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Abstract This paper deals with the characterization of the
probability distributions of the aggregated residential load. A
detailed statistical study has been performed on a set of data
referred to single-house extra-urban customers, in order to assess
the time evolution of the average value and standard deviation of
the aggregated load and its possible representation with some
typical probability distributions. The results have shown that the
aggregated residential load data can be satisfactorily represented
by using a Gamma probability distribution with parameters
variable in function of time and number of customers.
Index Terms Residential aggregated load, Probability
distributions, Goodness-of-fit, Monte Carlo simulations.
I. INTRODUCTION
he recent evolution of the electricity systems towards
time-dependent tariff rates and integration of distributed
generation is increasing the importance of assessing the
time evolution of the electricity consumption. Taking into
account the effects of the aggregation of residential loads is
now essential for studying the time evolution of the load in the
distribution system feeders. In fact, the electricity
consumption of the single residential customer is too variable
in time to allow for obtaining a sound estimate of its
individual load pattern [1]. The residential load aggregation
can be obtained by either working directly at the distribution
system level (if the results of measurements carried out on
several feeders are available) [2], or resorting to a bottom-up
approach in which the aggregated load patterns of single-
house customers are computed on the basis of information
obtained from real case investigations on customer behaviour,
lifestyle, and usage of the appliances [3]. In particular, it is
important to assess not only the average value of the
aggregated load, but also how its probability distribution
varies during the day and in function of the number of the
residential customers. Previous studies have shown that the
time evolution of the averagepower, normalized with respect
to the total contract power of the customers, has a predictable
behaviour, especially when the number of customers is
relatively high (e.g., over 100) [4]. Yet, when the number of
customers is low, the possible variations of the load power at
any given time instant are significantly high and strongly
depend on the number of customers and on the randomness in
the customer composition and lifestyle [5].
This paper presents the results of a study aimed at
characterizing the time evolution of the probability
distributions of the aggregated residential load when the
E. Carpaneto and G. Chicco are with the Dipartimento di IngegneriaElettrica, Politecnico di Torino, Corso Duca degli Abruzzi 24, 10129 Torino,Italy (e-mail [email protected], [email protected]).
number of residential customers varies. Starting from the
statistical characterization of the aggregated load patterns of
single-house customers carried out in [4] by using the bottom-
up approach, the aggregated load power has been assessed in
function of the number of residential customers by using
Monte Carlo simulations. Then, a goodness-of-fit analysis has
been extensively performed with several probability
distributions (Normal, Log-Normal, Gamma, Gumbel,
Inverse-normal, Beta, Exponential, Rayleigh and Weibull) inorder to assess which probability distribution fits the
distribution of the load power at each time instant most
satisfactorily. The results obtained allow for establishing a
sound basis to be used within a comprehensive probabilistic
evaluation of the residential load or to be integrated into more
general procedures of analysis where detailed knowledge of
the variability of the residential load patterns is required [6].
Running Monte Carlo simulations is essential to obtain the
customer data for variable numbers of customers. In fact, field
measurements [2,7-9] would be possible only on a pre-
selected set with fixed number of customers. In addition, it is
sometimes difficult to gather only the data of the residential
customers, without superposition of other loads (e.g. buildingservices). This difficulty emerges in particular in urban areas,
where the residential load and the general services of the
buildings are supplied by the same feeder.
Section II of the paper deals with the formation of the data
set for extra-urban customers. Section III illustrates the
characteristics of the statistical tests used. Section IV provides
the numerical results and their discussion. Section V contains
the concluding remarks.
II. FORMATION OF THE DATA SET
The analysis has been structured on the basis of the results
obtained for extra-urban customers in a previous study [4]
carried out by using a comprehensive approach including twophases. In the first phase, a direct investigation of the
customers electricity usage has been performed for a real set
of single-house extra-urban customers. The results were
related to the presence at home of the family members and to
the detailed usage of the appliances, and were processed and
validated on the subset of customers who gave acceptable
information. In the second phase, an overall Monte Carlo
simulation was conducted to form the data set for the
successive statistical study. Different types of days (working
days and weekend days) and periods (summer and winter)
were considered. For space limitations, only the results
obtained for winter working days are presented here.
T
Probability distributions of the
aggregated residential load
Enrico Carpaneto and Gianfranco Chicco
9th International Conference on Probabilistic Methods Applied to Power SystemsKTH, Stockholm, Sweden June 11-15, 2006
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III. PROBABILITY DENSITY FUNCTIONS FOR THE STATISTICAL
TESTS
Various probability distributions have been used for the
goodness-of-fit statistical tests [10], including two one-
parameter distributions (Exponential and Rayleigh), five two-
parameter distributions (Gamma, Gumbel, Weibull, Normal,Log-normal and Inverse Normal), and the three-parameter
Beta distribution (whose third parameter has been set to the
maximum value of the sample data). Table I contains some
details on the probability distributions tested, with the
corresponding expressions of the Probability Density Function
(PDF) and Cumulative Distribution Function (CDF).
The Chi-square, Kolmogorov-Smirnov (KS) and
geometrical adaptation statistical tests have been used for
investigating the goodness-of-fit of the various probability
distributions as a function of the load powerP.
TABLE I
PROBABILITY DISTRIBUTIONS USED FOR THE GOODNESS-OF-FIT TESTSname
PDF
f(P)
CDF
F(P)parameter
limits
Beta 1
11
)()(
)()(+
+ba
ba
cba
PcPba
( )
( ) dxxx
dxxx
ba
cPba
1
0
11
0
11
1
1
= Beta incomplete(P/c,a,b)
0 P c
a > 0
b > 0
Exponential
b
P
eb
1
bP
e1 P 0
b > 0
Gamma( )
b
P
a
a
eab
P 1 ( )
P
b
x
a
a
dxeab
x
0
1
= Gamma incomplete(P/b)
P 0
a > 0
b > 0
Gumbel
b
aP
eb
aP
eeb
1
b
aP
ee1 P
Inverse
Normal
( )
3
2
2
2
bP
eabP
aP
( ) ( )
++
bP
aPerfe
bP
aPerf b
a2
P 0
a > 0
b > 0
Lognormal
( )
2
2
2
2
ln
Pa
e abP
+
2
ln1
2
1
a
bPerf P 0
a> 0
Normal
( )
2
2
2
2
P
e
21
2
1
Perf P
> 0
Rayleigh
2
2
2
bP
eb
P
2
1
bP
e P 0
b > 0
Weibull
a
b
P
a
a
eb
Pa
1
a
b
P
e
1
P 0
a > 0
b > 0
A. Chi-square test
The parametric chi-square test has been used, adopting the
same data sample for the statistical test. The Yates correction
[11] has been introduced in order to better estimate the
significance level. The results of the test depend on the pre-
specified number and structure (uniform or non-uniform) of
the classes, and on the level of significance%. If the value of% is specified in advance, the observed value is compared
to the critical range of values (min, max), depending on the
number of degrees of freedom, so that the test is successful if
min, unsuccessful if > max, whereas for min< maxthe result is undefined. Alternatively, the maximum level of
significancemax% corresponding to = minsets the limits of
acceptance of the chi-square test results.
B. Kolmogorov-Smirnov (KS) test
The error of the KS test is given by the maximum mismatch
between the Empirical CDF (ECDF) obtained by the set of
data under analysis and the CDF of the probability distribution
under test. The error is compared to a critical value critand
the test is successful if crit. If the CDF under test is fullyspecified by assigning all its parameters, the result of the test
is independent of the distribution, and the critical values gencrit
are found in specific tables in function of the level of
significance (see [11] p.797 and Table 1 of [12]). However, if
the CDF parameters are estimated from the data, these critical
values are no longer valid and must be determined by
simulation or by specific tables. Specific tables have been
found for the Exponential distribution (p.798 of [11] and
Table 1 of [13]) and for the Normal distribution (p.799 of [11]
and Table 1 of [14]). For the other cases in which the
distribution parameters are extracted from the data, the critical
values corresponding to a generic distribution can be seen
only as upper bounds of the actual critical values. The
assessment of the critical values is then performed by using a
Monte Carlo simulation. At first, a set of m= 1 , ,Mvalues
is specified, at which the CDF under test is calculated. Then, a
specified numberKof Monte Carlo simulations is performed.
At each simulation, a vector of length H is filled with H
random values extracted from the CDF under test. The
extraction is carried out by using Hrandom extractions in the
interval (0,1) from a uniform probability distribution, that are
considered as the values of the CDF under test, whose
corresponding values are computed from the abscissa of the
CDF under test. Then, the simulated empirical CDF is built at
the Mpredefined locations, and the KS error is computed as
the absolute value of the maximum difference between the
points of the simulated empirical CDF and of the CDF under
test referred to the same values m= 1, ,M. TheKerrors of
the KS test are then used to build the related CDF, and the
critical value is evaluated for a given level of significance.
The Monte Carlo simulations performed in this paper assume
M= 1000,K= 5000 andHset to the sample set size.
C. Geometrical adaptation tests.
The assessment of the fitness of the Empirical CDF (ECDF) to
a reference CDF has been performed by using two graphical
representations, with suitable functions of the generic CDF
valueF. The first representation transforms each valueFinto
( )FaE = 1ln (1)
and plots aEversus the power P, so that an exponential CDF
would be represented by a straight line in the (P,aE) plane.
The second representation transforms each valueFinto
( )( )FaW =
1lnln (2)
9th International Conference on Probabilistic Methods Applied to Power SystemsKTH, Stockholm, Sweden June 11-15, 2006
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and plots aW versus ln(P), so that a Weibull CDF would be
represented by a straight line in the (ln(P),aW) plane. In
addition, plotting aWversusPwould represent a Gumbel CDF
as a straight line in the (P,aW) plane.
IV. NUMERICAL TESTS AND RESULTSA. Tests for a 100-customer case
A first set of tests has been performed on the data obtained
from the Monte Carlo simulation at the same time instant. An
example is presented for hour 12:00 of a winter working day
with N = 100 customers. The number of Monte Carlo
simulations carried out to obtain the ECDF for this situation is
100. The characteristics of the complete data sample include
the minimum value 23.69 kW, maximum value 51.69 kW,
average value 39.21 kW, standard deviation 5.77 kW (14.7%),
and skewness -0.0004. The results of the KS test with level of
significance 5% are shown in Table II. The critical values of
the KS test have been computed by running 5000 Monte Carlo
simulations for each probability distribution (other thanExponential and Normal), resulting in values less restrictive
than gencrit = 0.1360. In particular, in this case the tests are not
accepted only for the Exponential and Rayleigh probability
distributions, whereas all the other distributions exhibit
acceptable goodness-of-fit. Fig. 1 reports the various CDFs.
More details are reported for the Gamma CDF with average
value and standard deviation equal to the ones of the data
sample (shape factor a= 46.2 and scale factor b= 848.5 W
according to Table I). Fig. 2 shows the details of the KS test.
Fig. 3 reports the results of the chi-square test with 7 degrees
of freedom (maximum acceptable error 14.07). Appling the
Yates correction, the observed error (6.85) has been
acceptably low and the test has been passed with a maximum
level of significance 44.5%, and with a non-excessive
adaptation (the critical value being 2.17).
Fig. 1. ECDF of the load at hour 12:00 for N = 100 and CDFs of various
probability distributions with the same average value and standard deviation.
Fig. 4 shows the results of the geometrical adaptation tests.
The acceptability of the Normal distribution is also confirmed
by the high value of the shape factor of the Gamma
distribution. As indicated in Fig. 5, for the Gamma CDF the
KS observed error during the day never exceeds the 5%
acceptance threshold.
TABLE II
KSTEST ERRORS FOR THE POWER AT HOUR 12:00WITH 100CUSTOMERS
(LEVEL OF SIGNIFICANCE 5%)
CDF KS test error critical value result
Beta 0.0832 0.1255 accepted
Exponential 0.5101 0.1060 rejected
Gamma 0.0800 0.1313 acceptedGumbel 0.1160 0.1314 accepted
Inverse-Normal 0.0659 0.1225 accepted
Log-Normal 0.0887 0.1230 accepted
Normal 0.0653 0.0886 accepted
Rayleigh 0.3434 0.1318 rejected
Weibull 0.0855 0.1306 accepted
Fig. 2. KS test for the Gamma CDF.
Fig. 3. Results of the chi-square test for the Gamma CDF forN= 100.
Fig. 4. Geometrical adaptation tests for the Gamma CDF.
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0
0.1
0.2
0.3
0 240 480 720 960 1200 1440
time (min)
KSobserv
ederror
KS 5% acceptance threshold
Fig. 5. Results of the KS 5% test with the Gamma CDF forN= 100.
B. Tests for a 10- customer case
The results of the same tests indicated in the previous
subsection are shown here on the data obtained from 100
Monte Carlo simulations referred to hour 12:00 of a winterworking day withN= 10 customers. The characteristics of the
complete data sample include the minimum value 1.508 kW,
maximum value 11.011 kW, average value 3.805 kW,
standard deviation 1.618 kW (42.5 %), and skewness 0.1109.
Table III shows the results of the KS test with level of
significance 5%. The Log-Normal and Inverse Normal
distributions exhibit the better goodness-of-fit. In this case, the
Normal probability distribution no longer fits the data. The
Gamma CDF has shape factor 5.53 (much lower than in the
previous case) and scale factor 688 W.
TABLE III
KSTEST ERRORS FOR THE POWER AT HOUR 12:00WITH 10CUSTOMERS
(LEVEL OF SIGNIFICANCE 5%)CDF KS test error critical value Result
Beta 0.1134 0.1263 accepted
Exponential 0.3721 0.1060 rejected
Gamma 0.1007 0.1325 accepted
Gumbel 0.2108 0.1334 rejected
Inverse-Normal 0.0851 0.1280 accepted
Log-Normal 0.0889 0.1263 accepted
Normal 0.1469 0.0886 rejected
Rayleigh 0.1588 0.1346 rejected
Weibull 0.1208 0.1322 accepted
0.0
1.0
2.0
3.0
4.0
5.0
0 240 480 720 960 1200 1440
time(min)
KSe
rrorratio
Exponential
Rayleigh
Normal
Gumbel
Fig. 6. Observed error to critical value ratio of the KS test with significance
level 5% for a winter working day withN= 10.
The results obtained for hour 12:00 can be generalized by
considering the results of the KS test with the various CDFs
for the 1440 minutes of the day. Fig. 6 shows that the
Exponential and Rayleigh distributions do not fit the ECDF
satisfactorily. A zoom into a specific time interval (from hour
11:40 to hour 12:20, Fig. 7) allows for identifying the Log-Normal, Inverse Normal and Gamma CDFs as the ones
exhibiting the best values of goodness-of-fit, compared to the
corresponding thresholds. However, as indicated for the
Gamma CDF in Fig. 8, in some hours of the day the KS
observed error could exceed the 5% acceptance threshold.
0.0
0.5
1.0
1.5
2.0
700 710 720 730 740
time (min)
KSe
rrorratio
Normal
Weibull
GammaInverse Normal
Log-Normal
Beta (max)
Gumbel
Fig. 7. Observed errors of the KS test with significance level 5% from hour
11:40 to hour 12:20 forN= 10.
0
0.1
0.2
0.3
0 240 480 720 960 1200 1440
time (min)
KSobserv
ederror
KS 5% acceptance threshold
Fig. 8. Results of the KS 5% test with the Gamma CDF forN= 10.
V. EXTENDED TESTS AND RESULTS
A. Extended tests for variable numbers of customers
The same set of tests specified in the previous subsections
have been carried out for a different number of customers(from 10 to 300) for all the 1440 minutes of the day, and for
the 4 types of days considered (working day and weekend day
in the summer and winter seasons). Each customer has a
contract power of 3 kW. Some significant results are
summarized in the sequel.
B. Time evolution of the aggregated load patterns and
standard deviations (winter working days)
A first result can be achieved by comparing the time evolution
of the aggregated load power for different numbers of
customers. Fig. 9, Fig. 10 and Fig. 11 show the load patterns
for a winter weekday with N = 10, N = 100 and N = 300,
respectively. The internal filled band represents the regions
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(-,+), where is the average value and is the standard
deviation of the data concerning each minute. The upper and
lower lines represent the maximum and minimum values
obtained in the Monte Carlo simulation. It is evident how
whenNincreases there is a reduction in the range of variation
of the aggregated load power, as well as a trend to obtainmore symmetrical probability distributions. In particular, Fig.
12 shows how the uncertainty of aggregated load (represented
by the standard deviation in per cent of the average value)
depends on the number of aggregated customers and varies
during the day.
C. Evaluations at specific hours
Further evaluations have been carried out by comparing the
evolution of the load in function of the number of customers.
A first case is presented in Fig. 13, considering the CDF of the
load at hour 12:00. When the number of customers increases,
the CDFs move from left to right, but the standard deviation
does not increase in the same way as the increase of theaverage value. This fact is well highlighted by the
representation of the specific power (W/customers) shown in
Fig. 14, where it is clear that whenNvaries the average value
of the specific power remains within a narrow range, whereas
the standard deviation varies considerably. This fact is
important to establish a reference value of specific power that
can be used to make good estimates of the consumption of the
group of customers tested. Extending the calculation to all the
time instants allows for observing that the specific load power
profile shown in Fig. 15 remains very similar.
0
5
10
15
20
0 240 480 720 960 1200 1440
time (min)
power[kW]
Fig. 9. Aggregated load patterns forN= 10.
0
20
40
60
80
100
120
0 240 480 720 960 1200 1440
time (min)
power[kW]
Fig. 10. Aggregated load patterns forN= 100.
0
50
100
150
200
250
300
350
0 240 480 720 960 1200 1440
time (min)
power
[kW]
Fig. 11. Aggregated load patterns forN= 300.
0
5
10
15
20
25
30
35
40
0 240 480 720 960 1200 1440
time (min)
standarddeviation
(%ofaveragev
alue)
N = 20
N = 40
N = 80 N = 150 N = 300
Fig. 12. Time evolution of the standard deviation of the load power in per cent
of the average value.
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 10 20 30 40 50 60
load [kW]
CDF
N = 1020 30
40
50 60 7080
90 100
Fig. 13. CDF of the load at hour 12:00 forN= 10 to 100.
0
0.2
0.4
0.6
0.8
1
0 200 400 600 800 1000
specific power (W/customer)
CDF
N = 20
N = 300
N = 150N = 80
N = 40
Fig. 14. CDFs of the aggregated specific load power at 16:00 for
different numbers of customers.
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0
200
400
600
800
1000
0 240 480 720 960 1200 1440
time (min)
specificpower(W/customer)
Fig. 15. Specific load power profiles (winter working day).
In order to assess the most suitable probability distribution, a
comparison has been made by taking into account as
parameter the ratio between the observed error of the KS test
and the KS error threshold for the corresponding probabilitydistribution. For each number of customers, the probability
distributions for which this ratio is the lowest at the various
time instants have been identified. The results are summarized
in Table IV, showing the percentage of winning time instant
for the various probability distributions. From this point of
view, the Gamma distribution emerges as the most promising
one for the various numbers of customers. Only the Inverse
Normal distribution could be a viable alternative for a low
number of customers.
TABLE IV
PERCENTAGE OF WINNING TIME INSTANTS FOR THE VARIOUS PROBABILITY
DISTRIBUTIONS
probability distributions and percentages of winning timeinstants
N
Gamma
Exponential
Log-Normal
Normal
Inverse
Normal
Beta
Weibull
Rayleigh
Gumbel
10 43.1 0 2.9 0 46.0 2.2 4.8 1.0 0
20 58.9 0 4.7 0 32.4 1.7 2.2 0 0.1
30 74.9 0 7.1 0 14.5 1.7 1.8 0 0
40 70.5 0 11.5 0 8.7 3.2 5.8 0 0.3
50 86.0 0 7.8 0 3.2 1.5 1.5 0 0
60 81.5 0 12.5 0 3.5 1.6 0.9 0 0
70 80.8 0 11.3 0 3.1 2.7 2.0 0 0.1
80 76.0 0 13.5 0 5.5 2.8 2.1 0 0.1
90 80.3 0 11.1 0 5.1 2.1 1.4 0 0
100 80.1 0 12.1 0 5.1 1.9 0.8 0 0
VI. CONCLUDING REMARKS
The results presented in this paper form a useful basis for
preparing a meaningful set of probabilistic data concerning the
time-evolution of the aggregated residential load, to be used
into any tool for probabilistic simulation (e.g., based on
analytical or Monte Carlo simulations). The results shown are
specifically referred to groups of residential customers in
extra-urban areas. It has to be stressed that these values cannot
be generally applied to all residential customers, regardless of
their location. In fact, for urban areas generally lower values
of specific power are expected for the same number of
customers, due to the reduced size of the houses, reduced
number of persons per house, and different types of activity.The whole analysis could be repeated with a different data set,
with initial parameters concerning the composition of the
residential customer set (e.g., including new appliances,
customer preferences, or customer willingness to participate to
tariff-driven programs), to perform scenario studies and
assessing the effects of the penetration of new technologies on
the time evolution of the aggregated residential consumption.
Examples are the assessment of the distributed generation
impact on residential districts, distribution system load
forecasting, and simulation of unbalanced loads.
The Gamma probability distribution has clearly emerged as
the one with the best goodness-of-fit. This result is
particularly interesting, since the simple relationships betweenthe Gamma parameters and the average value and standard
deviation, as well as the existence and easy formulation of its
characteristic function, make the Gamma distribution
particularly flexible and powerful for many applications.
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