Sea Bed Logging Applications: ANOVA Analysis 2 for Synthetic Data from
Electromagnetic (EM) Simulator
Hanita Daud, Radzuan Razali
Department of Fundamental and Applied Sciences
UniversitiTeknologi PETRONAS,
Tronoh, Perak, MALAYSIA
hanita_daud@petronas.com.my
Vijanth Asirvadam
Department of Electrical and Electronics Engineering
UniversitiTeknologi PETRONAS,
Tronoh, Perak, MALAYSIA
Abstract—The aim of this work is to determine the significant
level of parameters such as sediment thickness, frequency and
step size for data generated from electromagnetic (EM)
simulator for sea bed logging (SBL) application that have been
processed using cubic spline interpolation using Analysis of
Variance (ANOVA) method. Synthetics data were generated
from a simulator that is able to replicate SBL environment.
SBL is a new technique that uses controlled source
electromagnetic (CSEM) for finding resistive layers or
hydrocarbon reservoir in deep water environment. It uses very
low frequency to obtain greater wavelength for longer wave
penetration. In this work frequencies of 0.5Hz, 0.25Hz,
0.125Hz and 0.0625Hz were used and sediment thicknesses
were varied from 1000m to 3000m incremented every 250m.
Collected data were interpolated using cubic spline with step
sizes variation of 4,8,12 and 16 and mean square error (MSE)
were calculated between original and interpolated data. The
ANOVA method was applied to these MSE to study any
significant different between frequency level and spline step
size level at each sediment thickness. It was found from the
ANOVA tables that frequency level and step sizes level were
having significant difference to the MSE for every sediment
thickness below 2250m. For sediment thicknesses of equal to
2250m and above, frequency level is not significance to the
MSE but the step sizes level are still significant to the MSE.
Keywords-sea bed logging, mean square error, cubic spline
interpolation, analysis of variance
I. INTRODUCTION
Hydrocarbon exploration is the research by petroleum
geologists for hydrocarbon beneath the Earth’s surface, such
as oil and natural gas. Various techniques are used for this
kind of exploration namely seismic method and Control
Source Electromagnetic (CSEM) [1]. Seismic methods are
widely accepted and considered as proven technology for
hydrocarbon exploration and reservoir characterization [2].
However, although seismic method can identify structures
that might be expected to contain hydrocarbons, it is
practically blind to the fluids contained in the formation [3].
This explains why geophysicists prefer CSEM technique for
seabed logging which is more accurate and detail in giving
the result before drilling.
Seabed logging is the measurement of electrical
resistivity beneath the seafloor which played a crucial role
in hydrocarbon exploration and reservoir assessment and
development [4]. Hydrocarbon reservoirs are known to have
higher resistivity than surrounding water filled sediments.
Hydrocarbon reservoirs are known to have resistivity value
of 30 – 500 m in contrast to sea water layer of 0.5 – 2 m
and sediments of 1 -2 m. The changes in electric field
around the reservoirs can be measured, and the data gained
can be used to interpret the presence of hydrocarbon [5].
This SBL technique is known to be expensive and due to
this it is used to complement seismic method. SBL uses
horizontal electric dipole (HED) source to emit low
frequency electromagnetic signal that will be received by an
array of seafloor receivers. The electromagnetic energy
from the source spread in all directions and rapidly
attenuated in the conductive subsurface sediments due to
water-filled pores. The rate of decay in the amplitude and
the phase shift of the signal are controlled by geometric and
skin depth effects [6]. Figure 1 from [14] shows the sea bed
logging schematic diagram with electromagnetic (EM) wave
transmitted are reflected, refracted and guided back from the
hydrocarbon reservoir and detected by electric or magnetic
field sensors placed on the sea floor [8-11].
Figure 1: Schematic Diagram of EM Transmitted and Reflected Waves
with Air, Water, Sediments and Hydrocarbon Layers [14]
In this paper, synthetic data are generated from EM
simulator from [12]. This simulator is able to replicate the
real sea bed environment and parameters are defined as
required before running the simulation. In this work,
parameters such as frequency are varied from 0.5Hz, 0.25Hz,
0.125Hz and 0.0625Hz and sediment thickness are varied
from 1000m to 3000m incremented every 250m. Data
10
10
m
1-2 m
30-500 m
1-2 m
HC
Half Space
Overburden
Water
Air
Ship
Source
Rx4 Rx1 Rx2 Rx3
2012 IEEE Asia-Pacific Conference on Applied Electromagnetics (APACE 2012), December 11 - 13, 2012, Melaka, Malaysia
9978-1-4673-3115-9/12/$31.00 ©2012 IEEE 110