analysis of seismic waves using modified periodogram...
TRANSCRIPT
ANALYSIS OF SEISMIC WAVES USING
MODIFIED PERIODOGRAM ALGORITHM
M.L.S.Prameela¹, Ch.Prem Abhinav², K.S.Ramesh³, S.
Koteswara Rao4,T.Vaishnavi Chandra5
Department of ECE, K L University, Vaddeswaram, Gunutr.
[email protected], [email protected]
Abstract
Earthquakes are the most terrible events on the earth. They are caused by
sudden breaks in the Earths rocky outer shell and shaking of ground. The
earthquake effect depends on breaking of rock and the distance which it shifts. So
by using signal processing techniques, power spectral density is estimated
through which the movement of earthquakes can be predicted. In this paper, non-
parametric methods are used for spectral estimation. Modified periodogram
technique is used to calculate spectral densities.
Keywords: Stochastic signal processing, Adaptive signal processing,
Seismology, Applied Statistics and Seismic signal processing.
1. INTRODUCTION
International Journal of Pure and Applied MathematicsVolume 114 No. 10 2017, 201-209ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-line version)url: http://www.ijpam.euSpecial Issue ijpam.eu
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The surface of the earth is known as the crust, and it is comprised of
plates, called structural plates, that move. Seismic tremors happen
when these plates knock, rub or drag against each other. These seismic
tremors are measured utilizing seismometers. Earthquakes frequently
happen in volcanic districts because of the stream of magma in
volcanoes and are an early cautioning of volcanic emissions.Seismology
is defined as the earthquakes study and elastic waves propagation
through earth and other planet-like bodies. This field also includes
earthquake environmental effects and seismic sources such as
Tsunamis and artificial processes such as explosions. A seismogram is
earth motion recordings as a function of time.
1.1 Detection of Seismic waves
Seismic waves are the energy waves caused due to sudden breaking
of rock in the earth.It is also defined as energy that travels through the
earth and is recorded on seismographs. There are various types of
seismic waves. Those are Body waves and Surface waves. Body waves
travel through earth’s inner layer along the planet’s surface. Surface
waves travel through the crust and have lower frequencies than body
waves. These seismic wave can be detected using seismometers.
Seismometers sense and record the earth motions propagating through
elastic waves. These are moved deep into the earth’s surface.
Seismograph is an instrument that records seismic signals. A geophone
is a device that changes ground motion (velocity) into voltage, which
might be recorded at a recording station.
1.2 Non Parametric method
For a random process signal, the Non parametric methods are used
to estimate the autocorrelation sequence. In 1898, Arthur Schuster in
his study of periodicities, first introduced periodogram which is easy to
compute. For short data records, periodogram has limited ability in
estimation of power spectrum. To improve the statistical properties of
periodogram, many modification have been made which is called
Modified Periodogram. It is the periodogram of a windowed data
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sequence. In order to smooth the edges of the signal, modified
periodogram windows the time domain signal earlier to DFT
computation.
2. MATHEMATICAL MODELLING
2.1 Spectral Analysis
Process of splitting a large data signal to simple parts is known as
Spectral Analysis. It is also known as Frequency Domain Analysis.
These graphs are plotted with respect to Amplitude or Phase on x-axis
and Frequency on y-axis. In this method Frequency is only term which
is not varying on the graphs (on y-axis) that are being plotted for
Spectrum Analysis. It is being performed by common method known as
Fourier Transformation.
2.2 Fourier Transformation
The term Fourier consists of both mathematical and frequency
domain modelling in it. In mathematical it can be represented by using
the equation.
𝑓 𝑧 = 𝑓 𝑥 ∞
−∞𝑒−2𝜋𝑧𝑥 dx (1)
It is used for both time variant and non-linear systems for
calculation of power spectral density. Now a days the software is using
DFT (Discrete Fourier Transformation) to generate frequency
estimation or spectrum.
𝐹 𝑥 =1
√𝑁 𝑓(𝑛)𝑁−1
𝑛=0 𝑒−𝑗2𝜋𝑥𝑛 /𝑁 (2)
It is time taking process for the frequency estimation. A separate
algorithm was developed to perform DFT known as FFT(Fast Fourier
Transformation).
𝑋 𝑧 = 𝑥(𝑛)𝑊𝑛𝑘𝑧𝑁−1
𝑛=0 , 0 ≤ k ≤ N-1 (3)
All these methods come under parametric methods. In addition to this
separate non parametric methods are also introduced for estimation of
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Power Spectral Density.
2.2 Modified Periodogram
The Non Parametric method which is used to calculate the power
spectral density of the input signal by using rectangular data window
is known as Periodogram. It can be represented by using mathematical
equation.
ṙ𝑥 𝑧 =1
𝑁 𝑥𝑛 𝑛 + 𝑧 𝑥𝑛
∗∞𝑛=−∞ 𝑛 =
1
𝑁𝑥𝑛 𝑧 ∗ 𝑥𝑛
∗ −𝑧 (4)
The process of reducing the side lobes or spectral leakage to
calculate power spectral density statistics of a particular signal is
known as Modified Periodogram.
2.4 Spectral estimation by averaging modified periodogram
In this method, before computing individual periodogram windows
W(n) is directly applied to data signals. Here length of the window is
given by formulae.
𝑈 =1
𝐾 𝑤(𝑛) ²𝐾−1
𝑛=0 (5)
We consider the expected value of modified periodogram to evaluate
the bias. Here W (𝑒𝑗𝜔 ) is the Fourier transform of the data window.
𝐸 Ṕ𝑀 𝑒𝑗𝜔 =1
2𝜋𝐾𝑈𝑃𝑥 𝑒
𝑗𝜔 ∗ 𝑊 𝑒𝑗𝜔 ² (6)
By Parseval’s theorem, U is the window energy divided by K
𝑈 =1
𝐾 𝑤 𝑛 2 =
1
2𝜋𝐾𝐾−1𝑛=0 𝑊(𝑒𝑗𝜔
𝜋
−𝜋²𝑑𝜔 (7)
Modified Periodogram will be asymptotically unbiased when
𝑊(𝑒𝑗𝜔 2
𝐾𝑈
will converge to a unit area impulse.
1
2𝜋𝐾𝑈 𝑊(𝑒𝑗𝜔 ) ²
𝜋
−𝜋 (8)
The advantage is that there is a trade-off between spectral solution
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and spectral masking. For a data window modified periodogram
resolution is 3dB bandwidth.
𝑅𝑒𝑠 Ṕ𝑀(𝑒𝑗𝜔 ) = (∆𝜔)3𝑑𝐵 (9)
3. SIMULATION AND RESULTS
Step 1:The input signal is considered as reference signal in the
modified periodogram algorithm. This input signal is called as
Synthetic signal as shown in Fig.1.
Step2: Power Spectrum analysis using normalized frequencies is
performed for the synthetic signal using modified Periodogram
algorithm as shown in Fig.2.
Step 3:Raw Seismic Signal is recorded during Dynamite Blast which is
performed within 80-100 feet below the Earth and is loaded to
MATLAB by using Book_Seismic_Data.mat as shown in Fig.3.
Step 4:In any random signal, Bias or shift is present. So the Raw Signal
is detrended which removes the mean by using modified periodogram is
shown in Fig.4.
Step 5: Power Spectral Analysis for the raw signal at different
frequency components is Estimated and shown in Fig.5.
Step 6:FIR band pass frequency Spectrum isplotted. It limits the signal
bandwidth and gives normalized frequency in the range 0.02-0.3 as
shown in Fig.6.
Step 7:FIR Band Pass filtered signal is obtained by removing noise in a
particular frequency and 8th order FIR signal is used for the detrended
seismic signal as shown in Fig.7.
Step 8: After BPF, FFT spectrum in Normal Frequency vs. Magnitude
dB representation is shown in Fig.8.
Step 9: Spectral estimation of modified periodogram is calculated and
observed in the MATLAB shown in Fig.9.
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The maximum peak frequency is observed at 0.0529 on X-axis and
16.5 on Y-axis.Only X-axis normalized frequency is considered. The
frequency is calculated by the equation.
𝑤 =2𝜋𝑓
𝑓𝑠 (10)
Here𝑓𝑠 = 500 and w=0.09594*π by replacing these values in the eq
(10) tonal frequency value is 𝑓 = 23.985 Hzobserved in Fig.9
Fig.1.Synthetic signal. Fig.2.Mod. periodogram spectral
analysis.
Fig.3. Raw seismic signal. Fig.4.Detrended raw Seismic signal.
Fig.5.Raw signal spectrum. Fig.6.FIR Band Pass filter o/p.
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Fig.7.FIR Band Pass filtered signal. Fig.8.Sspectrum of seismic
signal after BPF.
Fig.9.Modified periodogram spectral analysis.
4. CONCLUSION
Many statistical techniques are used in different ways to predict
the probability of earthquakes. In this paper, the earthquake
occurrences predicted by using modified periodogram algorithm which
provides a trade-off between spectral resolution and spectral
masking.
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