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Research Article Determination of the Transport Properties of Structural Concrete Using AC Impedance Spectroscopy Techniques Lipeng Wu, Peng Dai, and Yong Li School of Civil Engineering, Shijiazhuang Tiedao University, Shijiazhuang 050043, China Correspondence should be addressed to Lipeng Wu; [email protected] Received 11 July 2016; Accepted 5 October 2016 Academic Editor: Song Han Copyright © 2016 Lipeng Wu et al. is is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. All over the world, particularly in severe environmental conditions, there are reinforced concrete structures that develop nonnegligible phenomena of durability problems. Most of the durability problems are related to hazardous substances invasion. Both engineering practice and scientific studies have revealed that the transport property of near-surface concrete is a main factor in the durability of concrete structures. Among many transport parameters, the chloride ion diffusion coefficient is the most important one, which provides important information on material design and service life prediction. In this paper, AC impedance spectroscopy technology was employed in the measurement of chloride ion diffusion coefficient. e relationship between mesostructure parameters and chloride ion diffusion coefficient was deduced by introducing a reasonable equivalent circuit model. Taking into account the conductivity difference caused by various cementitious material systems, the diffusion coefficient can be corrected, and a diffusion coefficient determination method based on AC impedance spectroscopy technique was established. For the convenience of application, a relationship between the newly proposed method and a widely recognized standard method was obtained. e proposed method can be applied to laboratory testing and establishes the theoretical basis for field tests. 1. Introduction Durability of concrete structures is one of the unsolved problems in the field of civil engineering and is an interna- tional research concern [1]. Durability problems are largely caused by the intrusion of external hazardous substances, which means that the transport property of near-surface concrete is an important aspect that affects durability [2]. A generally accepted fact is that transport property is essentially determined by the mesostructure. Concrete is a typical porous material. Its pore system includes C-S-H gel pores, capillary pores, microcracks, and micropores. Many ions, such as Ca 2+ , Na + ,K + , OH , Cl , and SO 4 2− , exist, which constitute a complex dynamic electrochemical system. Under AC excitation, the system exhibits a characteristic of a resistor-capacitor combination, and the mesostructure can be studied by using AC impedance spectroscopy. To separate the desired mesostructure parameters from measured impedance data, researchers have proposed a number of equivalent circuit models [3–8]. Some model parameters can be obtained through numerical fitting by using measured data and a preset equivalent circuit model. ese parameters can be used as quantitative characterization of the mesostructure and hydration degree of cement-based material. 2. Concrete Mesostructure and Equivalent Circuit Model e selected scale should not be small when considering the role of pores in ion diffusion. e C-S-H gel pore does not contribute to permeability. erefore, only the capillary pores and the pores between C-S-H gels were considered. Basically, three conduction pathways exist for alternating current in concrete, that is, continuous conduction, dis- continuous conduction, and the so-called “insulating” con- duction paths. e continuous conduction path is a series of connected capillary pores or connected microcracks. If the pore connectivity is cut off by cementitious material or its hydration products, the discontinuous conduction path Hindawi Publishing Corporation Journal of Engineering Volume 2016, Article ID 2630186, 8 pages http://dx.doi.org/10.1155/2016/2630186
Transcript

Research ArticleDetermination of the Transport Properties of StructuralConcrete Using AC Impedance Spectroscopy Techniques

Lipeng Wu Peng Dai and Yong Li

School of Civil Engineering Shijiazhuang Tiedao University Shijiazhuang 050043 China

Correspondence should be addressed to Lipeng Wu lipengwuoutlookcom

Received 11 July 2016 Accepted 5 October 2016

Academic Editor Song Han

Copyright copy 2016 Lipeng Wu et al This is an open access article distributed under the Creative Commons Attribution Licensewhich permits unrestricted use distribution and reproduction in any medium provided the original work is properly cited

All over the world particularly in severe environmental conditions there are reinforced concrete structures that developnonnegligible phenomena of durability problems Most of the durability problems are related to hazardous substances invasionBoth engineering practice and scientific studies have revealed that the transport property of near-surface concrete is a main factorin the durability of concrete structures Among many transport parameters the chloride ion diffusion coefficient is the mostimportant one which provides important information on material design and service life prediction In this paper AC impedancespectroscopy technology was employed in the measurement of chloride ion diffusion coefficient The relationship betweenmesostructure parameters and chloride ion diffusion coefficient was deduced by introducing a reasonable equivalent circuit modelTaking into account the conductivity difference caused by various cementitious material systems the diffusion coefficient can becorrected and a diffusion coefficient determination method based on AC impedance spectroscopy technique was established Forthe convenience of application a relationship between the newly proposed method and a widely recognized standard method wasobtained The proposed method can be applied to laboratory testing and establishes the theoretical basis for field tests

1 Introduction

Durability of concrete structures is one of the unsolvedproblems in the field of civil engineering and is an interna-tional research concern [1] Durability problems are largelycaused by the intrusion of external hazardous substanceswhich means that the transport property of near-surfaceconcrete is an important aspect that affects durability [2] Agenerally accepted fact is that transport property is essentiallydetermined by the mesostructure

Concrete is a typical porous material Its pore systemincludes C-S-H gel pores capillary pores microcracks andmicropores Many ions such as Ca2+ Na+ K+ OHminus Clminusand SO4

2minus exist which constitute a complex dynamicelectrochemical system Under AC excitation the systemexhibits a characteristic of a resistor-capacitor combinationand themesostructure can be studied by usingAC impedancespectroscopy

To separate the desired mesostructure parameters frommeasured impedance data researchers have proposed anumber of equivalent circuit models [3ndash8] Some model

parameters can be obtained through numerical fitting byusing measured data and a preset equivalent circuit modelThese parameters can be used as quantitative characterizationof the mesostructure and hydration degree of cement-basedmaterial

2 Concrete Mesostructure and EquivalentCircuit Model

The selected scale should not be small when consideringthe role of pores in ion diffusion The C-S-H gel pore doesnot contribute to permeability Therefore only the capillarypores and the pores between C-S-H gels were consideredBasically three conduction pathways exist for alternatingcurrent in concrete that is continuous conduction dis-continuous conduction and the so-called ldquoinsulatingrdquo con-duction paths The continuous conduction path is a seriesof connected capillary pores or connected microcracks Ifthe pore connectivity is cut off by cementitious material orits hydration products the discontinuous conduction path

Hindawi Publishing CorporationJournal of EngineeringVolume 2016 Article ID 2630186 8 pageshttpdxdoiorg10115520162630186

2 Journal of Engineering

Discontinuous conduction path

Discontinuous point

ldquoInsulatingrdquo conduction path

Continuous conduction path

CDP RCP

Cmat

RCCP

Figure 1 Concrete mesostructure for AC conducting

C1 C2

R1 R2

Figure 2 Converted equivalent circuit

is formed In addition to continuous and discontinuousconduction paths isolated cementitious material particlesand their hydration products or even the entire solid concreteblock can also be conductive for alternating current Based onthe above considerations the concrete mesostructure for ACconducting can be described in Figure 1

The equivalent circuit model that corresponds to Figure 1can be expressed as

1119885 =11198851 +11198852 +11198853 (1)

where 1198851 is the impedance of the ldquoinsulatingrdquo conductionpath1198851 = 1(119895120596119862mat) and 119862mat is the capacitance of the testblock 1198852 is the impedance of the discontinuous conductionpath that is the sum of the capacitance of the discontinuouspoint and the resistance of the cut-off continuous conductionpath 1198852 = 119877CP + 1(119895120596119862DP) 119877CP is the resistance of the cut-off continuous conduction path and 119862DP is the capacitanceof discontinuous point and1198853 is the resistance of continuousconduction path 1198853 = 119877CCP

According to basic circuit theory the equivalent circuitdescribed in (1) can be converted to a circuit shown inFigure 2

The conversion relationship of the two equivalent circuitsis shown in

119877CP = (1198770 + 1198771) 11987701198771 119877CCP = 1198770 + 1198771119862DP = (1198620 + 1198621) ( 11987711198770 + 1198771)

2

119862mat = 119862011986211198620 + 1198621

(2)

600500400300200100 700 8000

Z998400 (ohm)

0

100

200

300

400

500

600

minusZ

998400998400(o

hm)

Figure 3 Nyquist plot of the equivalent circuit model shown inFigure 2

A parallel combination of a capacitor and a resistor pro-duces a semicircle in theNyquist plotTherefore two semicir-cles should appear on the plot of the equivalent circuit shownin Figure 2 Figure 3 shows the relationship between the resis-tance parameters and the location and size of the semicircles

Taking into account the second equation in (2) the resis-tance of the continuous conduction path is the intersectionpoint of the right semicircle with the real axis Howeverthe Nyquist plot of the measured impedance of cement-basedmaterials does not have two semicircles but often onlya semicircle appears Figure 4 is a typical Nyquist plot ofconcrete the concrete composition was 233 Kg silica fume4427 Kg normal Portland cement 750Kg sand 1125 Kggravel 1864 Kg water so 119908119887 = 04 the test age is 28 d

The left arc does not occur which indicates that 1198620 ismuch less than 1198621 Thus the diameter of the left arc is verysmall with respect to the right arc and therefore the left arcis not visible Cabeza et al [3 7] proved this point Thusthe equivalent circuit can be further simplified as shown inFigure 5 which also shows the corresponding Nyquist plot

The above discussion indicates that 119877CCP which is theparameter that characterizes the interconnecting porositythat is most relevant to permeability can be linked withmeasured impedance spectroscopy

Journal of Engineering 3

10MHz

1MHz

40Hz

0

100

200

300

400

500

600

minusZ

998400998400(o

hm)

100 200 300 400 500 600 700 8000

Z998400 (ohm)

Figure 4 High-frequency range Nyquist plot of typical concrete

C1

R1

R0

(a) Further simplified equivalent circuit

0

100

200

300

400

500

minusZ

998400998400(o

hm)

200 400 600100 500300 700

Z (ohm)

(b) Corresponding Nyquist plot of the simplified equivalent circuit

Figure 5 Further simplified equivalent circuit and its Nyquist plot

3 Relationship between AC ImpedanceParameters and Permeability

The relationship between AC impedance parameters andpermeability can be established in two ways An empir-ical relationship between the two can be mathematicallyregressed by conducting a large number of experimentsHowever the disadvantage of this approach is the lack ofreliable theoretical basis Another way to derive some kindof quantitative relationship between the two is through theo-retical derivation This paper adopted the latter approach

Einstein and Smoluchowski presented an equation onthe diffusion of charged particles in solution in 1905 and1906 respectively this equation is known as the EinsteinndashSmoluchowski equation [9] which is shown as follows

119863119902 = 120583119902119896119861119879119902 (3)

where 120583119902 is the ion mobility (m2(Vsdots)) 119896119861 is the Boltzmannconstant (138 sdot 10minus23 JK) q is the charge carried by ions(C) and 119879 is the absolute temperature (K) Through therelationship among the Boltzmann constant the Avogadroconstant (119873119860) the Faraday constant (119865) the elementaryelectric charge (119890) and the universal gas constant (119877) thatis 119896119861 = 119877119873119860 119865 = 119890119873119860 and 119902 = 119911119894119890 where 119911119894 is the absolutevalue of valence (4) was obtained

120583119902 = 119911119902119865119877119879 119863119902 (4)

As for the most significant chloride ion diffusion coef-ficient 119863Clminus which is directly relevant to the durability ofreinforced concrete structures (4) can be specifically writtenas [9]

119863Clminus = 119877119879119911Clminus119865120583Clminus (5)

To use (5) a certain concentration of chloride solutionmust be introduced and chloride ion mobility must be con-sidered InAC impedance spectroscopy testing themeasuredresistance (or resistivity conductivity) is a result of the jointaction of various ions in a pore solution To obtain thechloride ion diffusion coefficient the contribution of chlorideions to the conductance needs to be separated from the totalconductance To achieve this a 1molL NaCl solution wasused to saturate a concrete test block to weaken the influenceof other existing ions Thus the conductivity expression 120590 =119865sum119911119894120583119894119862119894 where119862119894 is the concentration and 119911119894 is the activitycoefficient (119911119894 = 1) can be written as

120590 = 119865 lowast (120583Clminus119862Clminus + 120583Na+119862Na+) (6)

To further differentiate the contribution of chlorideions and sodium ions to the conductance the contributionpercentage of chloride ions is 61 which is close to thatof an infinitely diluted sodium chloride solution (604)under the conditions of 25∘C and 1molL concentrationthis information was verified by consulting a chemistryhandbook Combining (5) and (6) obtains

119863Clminus = 1205901198771198791641198652119862Clminus (7)

Taking into account the relationship between resistance(120588) conductivity (120590) and cell constant (119886 = 119897119860 where 119897 isthe thickness of the test block and119860 is the contact area of theelectrode and the test block) (8) is obtained

120590 = 1120588 =119886119877CCP (8)

4 Journal of Engineering

Table 1 Chemical compositions of cement and mineral admixtures ( by weight)

Composition SiO2 Al2O3 Fe2O3 CaO MgO SO3 Na2O K2OCement 2109 434 281 625 181 287 015 062Slag 3455 1436 045 3394 1116 195 028 035Fly ash 5757 2191 772 387 168 041 154 251Silica fume 9263 105 117 034 073 030 022 093w mass fraction

Therefore the relationship between chloride ion diffusioncoefficient and the interconnecting pore resistivity can beexpressed as

119863Clminus = 1198861198771198791641198652119877CCP119862Clminus (9)

In (9) the influences of other ions on chloride ion dif-fusion coefficient determination have been largely removedTo further eliminate these effects some pastes (water-binderratio = 10) were prepared and the cementitious material thatwas used is as follows fly ash + Portland cement (cementreplacement level is 20 40 and 60 resp) slag +Portland cement (cement replacement level is 25 50 and75 resp) and silicon fume + Portland cement (cementreplacement level is 5 10 and 15 resp) The chemicalcompositions of cement and mineral admixtures are listed inTable 1

A conductivity cell with a length of 692 cm and anelectrode area of 962 cm2 was also made This experimentaims to investigate the influence of different pore solu-tions caused by different cementitious materials used onconductance Strictly speaking to carry out pore solutionconductivity tests the pore solution should be squeezed outof the concrete block However given the complexity of therequired equipment and the limited amount of the extractedpore solution this research adopted the simulation approachbymeasuring highwater-binder ratio paste that was preparedby using various cementitiousmaterials Before the age of 7 dthe paste will not solidify by shaking the container severaltimes every day The paste solution was shaken for 5 minutesthe day before the test and then left undisturbed for 24 hThen the upper solution was taken and injected into theconductivity testing cell The frequency of the alternatingcurrent is 2000Hz and the test ages are 28 and 90 d Figure 6shows the test results

Figure 6 shows that the addition of mineral admixturesreduces the concrete pore solution conductivity As gen-erally accepted the most important factor that influencespermeability is connected porosity rather than pore solutionconductivity To further eliminate the influence of other ionsonAC impedance testing for chloride iondiffusion coefficientdetermination a correction factor can be introduced Toperform this step the correction factor of ordinary Portlandcement concrete can be set as a benchmark For concrete thatuses other cementitious materials the correction factor maybe determined by interpolation in accordance with Table 2

000012

000010

000008

000006

000004

000002

000000

Con

duct

ivity

(Sm

minus1 )

28 90

Age (day)

100 cem25 sg50 sg75 sg20 fa

40 fa60 fa5 sf10 sf15 sf

Figure 6 Conductivity value of different paste solutions

Table 2 Diffusion coefficient correction factor

Types of mineraladmixtures

(Replacement ratio)diffusion coefficientcorrection factor

Fly ash (20) 12 (40) 13 (60) 17Slag (25) 11 (50) 13 (75) 18Silicon fume (5) 11 (10) 13 (15) 14

4 Experimental Studies

Table 3 shows the concrete mix that was used in the experi-ment

First Φ100mm times 300mm cylinder test blocks wereprepared for the experiment Steel mold was removed oneday after pouring and then concrete cylinders were curedfor 28 or 90 d before being cut into Φ100mm times 50mmblocks for vacuum saturation (using 1molL NaCl solutionthe saturating regime is the same as that of ASTM C1202)

Then a 100mm times 100mm stainless steel plate wasadopted as the electrode To ensure close contact betweenthe electrodes and the concrete surface soaked filter papers(using 1molL NaOH solution) were introduced Prepressurewas applied to the electrodes by using screw caps Agilent4294A precision impedance analyzer was employed (seeFigure 10) and the test frequency is 40Hz to 40MHz Five

Journal of Engineering 5

Table 3 Concrete mix

Specimen number Materials used (unit kgm3)Cement Fly ash Slag Silicon fume Water Fine aggr Coarse aggr

C0 4660 0 0 0 1860 7500 11250FA1 3728 923 0 0 1860 7357 11036FA2 2766 1864 0 0 1860 7205 10809FA3 1864 2766 0 0 1860 7053 10580GS1 3495 0 1165 0 1860 7476 11214GS2 2330 0 2330 0 1860 7442 11163GS3 1165 0 3495 0 1860 7408 11112SF1 4427 0 0 233 1860 7476 11214SF2 4194 0 0 466 1860 7442 11163SF3 3961 0 0 699 1860 7408 11112JH1 2660 1140 0 0 1440 7608 11412JH2 1900 950 950 0 1440 7612 11418JH3 1950 1300 650 0 1440 7528 11292

Figure 7 Concrete blocks for the impedance test

Figure 8 Stainless steel electrodes

test points were measured for each order of magnitude Thetest block electrode electrode installation and impedanceanalyzer are shown in Figures 7ndash9 respectively

Figure 11 shows the AC impedance spectroscopy testresult of the C0 test block (90 d)

To verify the validity of the measured impedance dataa validation check by using linear KramersndashKronig test [10]

Figure 9 Electrode mounting

Figure 10 Impedance tester

was conducted Figure 12 shows the validation results oftypical ordinary Portland cement concrete cement + flyash composite binder concrete cement + slag compositebinder concrete and cement + silica fume composite binderconcrete

In Figure 12 the abscissa axis represents the frequencyand the ordinate axis on both sides represents the residuals

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

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2 Journal of Engineering

Discontinuous conduction path

Discontinuous point

ldquoInsulatingrdquo conduction path

Continuous conduction path

CDP RCP

Cmat

RCCP

Figure 1 Concrete mesostructure for AC conducting

C1 C2

R1 R2

Figure 2 Converted equivalent circuit

is formed In addition to continuous and discontinuousconduction paths isolated cementitious material particlesand their hydration products or even the entire solid concreteblock can also be conductive for alternating current Based onthe above considerations the concrete mesostructure for ACconducting can be described in Figure 1

The equivalent circuit model that corresponds to Figure 1can be expressed as

1119885 =11198851 +11198852 +11198853 (1)

where 1198851 is the impedance of the ldquoinsulatingrdquo conductionpath1198851 = 1(119895120596119862mat) and 119862mat is the capacitance of the testblock 1198852 is the impedance of the discontinuous conductionpath that is the sum of the capacitance of the discontinuouspoint and the resistance of the cut-off continuous conductionpath 1198852 = 119877CP + 1(119895120596119862DP) 119877CP is the resistance of the cut-off continuous conduction path and 119862DP is the capacitanceof discontinuous point and1198853 is the resistance of continuousconduction path 1198853 = 119877CCP

According to basic circuit theory the equivalent circuitdescribed in (1) can be converted to a circuit shown inFigure 2

The conversion relationship of the two equivalent circuitsis shown in

119877CP = (1198770 + 1198771) 11987701198771 119877CCP = 1198770 + 1198771119862DP = (1198620 + 1198621) ( 11987711198770 + 1198771)

2

119862mat = 119862011986211198620 + 1198621

(2)

600500400300200100 700 8000

Z998400 (ohm)

0

100

200

300

400

500

600

minusZ

998400998400(o

hm)

Figure 3 Nyquist plot of the equivalent circuit model shown inFigure 2

A parallel combination of a capacitor and a resistor pro-duces a semicircle in theNyquist plotTherefore two semicir-cles should appear on the plot of the equivalent circuit shownin Figure 2 Figure 3 shows the relationship between the resis-tance parameters and the location and size of the semicircles

Taking into account the second equation in (2) the resis-tance of the continuous conduction path is the intersectionpoint of the right semicircle with the real axis Howeverthe Nyquist plot of the measured impedance of cement-basedmaterials does not have two semicircles but often onlya semicircle appears Figure 4 is a typical Nyquist plot ofconcrete the concrete composition was 233 Kg silica fume4427 Kg normal Portland cement 750Kg sand 1125 Kggravel 1864 Kg water so 119908119887 = 04 the test age is 28 d

The left arc does not occur which indicates that 1198620 ismuch less than 1198621 Thus the diameter of the left arc is verysmall with respect to the right arc and therefore the left arcis not visible Cabeza et al [3 7] proved this point Thusthe equivalent circuit can be further simplified as shown inFigure 5 which also shows the corresponding Nyquist plot

The above discussion indicates that 119877CCP which is theparameter that characterizes the interconnecting porositythat is most relevant to permeability can be linked withmeasured impedance spectroscopy

Journal of Engineering 3

10MHz

1MHz

40Hz

0

100

200

300

400

500

600

minusZ

998400998400(o

hm)

100 200 300 400 500 600 700 8000

Z998400 (ohm)

Figure 4 High-frequency range Nyquist plot of typical concrete

C1

R1

R0

(a) Further simplified equivalent circuit

0

100

200

300

400

500

minusZ

998400998400(o

hm)

200 400 600100 500300 700

Z (ohm)

(b) Corresponding Nyquist plot of the simplified equivalent circuit

Figure 5 Further simplified equivalent circuit and its Nyquist plot

3 Relationship between AC ImpedanceParameters and Permeability

The relationship between AC impedance parameters andpermeability can be established in two ways An empir-ical relationship between the two can be mathematicallyregressed by conducting a large number of experimentsHowever the disadvantage of this approach is the lack ofreliable theoretical basis Another way to derive some kindof quantitative relationship between the two is through theo-retical derivation This paper adopted the latter approach

Einstein and Smoluchowski presented an equation onthe diffusion of charged particles in solution in 1905 and1906 respectively this equation is known as the EinsteinndashSmoluchowski equation [9] which is shown as follows

119863119902 = 120583119902119896119861119879119902 (3)

where 120583119902 is the ion mobility (m2(Vsdots)) 119896119861 is the Boltzmannconstant (138 sdot 10minus23 JK) q is the charge carried by ions(C) and 119879 is the absolute temperature (K) Through therelationship among the Boltzmann constant the Avogadroconstant (119873119860) the Faraday constant (119865) the elementaryelectric charge (119890) and the universal gas constant (119877) thatis 119896119861 = 119877119873119860 119865 = 119890119873119860 and 119902 = 119911119894119890 where 119911119894 is the absolutevalue of valence (4) was obtained

120583119902 = 119911119902119865119877119879 119863119902 (4)

As for the most significant chloride ion diffusion coef-ficient 119863Clminus which is directly relevant to the durability ofreinforced concrete structures (4) can be specifically writtenas [9]

119863Clminus = 119877119879119911Clminus119865120583Clminus (5)

To use (5) a certain concentration of chloride solutionmust be introduced and chloride ion mobility must be con-sidered InAC impedance spectroscopy testing themeasuredresistance (or resistivity conductivity) is a result of the jointaction of various ions in a pore solution To obtain thechloride ion diffusion coefficient the contribution of chlorideions to the conductance needs to be separated from the totalconductance To achieve this a 1molL NaCl solution wasused to saturate a concrete test block to weaken the influenceof other existing ions Thus the conductivity expression 120590 =119865sum119911119894120583119894119862119894 where119862119894 is the concentration and 119911119894 is the activitycoefficient (119911119894 = 1) can be written as

120590 = 119865 lowast (120583Clminus119862Clminus + 120583Na+119862Na+) (6)

To further differentiate the contribution of chlorideions and sodium ions to the conductance the contributionpercentage of chloride ions is 61 which is close to thatof an infinitely diluted sodium chloride solution (604)under the conditions of 25∘C and 1molL concentrationthis information was verified by consulting a chemistryhandbook Combining (5) and (6) obtains

119863Clminus = 1205901198771198791641198652119862Clminus (7)

Taking into account the relationship between resistance(120588) conductivity (120590) and cell constant (119886 = 119897119860 where 119897 isthe thickness of the test block and119860 is the contact area of theelectrode and the test block) (8) is obtained

120590 = 1120588 =119886119877CCP (8)

4 Journal of Engineering

Table 1 Chemical compositions of cement and mineral admixtures ( by weight)

Composition SiO2 Al2O3 Fe2O3 CaO MgO SO3 Na2O K2OCement 2109 434 281 625 181 287 015 062Slag 3455 1436 045 3394 1116 195 028 035Fly ash 5757 2191 772 387 168 041 154 251Silica fume 9263 105 117 034 073 030 022 093w mass fraction

Therefore the relationship between chloride ion diffusioncoefficient and the interconnecting pore resistivity can beexpressed as

119863Clminus = 1198861198771198791641198652119877CCP119862Clminus (9)

In (9) the influences of other ions on chloride ion dif-fusion coefficient determination have been largely removedTo further eliminate these effects some pastes (water-binderratio = 10) were prepared and the cementitious material thatwas used is as follows fly ash + Portland cement (cementreplacement level is 20 40 and 60 resp) slag +Portland cement (cement replacement level is 25 50 and75 resp) and silicon fume + Portland cement (cementreplacement level is 5 10 and 15 resp) The chemicalcompositions of cement and mineral admixtures are listed inTable 1

A conductivity cell with a length of 692 cm and anelectrode area of 962 cm2 was also made This experimentaims to investigate the influence of different pore solu-tions caused by different cementitious materials used onconductance Strictly speaking to carry out pore solutionconductivity tests the pore solution should be squeezed outof the concrete block However given the complexity of therequired equipment and the limited amount of the extractedpore solution this research adopted the simulation approachbymeasuring highwater-binder ratio paste that was preparedby using various cementitiousmaterials Before the age of 7 dthe paste will not solidify by shaking the container severaltimes every day The paste solution was shaken for 5 minutesthe day before the test and then left undisturbed for 24 hThen the upper solution was taken and injected into theconductivity testing cell The frequency of the alternatingcurrent is 2000Hz and the test ages are 28 and 90 d Figure 6shows the test results

Figure 6 shows that the addition of mineral admixturesreduces the concrete pore solution conductivity As gen-erally accepted the most important factor that influencespermeability is connected porosity rather than pore solutionconductivity To further eliminate the influence of other ionsonAC impedance testing for chloride iondiffusion coefficientdetermination a correction factor can be introduced Toperform this step the correction factor of ordinary Portlandcement concrete can be set as a benchmark For concrete thatuses other cementitious materials the correction factor maybe determined by interpolation in accordance with Table 2

000012

000010

000008

000006

000004

000002

000000

Con

duct

ivity

(Sm

minus1 )

28 90

Age (day)

100 cem25 sg50 sg75 sg20 fa

40 fa60 fa5 sf10 sf15 sf

Figure 6 Conductivity value of different paste solutions

Table 2 Diffusion coefficient correction factor

Types of mineraladmixtures

(Replacement ratio)diffusion coefficientcorrection factor

Fly ash (20) 12 (40) 13 (60) 17Slag (25) 11 (50) 13 (75) 18Silicon fume (5) 11 (10) 13 (15) 14

4 Experimental Studies

Table 3 shows the concrete mix that was used in the experi-ment

First Φ100mm times 300mm cylinder test blocks wereprepared for the experiment Steel mold was removed oneday after pouring and then concrete cylinders were curedfor 28 or 90 d before being cut into Φ100mm times 50mmblocks for vacuum saturation (using 1molL NaCl solutionthe saturating regime is the same as that of ASTM C1202)

Then a 100mm times 100mm stainless steel plate wasadopted as the electrode To ensure close contact betweenthe electrodes and the concrete surface soaked filter papers(using 1molL NaOH solution) were introduced Prepressurewas applied to the electrodes by using screw caps Agilent4294A precision impedance analyzer was employed (seeFigure 10) and the test frequency is 40Hz to 40MHz Five

Journal of Engineering 5

Table 3 Concrete mix

Specimen number Materials used (unit kgm3)Cement Fly ash Slag Silicon fume Water Fine aggr Coarse aggr

C0 4660 0 0 0 1860 7500 11250FA1 3728 923 0 0 1860 7357 11036FA2 2766 1864 0 0 1860 7205 10809FA3 1864 2766 0 0 1860 7053 10580GS1 3495 0 1165 0 1860 7476 11214GS2 2330 0 2330 0 1860 7442 11163GS3 1165 0 3495 0 1860 7408 11112SF1 4427 0 0 233 1860 7476 11214SF2 4194 0 0 466 1860 7442 11163SF3 3961 0 0 699 1860 7408 11112JH1 2660 1140 0 0 1440 7608 11412JH2 1900 950 950 0 1440 7612 11418JH3 1950 1300 650 0 1440 7528 11292

Figure 7 Concrete blocks for the impedance test

Figure 8 Stainless steel electrodes

test points were measured for each order of magnitude Thetest block electrode electrode installation and impedanceanalyzer are shown in Figures 7ndash9 respectively

Figure 11 shows the AC impedance spectroscopy testresult of the C0 test block (90 d)

To verify the validity of the measured impedance dataa validation check by using linear KramersndashKronig test [10]

Figure 9 Electrode mounting

Figure 10 Impedance tester

was conducted Figure 12 shows the validation results oftypical ordinary Portland cement concrete cement + flyash composite binder concrete cement + slag compositebinder concrete and cement + silica fume composite binderconcrete

In Figure 12 the abscissa axis represents the frequencyand the ordinate axis on both sides represents the residuals

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

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International Journal of

Journal of Engineering 3

10MHz

1MHz

40Hz

0

100

200

300

400

500

600

minusZ

998400998400(o

hm)

100 200 300 400 500 600 700 8000

Z998400 (ohm)

Figure 4 High-frequency range Nyquist plot of typical concrete

C1

R1

R0

(a) Further simplified equivalent circuit

0

100

200

300

400

500

minusZ

998400998400(o

hm)

200 400 600100 500300 700

Z (ohm)

(b) Corresponding Nyquist plot of the simplified equivalent circuit

Figure 5 Further simplified equivalent circuit and its Nyquist plot

3 Relationship between AC ImpedanceParameters and Permeability

The relationship between AC impedance parameters andpermeability can be established in two ways An empir-ical relationship between the two can be mathematicallyregressed by conducting a large number of experimentsHowever the disadvantage of this approach is the lack ofreliable theoretical basis Another way to derive some kindof quantitative relationship between the two is through theo-retical derivation This paper adopted the latter approach

Einstein and Smoluchowski presented an equation onthe diffusion of charged particles in solution in 1905 and1906 respectively this equation is known as the EinsteinndashSmoluchowski equation [9] which is shown as follows

119863119902 = 120583119902119896119861119879119902 (3)

where 120583119902 is the ion mobility (m2(Vsdots)) 119896119861 is the Boltzmannconstant (138 sdot 10minus23 JK) q is the charge carried by ions(C) and 119879 is the absolute temperature (K) Through therelationship among the Boltzmann constant the Avogadroconstant (119873119860) the Faraday constant (119865) the elementaryelectric charge (119890) and the universal gas constant (119877) thatis 119896119861 = 119877119873119860 119865 = 119890119873119860 and 119902 = 119911119894119890 where 119911119894 is the absolutevalue of valence (4) was obtained

120583119902 = 119911119902119865119877119879 119863119902 (4)

As for the most significant chloride ion diffusion coef-ficient 119863Clminus which is directly relevant to the durability ofreinforced concrete structures (4) can be specifically writtenas [9]

119863Clminus = 119877119879119911Clminus119865120583Clminus (5)

To use (5) a certain concentration of chloride solutionmust be introduced and chloride ion mobility must be con-sidered InAC impedance spectroscopy testing themeasuredresistance (or resistivity conductivity) is a result of the jointaction of various ions in a pore solution To obtain thechloride ion diffusion coefficient the contribution of chlorideions to the conductance needs to be separated from the totalconductance To achieve this a 1molL NaCl solution wasused to saturate a concrete test block to weaken the influenceof other existing ions Thus the conductivity expression 120590 =119865sum119911119894120583119894119862119894 where119862119894 is the concentration and 119911119894 is the activitycoefficient (119911119894 = 1) can be written as

120590 = 119865 lowast (120583Clminus119862Clminus + 120583Na+119862Na+) (6)

To further differentiate the contribution of chlorideions and sodium ions to the conductance the contributionpercentage of chloride ions is 61 which is close to thatof an infinitely diluted sodium chloride solution (604)under the conditions of 25∘C and 1molL concentrationthis information was verified by consulting a chemistryhandbook Combining (5) and (6) obtains

119863Clminus = 1205901198771198791641198652119862Clminus (7)

Taking into account the relationship between resistance(120588) conductivity (120590) and cell constant (119886 = 119897119860 where 119897 isthe thickness of the test block and119860 is the contact area of theelectrode and the test block) (8) is obtained

120590 = 1120588 =119886119877CCP (8)

4 Journal of Engineering

Table 1 Chemical compositions of cement and mineral admixtures ( by weight)

Composition SiO2 Al2O3 Fe2O3 CaO MgO SO3 Na2O K2OCement 2109 434 281 625 181 287 015 062Slag 3455 1436 045 3394 1116 195 028 035Fly ash 5757 2191 772 387 168 041 154 251Silica fume 9263 105 117 034 073 030 022 093w mass fraction

Therefore the relationship between chloride ion diffusioncoefficient and the interconnecting pore resistivity can beexpressed as

119863Clminus = 1198861198771198791641198652119877CCP119862Clminus (9)

In (9) the influences of other ions on chloride ion dif-fusion coefficient determination have been largely removedTo further eliminate these effects some pastes (water-binderratio = 10) were prepared and the cementitious material thatwas used is as follows fly ash + Portland cement (cementreplacement level is 20 40 and 60 resp) slag +Portland cement (cement replacement level is 25 50 and75 resp) and silicon fume + Portland cement (cementreplacement level is 5 10 and 15 resp) The chemicalcompositions of cement and mineral admixtures are listed inTable 1

A conductivity cell with a length of 692 cm and anelectrode area of 962 cm2 was also made This experimentaims to investigate the influence of different pore solu-tions caused by different cementitious materials used onconductance Strictly speaking to carry out pore solutionconductivity tests the pore solution should be squeezed outof the concrete block However given the complexity of therequired equipment and the limited amount of the extractedpore solution this research adopted the simulation approachbymeasuring highwater-binder ratio paste that was preparedby using various cementitiousmaterials Before the age of 7 dthe paste will not solidify by shaking the container severaltimes every day The paste solution was shaken for 5 minutesthe day before the test and then left undisturbed for 24 hThen the upper solution was taken and injected into theconductivity testing cell The frequency of the alternatingcurrent is 2000Hz and the test ages are 28 and 90 d Figure 6shows the test results

Figure 6 shows that the addition of mineral admixturesreduces the concrete pore solution conductivity As gen-erally accepted the most important factor that influencespermeability is connected porosity rather than pore solutionconductivity To further eliminate the influence of other ionsonAC impedance testing for chloride iondiffusion coefficientdetermination a correction factor can be introduced Toperform this step the correction factor of ordinary Portlandcement concrete can be set as a benchmark For concrete thatuses other cementitious materials the correction factor maybe determined by interpolation in accordance with Table 2

000012

000010

000008

000006

000004

000002

000000

Con

duct

ivity

(Sm

minus1 )

28 90

Age (day)

100 cem25 sg50 sg75 sg20 fa

40 fa60 fa5 sf10 sf15 sf

Figure 6 Conductivity value of different paste solutions

Table 2 Diffusion coefficient correction factor

Types of mineraladmixtures

(Replacement ratio)diffusion coefficientcorrection factor

Fly ash (20) 12 (40) 13 (60) 17Slag (25) 11 (50) 13 (75) 18Silicon fume (5) 11 (10) 13 (15) 14

4 Experimental Studies

Table 3 shows the concrete mix that was used in the experi-ment

First Φ100mm times 300mm cylinder test blocks wereprepared for the experiment Steel mold was removed oneday after pouring and then concrete cylinders were curedfor 28 or 90 d before being cut into Φ100mm times 50mmblocks for vacuum saturation (using 1molL NaCl solutionthe saturating regime is the same as that of ASTM C1202)

Then a 100mm times 100mm stainless steel plate wasadopted as the electrode To ensure close contact betweenthe electrodes and the concrete surface soaked filter papers(using 1molL NaOH solution) were introduced Prepressurewas applied to the electrodes by using screw caps Agilent4294A precision impedance analyzer was employed (seeFigure 10) and the test frequency is 40Hz to 40MHz Five

Journal of Engineering 5

Table 3 Concrete mix

Specimen number Materials used (unit kgm3)Cement Fly ash Slag Silicon fume Water Fine aggr Coarse aggr

C0 4660 0 0 0 1860 7500 11250FA1 3728 923 0 0 1860 7357 11036FA2 2766 1864 0 0 1860 7205 10809FA3 1864 2766 0 0 1860 7053 10580GS1 3495 0 1165 0 1860 7476 11214GS2 2330 0 2330 0 1860 7442 11163GS3 1165 0 3495 0 1860 7408 11112SF1 4427 0 0 233 1860 7476 11214SF2 4194 0 0 466 1860 7442 11163SF3 3961 0 0 699 1860 7408 11112JH1 2660 1140 0 0 1440 7608 11412JH2 1900 950 950 0 1440 7612 11418JH3 1950 1300 650 0 1440 7528 11292

Figure 7 Concrete blocks for the impedance test

Figure 8 Stainless steel electrodes

test points were measured for each order of magnitude Thetest block electrode electrode installation and impedanceanalyzer are shown in Figures 7ndash9 respectively

Figure 11 shows the AC impedance spectroscopy testresult of the C0 test block (90 d)

To verify the validity of the measured impedance dataa validation check by using linear KramersndashKronig test [10]

Figure 9 Electrode mounting

Figure 10 Impedance tester

was conducted Figure 12 shows the validation results oftypical ordinary Portland cement concrete cement + flyash composite binder concrete cement + slag compositebinder concrete and cement + silica fume composite binderconcrete

In Figure 12 the abscissa axis represents the frequencyand the ordinate axis on both sides represents the residuals

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

4 Journal of Engineering

Table 1 Chemical compositions of cement and mineral admixtures ( by weight)

Composition SiO2 Al2O3 Fe2O3 CaO MgO SO3 Na2O K2OCement 2109 434 281 625 181 287 015 062Slag 3455 1436 045 3394 1116 195 028 035Fly ash 5757 2191 772 387 168 041 154 251Silica fume 9263 105 117 034 073 030 022 093w mass fraction

Therefore the relationship between chloride ion diffusioncoefficient and the interconnecting pore resistivity can beexpressed as

119863Clminus = 1198861198771198791641198652119877CCP119862Clminus (9)

In (9) the influences of other ions on chloride ion dif-fusion coefficient determination have been largely removedTo further eliminate these effects some pastes (water-binderratio = 10) were prepared and the cementitious material thatwas used is as follows fly ash + Portland cement (cementreplacement level is 20 40 and 60 resp) slag +Portland cement (cement replacement level is 25 50 and75 resp) and silicon fume + Portland cement (cementreplacement level is 5 10 and 15 resp) The chemicalcompositions of cement and mineral admixtures are listed inTable 1

A conductivity cell with a length of 692 cm and anelectrode area of 962 cm2 was also made This experimentaims to investigate the influence of different pore solu-tions caused by different cementitious materials used onconductance Strictly speaking to carry out pore solutionconductivity tests the pore solution should be squeezed outof the concrete block However given the complexity of therequired equipment and the limited amount of the extractedpore solution this research adopted the simulation approachbymeasuring highwater-binder ratio paste that was preparedby using various cementitiousmaterials Before the age of 7 dthe paste will not solidify by shaking the container severaltimes every day The paste solution was shaken for 5 minutesthe day before the test and then left undisturbed for 24 hThen the upper solution was taken and injected into theconductivity testing cell The frequency of the alternatingcurrent is 2000Hz and the test ages are 28 and 90 d Figure 6shows the test results

Figure 6 shows that the addition of mineral admixturesreduces the concrete pore solution conductivity As gen-erally accepted the most important factor that influencespermeability is connected porosity rather than pore solutionconductivity To further eliminate the influence of other ionsonAC impedance testing for chloride iondiffusion coefficientdetermination a correction factor can be introduced Toperform this step the correction factor of ordinary Portlandcement concrete can be set as a benchmark For concrete thatuses other cementitious materials the correction factor maybe determined by interpolation in accordance with Table 2

000012

000010

000008

000006

000004

000002

000000

Con

duct

ivity

(Sm

minus1 )

28 90

Age (day)

100 cem25 sg50 sg75 sg20 fa

40 fa60 fa5 sf10 sf15 sf

Figure 6 Conductivity value of different paste solutions

Table 2 Diffusion coefficient correction factor

Types of mineraladmixtures

(Replacement ratio)diffusion coefficientcorrection factor

Fly ash (20) 12 (40) 13 (60) 17Slag (25) 11 (50) 13 (75) 18Silicon fume (5) 11 (10) 13 (15) 14

4 Experimental Studies

Table 3 shows the concrete mix that was used in the experi-ment

First Φ100mm times 300mm cylinder test blocks wereprepared for the experiment Steel mold was removed oneday after pouring and then concrete cylinders were curedfor 28 or 90 d before being cut into Φ100mm times 50mmblocks for vacuum saturation (using 1molL NaCl solutionthe saturating regime is the same as that of ASTM C1202)

Then a 100mm times 100mm stainless steel plate wasadopted as the electrode To ensure close contact betweenthe electrodes and the concrete surface soaked filter papers(using 1molL NaOH solution) were introduced Prepressurewas applied to the electrodes by using screw caps Agilent4294A precision impedance analyzer was employed (seeFigure 10) and the test frequency is 40Hz to 40MHz Five

Journal of Engineering 5

Table 3 Concrete mix

Specimen number Materials used (unit kgm3)Cement Fly ash Slag Silicon fume Water Fine aggr Coarse aggr

C0 4660 0 0 0 1860 7500 11250FA1 3728 923 0 0 1860 7357 11036FA2 2766 1864 0 0 1860 7205 10809FA3 1864 2766 0 0 1860 7053 10580GS1 3495 0 1165 0 1860 7476 11214GS2 2330 0 2330 0 1860 7442 11163GS3 1165 0 3495 0 1860 7408 11112SF1 4427 0 0 233 1860 7476 11214SF2 4194 0 0 466 1860 7442 11163SF3 3961 0 0 699 1860 7408 11112JH1 2660 1140 0 0 1440 7608 11412JH2 1900 950 950 0 1440 7612 11418JH3 1950 1300 650 0 1440 7528 11292

Figure 7 Concrete blocks for the impedance test

Figure 8 Stainless steel electrodes

test points were measured for each order of magnitude Thetest block electrode electrode installation and impedanceanalyzer are shown in Figures 7ndash9 respectively

Figure 11 shows the AC impedance spectroscopy testresult of the C0 test block (90 d)

To verify the validity of the measured impedance dataa validation check by using linear KramersndashKronig test [10]

Figure 9 Electrode mounting

Figure 10 Impedance tester

was conducted Figure 12 shows the validation results oftypical ordinary Portland cement concrete cement + flyash composite binder concrete cement + slag compositebinder concrete and cement + silica fume composite binderconcrete

In Figure 12 the abscissa axis represents the frequencyand the ordinate axis on both sides represents the residuals

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

Journal of Engineering 5

Table 3 Concrete mix

Specimen number Materials used (unit kgm3)Cement Fly ash Slag Silicon fume Water Fine aggr Coarse aggr

C0 4660 0 0 0 1860 7500 11250FA1 3728 923 0 0 1860 7357 11036FA2 2766 1864 0 0 1860 7205 10809FA3 1864 2766 0 0 1860 7053 10580GS1 3495 0 1165 0 1860 7476 11214GS2 2330 0 2330 0 1860 7442 11163GS3 1165 0 3495 0 1860 7408 11112SF1 4427 0 0 233 1860 7476 11214SF2 4194 0 0 466 1860 7442 11163SF3 3961 0 0 699 1860 7408 11112JH1 2660 1140 0 0 1440 7608 11412JH2 1900 950 950 0 1440 7612 11418JH3 1950 1300 650 0 1440 7528 11292

Figure 7 Concrete blocks for the impedance test

Figure 8 Stainless steel electrodes

test points were measured for each order of magnitude Thetest block electrode electrode installation and impedanceanalyzer are shown in Figures 7ndash9 respectively

Figure 11 shows the AC impedance spectroscopy testresult of the C0 test block (90 d)

To verify the validity of the measured impedance dataa validation check by using linear KramersndashKronig test [10]

Figure 9 Electrode mounting

Figure 10 Impedance tester

was conducted Figure 12 shows the validation results oftypical ordinary Portland cement concrete cement + flyash composite binder concrete cement + slag compositebinder concrete and cement + silica fume composite binderconcrete

In Figure 12 the abscissa axis represents the frequencyand the ordinate axis on both sides represents the residuals

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

6 Journal of Engineering

10MHz

1MHz

40Hz

200 400 600 800 1000 1200 14000

Z998400 (ohm)

0

200

400

600

800

1000

minusZ

998400998400(o

hm)

Figure 11 Nyquist plot of spectroscopy test results of specimen number C0

Z998400

Z998400998400

minus2

minus1

0

1

2

3

Resid

uals

()

10 20 30 405 15 25 35Data point

(a) Specimen number C0 90 dZ

998400Z

998400998400

minus2

minus1

0

1

2

Resid

uals

()

10 20 30 40Data point

(b) Specimen number FA2 90 d

Z998400

Z998400998400

10 20 30 40 50Data point

minus08

minus06

minus04

minus02

00

02

04

06

08

Resid

uals

()

(c) Specimen number GS2 90 dZ

998400Z

998400998400

10 20 30 40 50Data point

minus15

minus10

minus05

00

05

10

Resid

uals

()

(d) Specimen number SF2 90 d

Figure 12 Validation results

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

Journal of Engineering 7

of Voigt model fitting Equation (10) is used to calculate theresiduals

Residuals (Re119885) = (119885Re minus 119885Re-cal)2

1198852Re

Residuals (Im119885) = (119885Im minus 119885Im-cal)21198852Im

(10)

where 119885Re and 119885Im are real part and the imaginary part ofthe measured impedance respectively and119885Re-cal and119885Im-calare the fitted values obtained by using the Voigt model Smallresiduals correspond to better validity

Only measured data that passed the KramersndashKronig testcan be used for further numerical fitting Figure 12 showsthat the obtained impedance data shows good validity whichcan be attributed to the measures employed in this sectionMoreover the repeatability of the test data is good becauseof reliable close contact between the test block and theelectrodes

Parameters 1198770 1198771 and 1198621 can be obtained throughnumerical fitting of the measured impedance data and thepreset equivalent circuit shown in Figure 5 The chloride iondiffusion coefficient can be calculated by using119877CCP = 1198770+1198771and (9)

The method of determining chloride ion diffusion coeffi-cient based on the AC impedance technique is performed asfollows

(1) Prepare Φ100mm times 50mm specimens and conductvacuum Clminus saturating using 1molL NaCl solution(the saturating regime is the same as that of ASTMC1202)

(2) Carry out AC impedance testing to obtain impedancespectroscopy data

(3) Perform data validation(4) Obtain 119877CCP from equivalent circuit fitting(5) Calculate chloride ion diffusion coefficient using (9)(6) Modify the diffusion coefficient according to the

cementitious material that was used

The rapid chloride permeability test ASTM C1202 hasbeen adopted as national standard by many countriesincluding China the United States and Canada The ASTMC1202 method specifies the rating of chloride permeability ofconcrete based on the charge passed through the specimenduring 6 h of testing period ASTM C1202 tests that use thesame concrete blocks were conducted to perform a compar-ison Figure 13 shows the relationship between chloride iondiffusion coefficients obtained from impedance-based tech-nology and 6 h electric flux A linear correlation (119876C1202 =930 times 119863Clminus ) between the rapid chloride permeability testand the proposed method was obtained with a correlationcoefficient of 09 see Figure 13 for details

As can be seen from Figure 13 some data points devi-ate from the straight line As reported by Shi [11] theASTMC1202 method is virtually a measurement of electricalconductivity of concrete which depends on both the pore

Testing resultLinear fit

0

1000

2000

3000

4000

Char

ge p

asse

d (C

oulo

mb)

1 2 3 4 50

DClminus (10minus12 m2sminus1)

Figure 13 Relationship between chloride ion diffusion coefficientusing ACIS and 6 h electric flux from ASTM C1202 tests

structure characteristics and pore solution chemistry ofconcrete Supplementary cementing materials such as silicafume fly ash and ground blast furnace slag may have asignificant effect on the chemistry or electrical conductivityof pore solution depending on the alkali content of the sup-plementary cementing material replacement level and agewhich has little to do with the chloride permeability ASTMC1202 method is susceptible to pore solution conductanceHowever the proposed method eliminates the effect of poresolution conductivity on permeability by using a carefullydesigned technique This effect may be an important reasonfor the moderate correlation between the two methods

5 Conclusions

(1) High-frequency AC impedance spectroscopy can reflectthe mesostructural properties of materials which enables usto indirectly study the permeability of concrete An equiva-lent circuit model with a clear physical meaning was adoptedthrough an investigation of AC conduction paths in concreteThrough numerical fitting of theNyquist plot of themeasuredimpedance spectroscopy and a preset model a parameterthat characterizes diffusion resistance that depends on theinterconnected porosity and pore solution conductivity wasobtained Based on the EinsteinndashSmoluchowski equationthe chloride ion diffusion coefficient was derived and theproposed formula was modified to eliminate the influenceof pore solution conductivity on diffusion coefficient mea-surementThen an accurate formula that reflects chloride iondiffusion resistance was obtained(2) With test block size specimen pretreatment im-

pedance test parameters equivalent circuit selection anddiffusion coefficient formula modification taken into consid-eration a method of determining the chloride ion diffusioncoefficient based on AC impedance spectroscopy was estab-lished In addition the test procedure was summarized forpractical purposes

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

8 Journal of Engineering

(3)The relationship between the proposed method andthe traditional ASTMC1202 method was established Resultsshowed that a certain but not very high degree of linear cor-relation exists which can be attributed to the fact that ASTMC1202 method is essentially a conductance method influ-enced by pore solution conductivity whereas pore solutionconductivity has little effect compared with interconnectedporosity on chloride ion diffusion behavior in concrete

Competing Interests

The authors declare that there is no conflict of interestsregarding the publication of this paper

Acknowledgments

The authors acknowledge the support from National NaturalScience Foundation of China (Grant nos 51408379 and51508350) and Natural Science Foundation of Hebei China(Grant no E2013210125)

References

[1] L Kong and Y Du ldquoEffect of lightweight aggregate and theinterfacial transition zone on the durability of concrete basedon grey correlationrdquo Indian Journal of Engineering andMaterialsSciences vol 22 no 1 pp 111ndash119 2015

[2] A E Long G D Henderson and F R Montgomery ldquoWhyassess the properties of near-surface concreterdquo Constructionand Building Materials vol 15 no 2-3 pp 65ndash79 2001

[3] M Cabeza M Keddam X R Novoa I Sanchez and HTakenouti ldquoImpedance spectroscopy to characterize the porestructure during the hardening process of Portland cementpasterdquo Electrochimica Acta vol 51 no 8-9 pp 1831ndash1841 2006

[4] G Dotelli and C M Mari ldquoThe evolution of cement pastehydration process by impedance spectroscopyrdquo Materials Sci-ence and Engineering A vol 303 no 1-2 pp 54ndash59 2001

[5] M Cabeza P Merino X R Novoa and I Sanchez ldquoElectricaleffects generated by mechanical loading of hardened Portlandcement pasterdquo Cement and Concrete Composites vol 25 no 3pp 351ndash356 2003

[6] P Gu P Xie J J Beaudoin and R Brousseau ldquoAC impedancespectroscopy (I) a new equivalent circuit model for hydratedportland cement pasterdquo Cement and Concrete Research vol 22no 5 pp 833ndash840 1992

[7] G Song ldquoEquivalent circuit model for AC electrochemicalimpedance spectroscopy of concreterdquo Cement and ConcreteResearch vol 30 no 11 pp 1723ndash1730 2000

[8] M Shi Z Chen and J Sun ldquoDetermination of chloridediffusivity in concrete by AC impedance spectroscopyrdquo Cementand Concrete Research vol 29 no 7 pp 1111ndash1115 1999

[9] C Andrade ldquoCalculation of chloride diffusion coefficients inconcrete from ionic migration measurementsrdquo Cement andConcrete Research vol 23 no 3 pp 724ndash742 1993

[10] J M Esteban and M E Orazem ldquoOn the application ofthe Kramers-Kronig relations to evaluate the consistency ofelectrochemical impedance datardquo Journal of the ElectrochemicalSociety vol 138 no 1 pp 67ndash76 1991

[11] C Shi ldquoEffect of mixing proportions of concrete on its elec-trical conductivity and the rapid chloride permeability test

(ASTMC1202 or ASSHTOT277) resultsrdquoCement and ConcreteResearch vol 34 no 3 pp 537ndash545 2004

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of

International Journal of

AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014

RoboticsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Active and Passive Electronic Components

Control Scienceand Engineering

Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

International Journal of

RotatingMachinery

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporation httpwwwhindawicom

Journal ofEngineeringVolume 2014

Submit your manuscripts athttpwwwhindawicom

VLSI Design

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Shock and Vibration

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Civil EngineeringAdvances in

Acoustics and VibrationAdvances in

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Electrical and Computer Engineering

Journal of

Advances inOptoElectronics

Hindawi Publishing Corporation httpwwwhindawicom

Volume 2014

The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014

SensorsJournal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Chemical EngineeringInternational Journal of Antennas and

Propagation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

Navigation and Observation

International Journal of

Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014

DistributedSensor Networks

International Journal of


Recommended