refrigerator, electric water heater, and the heating,
ventilation, and air-conditioning (HVAC) system account for more than half of total residential
energy consumption [1]. Research on optimal control for TCA loads has been a hot research
topic in the last several years. References [4] and [5] proposed optimal control schemes to
minimize the electricity cost for the HVAC system considering user climate comfort.
Dynamic programming was employed in [6] to compare several optimal control algorithms
applied to a thermostat. In [7], the authors introduced an appliance commitment algorithm that
schedules electric water heater power consumption to minimize user payment.
Electric vehicle (EV) is another important grid element that has significant economic and
environmental advantages compared to normal cars. The penetration of EVs is expected to
increase drastically in the next few years, which can reach one million by 2015 in US [9].
Therefore, EV charging will have significant impacts on the power distribution network if it is
not controlled appropriately [10]–[12]. EV travel pattern is an important factor to model potential
impacts of EVs on the grid [13], [14] and to develop efficient EV charging strategies [15].
Given electricity prices and EV driving pattern, Rotering et al. proposed a dynamic
programming based control scheme to optimize the charging for one EV [16]. In [17], Wu et al.
considered load scheduling and dispatch problem for a fleet of EVs in both the day-ahead market
and real-time energy market. In [18], an optimal charging strategy for EVs was proposed that
considers voltage and power constraints.
The problems of scheduling of grid energy usage and EV charging are often addressed
separately in the literature. In this paper, we propose a unified optimization model that jointly
optimizes the scheduling of EVs and TCAs. In particular, we utilize EVs as dynamic storage
International Journal of Pure and Applied Mathematics Special Issue
1692
facility to supply energy for residential buildings during peak hours where energy can be
transferred from EVs to charge other EVs and to provide energy for HVAC in a residential
community. There are some recent works that discuss potential benefits of vehicle to building
interactions [19], [20]. However, to the best of our knowledge, none of previous works have
considered detailed design and joint optimization of EV and building energy management.
The main contributions of this paper can be summarized as follows:
• We propose a comprehensive model to optimize the EV and HVAC scheduling in a
residential area. The formulation PIUTEA aims to achieve flexible tradeoff between minimizing
total electricity cost and maintaining user comfort preference.The model accounts for the
characteristics of the HVAC system, thermal dynamics, user climate comfort preference, battery
state model, user travel patterns, and grid occupancy patterns. We also discuss potential
extensions of the proposed framework to capture various modeling uncertainty factors.
• We show the impacts of different design and system parameters, which control the
electricity cost and user comfort, on the system operation and performance as well as the
economic benefits of applying our proposed control framework compared to a non-optimized
control scheme for a single-house scenario.
• We illustrate the advantages of applying the proposed control model for the multiple-house
scenario compared to the case where each grid optimizes its energy consumption separately.
Specifically, we demonstrate that optimization of EV and grid energy scheduling for multiple
houses in a residential community can achieve the significant saving in electricity cost and
reduce the high power demand during peak hours.
II CONSTRUCTION OF CHARGINGCONTROL MODEL OF ELECTRIC
VEHICLES
The hourly charging/discharging quantity of each electric vehicleconnected to the system
is used as the state variables in this formulation. The established optimal
Charging/discharging control is expressed as
A. State Variable
International Journal of Pure and Applied Mathematics Special Issue
1693
The charging/discharging power of EVs are chosen as state variables shown
in
Where and represents the charging and dischargingpower of No. i EV at time
t, respectively, andrepresents the maximal charging and discharging power of No.i EV
respectively, , and represent the arrival time and departuretime.
B. Operating Costs
The operating costs consist of energy cost and battery dischargingdegradation cost, described
as follows.
1) Energy Costs: This paper considers the charging/dischargingenergy cost as part of the
objective function, and the
Three-stage electricity price of Taiwan Power Company is used, as shown in Fig. 1. The
energy cost is expressed as
Where represents the electricity price at time t.
2) Battery Discharging Degradation Costs:
International Journal of Pure and Applied Mathematics Special Issue
1694
The V2G operationof an electric vehicle battery will influence battery lifeand increase
operating costs. Reference [17] discussed the revenueand cost of V2G, and proposed a battery
degradation costmodel. This model is suitable for the economic analysis of V2G.Therefore, the
V2G battery degradation cost is calculated bythis model in this paper. The charging and
discharging powerare under the rated values to protect the battery in the proposedmodel.
However, if the power company wants to draw morepower form vehicles, the battery
degradation cost can be calculatedbased on models proposed in [26] and [27] that have
discussedeffects of currents and temperatures on the battery cyclelife.Degradation cost is
calculated as wear for V2G due to extracycling of a battery. For a battery vehicle, is expressed as
[17]
Where is the capital cost of the battery, and is the battery life expressed as kWh
(described below).Battery lifetime is often expressed in cycles, and measured ata specific depth-
of-discharge. For (4), we express battery life in
Energy throughput defined as follows [17]:
Where is the lifetime in cycles , the total energy storageof the battery, and DoD is the
depth-of-discharge for which was determined.
To sum up, the objective function of this paper is expressedAs
Where is the battery discharging cost per kWh of vehicle .Take the Li-ion battery as an
example? The battery cost perkWh is USD 350, Nisson Leaf battery capacity is 24 kWh, 2000
Life cycles in 80% DoD, , and
0.2188 USD.
International Journal of Pure and Applied Mathematics Special Issue
1695
b. Constraint of Convenient Driving for EV Owner
When an EV is charged or discharged, the SOC value of thebattery must be between a
minimum value and maximum valuewhen the EV is connected to the power grid, and the set
SOCvalue must be reached before the electric vehicle owner leaves, which is expressed as
Where represents the initial value of SOC of theelectric vehicle,
represents the minimum value of SOC of the th EV, represents the charging
anddischarging efficiencies of the battery, respectively,
Represents the battery capacity of No. i EV, andrepresents the
expected SOC value of the battery at departureof the th EV owner.
D. System Constraints
When the aggregator controls EV charging and discharging, the constraints of system voltage
and line overload must beconsidered, as the power company hopes to reduce
equipmentinvestment expenses through appropriate charging and dischargingcontrol, these
constraints are described as follows.
1) Constraint of System Voltage: The voltage drop of eachline can be determined by [28]
Where is the voltage drop, R is the line resistance, X is theline reactance, P is the active
power through the line, Q is thereactive power through the line, and is the system voltage.
As shown in the distribution system of Fig. 2, the voltage drop of Line 1 is expressed as
Where, and are the original real and reactive power of node n at time t, and is the power
fromEVs of node n at time t. For the sake of explanation, Fig. 2 is
International Journal of Pure and Applied Mathematics Special Issue
1696
a simplified system diagram. A practical distribution system of TPC used as the test studies is
given in Section IV.The constraint of system voltage drop is established by (9), take node 4 as an
example, the constraint of voltage drop isexpressed as
Constraint of System Line Current:
The cable of a systemline has its acceptable maximum current value, where
overloadedoperation may damage the line, causing accidents. Becausethe real power is much
larger than the reactive power, thereactive power is neglected in order to maintain the linearity
ofthis formulation. The line current constraint is expressed as
International Journal of Pure and Applied Mathematics Special Issue
1697
International Journal of Pure and Applied Mathematics Special Issue
1698
III.EVPARAMETER SIMULATION
Based on the survey and measured data, EV usage scenariosare randomly simulated in this
paper, and stochastic models ofthese parameters are described [9] below.
1) EV Start Charging Time: The starting time of electricvehicle charging is related to the life
style of electric vehicleowners, and information can be obtained from measured valuesand
statistics [29], [30]. Fig. 3 is the distribution diagram of thestarting time of EV charging in an
EPRI report [30]. A distributionbased on Roulette wheel selection concept that depicts
theoccurrence frequency of the start charging time is used in thesimulations. The Roulette wheel
surface is divided into wedgesrepresenting the probabilities for each individual. The wedge kof
the stochastic model is calculated by
Where is the probability of the the representative load profile. Fig. 4 shows an unequally
divided uniform distribution ofstart charging time that is based on the probability densityshown
in Fig. 3. Random numbers can be generated to determinestart charging time of each vehicle. If
the number is between and , the th start charging time is selected.A start
charging time with higher probability is more likely tobe selected.
where is the charging power, is the
conversion efficiencyof charger, BatCap is the EV's battery capacity, and denote the
starting time and finishing time of charging, respectively.Based on measured values, Fig. 5
shows the probabilitydensity function of SOC values of a battery at the start ofcharging. Using
the same Roulette wheel selection conceptdescribed above, Fig. 6 shows an unequally divided
uniformdistribution of SOC at start charging time that is based on theprobability density shown
in Fig. 5. A.
International Journal of Pure and Applied Mathematics Special Issue
1699
IV. PROPOSED SYSTEM
BLOCK EXPLANATIONS Grid power: This is the grid power from where the source 230V Ac is obtained.
Ac –Dc converter: This is a rectifier, which converts 230V ac into 320V Dc.
Dc-Ac inverter: This is an inverter whose switching pulses can be controlled through
external drive circuits. So output easily controllable through PWM.
Load: A CFL lamp or any common AC load (230V)
E VEHICLE BATTERY – This is 12V battery, which is charged to drive a BLDC or
Switched reluctance motors. (May be we can such devices in series to build the voltage.
Fuzzy control – This is a method of Artificial intelligence to decide the PWM pulses based
on the various constraints inside a grid related to power consumption. Eg. Temperature, lighting
conditions, user comfort etc.
International Journal of Pure and Applied Mathematics Special Issue
1700
HARDWARE IMPLEMENTATION
VCC
VCC
VCC
U1
8052
31
19
18
9
12131415
12345678
3938373635343332
2122232425262728
171629301110
EA/VP
X1
X2
RESET
INT0INT1T0T1
P1.0/T2P1.1/T2XP1.2P1.3P1.4P1.5P1.6P1.7
P0.0P0.1P0.2P0.3P0.4P0.5P0.6P0.7
P2.0P2.1P2.2P2.3P2.4P2.5P2.6P2.7
RDWR
PSENALE/P
TXDRXD
U2
555alt1
2
3
4
5
6
7
8
GND
TRIGGER
OUTPUT
RESET
CONTROL
THRESHOLD
DISCHARGE
VCC
R31k
R410k
C10.1
R9
100k
1 234
MOSFET DUAL G/N23
1
4
T1
TRANSFORMER
1 5
4 8
1k
1k1k
1k1k1k
R61k
Q2BC547
12
3
K1
RELAY SPDT
35
412
Q2BC547
12
3
K1
RELAY SPDT
35
412
Q2BC547
12
3
K1
RELAY SPDT
35
412
K1
RELAY SPDT
35
412
Q2BC547
12
3
Q2BC547
12
3 Q2BC547
12
3
K1
RELAY SPDT
35
412
K1
RELAY SPDT
35
412
BT3
4V1
2
BT3
4V
12
LDR
R810k
Thermister
R810k
Switch1 2
Switch
1 2
1k 1k
11.0592Mhz
33pf
33pf
Switch
1 2
SoCEoC
D1
D2
D3
D4D5
D6
D7
D8
A0A1A2
100809
photovoltaicLoad
IN0
IN1
Grid
Fan
Step down transformer
Step down transformer converts a line voltage of 230 V into a voltage of 4.5 volts ac without
any change in the frequency. It remains unchanged as 50 Hz. The current capability that it can
withstand is about 500 mA. The voltage will be usually slightly higher than the specified voltage.
At load conditions the voltage will be the same as it has been mentioned in the transformer. The
value specified in the transformer is just the RMS value of the voltage.
Rectifier
Rectifier is of two types, as it is known already as center tapped rectifier and bridge rectifier
in the case of full rectifier. It is known that we are not going for half wave rectifier because it
will give an efficiency of only 40% approximately. Bridge rectifier needs four diodes whereas
the center tapped rectifier requires only two diodes. We have used a center tapped transformer.
Filter:
The rectified components are still Ac in nature because it never stays constant at a particular
voltage so it may be told as a varying DC or pulsating DC. So it has to be properly filtered. In
International Journal of Pure and Applied Mathematics Special Issue
1701
other words we can say that the line frequency has to be eliminated from the voltage. In order to
get the pure DC we have to employ the capacitor filter. Because it is the cheapest filter available
in the market. Even we can go for inductive filter. We are not doing so because it is bulky in
nature and also by cost wise it is not compatible with capacitors,
The power supply is extracted from a step down transformer via a rectifier and 7805 voltage
regulator. +5V supply is given to all the ICs used in the project.
Temperature is sensed from a thermistor and its voltage equivalent is sent to the
COMPARATOR to input PORT ‘. Similarly light is sensed through a LDR. These voltages will
be in the order of 0 to 5V. For example when the temperature exceeds 35 deg, C comparator
sends a ‗1‘ to a pin, if light exceeds a threshold, it sends ‗1‘.
Any information or status will be displayed in 2x16 LCD via port P0. For switching on the
load based on the light and temperature, Resistor divider based control chosen by choosing a gate
resistance via relay. In the same way, if any abnormal voltage arises, the relay is switched off via
another port as shown in the circuit. Buzzer is also done as in the same way. Anything abnormal
will be informed via a buzzer alert.
The power saved in excess can be utilized to charge the batteries of the E – vehicle.
As soon the panel is exposed to light, the battery gets charged, and simultaneously the
temperature and light in lumens value is sensed through the thermistors and LDR.
Also an MPPT controller using a mosfet is realized, for which the gate pulses are applied
from IC 555 which works in astable mode.
The speed of the fan and intensity of the light is controlled through a current controller
realized by a 40W, 35 ohms resistor. Here fuzzy logic is applied based on a rule base,
programmed in 89s52. Hence this saves almost 20% of power consumption and absorbs less
power from the Grid supply. The tappings from the series resistor is controlled through the
relays activated by micro controller 89s52 via ports p2.0, p2.1, p2.3 to p2.6
V. CONCLUSION
If EVs are popularized, uncontrolled charging will bring aserious impact on the power
system. In order to reduce the impactof EVs on the power system, the EV client-side must
beappropriately managed. An optimal charging/discharging controlmodel of EVs is proposed in
this paper, which can reduce the impact of EVs on the power systems. The test results showthat
the present electricity price of the Taiwan Power Companyand battery costs are inapplicable to
International Journal of Pure and Applied Mathematics Special Issue
1702
the V2G operation, butthrough the charging-only control still can save a great amountof energy
cost. With rising environmental considerations, thedevelopment of nuclear power plants and
thermal power plantswill certainly be severely challenged, and such power sources atlower
generating costs will be more and more difficult to obtain.Thus, the power companies must put
efforts in managing thedemand response. This paper implements optimal charging/discharging
Control for EVs, assuming the power company purchasesV2G energy at 1.5 times the
electricity price in peak loadhours, and the future battery costs decrease to half of the
currentlevel. In this case, V2G becomes a feasible scheme, as operationcost can be greatly
reduced for users, and the power companycan suppress the increase in peak load, thus reducing
systemlosses, and both the power company and users are benefited.
REFERENCES
[1] rong-cengleou,‖optimal charging/discharging control of electric vehicle
considering power system contraints& operation cost‖ in procIEEE, june 2015.
[2] J. A. P. Lopes, F. J. Soares, and P. M. R. Almeida, ―Integration ofelectric
vehicles in the electric power system,‖ Proc. IEEE, vol. 99,no. 1, pp. 168–183,
Jan. 2011.
[3] S. Srinivasaraghavan and A. Khaligh, ―Time management-
deterministicscheduling of a fleet of plug-in hybrid vehicles for distributed
generation,‖IEEE Power & Energy Mag., pp. 46–53, Jul./Aug. 2011.
[4] C. M. Chan, H. R. Liou, and C. N. Lu, ―Operation of distributionfeeders with
electric vehicle charging loads,‖ in Proc. IEEE 15th Int.Conf. Harmonics and
Quality of Power, 2012, pp. 695–700.
[5] R. Liu, L. Dow, and E. Liu, ―A survey of PEV impacts on electricutilities,‖ in
Proc. IEEE PES Innovative Smart Grid Technol. Conf.,Jan. 2011, pp. 1–8.
[6] J. Dowds, C. Farmer, P. Hines, R. Watts, and S. Blumsack, ―A reviewof results
from plug-in hybrid electric vehicle impact studies,‖ in Proc.43rd Hawaii Int.
Conf. System Sciences, 2010, pp. 1–8.
[7] K. J. Dyke, N. Schofield, and M. Barnes, ―The impact of transport
electrificationon electrical networks,‖ IEEE Trans. Ind. Electron., vol. 57,no.
12, pp. 3917–3926, Dec. 2010.
[8] K. C. Nyns, E. Haesen, and J. Driesen, ―The impact of charging plug-inhybrid
electric vehicles on a residential distribution grid,‖ IEEE Trans.Power Syst., vol.
25, no. 1, pp. 371–380, Feb. 2010.
International Journal of Pure and Applied Mathematics Special Issue
1703
[9] L. P. Fernández, T. G. S. Román, R. Cossent, C. M. Domingo, andP. Frías,
―Assessment of the impact of plug-in electric vehicles ondistribution networks,‖
IEEE Trans. Power Syste., vol. 26, no. 1, pp.206–213, Feb. 2011.
[10] R. C. Leou, C. L. Su, and C. N. Lu, ―Stochastic analyses of electricvehicle
charging impacts on distribution network,‖ IEEE Trans. PowerSyst., vol. 29, no.
3, pp. 1055–1063, May 2014.
[11] S. Deilami, A. S. Masoum, P. S. Moses, and M. A. S. Masoum,
―Realtimecoordination of plug-in electric vehicle charging in smart gridsto
minimize power losses and improve voltage profile,‖ IEEE Trans.Smart Grid,
vol. 2, no. 3, pp. 456–467, Sep. 2011.
[12] X. Luo and K. W. Chan, ―Real-time scheduling of electric vehiclescharging in
low-voltage residential distribution systems to minimize power losses and
improve voltage profiles,‖ IET Gener., Transm. Distrib.,vol. 8, no. 3, pp. 516–
529, 2014.
[13] M. Esmaili and M. Rajabi, ―Optimal charging of plug-in electric
vehiclesobserving power grid constraints,‖ IET Gener., Transm.Distrib.,vol. 8,
no. 3, pp. 583–590, 2014.
[14] R. A. Verzijbergh, M. O. W. Grond, Z. Lukszo, J. G. Slootweg, and M.D. Ilic,
―Network impacts and cost saving of controlled EV charging,‖IEEE Trans.
Smart Grid, vol. 3, no. 3, pp. 1203–1212, Sep. 2012.
[15] A. O'Connell, D. Flynn, and A. Keane, ―Rolling multi-period optimizationto
control electric vehicle charging in distribution networks,‖ IEEETrans. Power
Syst., vol. 29, no. 1, pp. 340–348, Jan. 2014.
[16] D. B. Richardson, ―Electric vehicles and the electric grid: A review ofmodeling
approaches, impacts, renewable energy integration,‖ Renewable
and Sustain. Energy Rev., vol. 19, pp. 247–254, 2013.
[17] H. Xu, I. U. Eronini, Z. H. Mao, and A. K. Jones, ―Towards
improvingrenewable resource utilization with plug-in electric vehicles,‖ in
Proc.IEEE PES Innovative Smart Grid Technol. Conf., Jan. 2011, pp. 1–6.
[18] W. Kempton and J. Tomic, ―Vehicle-to-grid power fundamentals:
Calculatingcapacity and net revenue,‖ J. Power Source, vol. 144, pp.268–279,
2005.
International Journal of Pure and Applied Mathematics Special Issue
1704
[19] W. Kempton and J. Tomic, ―Vehicle-to-grid power implementation:From
stabilizing the grid to supporting large-scale renewable energy,‖J. Power
Source, vol. 144, pp. 268–279, 2005.
[20] W. Kempton and J. Tomic, ―Using fleets of electric-drive vehicles forgrid
support,‖ J. Power Source, vol. 168, pp. 459–468, 2007.
[21] C. Sandel, U. Franke, N. Ingvar, L. Nordstrom, and R. Hamren, ―Vehicleto
grid—Monte Carlo simulations for optimal aggregator strategies,‖in Proc. Int.
Conf. Power Syst. Technol., 2010, pp. 1–8.
[22] P. S. Martín, G. Sánchez, and G. M. España, ―Direct load control
decisionmodel for aggregated EV charging points,‖ IEEE Trans. PowerSyst.,
vol. 27, no. 3, pp. 1577–1584, Aug. 2012.
[23] S. I. Vagropoulos and A. G. Bakirtzis, ―Optimal bidding strategy forelectric
vehicle aggregators in electricity markets,‖ IEEE Trans. PowerSyst., vol. 28, no.
4, pp. 4031–4041, Nov. 2013.
[24] S. Han, S. Han, and K. Sezaki, ―Development of an optimal vehicleto-grid
aggregator for frequency regulation,‖ IEEE Trans. Smart Grid,vol. 1, no. 1, pp.
65–72, Jun. 2010.
[25] A. Schuller, B. Dietz, C. M. Flath, and C. Weinhardt, ―Charging strategiesfor
battery electric vehicles: Economic benchmark and V2G potential,‖IEEE Trans.
Power Syst., vol. 29, no. 5, pp. 2014–2022, Sep.2014.
International Journal of Pure and Applied Mathematics Special Issue
1705
1706