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College Station, TX
Posted:
November 12, 2012

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Resume:

Impact Analysis of Electric Vehicle Charging on

Distribution System

Qin Yan Mladen Kezunovic

Department of Electrical and Computer Engineering Department of Electrical and Computer Engineering

Texas A&M University Texas A&M University

College Station, TX USA College Station, TX USA

**************@*****.*** *******@***.****.***

compare the impacts. Paper [3] published in 2012 developed a

Abstract With the growing penetration of various types of

probabilistic model for vehicle arriving time and charge left on

electrical vehicles (EVs) such as Plug-in Hybrid Vehicles/

Battery Electric Vehicles (PHEVs/ BEVs), EV charging has the arrival. Paper [4] in 2012 considered both loss and thermal

potential to affect the existing distribution system, especially the models of transformer and analyzed load loss due to current

service lifetime of distribution components. This paper aims at harmonics. The importance of ambient temperatures to the

analyzing the potential impact of EV charging on distribution impact on transformer aging was illustrated in [5]. In this

transformers at residential level. Based on the load consumption paper, the authors combined single residence hourly load from

in East Texas and different assumptions of EV charging RELOAD database and travel demand data from the National

scenarios, the impact is demonstrated and compared on monthly

Household Transportation Survey for EV demand, but they

basis.

applied the same daily base load repeatedly to 365 days

through a year. Paper [6] analyzed the impact over a year

Keywords EV charging scenarios, Transformer loss of life

under different charging scenarios, i.e. simultaneous charging,

staggered charging, and proportional charging. A Monte-Carlo

I. INTRODUCTION

scheme simulated each day of the year, evaluating 100 load

Power transformers are one of the most expensive scenarios, in [7]. In these papers, however, the results for four

components in a distribution network. With the increasing seasons were not separately discussed.

penetration of electric vehicles, new load peak may be created,

Our paper focuses on the impact of electric vehicle

which may exceed the transformer capacity. Therefore, in a

charging on distribution system, especially distribution

residential house, owning an electric vehicle may mean a need

transformers. The actual 15-minute load profiles around

to upgrade the utility s local transformer or lead to early

College Station area (East Texas) available from ERCOT

replacement [1]. Reduction in transformer life expectancy will

website are used as base load [8]. Various charging scenarios

result in an increase of costs to utilities and consumers. Hence,

are assumed under different charging start times, penetration

the reduced transformer life becomes a very important impact

rates and usage ratios. Several EV cases are defined based on

when extra load is taken into consideration. According to the

actual routes in College Station. A MATLAB program is

latest IEEE guide, the relationship between insulation life and

developed to simulate aging acceleration factor and loss-of-

transformer life still remains a question. However, percent loss

insulation life of distribution transformer through a year. The

of total insulation life is usually used to evaluate transformer's

simulation results for four seasons are compared and analyzed.

aging [2].

The paper is organized as follows: Section II describes and

To analyze the impact of electric vehicle (EV) penetration

summarizes base load model, EV model, and transformer

on transformers, three models are required: base load model,

thermal model, which are used for the impact analysis. Based

non-base load (electric vehicle load) model, and transformer

on the total load profiles for different EV charging scenarios

model.

provided in Section II, the aging acceleration factor and the

Non-EV loads are obtained from different sources. Since transformer loss-of-life are simulated in MATLAB. The

there are no actual data for distribution of electric vehicle simulation results for different load profiles are tabulated and

chargers, EV models are based on assumptions of charging illustrated in Section III, and compared with the original base

scenarios with different charging start times and different residential load. Also, a comparison is made between the

penetration rates, or in some cases statistical methods are used results through different seasons. Section IV concludes the

to build models. To analyze the impact on distribution impact analysis (considering potential scenarios of EV

transformers, different factors are used to evaluate and charging in East Texas).

This study is sponsored by NSF I/UCRC: Electric Vehicle

Transportation and Electricity Convergence (EV-TEC) under project titled:

The Impact of PHEV/BEV Charging on Utility Distribution System

vehicle type, or charging duration. For instance, case 1 differs

II. MODELS

from case 3 because case 1 vehicle charges only at home

In this paper, three models are built: base load model, EV

load model, and transformer s thermal model.

A. Base Load Model

Base load is obtained from ERCOT website [8]. Fig. 1

demonstrates 15-minute interval load consumed by an average

residential individual customer for different seasons in East

Texas. Fig. 2 is the daily peak load per residential customer

through 2011. The red points are labeled with the amount and

the exact time of the peak load in that day. In East Texas

where College Station is located, the load consumed in

summer is higher than the load consumed in winter in general.

However, different from the load profile obtained from

RELOAD Database Documentation and Evaluation and Use

in NEMS [5], for some days in February, the peak load

happens in the early morning and is pretty high (For instance,

in 2009, the peak load of the year happened in winter [8]).

Hence, in some winter days (e.g. Feb.11th), the load consumed

Figure 2. Daily peak load per residential customer in East Texas

in the early morning is higher than that in summer days. For

the purpose of fair analysis, the load consumption in Feb.11th TABLE II. EV MODEL CASES

is added to Fig. 1. The results of this phenomenon will be

presented in Section III. Energy Charging

Vehicle Charging SOC

Case Daily Route Needed Duration

Type Location (kWh) (hour)

Home-Work

(9 miles)

Chevy 2.457

1 Work-Shop- Home 59 6.552

Volt (2.5)

Home

(9.2 miles)

Home-Work

(9 miles)

Nissan 1.805

2 Work-Shop- Home 74.2 6.188

Leaf (2.0)

Home

(9.2 miles)

Home-Work

(9 miles)

Chevy Home & 1.242

3 Work-Shop- 79.3 3.312

Volt Work (1.25)

Home

(9.2 miles)

Home-Work

(9 miles)

Figure 1. 15-minute interval data of average residential individual customer Nissan Home & 0.912

4 Work-Shop- 87 3.128

in East Texas Leaf Work (1.0)

Home

(9.2 miles)

B. EV Load Model Home-Work

(22.5 miles)

The EPA estimation results of two representative auto Chevy

5 Work-Shop- Home X X X

models, Nissan Leaf and Chevy Volt, are employed in this Volt

Home

study (in Table I). (22.7 miles)

Home-Work

TABLE I. EPA ESTIMATION RESULTS (22.5 miles)

Nissan 4.482

6 Work-Shop- Home 36 15.368

Leaf (4.5)

Auto EV Battery Electricity Electric Charging Home

Model Type Size Consumption Range Time (22.7 miles)

Home-Work

Nissan 34 kWh / 7 hours

(22.5 miles) Home

EV 24 kWh 73 miles

Chevy 3.065

Leaf 100 miles (240 V)

7 Work-Shop- & 48.9 8.172

Volt (3.0)

Chevy 36 kWh / 6-6.5 hours Home Work

EREV 16 kWh 35 miles

Volt 100 miles (240 V) (22.7 miles)

Home-Work

(22.5 miles) Home

Nissan

Eight EV cases are defined in Table II. Charging duration 8 Work-Shop- & 67.8 7.718 2.25

Leaf

indicates the time required to fully charge the battery. The Home Work

driving cycle for each case is based on the actual routes in (22.7 miles)

College Station [9]. The cases differ in state of charge (SOC),

whereas case 3 vehicle charges both at work and home. Hence start time is defined based on the driving time in Table IV by

case 1 vehicle when reaching home has less state of charge assuming people start driving home from workplace at 5 pm

compared with case 3 vehicle. and charge on arriving home. EV load model for charging on

arriving home is shown in Fig. 3, which will be added to

Since the electric range of Chevy Volt is only 35 miles everyday base load data. Figures 4 and 5 show the daily total

(from Table I), the EV case 5 (from Table II) for Chevy Volt load in one typical day per season for scenarios 2 and 4 with

involving driving from home to work for 22.5 miles and from EV charging on arriving home. Figures 6 and 7 show the total

work to home via supermarket for 22.7 miles, while charging load of a specific day for charging at 1 am and charging at

only at home, is not considered. distributed timing.

Based on different charging start time, three charging

assumptions are defined: charging on arriving home, charging

at 1 am, and charging at distributed timing. Generally

speaking, the peak load of a day happens at early evening

(Fig.1). Thus, without any power management and charge

distribution, charging on arriving (starting to drive back at 5

pm and charging on arrival) may be the worst case of EV

penetration [6]. Usually, it is recommended to charge electric

vehicles at midnight since the load consumption is low then

and it may avoid increasing the existing load peak of the day.

Moreover, the impact of EV charging with a controlled

charging strategy (e.g. distributed charging through a day) will

be analyzed. For each charging assumption, four charging

scenarios are analyzed. In our case study, assuming that the

distribution transformer serves 14 residential households, 4

scenarios are proposed (in Table III): Figure 3. EV load for charging on arriving

Scenario 1 includes 7 electric vehicles (corresponding to

EV cases in Table II), only considering driving to and from

work via supermarket. Scenario 2 includes 14 electric vehicles

(considering each case in Table II twice). Scenario 3 includes

7 electric vehicles, with zero charge at the beginning of

charging. Scenario 4 includes 14 electric vehicles, with zero

charge before charging starts.

TABLE III. CHARGING SCENARIOS

Scenario Vehicle Quantity Usage

Limited to

1 7

Home-Work-Shop-Home

Limited to

2 14

Home-Work-Shop-Home

Charge depleted on

3 7

arriving home Figure 4. Load with EV charging on arriving home - Scenario 2

Charge depleted on

4 14

arriving home

TABLE IV. DRIVING TIME FOR EACH DRIVING CYCLE

Cycle Cycle 1 Cycle 2 Cycle 3 Cycle 4

Work-Shop- Work-Shop-

Home-Work Home-Work

Route Home Home

(9 miles) (22.5 miles)

(9.2 miles) (22.7 miles)

Driving

778-****-**** 2361

Time (s)

Driving

13 29 23 39

Time (min)

The SOC, energy needed, and charging duration in Table

II which indicate limited usage of electric vehicles are used in

scenarios 1 and 2. For charging on arriving home, the charging Figure 5. Load with EV charging on arriving home - Scenario 4

2) Aging acceleration factor and percent loss-of-life:

Aging acceleration factor is a function of ambient

temperature, transformer loading, and certain specific

transformer parameters. Loss of life (LOL) is the equivalent

aging in hours over a time period times 100 divided by the

total normal insulation life in hours at the reference hottest-

spot temperature. Normal insulation life for a transformer is

the expected lifetime when operated with a continuous hot-

spot temperature of 110, which is 180,000 hours in this

paper. Table V shows the specifications used for the

transformer s loss of life calculation [2].

Procedure for calculating the thermal factors:

a) Hottest-spot temperature

b) Aging acceleration factor for every 15 min

Figure 6. Load with EV charging at 1 am August 18th

FAA e (2)

H

c) Equivalent aging factor for each month

N FAA,

FEQA (3)

N

d) Annual average factor and the corresponding percent

loss of insulation life

FEQA

%Loss of life (4)

N

TABLE V. DISTRIBUTION TRANSFORMER PROPERTIES

Symbol Property Units

Ratio of load loss at rated load to no-

R

Figure 7. Load with EV charging at distributed timing August 18th load losses

Oil time constant hr

C. Transformer Thermal Model

Winding time constant min

1) Correlation between load and ambient temperature:

Top-oil temperature rise

Ambient temperature is an important factor in determining,

at rated load

the load capacity of a transformer since the temperature rise Winding hottest-spot rise

for the load should be added to the ambient temperature to,

at rated load

determine operating temperature [2]. n Empirically derived exponent

H A TO H (1) m Empirically derived exponent

Time variable Top-oil rise

where H is the winding hottest-spot temperature which is

Top-oil rise over

used to calculate loss-of-life factor. A is the average ambient

ambient temperature

temperature. The average temperature used in this paper is Time variable winding

the actual data obtained from Weather Channel website [10]. hottest-spot rise

TO is the top-oil rise over ambient temperature, H is the Winding hottest-spot rise

over top-oil

winding hottest-spot rise over top-oil temperature.

Normal insulation life hr

Positive correlation: The electric cooling load is

dominant in summer. Higher temperature will lead to

III. SIMULATION RESULTS

more power consumption, and thus will result in

higher temperature rise. Results of transformer aging acceleration factor and loss of

life according to different EV charging assumptions are

Negative correlation: The temperature is lower in

tabulated in Table VI-VIII. The actual load data for every 15

winter. If the temperature decreases, the electric

minutes through a year are used. The original column in these

heating will increase accordingly.

tables refers to the scenario with no EV charging.

Therefore, generally, the positive correlation provides

more severe transformer duty than the negative one.

TABLE VI. FEQA AND LOL (CHARGING ON ARRIVING HOME)

Original Charging on arriving home

Base

Scenario 1 Scenario 2 Scenario 3 Scenario 4

Load

FEQA 0.0021 0.0757 7.1464 0.1631 20.2431

LOL 0.0104 0.3685 34.779 0.7935 98.5163

TABLE VII. FEQA AND LOL (SCENARIO 2)

Original Scenario 2

Base Charging on Charging at Distributed

Load arriving at 5:00 pm 1:00 am Charging

FEQA 0.0021 7.1464 0.1001 0.0039

LOL 0.0104 34.779 0.4871 0.0192

Figure 8. Monthly FEQ results for Charging on arriving

TABLE VIII. FEQA AND LOL (SCENARIO 4)

Original Scenario 4

Charging

Base Charging Distributed

Month on arriving

Load at 1:00 am Charging

at 5:00 pm

FEQ_

Jan 0.00012 0.785033 0.002730

1.357234

1

FEQ_

Feb 0.00057 2.377044 0.015482

8.422275

2

FEQ_

Mar 1.87E-05 0.028636 0.000109

0.008801

3

FEQ_

Apr 5.62E-05 0.219824 0.000446

0.013729

4

FEQ_

May 0.00021 1.180658 0.002139

0.039392

5

FEQ_

Jun 0.00271 26.33804 0.040787

0.320498

6

FEQ_

Jul 0.00468 42.80368 0.069685

0.557542

7

FEQ_

Aug 0.01597 158.4035 0.263961

1.090655

8

FEQ_

Figure 9. Monthly FEQ results for Scenario 2

Sep 0.00121 10.38140 0.016797

0.122107

9

FEQ_

Figures 8 and 9 indicate that under the same time-of-

Oct 5.21E-05 0.103050 0.000313

0.008600

10

charge, higher penetration rate of electric vehicles will

FEQ_

Nov 2.29E-05 0.046522 0.000176

0.037412

significantly increase transformers loss-of-life factor. With

11

higher penetration rate, the rise of usage ratio will exert even

FEQ_

Dec 3.99E-05 0.249521 0.000646

0.242704

12 more influence on transformers; under the same penetration

rate of electric vehicle, charging at midnight will considerably

decrease the loss-of-life factor, while distributed charging

Year FEQA 0.0021 20.2431 1.0184 0.0344

through the day will help to almost eliminate the impact of EV

charging on distribution transformers.

Year LOL 0.0104 98.5163 4.9563 0.1676

The monthly data in Table VIII are the equivalent aging

factors per month, which are the average value of all the 15

Table VI and Fig. 8 indicate that when charging on min load data of the month (as given in (3)). The fifth column

arriving, scenario 4, which has the highest penetration ratio of in Table VIII shows the results for charging scenario 4 and

EV and requires the most amount of electricity, has much charging at 1 am. It has been mentioned that some days in

higher aging acceleration factor and loss of life. And for February have very high daily peak load and the peak load

scenario 2, as shown in Table VII and Fig. 9, charging on occurs in the early morning. As shown in this column, it is

arriving home tremendously increases loss-of-life factor, obvious that the aging acceleration factor in February is higher

while controlled EV charging will help reduce transformer s than that in summer. The reason may be that the charging

loss of life. event, which begins at 1am with zero charge left in the battery

before charging, will last till early morning, when the peak

load of the day happens. Even though the correlation between

ambient temperature and load in winter is negative, charging months, winter months with peak load (e.g. February in 2011)

at 1 am in February will have more severe impact on should also be considered.

transformer life.

ACKNOWLEDGMENT

IV. CONCLUSION

We would like to express our greatest gratitude to the

In this paper the potential impacts of different EV persons and organizations that supported this Project. Funding

penetration scenarios with different usage and charging start for this project is provided by National Science Foundation

time are discussed and compared. The actual load data, the Industry/ University Cooperative Research Center: Electric

driving routes in College Station, and the real ambient Vehicle Transportation & Electricity Convergence (EV-TEC).

temperature data are employed to simulate the transformer

factors. The result data demonstrate the effect of possible EV REFERENCES

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For charging at 1:00 am, besides the abovementioned summer



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