Application of statistical methods and artificial neural networks for approximating ships roll in...

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See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/277308036 Application of statistical methods and artificial neural networks for approximating ships roll in beam waves Article in Polish Maritime Research · January 2005 Impact Factor: 0.33 READS 7 1 author: Tomasz Cepowski Maritime University of Szczecin 17 PUBLICATIONS 12 CITATIONS SEE PROFILE All in-text references underlined in blue are linked to publications on ResearchGate, letting you access and read them immediately. Available from: Tomasz Cepowski Retrieved on: 28 April 2016

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Applicationofstatisticalmethodsandartificialneuralnetworksforapproximatingship srollinbeamwaves

ArticleinPolishMaritimeResearch·January2005

ImpactFactor:0.33

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1author:

TomaszCepowski

MaritimeUniversityofSzczecin

17PUBLICATIONS12CITATIONS

SEEPROFILE

Allin-textreferencesunderlinedinbluearelinkedtopublicationsonResearchGate,

lettingyouaccessandreadthemimmediately.

Availablefrom:TomaszCepowski

Retrievedon:28April2016

22 POLISH MARITIME RESEARCH, No 2/2005

INTRODUCTION

Within the contemporary shipping problems there is a pro-blem of searching for ship voyage route satisfying several crite-ria among which the following usually are the most important :

Ü voyage duration time (at assumed parameters of ship pro-pulsion system)

Ü operational cost which mainly depends on fuel consumption.

A limitation which seriously influence route choice is thecondition of safe shipping, which consists of many factorsamong which ship�s behaviour in rough seas should be distin-guished.

So many parameters influence ship�s behaviour in wavesthat accounting for all of them makes the voyage routing pro-cess very complicated. Hence, out of all the parameters, shipmaster is forced to take into account only most important ones,among which wave parameters, ship�s motion parameters oralso selected hydromechanical parameters of the ship, are num-bered. The small amount of available information does not makeit possible to use exact methods of determination of ship mo-tion in waves.

In the subject-matter literature, methods making it possibleto solve the problem in a satisfactory way, are still lacking.Design recommendations dealing with ship seakeeping quali-ties, given in classification rules, are of a very limited charac-ter. The calculation procedures there presented are rather inac-curate and they allow to determine only �designed� ship mo-tion amplitudes and accelerations which are connected only toa certain degree with real ship behaviour in waves. The appro-ximations of ship seakeeping qualities published in the scienti-fic literature are too general, rather inaccurate, and usually ap-plicable only to a given hull form [1,5].

Application of statistical methodsand artificial neural networks

for approximating ship�s roll in beam waves

Tomasz Cepowski

Maritime University of Szczecin

ABSTRACT

In the paper, were presented approximations of numerical calculations of ship�s roll on thebasis of main service parameters of the ship. This way were obtained several relationshipswhich make it possible to approximate ship roll in regular and irregular waves by usingthe parameters available in the phase of voyage routing. The relationships were elabora-ted by means of artificial neural networks as well as linear and non-linear regressionmethods. A comparative analysis of the methods regarding approximation accuracy

against standard data was also performed.

Keywords : ship's roll, regular wave, irregular wave, approximation, neural networks, regression methods

In this paper an attempt to solve the problem has been un-dertaken, aimed at elaboration of a simplified but exact modelof predicting ship�s roll on the basis of main ship service para-meters.

METHOD

The research in question was limited to approximation ofship�s roll in regular and irregular waves coming from the di-rection perpendicular to ship�s plane of symmetry. It was assu-med that approximations of the oscillations have to be elabora-ted on the basis of the parameters taken into account in shipvoyage routing and simultaneously having significant influen-ce on the motions. Among such parameters the following areusually numbered :

ª wave parameters in the form of its height and period (in thecase of aproximation of ship roll in irregular waves)

ª ship motion parametersª ship service parameters associated with, a.o., ship mass dis-

tribution and its hull hydrostatic characteristics.

In the research in question it was adopted an approach ofapproximating the standard values of the roll angles (deter-mined by means of exact numerical methods) by using the ap-proximating function f on the basis of the n-element set of in-put parameters W[X1, X2, ... Xn] :

(1)

where :

W - n-element set of input parameters : X1, X2, ... Xn

- standard values of roll angles calculated by me-ans of the exact method

f - approximating function searched for.

= f(W)

23POLISH MARITIME RESEARCH, No 2/2005

STANDARD VALUES OF ROLL ANGLES

Standard values of roll angles were determined by usingexact numerical methods based on the two-dimensional flowtheory, i.e. the SEAWAY

software (was elaborated by Shiphy-

dromechanics Laboratory, Delft University of Technology, TheNetherlands) which calculates ship motions in regular and irre-gular waves. In Fig.1 are presented the ship roll amplitude cha-racteristics calculated by means of the software, and showedtogether with the characteristics obtained from model tests [10].

The approximations and numerical calculations were car-ried out for the S-175 model containership of the followingmain dimensions :

Its hull form is given in Fig.2.

The numerical calculations were performed by applying,a. o., the modified method of two-dimensional flow, accoun-ting for diffraction of wave loads [4] , and assuming ITTC wavespectrum.

On the basis of literature data, were selected the parame-ters which have decisive influence on ship roll, and simultane-ously considered as the service ones. To them it belongs, a.o. :

Taking into account that the volumetric displacement Ñ canbe expressed in the form of the mean draught d , and that theinitial transverse metacentric height GM depends on the hei-ght of ship gravity centre ZG, one decided to determine theship roll approximations by using :

for which the following rangesof their values were assumed :

and

Additionally, for approximationof ship roll in irregular waves it was assumed :

For all the above mentioned variants roll angle amplitudesof ship in regular and irregular waves were calculated, and thisway the set of standard data for approximations was obtained.

APPROXIMATION OF ROLL AMPLITUDES

OF S-175 CONTAINERSHIP

IN REGULAR WAVES

The approximation of ship roll amplitudes in regular wa-ves (in irregular waves as well) was carried out by means ofstatistical methods, i.e. linear and non-linear regression, as wellas artifical neural networks. The latter method belongs to rela-tively novel mathematical-numerical methods placed in the fieldof �artificial intelligence�, and it finds more and more applica-tions in different domains of science and engineering. The re-search results published in [6, 8, 9] show broader and broaderpossiblities of application of artificial neural networks to theproblems of ship design and operation.

On the basis of [1,8] and the performed investigations ithas appeared that the best model of roll amplitude characteri-stics against the assumed standard data is the following :

(2)

where :

a , b � coefficients dependent on ship service parameters� wave frequency [s

-1].

The coefficients a and b were approximated by using thestatistical methods and artificial neural networks, as shownbelow.

Approximation of the coefficients a and bby using statistical methods

To approximate the coefficients a and b in the equation (2)linear and non-linear regression was used. When using the li-near regression the following relationships appeared the bestout of all investigated models :

Fig. 1. Roll angle amplitude characteristics of the containership�Nedlloyd Dejima� of : L = 270 m, B = 32.20 m, d = 10.85 m, CB = 0.596,

ZG = 16.45 m, in beam waves, acc. [10]

L (length between perpendiculars) = 175 mB (breadth) = 25.4 md (design draught) = 9.5 m.

Fig. 2. Theoretical hull frames of S-175 containership, acc. [4]

ð the ship volumetric displacement ð the initial transverse metacentric height GMð the height of the ship gravity centre ZG.

« the mean draught d« the initial metacentric height GM

© for d : from 7 to 9 m© for GM : from 0.3 to 1.5 m

© for the ship speed V : from 0 to 20 knots.

¯ values of the significant wave height Hs :from 2 to 4.5 m, taken with 0.5 m step

¯ values of the characteristic wave period T :from 6.5 to 14.5 s, taken with 2 s step.

2

b1

a)(Y

24 POLISH MARITIME RESEARCH, No 2/2005

(3)

(4)

where :

0 , ..., 8 � coefficients whose values are given in Tab. 1The remaining symbols � as explained above.

When applying non-linear regressionthe following relationships appeared the best ones :

(5)

(6)

where :

GMVdb 98760

GMVdb 131211101

10 if 140b otherwise 00

11 if 141b otherwise 01

0 , ..., 14 � coefficients whose valuesare given in Tab.2 and 3.

Approximation of the coefficients a and b

by means of artificial neural networks

Among all investigated networks used for approximatingthe coefficients a and b in the equation (2) the MLP neural net-works of the below given form, showed the highest accuracy :

(7)

where :

the symbols : d, GM, V � as explained above.S � the vector of normalizing values : [0.5 0.05 0.833]P � the vector of displacement values : [- 3.5 0 - 0.250]

The matrices, vectors and constantsnecessary to determine the coefficient a :

A � matrix of weight values :

B � vector of threshold values :

[-0.93 -0.764 0.847 -0.201 1.02 0.635 -0.568 -0.181 -0.522 0.926 1.109 -0.516 -0.863]

C � vector of weight values :

[1.03 -0.025 -0.528 -0.34 -0.469 -0.64 -0.259 -0.053 0.275 -0.588 -0.810 0.804 -0.082]

0, 1, 2 � the coefficients having the values :

0 = - 0.323, 1 = - 0.305, 2 = 0.496.

The matrices, vectors and constantsnecessary to determine the coefficient b :

A � matrix of weight values :

B � vector of threshold values :

[-0.515 0.813 -1.374 1.575 -0.769]

C � vector of weight values :

[1.562 -1.461 -2.731 -3.637 2.197]

0, 1, 2 � the coefficients having the values :

0 = - 0.773, 1 = - 0.547, 2 = 3.475.

Assessment of the approximations

To assess accuracy of the approximations,were used RMS values calculated from the expression :

(8)

where :

RMS � error valueY w � standard values of ship roll amplitudesY � approximated values of ship roll amplitudesn � number of considered variantsm � number of the values approximated

on the amplitude characteristics.

The accuracy analysis was carried out for :

Values of the RMS errors regarding the elaborated rela-tionships, for the above mentioned cases, are given in Tab.4.And, in Figs.3 to 5 the elaborated approximations are compa-red respective to selected variants.

From Tab.4 and Fig.3 to 5 it results that the approximationsobtained by using the MLP artificial neural network show thegreatest accuracy regarding interpolation and extrapolation.

APPROXIMATION OF ROLL AMPLITUDES

OF S-175 CONTAINERSHIP

IN IRREGULAR WAVES

Approximations of numerically calculated significant va-lues of roll angle amplitudes in irregular waves were perfor-med on the basis of ship service parameters as well as waveparameters. To this end also statistical methods (linear and non--linear regression) and artificial neural networks were applied.

dGMVd

GM

dGMda

543

2

210

2

8

2

76 dd

GMdb

Table 1

d

GMGM

Vd

expa54

321

0

1100 bbb

Table 2

Table 3

m

YY

n

1RMS

2

w

Table 4

1) values of the input parameters for which approximationswere elaborated

2) the value of the initial metacentric height GM = 2 m,being out of the range of the elaborated approximations.

25POLISH MARITIME RESEARCH, No 2/2005

Approximation of ship roll amplitudesin irregular waves

by means of statistical methods

When using linear regression, out of all consideredrelationships, the following one appeared the best :

(9)

where :

1/3 � significant roll angle amplitude [°]

0 , 1 , 2 , 3 , 4 � the coefficientswhose values are given in Tab.5d, GM, V � as explained above

T � characteristic wave period [s]Hs � significant wave height [m].

And, when applying non-linear regression, the exponentialrelationship of the below given form appeared the best out ofall considered models :

(10)

where :

0 , 1 , 2 , 3 , 4 , 5 , 6 � the coefficientswhose values are given in Tab.6.

In both relationships the values of the determining coeffi-cient prove that the proposed relationships well match up withthe standard data. From variance analysis it results that bothequations are essential. Simultaneously the regressions of de-pendent variables 1/3 indicate that all components of both equa-tions (including their free terms) are essential.

Approximation of ship roll amplitudesin irregular waves

by means of artificial neural networks

Out of all considered networks, the following neuralnetworks revealed the best approximation features :

Statistically significant roll angle amplitudes 1/3 approxima-ted by means of the MLP neural network can be calculatedwith the use of the following equation :

(11)

where :

1/3 , d, GM, V, T, Hs � as explained above

A � matrix of weight values :

B � vector of threshold values :[0.2133 2.9327 -0.6466 -1.6343 -0.2292 0.7501 -2.5607 -1.9524 2.1205 0.9054 2.9620]

C � vector of weight values :[0.2687 -1.7393 -1.0205 -1.7328 0.3104 0.7946 2.5177 -1.0679 -2.2512 0.7164 2.6939]

S � vector of values :[0.500 0.833 0.050 0.125 0.400]

P � vector of displacement values :[-3.500 -0.250 0.000 -0.813 -0.800]

0, 1, 2 � coefficients having the values :

0 = - 0.2061, 1 = - 0.017, 2 = 0.102.

To calculate values of the ship roll amplitudes 1/3 appro-ximated with the use of the RBF neural network one can applythe following generalized equations :

Table 5

Table 6

Fig. 3. Values of the ship roll transfer function Y ,at V = 10 kts, d = 9 m, GM = 0.3 m

Fig. 4. Values of ship roll transfer function Y ,at V = 20 kts, d = 7 m, GM = 0.3 m

Fig. 5. Values of ship roll transfer function Y ,at V = 10 kts, d = 8 m, GM = 2.2 m

Explanation to Figs 3÷5 :

Ø the MLP network of 5 inputs x 11 hidden neuronsx 1 output

Ø the RBF (Radial Basic Functions) network of 5 inputsx 180 hidden neurons x 1 output.

26 POLISH MARITIME RESEARCH, No 2/2005

(12)

where :

Input values for the equation (12) were normalized to be con-tained within the interval : 0...1, and the neurons of hidden layerwere activated by means of an exponential function. Because oftoo large dimensions of the matrix A and remaining vectors itwas decided not to present values of elements of the matricesand vectors as well as values of normalizing coefficients.

Values of correlation coefficients of both networks show thatboth proposed models well match up with standard values.

Assessment of the approximations

To assess accuracy of the approximations, RMS� valuescalculated from the following expression, were applied :

(13)

where :

RMS' � error value

w � standard values of ship roll amplitudes

1/3 � approximated values of ship roll amplitudesn � number of considered variants.

The accuracy analysis was carried out for :

1) values of the input parameters for which approximationswere elaborated

2) the value of the initial metacentric height GM = 2 m, andthat of the significant wave height Hs = 3 ÷ 6 m, beingbehind the range of the elaborated approximations.

Values of the RMS� errors associated with the elaboratedrelationships for the above mentioned cases are given in Tab.7.

From the table it results that in both cases the most accurateappear the approximations obtained with the use of the MLPartificial neural network. The approximations elaborated bymeans of linear regression are loaded with a small error in thecase of interpolation, and with rather large one as far as extra-polation operations are concerned.

Addtionally, to more precisely verify the proposed rela-tionships the falsification method was applied [7]. To this end,such ranges of input parameters were searched for which theelaborated approximations appeared the least accurate. Re-sults of the investigations are graphically presented in Fig.6÷÷8 (for interpolation), and in Fig.9 (for extrapolation). Thediagrams confirm that in both cases the approximation withthe use of the MLP artificial neural network appears the mostaccurate.

C)BAHs] T, V, GM, [d,(3/1

Table 7

Fig. 6. Significant ship roll amplitudes 1/3 ,at GM = var , d = 7 m , V = 0 , T = 14.5 s , Hs = 4 m.

Fig. 7. Significant ship roll amplitudes 1/3 ,at d = var , GM = 1.5 m , V = 0 , T = 14.5 s , Hs = 4 m

Fig. 8. Significant ship roll amplitudes 1/3 ,at V = var , d = 9 m , GM = 1.5 m , T = 14.5 s , Hs = 4 m

Fig. 9. Significant ship roll amplitudes 1/3 ,at V = var , d = 9 m , GM = 2 m , T = 9.5 s , Hs = 6 m

A � [5 x 180] matrix of weight valuesB � 180-element vector of constantsC � 180-element vector of weight values.

Explanation to Figs 6÷9 :

n'RMS

2

3/1w

27POLISH MARITIME RESEARCH, No 2/2005

ACCURACY ASSESSMENT

OF THE ELABORATED APPROXIMATIONS

WITH A VIEW OF PREDICTING SHIP ROLL

IN IRREGULAR WAVES

The above presented relationships make it possible to ap-proximate ship roll in regular and irregular waves. The firstmethod allows to approximate roll amplitude characteristicson the basis of the ship service parameters (d, GM, V) and nextto calculate any statistical values of roll amplitudes for anywave spectrum. And, the second method makes it possible todirectly approximate ship roll amplitudes in irregular waves.

In this part of the investigations the two approaches werecompared regarding their accuracy in predicting ship roll mo-tion in irregular waves against the standard values. The analy-sis was performed on assuming the values of input parametersto be contained within :

v the ranges of the parameters for which the approximationswere elaborated

v behind the ranges of the parameters, in order to test thisway extrapolation capabilities of the elaborated relationships.

In the first case the calculations were carried out for :d = 8 m GM = 0.9 m Hs = 4 m.

And in the second case for :d = 9.5 m GM = 2 m Hs = 6 m.

In both cases the characteristic wave period T was assumedequal to10 s, and the ship speed V within the range from 0 to20 knots.

The analysis was performed for the approximations whoseaccuracy was the greatest and which were described by :

Ø for ship roll in regular waves the relationship (2) having thecoefficients approximated with the use of (3), (4), and (7)

Ø for ship roll in irregular waves the relationships (9) and (11).

In order to determine ship roll in irregular waves the expres-sion (2) and the wave energy spectrum recommended by ITTCwas used. Results of the calculations are graphically presentedin Fig.10 and 11.

From the diagrams given in Fig.10 and 11 it results thatboth presented approaches show similar interpolation capabi-lities. The extrapolation of roll amplitudes in irrerular wavesby using (9) and (11) yields rather accurate results against the

standard values. Whereas the application of the approximation(2) to determine significant roll amplitudes in irregular wavesbrought in erronous solutions, especially in the case of extra-polation.

RECAPITULATION

¦ In the paper were presented approximations of ship roll inregular and irregular waves by means of artificial neuralnetworks and linear and non-linear regression methods, onthe basis of main ship service parameters (speed, draught,initial transverse metacentric height), and � in the case ofapproximation ship roll in irregular waves � wave parame-ters (significant height and characteristic period of waves).The example approximations were elaborated for S-175model containership.

¦ From the performed investigations it results that the rela-tionships obtained by means of MLP artificial neural net-works show the largest accuracy regarding interpolation andextrapolation of ship roll amplitudes both in regular andirregular waves.

¦ Next, basing on the above mentioned approximations, twoapproaches to predicting ship roll amplitudes in irregularwaves were analyzed :

s approximation of roll amplitudes in regular waves, andnext calculation of their significant values in irregularwaves

s direct approximation of roll amplitudes in irregularwaves.

¦ From the performed investigations it results that the appro-ximation of ship roll angles by means of amplitude charac-teristics yields satisfactory results only in the case of inter-polation. Whereas the second approach provides relativelyaccurate solutions both in the case of interpolation and extra-polation.

¦ The presented method makes it possible to approximate shiproll angle amplitudes calculated by using exact numericalmethods, and they can be also applied to determine opti-mum ship voyage routes. The proposed approach may bealso used to approximate real values of roll angle amplitu-des on the basis of data recorded onboard the ship duringits service.

NOMENCLATURE

B - ship breadthCB - block coefficientd - ship draughtFn - Froude numberGM - initial transverse metacentric height

Fig. 10. The significant ship roll amplitudes 1/3 ,at V = var , d = 8 m , GM = 0.9 m , H = 4 m , T = 10 s

Fig. 11. The significant ship roll amplitudes f1/3 ,at V = var , d = 9.5 m , GM = 2 m , H = 6 m , T = 10 s

Explanation to Figs 10,11 :

28 POLISH MARITIME RESEARCH, No 2/2005

Hs - wave heightL - ship length between perpedicularsT - characteristic wave periodV - ship speedZG - height of the ship gravity centre

- ship volumetric displacement- wave length- roll amplitude- wave frequency

Akcronyms

ICLL - International Convention on Load LinesMLP - Multilayer PerceptronRAO - Response Amplitude OperatorRBF - Radial Basic FunctionsUBS - Universal Bulk Cargo Ship

BIBLIOGRAPHY

1. Cepowski T: The Proposal of Optimization Method of ShipsDesign Parameters on The Basis of Short-Term RollingPrediction. 13th International Conference on Hydrodynamics inShip Design, HYDRONAV�99, Gdañsk-Ostróda. 1999

2. Calisal S.M., Howard D., Mikkelsen J.: A Seakeeping Study ofthe UBS Series. Marine Technology, Vol. 34, No.1, Jan. 1977

3. Journée J.M.J.: Verification and Validation of Ship MotionsProgram SEAWAY, Report1213a. Delft University of Techno-logy, The Netherlands. 2001

4. Journée J.M.J.: Theoretical Manual of SEAWAY. Report1216a,Delft University of Technology, The Netherlands. 2001

CONTACT WITH THE AUTHOR

Tomasz Cepowski, D.Sc., Eng.Institute of Marine Navigation,

Maritime University of SzczecinWa³y Chrobrego 1/2

70-500 Szczecin, POLANDe-mail : [email protected]

Under auspices of EFC technical scientific projectsare carried out as the task force 2 dealing with :

Corrosion and protection of steel structuresagainst corrosion

The activity is supervised by Prof. K. Darowicki, Headof the Department of Electrochemistry, Corrosion and Ma-terials Engineering, Chemical Faculty, Gdañsk Universityof Technology.

On 20-21 June 2004 in Prague, the Department in co-operation with the Department of Metals and CorrosionEngineering, Czech's Institute of Chemical Technology, or-ganized the workshop on :

Industrial heat exchanger problems Non-destructive Testing (NDT) inspection

Results of altogether 17 projects were presented, 12 outof which were prepared by scientific workers from GdañskUniversity of Technology. It was the following presenta-tions :

¯ Darowicki K., Felisiak W.: Applications of ellipsometryin corrosion measurements

¯ Darowicki K., Kawula J.: Applications of conductingpolymers to corrosion protection a review

¯ Darowicki K., Mirakowski A.: Use of acoustic emissionto detect the pitting corrosion of aluminum

Task force 2 workshopof European Federation of Corrosion (EFC)

5. Kukner A., Aydm M.: Influence of Design Parameters onVertical Motions of Trawler Hull Forms in Head Seas, MarineTechnology, Vol. 34, No.3, July 1997

6. Mesbashi E., Bertram V.: Empirical Design Formuale UsingArtificial Neural Nets. 1st International EuroConference onComputer Applications and Information Technology in theMaritime Industries, COMPIT�2000. Potsdam. 2000

7. Popper K.: The Logic of Scientific Discovery. Routledge, 14thPrinting. 1977

8. Szelangiewicz T., Cepowski T.: Application of Artificial NeuralNetworks to Investigation of Ship Seakeeping Ability, Part 1.Polish Maritime Research, Vol 8, No.3, September 2001

9. Szelangiewicz T., Cepowski T.: Application of Artificial NeuralNetworks to Investigation of Ship Seakeeping Ability, Part 2.Polish Maritime Research, Vol 8, No.4, December 2001

10.Zhou, Z., Zhou, D., Xie, N: A Seakeeping Experiment Research onFlokstra Container Ship Model. Technical Report 4 of Study onReviewing Freeboards of ICLL 1966. China Classification Society,Shanhai Rules and Research Institute Shanhai. China. 1996

¯ Darowicki K., Orlikowski J., Arutunow A.: Detailedanalysis of the passive-active transition during the pas-sive layer cracking using dynamic electrochemical im-pedance spectroscopy

¯ Darowicki K, �lepski P.: Electrode impedance measu-rement of non-stationary systems

¯ Darowicki K., Szociñski M.: Impedance investigationof organic coatings subjected to alternating mechanicalstress impact

¯ Darowicki K., Zieliñski A.: Application of electroche-mical noise technique in corrosion monitoring

¯ Klenowicz Z., Darowicki K., Krakowiak S., KrakowiakA.: Flow monitoring shows the way to diminish erosionof tube outer surfaces

¯ Krakowiak S., Darowicki K., �lepski P.: Pitting corro-sion practical experience and laboratory investiga-tions

¯ Miszczyk A., Darowicki K.: Intercoat adhesion moni-toring using impedance spectroscopy

¯ Orlikowski J., Krakowiak S., �lepski P., Darowicki K.,Arutunow A.: Digital monitoring system of corrosion inelectrochemical environments

¯ ¯akowski K.: A time-frequency method for detection ofelectromagnetic field interference on metal constructions.

Apart from the above, 4 reports were presentedby scientists from Chech Republic

and one from Portugal.