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Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 129 | P a g e
Fractal Approach to Identify Quantitatively Intracardiac Atrial
Fibrillation from ECG Signals
Prof. (Dr.) Dipak Chandra Ghosh1
, Dr. Monisha Chakraborty2,*
And Tithi Das3
1
Emeritus Professor, Sir C. V. Raman Centre for Physics and Music, Jadavpur University; Former, UGC
Emeritus Fellow, Department of Physics, Jadavpur University, Director (Hony), Biren Roy Research Laboratory
for Radioactivity and Earthquake Studies, Jadavpur University, Kolkata, India
2
Assistant Professor, School of Bio-Science & Engineering, Jadavpur University, Kolkata, India
3
Ph. D Student, Department of Physics, Jadavpur University, Kolkata, India
ABSTRACT:
In this paper it has been studied how ECG signals show fractal pattern and thus it has been tried to find the
fractal dimension of the ECG time series. For this we have used Hurst’s Rescaled Range Analysis method. In
this work, ECG signals are acquired from normal subjects. Intracardiac Atrial Fibrillation ECG time series data
are collected from MIT-BIH Physionet database. From this analysis, we have tried to identify this type of
disease by looking at the Fractal dimension.
I. INTRODUCTION
Electrocardiogram (ECG) is a graphic recording of
the time variant voltages produced by the myo-
cardiogram during the cardiac cycle. Time domain
and frequency domain features of ECG signals can
be extracted using Digital Signal Processing (DSP)
techniques and these help to detect cardiac
abnormalities. It has been seen that if there is
fibrillation present in the ECG then this is indicated
by the presence of distinct peaks in the range of 3
Hz-7 Hz in the frequency band of its frequency
spectrum [1-2]. Noise elimination from ECG signals
contaminated with background noise is a challenging
task. Savitzky Golay filter works well in noise
elimination [3-5].
Atrial fibrillation is a common type of arrhythmia. It
is much common than atrial flutter, affecting 5-10%
of elderly people. The basis of atrial fibrillation is
rapid and chaotic depolarization occurring
throughout the atria. No “P” waves are seen and the
ECG baseline consists of low-amplitude oscillations.
Although around 400-600 impulses reach the AV
node every minute, only 120-180 of these impulses
will reach the ventricles to produce QRS complexes
[6]. Transmission of atrial impulses throughout the
AV node is erratic, making the ventricular (QRS
complex) rhythm “irregularly irregular”. The erratic
atrial depolarization leads to a failure of effective
atrial contraction. Loss of “atrial kick” reduces
ventricular filling and this leads to a fall of 10-15%
in cardiac output [6]. The symptoms of atrial
fibrillation include angina, breathlessness, dizziness,
palpitation, syncope, weakness etc. Studies on scatter
plots of normal, Intracardiac atrial fibrillation and
other arrhythmic ECGs can be done
using DSP techniques [7-9]. Normal and abnormal
ECGs can be effectively studied in terms of Power
spectrum Density [10]. These techniques of DSP can
be considered as effective tools for identifying
cardiac abnormalities. In this paper, attempts have
been made to identify Intracardiac atria fibrillation
from ECG time series in terms of Fractal Dimension.
It has been seen that many Physical, Bio-physical,
Geo-physical signals are irregular and in many times
these follow Gaussian distribution [11]. But many a
times it is impossible to get a trend to these signals.
Fractal statistics appears to be useful in studying this
type of irregular signals. Bio-signals like ECG
signals are non-stationary and they have shown a
self-similarity pattern i.e. a fractal pattern [12-13].
This similarity can contain important information
about the robustness of health and can indicate types
of disease. Therefore, studying the irregularity is
important.
Recently many methods were proposed to study this
irregularity. The simplest method was the standard
partition function method [14]. But it requires the
data set to be stable and temporal. But heart rate of
any healthy person is not constant even under ideal
conditions and it changes throughout a day. Diseased
heart also shows irregularity in the ECG pattern. To
avoid this problem, Wavelet transform modulus
maxima method was proposed [15], which was based
on the wavelet analysis. But this method is difficult
and requires large computation. Later on, Hurst
developed Rescaled Range Analysis [16-18] which is
a statistical method to analyze long range data set by
choosing discrete set of time series. There are many
other methods namely ANN, DFA, MF-DFA etc
which can also be used to study the fractal geometry.
RESEARCH ARTICLE OPEN ACCESS
Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 130 | P a g e
Fractal geometry mathematically
characterizes systems that are fundamentally
irregular at all scales. A fractal structure has the
property that if one magnifies a small portion of it, it
would show the complexity of the entire system. In
short, they are made of transformed copies of
themselves. This property implies the absence of
analytical regularity of the system.
Furthermore, fractals are divided into two categories:
monofractal and multifractal. Monofractals are those
whose scaling property is same in different regions
of the system. Multifractals are more complicated
self-similar objects. They consist of differently
weighted fractals, with different non-linear
dimensions .Thus the fundamental property is that
the scaling property may be different in different
regions of the system.
In an attempt to explore
the underlying structure and the governing
mechanism of manifestly aberrant appearance of the
time series, fractal statistics have been pursued with
time dependent experimental data. Hence, we will
use Rescaled Range Fractal analysis method to study
the ECG signals in this paper.
II. DATA SELECTION
Normal ECG signals are recorded using
POLYPARA module with a sampling rate of 200
samples per second. Intracardiac Atrial Fibrillation
ECG signals are collected from MIT-BIH Physionet
database [19]. This database is a large and growing
archive of well-characterized digital recordings of
physiologic signals and related data. Physio-Bank
currently includes databases of multi-parameter
cardiopulmonary, neural, and other biomedical
signals from healthy subjects and patients with a
variety of conditions with major public health
implications including sudden cardiac death,
congestive heart failure, epilepsy, gait disorders,
sleep-apnea and aging (Goldberger et al., 2000).
In MIT-BIH Physionet database all the Intracardiac
atrial fibrillation ECG signals were recorded using a
decapolar catheter with 2-5-2mm spacing (7mm
spacing between bipoles). This catheter was placed
in four separate regions of the heart. In each region,
the 5 bipolar signals were recorded along with 3
surface ECG leads [19]. Data were digitized at 1
kHz. Catheter bipoles are labeled (distal to proximal)
as CS12, CS34,..., CS90 [19]. The catheter positions
in the relevant regions of the heart are shown in Fig-
1.
Fig-1: Catheter Positions in the Four Regions of
the Heart [19]
At “SVC”, the distal tip of the catheter (CS12) is
close to the annulus of the superior vena cava.
At “IVC”, the proximal tip of the catheter (CS90) is
close to the annulus of the inferior vena cava
At “TVA”, the distal tip (CS12) is close to the
tricuspid valve annulus
At “AFW”, the entire catheter rests against the atrial
free wall.
III. MATHEMATICAL ANALYSIS:
RESCALED RANGE ANALYSIS:
The rescaled range analysis is simple yet
robust non-parametric method for fast fractal
analysis. This is performed on the discrete time
series data set xt of dimension N by calculating the
mean ( )x N ;the standard deviation S(N) and the
cumulative departure X(n,N),where,
( ) tx
x N
N
  (1)
1
2 2
1
( ) [ ( ( )) ]tS N x x N
N
  (2)
Range of cumulative departure of the
data is
R(N)=max[x(n,N)]-min[x(n,N)] (3)
Where cumulative departure is given
by
( , ) ( ( ))tX n N x x N  , 0≤n≤N (4)
The associated R/S analysis for the
ECG signals is discussed in detail in the Result
section of this paper. It is computed as
HR
n
S
 (5)
The slope of the plot of log (R/S)
vs. log (n) gives rise to H. The magnitude of H
indicates whether a time series is random or
successive increments in time series.
The fractal dimension D [20-21] is
determined as
D = 2-H. (6)
Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 131 | P a g e
The correlation ‘ρ’ [21] between
two successive steps or increment is given by
ρ = 22H-1
-1 (7)
. If H = 0.5 then ρ = 0. For this the time
series represents random walk and each observation
is totally independent of the prior observations. If ρ
is positive then 0.5<H<1, meaning the time series is
persistent and has long memory effect, that is the
preceding observations has a positive correlation
with the successive observations. On the other hand
if ρ is negative then 0<H<0.5, meaning the
observations are non-persistent and the each value
has negative correlation with the previous value [17].
IV. RESULTS AND DISCUSSIONS
The plots for normal ECG and diseased
ECG e.g. Intracardiac Atrial Fibrillation are shown in
Fig-2 and Fig-3 respectively.
0 20 40 60 80 100 120 140 160 180 200
1500
2000
2500
3000
Amplitude
Sample number
Fig-2: Normal ECG
0 20 40 60 80 100 120 140 160 180 200
0
50
100
150
200
250
300
Sample number
Amplitude
Fig-3: Intracardiac Atrial Fibrillation ECG
Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 132 | P a g e
Normal ECG signals are recorded using
POLYPARA module with a sampling rate of 200
samples per second. Both normal and diseased ECG
time series are loaded on MATLAB platform.
Rescaled range analysis method as explained in the
earlier section is applied to these time series. For this
method, we choose a set of dimension N (which is
200, in our case).Then the mean ( )x N , standard
deviation S(N), range R(N), cumulative departure
X(n ,N) are found using eqns. 1, 2, 3, and 4
respectively. Subsequently, (R/S) value is calculated.
A graph log10(R/S) vs. log10(n) is then plotted, where
‘n’ is the length of the data set. Hurst exponent is
then found from the slope of this plot using eqn. 5.
The graph log10(R/S) vs. log10 (n) for a normal ECG
time series is shown in Fig-4 as a sample plot.
0 0.5 1 1.5 2 2.5
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
log10(R/S)
log10(n)
Fig-4: log 10(R/S) vs log 10(n) for a normal ECG time series
Similarly, the graph log10(R/S) vs. log10 (n) for an
Intracardiac Atrial Fibrillation ECG time series is
shown in Fig-5 as a sample plot.
0 0.5 1 1.5 2 2.5
0.2
0.25
0.3
0.35
0.4
0.45
0.5
log10(R/S)
log10(n)
Fig-5: log 10(R/S) vs log 10(l) for an Intracardiac
Atrial Fibrillation ECG time series
In all these plots, it appears that there is no
linear dependency, thus ensuring the fact that,
multifractal nature is present in all the cases. Now
random Brownian motion produces a value H=0.5.
Generally a value above this indicates positive
autocorrelation in the signal .That is, it indicates an
increased likelihood that the next value in the series
Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 133 | P a g e
will be in the same direction as the current value and that the direction of movement of the signal will continue
or persist. On the other hand a value less than 0.5 indicates a negative correlation and it implies that the next
values will be in the opposite direction. Hurst exponents may vary between 0 and 1.
As in our case, Hurst exponent is found to be below 0.5; there will be increasing irregularity or
‘roughness’ to the curve.
Now Fractal Dimension of each data set are obtained using eqn.(6), which is D = 2-H. We also find the
correlation between two successive steps by using equ. (7), i.e. ρ = 22H-1
-1.
Fractal dimension values obtained for normal and Intracardiac Atrial Fibrillation ECG time series are
tabulated in Table-1 and Table-2 respectively as sample results.
Table 1: For Normal ECG Time Series
S. No. H D ρ
1 0.3603 1.6397 -0.1761
2 0.3603 1.6397 -0.1761
3 0.4053 1.5947 -0.1230
4 0.3569 1.6431 -0.1799
5 0.3475 1.6525 -0.1905
6 0.3962 1.6038 -0.1340
7 0.3603 1.6397 -0.1761
Table 2: For Intracardiac Atrial Fibrillation
S. No. H D ρ
1 0.2309 1.7691 -0.3114
2 0.2285 1.7715 -0.3136
3 0.2068 1.7932 -0.3340
4 0.2291 1.7709 -0.3131
5 0.2480 1.7520 -0.2949
6 0.2240 1.7760 -0.3179
7 0.2365 1.7635 -0.3061
Mean and Standard Deviation are obtained
from the whole data set considered in this work and
these results are tabulated in Table-3 for normal and
Intracardiac Atrial Fibrillation ECG time series.
These results are compared.
Table-3: Fractal Dimension for Normal and Intracardiac Atrial Fibrillation ECG Time Series.
V. CONCLUSION
Fractal Dimension of Intracardiac Atrial
Fibrillation ECG time series lies in between 1.7725 ±
0.0126. Whereas, the Fractal Dimension of normal
ECG time series is 1.6271 ± 0.0260. It is observed
that the Fractal Dimension value is higher for the
case of Intracardiac Atrial Fibrillation ECG time
series as compared to that of normal ECG time
Time Series
Type
Mean Standard
Deviation
Maximum
limit
Minimum
limit
Mean-
Std
Mean
+ Std
Normal 1.6271 0.0260 1.6525 1.5824 1.6011 1.6530
Intracardiac
Atrial
Fibrillation
1.7725 0.0126 1.7968 1.7410 1.7599 1.7851
Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134
www.ijera.com 134 | P a g e
series. Moreover, the variation of Fractal Dimension
amongst the data set for Intracardiac Atrial
Fibrillation ECG time series is small as compared to
that of normal ECG time series. This analysis does
have a significant clinical advantage. So, this range
of Fractal Dimension for Intracardiac Atrial
Fibrillation ECG time series can be used as a disease
index to identify this disease.
REFERENCES
[1] W. J. Tompkins, Biomedical Digital Signal
Processing, Prentice Hall India
[2] Shreya Das and Monisha Chakraborty,
“Extraction of Fibrillation Components
from Ventricular Arrhythmic
Electrocardiograms”, National Conference
on Computer Vision, Pattern Recognition,
Image Processing and Graphics, Karnataka,
December, 15-17, 2011, published in IEEE
Xplore Conference Publishing Service
(CPS), pp-138-141.
http://doi.ieeecomputersociety.org/10.1109/
NCVPRIPG.2011.37)
[3] Monisha Chakraborty and Shreya Das,
“Determination of Signal to Noise Ratio of
Electrocardiograms Filtered by Band Pass
and Savitzky-Golay Filters”, Elsevier
Procedia Technology, Vol. 4, 2012, pp-830
– 833.
[4] Sayanti Sankhari and Monisha Chakraborty,
“Optimisation of Filter Order and Frame
Length of Savitzky-Golay Filter in
Eliminating Noise From
Electrocardiograms”, CSIR Sponsored
National Conference on Modern Trends in
Electronic Communication and Signal
Processing, August, 3-4, 2012, pp-10-12.
[5] Shreya Das and Monisha Chakraborty,
“QRS Detection Algorithm Using Savitzky-
Golay Filter”, ACEEE Int. J. on Signal and
Image Processing, Vol. 03, No. 01, Jan
2012, pp-55-58
[6] Andrew R Houghton, David Gray, “Making
Sense of the ECG”, Arnold Publishers,
London, pp-44-48.
[7] Shreya Das and Monisha Chakraborty,
“Comparison of Normal, Ventricular
Tachyarrhythmic and Atrial Fibrillation
Electrocardiograms using Scatter Plots”
International Journal of Electronics Signals
and Systems, Vol-1, Issue-2, 2012, pp-20-
24
[8] Shreya Das and Monisha Chakraborty,
“Comparison of Normal and Arrhythmic
Electrocardiograms using Scatter Plots”,
International Journal on Recent Trends in
Engineering and Technology (IJRTET),
Vol-6, No.1 November, 2011, pp-16-19.
[9] Shreya Das and Monisha Chakraborty,
“Comparison of Normal and Ventricular
Tachyarrhythmic Electrocardiograms using
Scatter Plots”, ACEEE Int. J. on
Information Technology, Vol. 02, No. 02,
April 2012, pp-32-34.
[10] Shreya Das and Monisha Chakraborty,
“Comparison of Power Spectral Density
(PSD) of Normal and Abnormal ECGs”,
IJCA, Special Issue on 2nd National
Conference- Computing, Communication
and Sensor Network, (2): pp-10-14, 2011.
[11] D.L.Turcotte “Fractals and Chaos in
geology and geophysics”;
Cambridge University Press, Cambridge,
England 1992.
[12] B.B. Mandelbort, “The Fractal geometry of
Nature” (Freeman, New York ,1982).
[13] D. Ghosh, A. Deb, D. Dutta, R. Sengupta,
S. Samanta, “Multifractality of radon
concentration fluctuation in earthquake
related signal”, World Scientific; Vol. 20,
No. 1 pp-33-39, 2012.
[14] H.E.Stanley, L.A.N.Amaral,
A.l.Goldberger, S.Havlin, P.C.Ivanov ,
C.K.Peng, “ Statistical Physics and
Physiology: Monofractal and Multifractal
approaches” Physica A, 270, pp-309-324,
1999
[15] P.Vanouplines “Rescaled range analysis and
the fractal dimension of pi”. University
Library, Pleinlaan 2, 1050 Brussels,
Belgium.
[16] Nahina Islam, Nafiz Imtiaz Bin Hamid,
Adnan Mahmud, Sk. M. Rahman, Arafat H.
Khan “Detection of some Major Heart
Diseases using fractal Analysis”, Vol 4,
Issue 2, pp-63-70
[17] N.K. Das, P. Sen, R.K. Bhandari, Bikash
Sinha; “Non linear response of Radon its
Progeny in Spring Emission”; Applied
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313-318, 2009
[18] J. Wang, K. Cheng, “Scale Invariance
analysis of the Premature ECG Signal”,
Physica A, Elsevier, 391,pp-3227-
3233,2012
[19] Website:
http://www.physionet.org/physiobank/datab
ase/iafdb
[20] H.E. Hurst, “Long term storage capacity of
reservoirs, Trans. Am. Soc. Civ. Eng, 116,
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[21] J. Feder “Fractals”; Plenum Press, NY, 283,
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X35129134

  • 1. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 129 | P a g e Fractal Approach to Identify Quantitatively Intracardiac Atrial Fibrillation from ECG Signals Prof. (Dr.) Dipak Chandra Ghosh1 , Dr. Monisha Chakraborty2,* And Tithi Das3 1 Emeritus Professor, Sir C. V. Raman Centre for Physics and Music, Jadavpur University; Former, UGC Emeritus Fellow, Department of Physics, Jadavpur University, Director (Hony), Biren Roy Research Laboratory for Radioactivity and Earthquake Studies, Jadavpur University, Kolkata, India 2 Assistant Professor, School of Bio-Science & Engineering, Jadavpur University, Kolkata, India 3 Ph. D Student, Department of Physics, Jadavpur University, Kolkata, India ABSTRACT: In this paper it has been studied how ECG signals show fractal pattern and thus it has been tried to find the fractal dimension of the ECG time series. For this we have used Hurst’s Rescaled Range Analysis method. In this work, ECG signals are acquired from normal subjects. Intracardiac Atrial Fibrillation ECG time series data are collected from MIT-BIH Physionet database. From this analysis, we have tried to identify this type of disease by looking at the Fractal dimension. I. INTRODUCTION Electrocardiogram (ECG) is a graphic recording of the time variant voltages produced by the myo- cardiogram during the cardiac cycle. Time domain and frequency domain features of ECG signals can be extracted using Digital Signal Processing (DSP) techniques and these help to detect cardiac abnormalities. It has been seen that if there is fibrillation present in the ECG then this is indicated by the presence of distinct peaks in the range of 3 Hz-7 Hz in the frequency band of its frequency spectrum [1-2]. Noise elimination from ECG signals contaminated with background noise is a challenging task. Savitzky Golay filter works well in noise elimination [3-5]. Atrial fibrillation is a common type of arrhythmia. It is much common than atrial flutter, affecting 5-10% of elderly people. The basis of atrial fibrillation is rapid and chaotic depolarization occurring throughout the atria. No “P” waves are seen and the ECG baseline consists of low-amplitude oscillations. Although around 400-600 impulses reach the AV node every minute, only 120-180 of these impulses will reach the ventricles to produce QRS complexes [6]. Transmission of atrial impulses throughout the AV node is erratic, making the ventricular (QRS complex) rhythm “irregularly irregular”. The erratic atrial depolarization leads to a failure of effective atrial contraction. Loss of “atrial kick” reduces ventricular filling and this leads to a fall of 10-15% in cardiac output [6]. The symptoms of atrial fibrillation include angina, breathlessness, dizziness, palpitation, syncope, weakness etc. Studies on scatter plots of normal, Intracardiac atrial fibrillation and other arrhythmic ECGs can be done using DSP techniques [7-9]. Normal and abnormal ECGs can be effectively studied in terms of Power spectrum Density [10]. These techniques of DSP can be considered as effective tools for identifying cardiac abnormalities. In this paper, attempts have been made to identify Intracardiac atria fibrillation from ECG time series in terms of Fractal Dimension. It has been seen that many Physical, Bio-physical, Geo-physical signals are irregular and in many times these follow Gaussian distribution [11]. But many a times it is impossible to get a trend to these signals. Fractal statistics appears to be useful in studying this type of irregular signals. Bio-signals like ECG signals are non-stationary and they have shown a self-similarity pattern i.e. a fractal pattern [12-13]. This similarity can contain important information about the robustness of health and can indicate types of disease. Therefore, studying the irregularity is important. Recently many methods were proposed to study this irregularity. The simplest method was the standard partition function method [14]. But it requires the data set to be stable and temporal. But heart rate of any healthy person is not constant even under ideal conditions and it changes throughout a day. Diseased heart also shows irregularity in the ECG pattern. To avoid this problem, Wavelet transform modulus maxima method was proposed [15], which was based on the wavelet analysis. But this method is difficult and requires large computation. Later on, Hurst developed Rescaled Range Analysis [16-18] which is a statistical method to analyze long range data set by choosing discrete set of time series. There are many other methods namely ANN, DFA, MF-DFA etc which can also be used to study the fractal geometry. RESEARCH ARTICLE OPEN ACCESS
  • 2. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 130 | P a g e Fractal geometry mathematically characterizes systems that are fundamentally irregular at all scales. A fractal structure has the property that if one magnifies a small portion of it, it would show the complexity of the entire system. In short, they are made of transformed copies of themselves. This property implies the absence of analytical regularity of the system. Furthermore, fractals are divided into two categories: monofractal and multifractal. Monofractals are those whose scaling property is same in different regions of the system. Multifractals are more complicated self-similar objects. They consist of differently weighted fractals, with different non-linear dimensions .Thus the fundamental property is that the scaling property may be different in different regions of the system. In an attempt to explore the underlying structure and the governing mechanism of manifestly aberrant appearance of the time series, fractal statistics have been pursued with time dependent experimental data. Hence, we will use Rescaled Range Fractal analysis method to study the ECG signals in this paper. II. DATA SELECTION Normal ECG signals are recorded using POLYPARA module with a sampling rate of 200 samples per second. Intracardiac Atrial Fibrillation ECG signals are collected from MIT-BIH Physionet database [19]. This database is a large and growing archive of well-characterized digital recordings of physiologic signals and related data. Physio-Bank currently includes databases of multi-parameter cardiopulmonary, neural, and other biomedical signals from healthy subjects and patients with a variety of conditions with major public health implications including sudden cardiac death, congestive heart failure, epilepsy, gait disorders, sleep-apnea and aging (Goldberger et al., 2000). In MIT-BIH Physionet database all the Intracardiac atrial fibrillation ECG signals were recorded using a decapolar catheter with 2-5-2mm spacing (7mm spacing between bipoles). This catheter was placed in four separate regions of the heart. In each region, the 5 bipolar signals were recorded along with 3 surface ECG leads [19]. Data were digitized at 1 kHz. Catheter bipoles are labeled (distal to proximal) as CS12, CS34,..., CS90 [19]. The catheter positions in the relevant regions of the heart are shown in Fig- 1. Fig-1: Catheter Positions in the Four Regions of the Heart [19] At “SVC”, the distal tip of the catheter (CS12) is close to the annulus of the superior vena cava. At “IVC”, the proximal tip of the catheter (CS90) is close to the annulus of the inferior vena cava At “TVA”, the distal tip (CS12) is close to the tricuspid valve annulus At “AFW”, the entire catheter rests against the atrial free wall. III. MATHEMATICAL ANALYSIS: RESCALED RANGE ANALYSIS: The rescaled range analysis is simple yet robust non-parametric method for fast fractal analysis. This is performed on the discrete time series data set xt of dimension N by calculating the mean ( )x N ;the standard deviation S(N) and the cumulative departure X(n,N),where, ( ) tx x N N   (1) 1 2 2 1 ( ) [ ( ( )) ]tS N x x N N   (2) Range of cumulative departure of the data is R(N)=max[x(n,N)]-min[x(n,N)] (3) Where cumulative departure is given by ( , ) ( ( ))tX n N x x N  , 0≤n≤N (4) The associated R/S analysis for the ECG signals is discussed in detail in the Result section of this paper. It is computed as HR n S  (5) The slope of the plot of log (R/S) vs. log (n) gives rise to H. The magnitude of H indicates whether a time series is random or successive increments in time series. The fractal dimension D [20-21] is determined as D = 2-H. (6)
  • 3. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 131 | P a g e The correlation ‘ρ’ [21] between two successive steps or increment is given by ρ = 22H-1 -1 (7) . If H = 0.5 then ρ = 0. For this the time series represents random walk and each observation is totally independent of the prior observations. If ρ is positive then 0.5<H<1, meaning the time series is persistent and has long memory effect, that is the preceding observations has a positive correlation with the successive observations. On the other hand if ρ is negative then 0<H<0.5, meaning the observations are non-persistent and the each value has negative correlation with the previous value [17]. IV. RESULTS AND DISCUSSIONS The plots for normal ECG and diseased ECG e.g. Intracardiac Atrial Fibrillation are shown in Fig-2 and Fig-3 respectively. 0 20 40 60 80 100 120 140 160 180 200 1500 2000 2500 3000 Amplitude Sample number Fig-2: Normal ECG 0 20 40 60 80 100 120 140 160 180 200 0 50 100 150 200 250 300 Sample number Amplitude Fig-3: Intracardiac Atrial Fibrillation ECG
  • 4. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 132 | P a g e Normal ECG signals are recorded using POLYPARA module with a sampling rate of 200 samples per second. Both normal and diseased ECG time series are loaded on MATLAB platform. Rescaled range analysis method as explained in the earlier section is applied to these time series. For this method, we choose a set of dimension N (which is 200, in our case).Then the mean ( )x N , standard deviation S(N), range R(N), cumulative departure X(n ,N) are found using eqns. 1, 2, 3, and 4 respectively. Subsequently, (R/S) value is calculated. A graph log10(R/S) vs. log10(n) is then plotted, where ‘n’ is the length of the data set. Hurst exponent is then found from the slope of this plot using eqn. 5. The graph log10(R/S) vs. log10 (n) for a normal ECG time series is shown in Fig-4 as a sample plot. 0 0.5 1 1.5 2 2.5 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 log10(R/S) log10(n) Fig-4: log 10(R/S) vs log 10(n) for a normal ECG time series Similarly, the graph log10(R/S) vs. log10 (n) for an Intracardiac Atrial Fibrillation ECG time series is shown in Fig-5 as a sample plot. 0 0.5 1 1.5 2 2.5 0.2 0.25 0.3 0.35 0.4 0.45 0.5 log10(R/S) log10(n) Fig-5: log 10(R/S) vs log 10(l) for an Intracardiac Atrial Fibrillation ECG time series In all these plots, it appears that there is no linear dependency, thus ensuring the fact that, multifractal nature is present in all the cases. Now random Brownian motion produces a value H=0.5. Generally a value above this indicates positive autocorrelation in the signal .That is, it indicates an increased likelihood that the next value in the series
  • 5. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 133 | P a g e will be in the same direction as the current value and that the direction of movement of the signal will continue or persist. On the other hand a value less than 0.5 indicates a negative correlation and it implies that the next values will be in the opposite direction. Hurst exponents may vary between 0 and 1. As in our case, Hurst exponent is found to be below 0.5; there will be increasing irregularity or ‘roughness’ to the curve. Now Fractal Dimension of each data set are obtained using eqn.(6), which is D = 2-H. We also find the correlation between two successive steps by using equ. (7), i.e. ρ = 22H-1 -1. Fractal dimension values obtained for normal and Intracardiac Atrial Fibrillation ECG time series are tabulated in Table-1 and Table-2 respectively as sample results. Table 1: For Normal ECG Time Series S. No. H D ρ 1 0.3603 1.6397 -0.1761 2 0.3603 1.6397 -0.1761 3 0.4053 1.5947 -0.1230 4 0.3569 1.6431 -0.1799 5 0.3475 1.6525 -0.1905 6 0.3962 1.6038 -0.1340 7 0.3603 1.6397 -0.1761 Table 2: For Intracardiac Atrial Fibrillation S. No. H D ρ 1 0.2309 1.7691 -0.3114 2 0.2285 1.7715 -0.3136 3 0.2068 1.7932 -0.3340 4 0.2291 1.7709 -0.3131 5 0.2480 1.7520 -0.2949 6 0.2240 1.7760 -0.3179 7 0.2365 1.7635 -0.3061 Mean and Standard Deviation are obtained from the whole data set considered in this work and these results are tabulated in Table-3 for normal and Intracardiac Atrial Fibrillation ECG time series. These results are compared. Table-3: Fractal Dimension for Normal and Intracardiac Atrial Fibrillation ECG Time Series. V. CONCLUSION Fractal Dimension of Intracardiac Atrial Fibrillation ECG time series lies in between 1.7725 ± 0.0126. Whereas, the Fractal Dimension of normal ECG time series is 1.6271 ± 0.0260. It is observed that the Fractal Dimension value is higher for the case of Intracardiac Atrial Fibrillation ECG time series as compared to that of normal ECG time Time Series Type Mean Standard Deviation Maximum limit Minimum limit Mean- Std Mean + Std Normal 1.6271 0.0260 1.6525 1.5824 1.6011 1.6530 Intracardiac Atrial Fibrillation 1.7725 0.0126 1.7968 1.7410 1.7599 1.7851
  • 6. Dr. M. Chakraborty et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.129-134 www.ijera.com 134 | P a g e series. Moreover, the variation of Fractal Dimension amongst the data set for Intracardiac Atrial Fibrillation ECG time series is small as compared to that of normal ECG time series. This analysis does have a significant clinical advantage. So, this range of Fractal Dimension for Intracardiac Atrial Fibrillation ECG time series can be used as a disease index to identify this disease. REFERENCES [1] W. J. Tompkins, Biomedical Digital Signal Processing, Prentice Hall India [2] Shreya Das and Monisha Chakraborty, “Extraction of Fibrillation Components from Ventricular Arrhythmic Electrocardiograms”, National Conference on Computer Vision, Pattern Recognition, Image Processing and Graphics, Karnataka, December, 15-17, 2011, published in IEEE Xplore Conference Publishing Service (CPS), pp-138-141. http://doi.ieeecomputersociety.org/10.1109/ NCVPRIPG.2011.37) [3] Monisha Chakraborty and Shreya Das, “Determination of Signal to Noise Ratio of Electrocardiograms Filtered by Band Pass and Savitzky-Golay Filters”, Elsevier Procedia Technology, Vol. 4, 2012, pp-830 – 833. [4] Sayanti Sankhari and Monisha Chakraborty, “Optimisation of Filter Order and Frame Length of Savitzky-Golay Filter in Eliminating Noise From Electrocardiograms”, CSIR Sponsored National Conference on Modern Trends in Electronic Communication and Signal Processing, August, 3-4, 2012, pp-10-12. [5] Shreya Das and Monisha Chakraborty, “QRS Detection Algorithm Using Savitzky- Golay Filter”, ACEEE Int. J. on Signal and Image Processing, Vol. 03, No. 01, Jan 2012, pp-55-58 [6] Andrew R Houghton, David Gray, “Making Sense of the ECG”, Arnold Publishers, London, pp-44-48. [7] Shreya Das and Monisha Chakraborty, “Comparison of Normal, Ventricular Tachyarrhythmic and Atrial Fibrillation Electrocardiograms using Scatter Plots” International Journal of Electronics Signals and Systems, Vol-1, Issue-2, 2012, pp-20- 24 [8] Shreya Das and Monisha Chakraborty, “Comparison of Normal and Arrhythmic Electrocardiograms using Scatter Plots”, International Journal on Recent Trends in Engineering and Technology (IJRTET), Vol-6, No.1 November, 2011, pp-16-19. [9] Shreya Das and Monisha Chakraborty, “Comparison of Normal and Ventricular Tachyarrhythmic Electrocardiograms using Scatter Plots”, ACEEE Int. J. on Information Technology, Vol. 02, No. 02, April 2012, pp-32-34. [10] Shreya Das and Monisha Chakraborty, “Comparison of Power Spectral Density (PSD) of Normal and Abnormal ECGs”, IJCA, Special Issue on 2nd National Conference- Computing, Communication and Sensor Network, (2): pp-10-14, 2011. [11] D.L.Turcotte “Fractals and Chaos in geology and geophysics”; Cambridge University Press, Cambridge, England 1992. [12] B.B. Mandelbort, “The Fractal geometry of Nature” (Freeman, New York ,1982). [13] D. Ghosh, A. Deb, D. Dutta, R. Sengupta, S. Samanta, “Multifractality of radon concentration fluctuation in earthquake related signal”, World Scientific; Vol. 20, No. 1 pp-33-39, 2012. [14] H.E.Stanley, L.A.N.Amaral, A.l.Goldberger, S.Havlin, P.C.Ivanov , C.K.Peng, “ Statistical Physics and Physiology: Monofractal and Multifractal approaches” Physica A, 270, pp-309-324, 1999 [15] P.Vanouplines “Rescaled range analysis and the fractal dimension of pi”. University Library, Pleinlaan 2, 1050 Brussels, Belgium. [16] Nahina Islam, Nafiz Imtiaz Bin Hamid, Adnan Mahmud, Sk. M. Rahman, Arafat H. Khan “Detection of some Major Heart Diseases using fractal Analysis”, Vol 4, Issue 2, pp-63-70 [17] N.K. Das, P. Sen, R.K. Bhandari, Bikash Sinha; “Non linear response of Radon its Progeny in Spring Emission”; Applied Radiation and Isotopes, Elsevier, 67, pp- 313-318, 2009 [18] J. Wang, K. Cheng, “Scale Invariance analysis of the Premature ECG Signal”, Physica A, Elsevier, 391,pp-3227- 3233,2012 [19] Website: http://www.physionet.org/physiobank/datab ase/iafdb [20] H.E. Hurst, “Long term storage capacity of reservoirs, Trans. Am. Soc. Civ. Eng, 116, pp-770-808, 1951. [21] J. Feder “Fractals”; Plenum Press, NY, 283, 1998.