art%3a10.1007%2fs12665-012-1783-z
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O R I G I N A L A R T I C L E
Prediction of unconfined compressive strength of carbonate rocksusing artificial neural networks
Nurcihan Ceryan Umut Okkan Ayhan Kesimal
Received: 7 August 2011 / Accepted: 14 June 2012/ Published online: 3 July 2012
Springer-Verlag 2012
Abstract The unconfined compressive strength (UCS) of
intact rocks is an important geotechnical parameter forengineering applications. Determining UCS using standard
laboratory tests is a difficult, expensive and time consum-
ing task. This is particularly true for thinly bedded, highly
fractured, foliated, highly porous and weak rocks. Conse-
quently, prediction models become an attractive alternative
for engineering geologists. The objective of study is to
select the explanatory variables (predictors) from a subset
of mineralogical and index properties of the samples, based
on all possible regression technique, and to prepare a
prediction model of UCS using artificial neural networks
(ANN). As a result of all possible regression, the total
porosity and P-wave velocity in the solid part of the sample
were determined as the inputs for the LevenbergMarqu-
ardt algorithm based ANN (LM-ANN). The performance
of the LM-ANN model was compared with the multiple
linear regression (REG) model. When training and testing
results of the outputs of the LM-ANN and REG models
were examined in terms of the favorite statistical criteria,
which are the determination coefficient, adjusted determi-
nation coefficient, root mean square error and variance
account factor, the results of LM-ANN model were more
accurate. In addition to these statistical criteria, the non-parametric MannWhitneyU test, as an alternative to the
Studentsttest, was used for comparing the homogeneities
of predicted values. When all the statistics had been
investigated, it was seen that the LM-ANN that has been
developed, was a successful tool which was capable of
UCS prediction.
Keywords Carbonate rock Unconfined compressivestrength Porosity Wave velocity All possible
regression Artificial neural networks LevenbergMarquardt algorithm
Introduction
One of the important rock mechanic parameters for engi-
neering geologists, geotechnical engineers and mining
engineers is the determination of the unconfined com-
pressive strength of rocks (UCS), which is considered by
many researchers to be the most essential rock material
property (Bieniawski 1974). This parameter has great
importance in rock mechanic applications such as tunnel
and dam design, rock blasting and drilling, mechanical
rock excavation and slope stability. There are basically two
methods for assessing the UCS of rocks. One, known as the
direct method, is to test the specimens in the laboratory, the
other, known as the indirect method, is to use previously
derived empirical equations from the literature (Baykaso-
glu et al.2008). Testing procedures for the direct method
have been standardized by both the American Society for
Testing and Materials (ASTM) and International Society
for Rock Mechanics (ISRM). High-quality core specimens
are needed for direct determination of UCS in a laboratory.
N. Ceryan (&)
Department of Geological Engineering,Balkesir University, Balikesir, Turkey
e-mail: [email protected]
U. Okkan
Department of Civil Engineering,
Balkesir University, Balikesir, Turkey
e-mail: [email protected]
A. Kesimal
Department of Mining Engineering,
Karadeniz Technical University, Trabzon, Turkey
e-mail: [email protected]
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However, high quality cores in sufficient quantities cannot
always be extracted from weak, highly fractured, weath-
ered and thinly bedded rocks. In addition, careful execution
of this test is very difficult, time consuming, and expensive
and involves destructive tests (Gokceoglu and Zorlu2004;
Baykasoglu et al.2008). To overcome these difficulties, the
indirect method considering simple index parameters and/
or mineralogical analyses and basic mechanical tests of thephysical properties, were developed, including the P-wave
velocity, Schmidt hammer, Point load index (e.g., Kahr-
aman 2001; Chang et al.2006; Ceryan et al.2008; Oyler
et al.2010), block punch test (Ulusay et al.2001; Altindag
et al.2004) and core strangle test (Yilmaz2010). For some
of these studies, rock fabric, mineralogic and petrographic
properties were obtained using image analysis (Akesson
et al. 2001; Lindqvist and Akesson 2001; Jensen et al.
2010). This is because these tests and analyses have smaller
samples and are simpler, faster and more economical (Bell
1978; Fahy and Guccione1979; Brooks1985; Doberenier
and De Freitas 1986; Hawkins and McConnell 1990;Shakoor and Bonelli 1991; Ulusay et al. 1994; Romana
1999; Alvarez Grima and Babuska1999; Singh et al.2001;
Gokceoglu2002; Gokceoglu and Zorlu2004; Sonmez et al.
2004; Chang et al. 2006; Oyler et al. 2010). Indirect
methods for UCS prediction are generally preferred, par-
ticularly when there are limited laboratory facilities
(Baykasoglu et al.2008).
The statistical methods used in rock engineering, for
example the simple and multiple regression techniques, are
conversional predictive models for estimating the
mechanical properties of rock materials including UCS. In
addition to these conventional methods, new techniques
such as artificial neural networks, fuzzy inference systems,
genetic programming, and regression trees are also gaining
considerable attention for estimating UCS (Meulenkamp
1997; Alvarez Grima and Babuska1999; Meulenkamp and
Alvarez Grima 1999; Singh et al. 2001; Kahraman and
Alber2006; Baykasoglu et al.2008; Yilmaz and Yuksek
2009; Sarkar et al. 2010; Yagiz et al. 2012). Since the
1990 s, ANN have recently become more popular, espe-
cially where fewer correlation coefficients of regression
equations with more input variables are required to com-
pletely define rock characteristics and the more flexible
operations between input and output variables (Garret
1994; Huang and Wanstedt1998; Baykasoglu et al.2008).
It is a form of nonlinear analysis which is based on the
understanding of the brain and nervous system (Ghabousi
et al.1991; Ham and Kostanic2001). Furthermore, it is a
fundamentally different approach that has to learn and
generalize interactions between many variables. Conse-
quently, ANN has great potential for modeling material
behavior from experimental data (Ghabousi et al. 1991;
Ellis et al.1992). One of the major advantages of ANN is
its efficient handling of highly non-linear relationships in
data, even when the exact nature of such relationships is
unknown (Dehghan et al. 2010). ANN models are well
suited for UCS predictions, because of the complex nature
of the interrelationships between the various quality
parameters, composition and processing conditions (Deh-
ghan et al. 2010). In the last few years, artificial neural
networks (ANN) have generally been used to establishedpredictive models of UCS for rock engineering applica-
tions (Meulenkamp and Alvarez Grima 1999; Singh and
Dubey2000; Kahraman and Alber2006; Zorlu et al.2008;
Yilmaz and Yuksek2008; Sarkar et al.2010; Cevik et al.
2011; Yagiz et al. 2012). The performance of the ANN
models was also compared with other statistical methods
(e.g., regression analysis). These studies demonstrated that
the results of ANN were more precise than the conven-
tional statistical approaches (Nie and Zhang1994; Tiryaki
2008; Baykasoglu et al.2008; Dehghan et al.2010; Yagiz
et al.2012).
The mechanical strength of carbonate rocks such aslimestone is predominantly governed by five parameters:
porosity, cleavage properties, crystal size, lithification and
micro cracks (Chang et al. 2006, Jensen et al. 2010).
However, porosity in many studies has been considered a
basic input parameter when estimating the UCS of car-
bonate rocks. (Mohd 2009; Asef and Farrokhrouz 2010;
Jensen et al.2010). Furthermore, ultrasonic wave velocity
has often been used in estimation models as a nonde-
structive method that is portable, cheap and easy to use.
(e.g., DAndrea et al.1965; Youash1970; Saito et al.1974;
Lama and Vutukuri1978; Gaviglio1989; Baykasoglu et al.
2008; Diamantis et al. 2009; Yilmaz and Yuksek 2009;
Ameen et al.2009; Moradian and Behnia2009; Kahraman
et al.2009; Dehghan et al.2010, Sarkar et al.2010; Yagiz
et al.2012). However, some significant rock indices such
as the P-wave velocity in the solid parts of rock materials
have not yet been considered in building predictive models
for the UCS of sedimentary rocks.
In this study, the aim is to establish predictive models
for the UCS of carbonate rocks formed from various facies
exposed in the Tasonu quarry, Trabzon, NE Turkey, used
in rock engineering applications. The fabric and its com-
ponents (calcite, clay and, rock and mineral fragments) of
carbonate rocks in the field of study are highly variable due
to the development of different facies. They are mostly
hollow macro- and micro-cracks. The surface structure has
pitted, pitted to vuggy and vuggy shapes. For these reasons,
the rocks studied are known as a group of problematic
rocks such as clay and much-fractured rocks. Conse-
quently, the use of estimation methods was seen to be
useful in determining the UCS. The objective in this study
is to select the explanatory variables (predictors) from a
subset of mineralogical and index properties of the
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samples, based on an all possible regression technique, and
to prepare a prediction model of UCS using ANN. ANN
method was preferred because the main advantage of it
over conventional methods is that it does not require
detailed information about the complex nature of the
underlying process under consideration to be explicitly
described in mathematical form. Some extensive applica-
tion and reviews of such models proposed for the predic-tion of geological variables were reported (Nie and Zhang
1994; Yilmaz and Yuksek2008,2009; Yagiz et al.2012).
The LevenbergMarquardt algorithm based ANN model
was used as the prediction method in this study. The
advantages of LevenbergMarquardt algorithm are that it is
usually faster and more reliable than any other back
propagation algorithms (Hagan and Menhaj1994). Thus it
can handle situations when the relationship between input
and output variables is nonlinear. The performance of LM-
ANN was also compared with the conventional method of
multiple linear regression (REG).
Material and testing procedures
The carbonate rocks samples developed in different facies
and were taken from the Tasonu Quarry, Trabzon, north-
east Turkey (Fig.1). These rocks are used as the raw
materials by Trabzon Askale Cement Factory. They are
part of the Kirechane Formation, which developed in the
Campanian (Fig.2).
The mineralogical composition of the samples from the
Kirechane Formation was studied using X-ray diffraction
(XRD) at Hacettepe University. Semi-quantitative per-
centages of the minerals are calculated by the method
developed by Gundogdu (1982). Details of the method can
be found in Temel and Gundogdu (1996). The some sam-
ples from the quarry were 100 % CaCO3. In other samples,
there were significant variations in other components (clay,
feldspar, biotite and opaque minerals; Table1). In Table1,
the result of XRD analysis, index and strength properties of
the samples examined are given.
In this study, 56 groups of block samples, each sample
having the approximate dimensions of 30 930 930 cm,
were collected in the field for the rock mechanics tests
using core drilling machine of the Rock Mechanics Labo-
ratory in the Engineering Faculty of Karadeniz Technical
University. Core samples were prepared from the rockblocks: they were 50 mm in diameter, and the edges of the
specimens were cut parallel and smooth (ISRM 2007;
Fig.3). Some tests, such as specific density, unit weight,
porosity, effective porosity, P-wave velocity, slake dura-
bility, aggregate impact value and UCS, were carried out in
the laboratory. The physical property and UCS tests were
performed on 15 samples for each sample group. The slake
durability and aggregate impact value test were performed
on three samples for each group. ISRM (1981) suggests
two cycles slake durability. However, Gokceoglu et al.
(2000) proposed four cycles. Similarly, four cycles slake
durability index were used in this study.The total porosity (n) and effective porosity of the rock
were estimated from the following equations:
n 1qsqd
1
neWs Wd
qwV 2
whereqsis the dry density,qdthe density of solid particles,
qw the water density, Wd the weight of the sample in theFig. 1 Location of Tasonu quarry (Trabzon, NE Turkey)
L7
L0 L4b
20
9
23
13
18
11
L4b
L4b
L8c
L8c
L8b
L8b
L8a
L6
L0
L8b
L8b
L1
L1
L0
L0
L2
L2
L2
L3a
8
12
18
25
15
7
21
20
15
L0
15 12
L3b
L0
L5
L5
15
16
L4b 15
L8b
L8b
L4a
L3a
L3a
L3a
584800 585000 585200
N
100 m0
Fig. 2 Geological map of Tasonu quarry (L0basalt, andesit and their
piroklastic, L1 volcanic pebbly red tuff, L2 red tuff alternate with
white limestone, L3 common macro shelly karstic voided limestone
(a), intercalated with red tuff (b), L4 fine grained karstic voided
carbonate mudstone (a) that overlie red sandy clayey limestone (b),
L5 alternate with sandy limestone clayey limestone and marl, L6
volcanic tuff intercalate with clayey limestone and mar, L7 sandypebbly limestone,L8 carbonate cemented sandstone intercalated with
clayey limestone and marl (b). Lower part of the sandstone contain
silicified level (a), Interbedded common macro fossiliferous with
biotite tuffacous carbonate cemented sandstone and sandy limestone
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Table 1 Mineralogical, index and strength properties of the samples examined
Smpl Clt Cly Fld Qrz Qq Bi n ne Id Vp Vm UCS
1a 82 18 16.5 12.9 91.2 3,202 4,245 14.50
1b 72 9 19 16.7 13.4 91.5 3,299 4,458 16.12
2a1 69 26 5 17.3 14.8 2,449 3,475 8.98
2a2 71 20 9 20.3 16.1 88.4 2,650 3,903 13.90
2b1 54 46 18.8 11.8 84.4 2,455 2,834 8.85
2b2 55 45 20.8 13.5 85.2 2,354 2,631 7.77
3a1 95 5 17.9 14.9 3,672 5,418 17.05
3a2 93 4 3 18.2 15.6 3,517 5,507 16.72
3b1 66 34 25.6 22.7 85.9 2,293 3,255 11.34
3b2 60 36 6 25.9 22.5 87.9 2,286 3,249 13.48
3c 62 31 5 1 18.7 14.4 89.5 2,159 3,061 9.51
4a 68 23 8 1 25.0 17.4 92.5 2,991 4,458 15.37
4b 67 20 10 3 26.8 21.7 90.3 2,875 4,422 14.13
4c 51 43 4 2 21.3 12.3 91.3 2,492 2,941 12.79
j1a 56 42 2 25.0 21.6 86.5 2,200 3,362 11.38
j1b 43 51 6 33.9 30.9 83.5 1,963 2,739 9.63
j2 82 12 4 2 15.2 11.6 93.5 3,379 4,648 14.97
j3 76 8 12 2 7.4 5.0 0.0 3,787 5,391 22.69
j4 34 31 7 4 24 24.7 19.7 93.9 3,074 3,914 13.12
j5 77 22 9.6 5.8 92.8 2,913 3,589 11.92
j6a 63 18 9 11 15.8 16.8 93.0 2,780 4,391 13.62
j6b 68 11 5 20 17.6 12.5 92.9 3,263 4,762 14.32
j6c 56 34 8 2 11.8 9.1 92.9 2,652 3,579 12.47
j7 73 15 14 0 10.5 9.4 95.6 3,259 4,641 17.40
jtb8a 43 45 8 4 31.2 27.6 83.3 2,466 3,353 8.31
j8bc 87 13 0 26.6 23.2 85.4 2,522 3,858 9.86
j9a 50 38 5 2 5 12.3 9.8 91.2 2,836 3,440 12.34
j9bc 75 10 11 4 16.7 11.9 93.6 3,329 4,746 13.71j9d 86 14 8.0 6.2 95.9 3,574 5,216 17.92
j10a 83 8 5 4 16.3 14.3 91.6 3,035 4,689 15.49
j10bc 38 22 16 21 9 15.8 13.9 93.3 3,002 4,424 13.80
j11a 100 12.3 10.7 96.3 3,634 5,279 18.62
j11b 67 8 8 5 2 10 8.0 7.3 93.6 3,528 4,851 18.21
j12 100 7.4 4.7 95.2 3,649 5,321 20.76
j13 17.3 14.8 0.0 2,449 8.98
j14 53 19 7 1 10 25.2 19.9 0.0 3,286 4,946 13.16
j15 87 2 3 8 11.5 10.6 93.0 3,527 5,763 15.84
j16 10 69 6 16 33.2 31.6 80.3 1,319 1,401 7.32
j17 90 9 1 9.7 7.2 94.1 3,576 5,168 18.87
j18 10.9 7.5 3,124 4,439 11.70
j19 31 46 23 16.6 13.8 2,736 2,973 10.61
j20 86 14 11.9 9.4 90.8 3,350 4,965 15.41
j21 82 13 5 22.1 16.5 91.3 2,883 53.9 13.42
j22 82 18 17.4 13.7 93.5 3,232 57.6 14.04
j23 87 11 2 17.8 15.5 92.6 2,965 53.3 13.18
j2527 34 41 7 4 14 18.1 17.3 89.4 1,902 41.5 12.21
j26a 95 0 5 9.2 6.7 96.0 4,259 37.8 21.02
j26b 90 5 5 12.4 8.6 95.0 3,521 21.42
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dried condition, Ws the weight of the sample in the satu-
rated condition, andVthe volume of the sample.
In this study, ultrasonic pulse velocity (UPV) tests were
conducted using the first method suggested in ISRM
(1981). UPV measurements were performed on the sam-
ples in the both dried and saturated conditions. The pulsewas generated by a source-transducer: it was transmitted
through the sample and registered by a receiver-transducer.
Using an epoxy polymer between the transducers and the
test sample produced an improvement in the energy
transmission. After measurements, velocity of P-wave of
the V-wave,Vp, was calculated from measured travel time
and the distance between the transmitter and receiver. In
addition to P-wave velocity in the rock samples that lacked
pores and fissures, Vm, were calculated by employing the
Eq.3 (from Barton2007):
1
Vp /
Vfl
1 /
Vm3
where Vp is the P-wave velocity in the sample, Vfl the
velocity in the fluid, / the ratio of the path length in
the fluid to the total path length (i.e., the porosity), andVmthe P-wave velocity in rock samples lacking pores and
fissures (in other words, P-wave in the solid). In this study,
to calculate the Vm value, Vp was used for the P-wave
velocity measured in saturated samples,Vflfor the P-wave
velocity measured in the fluid, and/ for effective porosity.
UCS tests were carried out according to International
Society for Rock Mechanics (ISRM) (2007). Core samples
were prepared in 2.5:1 height/diameter ratio, with adiameter of 50 mm and height of 125 mm. Experiments
were performed on 15 samples in dried condition for each
group. During the test, samples were loaded to be broken in
10 and 15 min.
Aggregate impact tests are included in British Standards
for measurement of the mechanical properties of crushed
rock aggregate, including the aggregate impact value (AIV)
tests (BS 812 1990). In the test, samples ranging in size
from 10 to 14 mm are subjected to shock and static load.
The proportion of material passing BS 2.36-mm sieve after
loading is calculated as a percentage of the original sample
weight, and expressed as the aggregate impact and aggre-
gate crushing values for shock and static loading,
respectively.
Method
Selection of explanatory predictors
The selection of the model inputs depends on the depen-
dent variables generally. Any type of input can be used in
modeling as long as they have acceptable correlation or
determination with the dependent variables. But, the large
number of the predictors may not produce in better results.
Hence, principal component analysis (PCA) and canonical
correlation have been used in some studies to reduce thedimension in the relationship. These types, involve a pro-
cedure that transforms a number of possibly correlated
variables into a smaller number of uncorrelated variables in
order to reduce the number of predictors (Singh and Har-
rison1985; Sharma1996).
There are several ways of selecting predictors if a large
number is available. One common method is a detailed
search in which all possible regressions are tried and one is
selected as the most appropriate predictor according to
statistical performance criteria (Neter et al.1996). Maxi-
mum adjusted determination coefficient (AdjR2), or min-
imum MallowsCpvalues can be used as such performancecriteria (McQuarrie and Tsai1998).
R2 (Eq.4) describes the proportion of the variation in
the dependent variable as explained by the predictors in
the model.R2 increases with the increase in the number of
parameters in the model. Thus, it does not by itself
indicate the correct regression model. AdjR2 (Eq.5) is
the modified version of R2 that has been adjusted for the
number of predictors in the model. AdjR2 is generally
considered a more accurate goodness-of-fit measure than
Table 1 continued
Smpl Clt Cly Fld Qrz Qq Bi n ne Id Vp Vm UCS
j28 83 7 8 2 6.8 3.7 97.4 3,980 31.6 15.24
j29 10.3 6.7 95.7 36,827 19.22
j30 12 49 16 1 22 21.3 19.7 80.5 2,072 68.3 9.75
j31 56 26 6 2 10 18.2 13.9 88.3 3,081 45.7 12.63
j33a 53 41 5 1 9.7 7.2 2,700 36.1 12.49
j33b 88 3 9 0 4.9 3.5 96.3 3,825 21.1 24.06
j33d 82 8 8 2 15.8 13.7 92.5 3,440 37.4 14.57
Clt (%), calsite; Cly (%), clay; Qrt (%), quartz; Qq (%), opacue; Bi (%), biotite; G, spesific density; ck(kN/m3), dry unit weight; n (%), total
porosity; ne (%), effective porosity; Id (%), slake durability index (fourth cycle); Vp (m/s), P-wave velocity in dry samples; Vm (m/s), P-wave
velocity in solid part of the sample; UCS (MPa), unconfined compressive strength
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R2. If Adj R2 is a criterion to select the explanatory
variables, it should only be used for the models with the
same number of parameters. If the selection of explana-
tory parameters is based on R2 and/or AdjR2, then the
problem of collinear variables in the model may arise.
This problem reduces the estimation capability of the
regression model in the verification stage (Hinnes andMontgomery 1990). An alternative criteria proposed by
Mallows (1973) is useful to correlate the predictor set and
to compare the models which have different number of
parameters.
MallowsCp(Eq.6) is a measure of the error in the best
subset model, relative to the error incorporating all vari-
ables. Adequate models are those for whichCp is roughly
equal to the number of parameters in the model (Mallows
1973).
R2 1MSEi
r2 4
AdjR2 1 n1
ni11R2 5
Cp nkMSEi
MSEF n2i1 6
where R2 is determination coefficient, AdjR2 is adjusted
determination coefficient, Cp is Mallows Cp, MSEi is
mean of residual squares in the model with j parameter,
MSEFis mean of residual squares in the full model with
kparameter,r2 is variance of the dependent variable,n is
the number of data, i is the number of parameters in the
model and k is the number of parameters in the full
model.
Fig. 3 Test samples with 50 mm diameter
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Artificial neural networks (ANN)
The basic concept of the ANN is that they are typically
made up of neurons. And in ANN, the neurons are orga-
nized in the form of layers (Fig.4).
The first and last layer of ANN is called the input and
the output layers, respectively. The input layer does not
perform any computations, but only serves to feed the inputdata to the hidden layer which is between the input and
output layers.
In general, there can be any number of hidden layers in
the ANN structures, however, from practical applications,
only one or two hidden layers are used. In addition to this,
the number of hidden layers and also the number of neu-
rons of hidden layers can be determined by the trial and
error (Ham and Kostanic2001).
There are also three important components of an ANN
structure: weights, summing function and activation func-
tion. The importance and functionality of the inputs on
ANN models are obtained with weights (W).So the successof the model depends on the precise and correct determi-
nation of weight values. The summing function (net) acts
to add all outputs; that is each neuron input is multiplied by
the weights and then summed. After computing the sum of
weighted inputs for all neurons, the activation functionf(.)
serves to limit the amplitude of these values. The activation
functions are usually continuous, non-decreasing and
bounded functions. Various types of the activation function
are possible but generally log-sigmoid function is preferred
in applications (Ham and Kostanic2001). This activation
function generates outputs between 0 and 1 as the input
signal goes from negative to positive infinity.
Weight matrix for layer 1W
(1)Weight matrix for layer 2
W(2)
1nxx R
Hidden layer
hneuronsOuput layer
mneurons 1mxx R
Fig. 4 ANN structure
Table 2 Summary of all possible regression analyses
Number of
Inputs
R2 Adj R
2Cp n ne ld Vp Vm
1 0.744 0.738 5.8
1 0.704 0.697 13.0
2 0.777 0.767 1.7
2 0.769 0.758 3.2
3 0.783 0.767 2.7
3 0.779 0.762 3.4
4 0.786 0.765 4.1
4 0.783 0.761 4.7
5 0.786 0.759 6.0
Table 3 LM-ANN and REG performances for the training and testing periods
Models Model structures R2 Adj R2 VAF RMSE(MPa)
Training Testing Training Testing Training Testing Training Testing
LM-ANN n = 2; h = 4; m = 1 0.8837 0.8126 0.8751 0.7814 87.64 81.02 1.1079 1.8970
REG rc = 5.77 ? 0.00225Vm - 0.132n 0.7950 0.7406 0.7798 0.6974 79.21 73.75 1.4298 2.2189
Table 4 Measured and LM-
ANN descriptive statistics forthe training and testing periods
Mean (MPa) Standard
deviation (MPa)
Skewness Maximum
(MPa)
Minimum
(MPa)
Training
Measured 13.52 3.19 0.18 20.76 7.77
LM-ANN 13.41 2.73 0.40 19.74 8.88
REG 13.54 2.63 -0.01 18.94 8.28
Testing
Measured 15.27 4.48 0.38 24.06 7.32
LM-ANN 15.46 4.26 -0.48 21.06 7.39
REG 15.22 4.10 -1.28 19.58 4.97
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f: ffi 1
1e: 7
In addition to thestructure andits components of ANN, the
running procedure is also important which involves typically
two phases; forward computing and backward computing.
In forward computing, each layer uses a weight matrix
[W
(v)
, for v=
1, 2] associated with all the connectionsmade from the previous layer to the next layer (Fig.4). The
hidden layer has the weight matrixW1 2Rhn, the output
layers weight matrix is W2 2Rmh. Given the network
input vector x2 Rn1, the output of the hidden layer
xout;12 Rh1 can be written as
xout;1 f1net1 f1W1x 8
which is the input to the output layer. The output of the
output layer, which is the response (output) of the network
y xout;22Rm1, can be written as
y xout;2f2net2 f2W2xout;1 9
Substituting (Eq.8) into (Eq.9) for xout,1gives the final
output y = xout,2of the network as
y f2W2f1W1x 10
After the phase of forward computing, backward
computing which depending on the algorithms to adjust
weights is used in the ANN. The process of adjusting these
weights to minimize the differences between the actual and
the desired output values is called training or learning
the network. If these differences (error) are higher than the
desired values, the errors are passed backwards through the
weights of the network. In ANN terminology, this phase isalso called the back-propagation. Once the comparison
error is reduced to an acceptable level for the whole
training set, the training period ends, and the network is
also tested for another known input and output data set in
order to evaluate the generalization capability of the ANN
(Ham and Kostanic2001).
Depending on the techniques to train ANN models,
different back propagation algorithms have been used for
modeling of UCS. These modeling studies generally
include the standard feed forward back propagation (FFBP)
algorithms such as gradient-descent (Yilmaz and Yuksek
2008; Sarkar et al.2010), gradient-descent with momentumrate (Singh et al.2001; Kahraman et al.2010; Yilmaz and
Yuksek2009), conjugate gradient (Canakci and Pala2007)
etc. As the standard FFBP algorithms have some disad-
vantages relating to the time requirement and slow con-
vergency in training, LevenbergMarquardt algorithms,
which are alternative approaches to standard FFBP algo-
rithms, were also used in some engineering applications
(Meulenkamp and Alvarez Grima 1999; Tiryaki 2008;
Fistikoglu and Okkan2011; Okkan2011).
In this study LevenbergMarquardt algorithm was used
for training. This algorithm is a second order nonlinear
optimization technique that is usually faster and more
reliable than any other standard back propagation tech-
niques (Meulenkamp and Alvarez Grima 1999; Tiryaki
2008; Fistikoglu and Okkan2011; Okkan2011, Okkan and
Dalkilic2011). It represents a simplified version of New-
tons method (Marquardt 1963) applied to the trainingANN (Hagan and Menhaj 1994).
Consider ANN structure shown in Fig.4, the running of
the network training can be viewed as finding a set of
weights that minimized the error (ep) for all samples in the
training set (Q). If the performances function is a sum of
squares of the errors as
EW 1
2
XPp1
dp yp2
1
2
XPp1
ep2; P mQ 11
where Q is the total number of training samples, m is the
number of output layer neurons, W represents the vector
containing all the weights in the network,yp is the actual
network output, anddp is the desired output.
When training with the LevenbergMarquardt optimi-
zation algorithm, the changing of weights DW can be
computed as follows
DW JTkJk lkI 1
JTkek 12
whereJis the Jacobian matrix,Iis the identify matrix,l is
the Marquardt parameter which is to be updated using the
decay rateb depending on the outcome. In particular,l is
multiplied by the decay rateb (0\b\ 1) wheneverE(W)
decreases, while l is divided by b whenever E(W)increases in a new step (k).
The LM-ANN training process can be illustrated in the
following pseudo-codes,
1. Initialize the weights andl (l = 0.001 is appropriate).
2. Computethe sum of squarederrors over all inputs,E(W).
3. Compute the Jacobian matrixJ.
4. Solve Eq.12 to obtain the changing of weightsDW.
5. Recompute the sum of squared errors E(W) using
Wk1 Wk JTkJk 1
JTkek as the trial W, and
judge
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Results
Explanatory predictors of UCS
To evaluate the strength and direction of the relationships
between the input and output, all possible regression results
of five predictor variables: n (%) total porosity, ne (%)
effective porosity, Id (%) slake durability index (fourth
cycle),Vp (m/s) (P-wave velocity in dry samples), andVm(m/s) (P-wave velocity in solid parts of the sample), and
UCS are given in Table2.
Once the explanatory predictor variables are selected,
based on the MallowsCpcoefficient, theAdjR2 values are
calculated as in Table2. Performance of the model with
n and Vm is nearly the same as that of the full model with
five variables; that is, the explained variance of UCS using
the two effective variables is nearly equal to the variance
explained using the full model. On the other hand, Mal-
lowsCp decreases rapidly with up to two variables (nand
Vm) and then increases with every addition of a variable.
Modeling of UCS using ANN
As a result of the MallowsCpbased all possible regression
analyses, the total porosity (n) and P-wave velocity in the
solid part of the sample (Vm), which are the explanatory
predictor variables of UCS, were selected as inputs for the
LevenbergMarquardt algorithm based ANN model (LM-
ANN). In the implementation of the LM-ANN, MATLAB
code was used. To compare the generalization capabilities
of the LM-ANN model, the inputoutput data were divided
into training and testing in the proportions of 2/3 and 1/3.Before presenting the inputoutput data to the LM-
ANN, all data sets were scaled to the range of 01 so that
the different input signals had the same numerical range.
The training and testing subsets were scaled to the range of
Fig. 5 Determination of number of neurons in hidden layer for the
testing period
y = 0,8564x + 2,3911
R = 0,8126
5
7
9
11
13
15
17
19
21
23
25
5 7 9 11 13 15 17 19 21 23 25
LM-ANN(2,4,
1)(M
pa)
Measured (Mpa)
Test
y = 0,8032x + 2,5519
R = 0,8837
5
7
9
11
13
15
17
19
21
5 7 9 11 13 15 17 19 21
LM-ANN(2,4,
1)(M
pa)
Measured (Mpa)
Training
y = 0,7468x + 3,4416
R = 0,795
5
7
9
11
13
15
17
19
21
5 7 9 11 13 15 17 19 21
c=5.7
7+0.00
255vm-
0.1
32n
Measured (Mpa)
Training
y = 0,7883x + 3,1954
R = 0,7406
5
7
9
11
13
15
17
19
21
23
25
5 7 9 11 13 15 17 19 21 23 25
c=5.7
7+0.00
255vm-
0.1
32n
Measured (Mpa)
Test
Fig. 6 Scatter plots of REG
and LM-ANN models for the
training and testing period
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01 using the equation zt=(xt- xmin)/(xmax - xmin),
wherextis the unscaled data,ztis the scaled data, andxmaxand xmin are the maximum and minimum values of the
unscaled data. The output values of the LM-ANN model,
which were in the range of 01, were then transformed to
real-scaled values using the equation xt= zt (xmax -
xmin) ? xmin. In this study, three widely used transfer
functions, namely tangent sigmoid, linear, and log-sigmoidare evaluated in LM-ANN structure trials. The best results
are achieved by using the log-sigmoid function which
described in Eq. (7). Otherwise, the number of the neurons
in the hidden layer, the initial Marquardt parameter (l0)
and decay rate (b) of the LM-ANN model, were also
determined by trial and error. The suitable network struc-
ture provided the best training result in terms of minimum
E(W) or root of mean E(W). The root mean square error
(RMSE), variance account factor (VAF) and the maximum
determination coefficient value (R2) were also employed in
the testing. RMSE and VAF are calculated as follows:
RMSE
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi1
n
Xni1
diyi2
s 13
VAF 1vardi yi
vardi
100 14
wherenis the number of training or testing samples,yiis the
actual network output, anddiis the measured (desired) data.
A model denoted as LM-ANN (n, h, m) (with
l0 = 0.01; b =0.10; k= 20 iterations) in Tables3and 4
comprisesn = 2 neurons in the input layer,h = 4 neurons
in the hidden layer andm = 1 neuron in the output layer.
The number of neurons in the hidden layer was deter-mined after trying various values (h = 220) for the
selected two input variables (Fig.5).
When the scatter plots of the training and testing data
sets for the LM-ANN and REG are examined, it is
observed that the standard deviations around they = x line
are much lower in the LM-ANN model. The LM-ANN
results for the training and testing periods were compared
with the desired UCS values (Figs.6, 7)
In addition to these preferred statistical criteria, homo-
geneities of the model predictions were also examined with
the MannWhitneyU(MW) test to present more evidence
on the acceptable application and success of the LM-ANN
model. This non-parametric statistical test is used to ana-
lyze two comparison groups to identify whether they have
the same distribution or not (Mann and Whitney 1947).
MW is based on the bringing together and arranging of
two groups (e.g., predicted and measured values). When
these group members are lined up, a line number is
assigned to each member. The membership status of these
members (to which group they belong) is ignored. These
line numbers are then summed up. The sum of the
members of the first group is R1and of the second group is
R2. The Uvalues can then be calculated using
Ui N1N2NiNi1
2 Ri; i 1; 2 15
After the calculation fori =1 andi = 2, U1and U2are
obtained, and the larger is chosen (U*) to determine the test
statistics.
z U N1N2
2ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiN1N2N1N21
12
q 16
5
7
9
11
13
15
17
19
21
23
25
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
c
Data Points
TestingMeasured (Mpa)
LM-ANN (2,4, 1) (Mpa)
5
7
9
11
13
15
17
19
21
1 2 3 4 5 6 7 8 910
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
c
Data Points
TrainingMeasured (Mpa)LM-ANN (2,4, 1) (Mpa)
Fig. 7 LM-ANN results with the data points for the training and
testing period
Table 5 MW statistics of LM-ANN and REG models for training
and testing periods
MW test statistics LM-ANN REG
Training Testing Training Testing
MannWhitney U 440 104 439 102
z 0.148 0.353 0.163 0.436
Asymptotic. Sig.
(2-tailed)
0.882 0.744 0.871 0.683
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where N1 and N2 are the quantities of data for the groups
compared.
The z value is compared with a 0.05 significance level
(zcr =1.96). For the values of z\ 1.96, there is no sig-
nificant difference between the measured data and model
predictions. The asymptotic significance of the z test sta-
tistics was also used when making a comparison (Table5).
When MW statistics were examined, it was shown thatboth LM-ANN and REG predictions have homogeneities
for the training and testing set. When the z statistics and
asymptotic significance values are taken as a basis, LM-
ANN again has the best performance.
Conclusions
In this study, a model was developed to estimate, by con-
sidering the index properties, the unconfined compressive
strength value of carbonate rocks formed at the differentfacies. The mineralogical and index properties of the
samples were used for modeling the UCS. The explanatory
predictors from these measured samples were selected by
performing a comprehensive all possible regression anal-
ysis, in which best parameters were determined using the
Mallows Cp value and the UCS was considered as the
dependent variable. As a result of all the possible regres-
sion analyses, total porosity (n) and P-wave velocity in the
solid part of the sample (Vm) were selected as the inputs for
the LevenbergMarquardt algorithm based ANN model
(LM-ANN).
In previous studies, elastic wave velocity measured indried samples, and seismic attenuation or P-wave velocity
ratio measured in dried and fluid conditions were used to
estimate the strength and deformation of the rocks.
P-wave velocity used for determining the mineralogical
composition in the solid part of the rock, namelyVm, was
used as an initial parameter for estimating the UCS value
in this study.
When the model training and testing outputs were
investigated, in terms of the statistics (R2, Adj R2, RMSE,
VAF, descriptive statistics) of the measured and the pre-
dicted values, LM-ANN results fitted well. In addition to
these, the non-parametric MannWhitney U test was alsoused for comparing the homogeneities of predicted values.
When all the statistics were investigated, it was seen that
the LM-ANN that was developed, was a successful ANN
algorithm that was capable of UCS modeling. The authors
also suggest that this approach can be used for the pre-
diction of other geotechnical parameters where rapid
assessment and robustness are essential.
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