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Practical aspects of correlation analysis of compressive strength from destructive and non-destructive methods in different directions

Abstract

The research presented here demonstrates the practical aspects of the numerical correlation of the results of the compressive strength test. The destructive test (DT) in a hydraulic press and the non-destructive test (NDT) using a Schmidt hammer in several process variations were evaluated. The aim was to evaluate the real differences between the tool supplier’s curve and testing. Therefore, 150 concrete cube specimens with an edge length of 150 mm were produced using a mixture of three types of concrete classes: C30, C35, and C40. The test was carried out 7 and 28 days of age of the concrete. The Schmidt hammer test was carried out in horizontal (θ = 0) and vertical (θ = 90) directions and using a series of 10 measurements. Furthermore, the tests were performed in two sets: first, the sample was placed on the ground, and second, under a hydraulic jack with a load of 50% of the maximum bearing capacity of specific concrete. Then, regression analysis was performed on the data sets to establish linear mathematical relationships between compressive strength and number of bounces. The results showed that the correlation between the DT and NDT tests has a high value for each group, but the correlation equations are different and must be taken into account.

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Practical aspects of correlation analysis of compressive strength from destructive and non-destructive methods in different directions

Author: Badarloo, Baitollah
Publisher: MDPI
Year: 2023
DOI: 10.3390/infrastructures8110155
Source: https://dspace.vsb.cz/bitstreams/024347e8-7931-41d0-aa04-2d5e85980147/download
Ci a ion: Bada loo, B.; Lehne , P.
P ac ical Aspec s o Co ela ion
Analysis o Comp essi e S eng h
om Des uc i e and
Non-Des uc i e Me hods in
Di e en Di ec ions. In as uc u es
2023,8, 155. h ps://doi.o g/10.3390/
in as uc u es8110155
Academic Edi o : Ma co Bonope a
Recei ed: 28 Augus 2023
Re ised: 11 Oc obe 2023
Accep ed: 20 Oc obe 2023
Published: 24 Oc obe 2023
Copy igh : © 2023 by he au ho s.
Licensee MDPI, Basel, Swi ze land.
This a icle is an open access a icle
dis ibu ed unde he e ms and
condi ions o he C ea i e Commons
A ibu ion (CC BY) license (h ps://
c ea i ecommons.o g/licenses/by/
4.0/).
in as uc u es
Technical No e
P ac ical Aspec s o Co ela ion Analysis o Comp essi e
S eng h om Des uc i e and Non-Des uc i e Me hods in
Di e en Di ec ions
Bai ollah Bada loo 1and Pe Lehne 2,*
1Depa men o Ci il Enginee ing, Qom Uni e si y o Technology (QUT), Qom 37181-46645, I an
2Depa men o S uc u al Mechanics, Facul y o Ci il Enginee ing, VSB-Technical Uni e si y o Os a a,
Lud íka Podéš ˇe 1875/17, 708 33 Os a a-Po uba, Czech Republic
*Co espondence: pe [email p o ec ed]
Abs ac :
The esea ch p esen ed he e demons a es he p ac ical aspec s o he nume ical co ela ion
o he esul s o he comp essi e s eng h es . The des uc i e es (DT) in a hyd aulic p ess and he
non-des uc i e es (NDT) using a Schmid hamme in se e al p ocess a ia ions we e e alua ed.
The aim was o e alua e he eal di e ences be ween he ool supplie ’s cu e and es ing. The e o e,
150 conc e e cube specimens wi h an edge leng h o 150 mm we e p oduced using a mix u e o
h ee ypes o conc e e classes: C30, C35, and C40. The es was ca ied ou 7 and 28 days o age o
he conc e e. The Schmid hamme es was ca ied ou in ho izon al (
θ
= 0) and e ical (
θ
= 90)
di ec ions and using a se ies o 10 measu emen s. Fu he mo e, he es s we e pe o med in wo se s:
i s , he sample was placed on he g ound, and second, unde a hyd aulic jack wi h a load o 50% o
he maximum bea ing capaci y o speci ic conc e e. Then, eg ession analysis was pe o med on he
da a se s o es ablish linea ma hema ical ela ionships be ween comp essi e s eng h and numbe o
bounces. The esul s showed ha he co ela ion be ween he DT and NDT es s has a high alue o
each g oup, bu he co ela ion equa ions a e di e en and mus be aken in o accoun .
Keywo ds:
comp essi e s eng h; conc e e; des uc i e es ing; non-des uc i e es ing; eg ession;
Schmid hamme
1. In oduc ion
Conc e e is one o he impo an cons uc ion ma e ials ha is widely used in building
s uc u es due o i s a ailabili y, low cos , and wo kabili y [
1
,
2
]. Because conc e e unde
load p essu e can ail, de e mining i s comp essi e s eng h plays a i al ole in judging i s
quali y. Bo h des uc i e and non-des uc i e es ing me hods ha e been applied o es ima e
comp ession s eng h. A conside able amoun o wo k has ocused on he comp essi e
s eng h o conc e e. Rega ding des uc i e es ing (DT) me hods, such as he use o a
hyd aulic jack, i should be men ioned ha he esul s ob ained om his me hod a e
accu a e [
3
–
7
]. Howe e , his me hod su e s om d awbacks such as high cos , ene gy
consump ion, labo , ime, and lack o abili y o measu e in si u conc e e. The e o e, non-
des uc i e es ing (NDT) me hods a e now popula in ha hey a e ca ied ou wi hou
des oying he conc e e specimen, while in DT me hods he specimen should be c ushed o
ail [
8
–
10
]. These NDT me hods a e sui able o in si u measu emen s on exis ing s uc u es
o o long- e m measu emen s, whe e i is necessa y o de e mine he changes in conc e e
s eng h o e ime.
NDT me hods can di ec ly e alua e he quali y o a building e en on-si e by es ima ing
he comp essi e s eng h o he conc e e s uc u e, and he mos commonly used NDT
me hod is he Schmid hamme [
8
,
11
,
12
]. Se e al au ho s ha e used he Schmid hamme
o measu e conc e e s eng h [
8
,
13
–
16
]. A Schmid hamme , also known as a Swiss hamme
o a ebound hamme , is a po able de ice ha measu es he elas ic p ope ies o he
In as uc u es 2023,8, 155. h ps://doi.o g/10.3390/in as uc u es8110155 h ps://www.mdpi.com/jou nal/in as uc u es
In as uc u es 2023,8, 155 2 o 14
s eng h o conc e e. Mo eo e , NDT me hods a e highly bene icial o measu ing di e en
pa ame e s o conc e e, i.e., s eng h, du abili y, and homogenei y [
9
]. P e iously, some
s udies ha e compa ed a des uc i e es ing me hod (co e es ing) wi h an NDT me hod.
NDT me hods a e used o he analysis o conc e es o di e en basic ma e ials and di e en
applica ions [10,17].
Acco ding o hei esea ch, he NDT me hod has he ollowing ad an ages in com-
pa ison o DT me hods: (1) lowe cos , (2) simplici y, (3) educ ion in labo consump ion,
(4) g ea e speed, and (5) e alua ion o conc e e p ope y wi hou damaging i [
18
]. The
amoun o ebound depends on se e al conc e e pa ame e s, i.e., ha dness, coe icien
o elas ici y, o e, wa e con en mo phology o he sample, su ace oughness, ype o
agg ega ion, and conc e e ing edien [
19
,
20
]. Mo eo e , small es a eas, lack o equipmen ,
and es di ec ion should be conside ed as de e mining pa ame e s in NDT me hods [
21
].
Rega dless o he ad an ages associa ed wi h NDT me hods, his me hod is aniso opy
in which di e en di ec ions o measu ing can a ec hei alue. Mo eo e , because he
esul s ob ained om using a Schmid hamme can be a ec ed by se e al pa ame e s such
as he amoun o po osi y, mois u e, ha dness, oughness, e c., he esul s a e mo e o an
app oxima ion han a p ecise alue. Consequen ly, esea che s ha e ied o o e come his
limi a ion by inding a co ela ion be ween DT and NDT alues o inc ease he accu acy o
measu ing comp essi e s eng h.
In ecen yea s, o he au ho s ha e also sea ched o he co ec co ela ion ela ions
be ween NDT me hods and DT me hods, because hese co ela ions we e no de e mined
on non-s anda d conc e es [
22
,
23
]. The e a e also s udies using machine lea ning me hods
o p edic he dynamic comp essi e esponse o composi e ma e ials [24].
In he p esen ed esea ch, bo h DT (hyd aulic p ess machine) and NDT ( ebound
hamme ) me hods we e p oposed o e alua e he comp essi e s eng h o C30, C35, and
C40 o de ine a me hod mo e eliable and p ac ical. I should be no ed ha in o de o
minimize e o s in in es iga ions, wa e con en , p ocessing, and a mosphe e empe a u e
we e kep cons an . Then, a emp s we e made o compa e he esul s ob ained om he
cube samples by eg ession o ind an accu a e ela ionship be ween he DT and he NDT
da a in which he co ela ion coe icien is g ea e han 0.85. The esul s o a la ge numbe
o es s we e used o e alua e he p ac ical use o he Schmid hamme in many aspec s.
The s a is ical and nume ical e alua ion o accu a e measu ed da a in la ge quan i ies is o
g ea impo ance o bo h academia and p ac ice, whe e he Schmid hamme is used and
has signi ican alue. This is no he only eason why he esul s p esen ed and e alua ed
a e placed in he con ex o cu en ends and habi s.
2. Ma e ials and Me hods
2.1. Mix u es and Samples
Th ee ypes o conc e e wi h di e en equi ed s eng hs had o be p epa ed o he
expe imen s. The conc e e composi ion is based on o dina y Po land cemen o he Teh an
b and (OPC), po able wa e (as pe ASTM D1067 [
25
]), ine agg ega e (sand), and coa se
agg ega e (g a el) om a local sou ce (Qom, I an). The design o he mix u es was ca ied
ou in acco dance wi h ACI-211 [26], and he composi ion is shown in Table 1.
Table 1. Mix u e design.
Conc e e Sand
(kg)
G a el
(kg)
Cemen
(kg)
Wa e
(li ) Slump Wa e /Cemen
C30 950 852 400 228 7.5–10 0.57
C35 950 852 450 234 7.5–10 0.52
C40 950 852 500 240 7.5–10 0.48
These h ee ypes o conc e e we e selec ed because hey a e he mos commonly used
in he cons uc ion indus y. The eason o he h ee ypes was o accoun o di e ences
In as uc u es 2023,8, 155 3 o 14
in he case o s eng h. All conc e es had he same ine agg ega e and coa se agg ega e,
bu di e en cemen and wa e con en s. This esul ed in di e en w/c a ios and hus
di e en esul ing s eng hs.
The manu ac u e o he conc e e was ca ied ou in acco dance wi h BS 1881: Pa
108:1983 [
27
]. In he p oduc ion o conc e e, he d y ing edien s we e mixed wi h each
o he a ambien empe a u e, hen hal o he wa e was added, and all he ing edien s
we e mixed o 2 min o o m a homogeneous mix u e. The es o he wa e was hen
added and he ma e ials we e mixed o 2 min. The samples we e hen cas in o cube
molds, compac ed, and le a oom empe a u e o 24 h; hey we e ans e ed o a ank
o wa e and cu ed o 7 and 28 days. A o al o 150 cubic specimens (50 samples o each
class) cubic specimens (150 mm
×
150 mm
×
150 mm) we e p oduced in 3 di e en classes.
The e o e, each es se is based on 25 iden ical es samples. Thus, as shown below, i was
es ed in wo di e en di ec ions, and a la ge s a is ical e alua ion was ob ained due o he
numbe o 25 samples pe condi ion.
2.2. Expe imen al P og am
Th ee es s we e p epa ed in he expe imen al p og am—non-des uc i e e ical
hamme es , non-des uc i e ho izon al hamme es on a loaded specimen, and des uc i e
p essu e es in a hyd aulic p ess machine. A 50% alue o he maximum p edic ed o ce
was used o each ype o conc e e— o conc e e C30, i was 15 MPa, o conc e e C35 i was
17.5 MPa, and o conc e e C40 i was 20 MPa. All es s we e pe o med sequen ially on
he same specimens o main ain a comple e co ela ion o esul s. Figu e 1shows he s eps
o use a Schmid hamme . The i s pic u e is he calib a ion sample, he second pic u e is
he es measu emen in a e ical way, and he hi d pic u e is he es measu emen in a
ho izon al way.
In as uc u es 2023, 8, x FOR PEER REVIEW 3 o 14
These h ee ypes o conc e e we e selec ed because hey a e he mos commonly used
in he cons uc ion indus y. The eason o he h ee ypes was o accoun o diffe ences
in he case o s eng h. All conc e es had he same ine agg ega e and coa se agg ega e,
bu diffe en cemen and wa e con en s. This esul ed in diffe en w/c a ios and hus
diffe en esul ing s eng hs.
The manu ac u e o he conc e e was ca ied ou in acco dance wi h BS 1881: Pa
108:1983 [27]. In he p oduc ion o conc e e, he d y ing edien s we e mixed wi h each
o he a ambien empe a u e, hen hal o he wa e was added, and all he ing edien s
we e mixed o 2 min o o m a homogeneous mix u e. The es o he wa e was hen
added and he ma e ials we e mixed o 2 min. The samples we e hen cas in o cube
molds, compac ed, and le a oom empe a u e o 24 h; hey we e ans e ed o a ank
o wa e and cu ed o 7 and 28 days. A o al o 150 cubic specimens (50 samples o each
class) cubic specimens (150 mm × 150 mm × 150 mm) we e p oduced in 3 diffe en classes.
The e o e, each es se is based on 25 iden ical es samples. Thus, as shown below, i was
es ed in wo diffe en di ec ions, and a la ge s a is ical e alua ion was ob ained due o
he numbe o 25 samples pe condi ion.
2.2. Expe imen al P og am
Th ee es s we e p epa ed in he expe imen al p og am—non-des uc i e e ical
hamme es , non-des uc i e ho izon al hamme es on a loaded specimen, and des uc-
i e p essu e es in a hyd aulic p ess machine. A 50% alue o he maximum p edic ed
o ce was used o each ype o conc e e— o conc e e C30, i was 15 MPa, o conc e e
C35 i was 17.5 MPa, and o conc e e C40 i was 20 MPa. All es s we e pe o med sequen-
ially on he same specimens o main ain a comple e co ela ion o esul s. Figu e 1 shows
he s eps o use a Schmid hamme . The i s pic u e is he calib a ion sample, he second
pic u e is he es measu emen in a e ical way, and he hi d pic u e is he es measu e-
men in a ho izon al way.
(a) (b) (c)
Figu e 1. S eps o use a Schmid hamme : (a) placing he calib a ion elemen , (b) es ing e ically,
(c) es ing ho izon ally.
Be o e s a ing he es , he hamme should be calib a ed; he a e age o en eading
numbe s should be conside ed as calib a ion be o e each es . Fu he mo e, he es su -
ace should be smoo h, e en in he labo a o y o on si e. The specimen should also be held
Figu e 1.
S eps o use a Schmid hamme : (
a
) placing he calib a ion elemen , (
b
) es ing e ically,
(c) es ing ho izon ally.
Be o e s a ing he es , he hamme should be calib a ed; he a e age o en eading
numbe s should be conside ed as calib a ion be o e each es . Fu he mo e, he es su ace
should be smoo h, e en in he labo a o y o on si e. The specimen should also be held
by a igid keepe o a oid shaking. I should be no ed ha he di ec ion o he hamme
can a ec he ha dness alues. Acco ding o ASTM C805-02 [28], he hamme should i s
In as uc u es 2023,8, 155 4 o 14
be kep e ical and hen he specimen placed on a hyd aulic jack o ake he numbe o
opposi e aces o he cube specimen. An a e age o 10 eading numbe s o each su ace was
conside ed as a hamme ebound numbe . I he measu ed alue de ia ed om he a e age
by 20%, i was no included in he inal in es iga ion. Fu he mo e, i hese neglec ed
eading numbe s we e mo e han 2 on each su ace, hen he es was no eliable and was
cancelled. Finally, he specimen was des uc i ely es ed o de e mine he comp essi e
s eng h o he hyd aulic p ess machine. The comp essi e s eng h o conc e e is a es
ca ied ou on a cube, a cylinde , o a sui able piece o b oken beam, some imes on co e
holes. A minimum o h ee bodies a e always es ed. Be o e he ac ual es , he geome y o
he es body is e i ied. Specimens ha ail non-s anda dly a e excluded om he es . A
eco d o each es and i s esul s shall be kep .
2.3. S a is ics
The main aim was o ind a ela ionship be ween he DT and NDT esul s. These
wo g oups we e i s co ela ed o all conc e es using Pea son’s co ela ion coe icien
(PCC) [
29
]. The Pea son co ela ion coe icien is a desc ip i e s a is ic ha sums up he
cha ac e is ics o a da a se . Speci ically, i desc ibes he s eng h and di ec ion o he
linea ela ionship be ween wo quan i a i e a iables. Fo example, a PCC g ea e han
0.5 means s ong s eng h. The same se was hen analyzed using linea eg ession [
30
] and
he de e minan R
2
[
31
,
32
]. R
2
is a s a is ic used in he con ex o s a is ical models whose
main pu pose is o p edic u u e ou comes.
This analysis p o ides a measu e o how well obse ed ou comes a e eplica ed by
he model, based on he p opo ion o o al a ia ion o ou comes explained by he model.
Linea eg ession analysis is used o p edic he alue o a a iable based on he alue
o ano he a iable. The a iable you wan o p edic is called he dependen a iable.
The a iable you use o p edic he alue o ano he a iable is called he independen
a iable. This o m o analysis es ima es he coe icien s o a linea equa ion in ol ing one
o mo e independen a iables ha bes p edic he alue o he dependen a iable. A
linea eg ession co esponds o a line o a ea ha minimizes he di e ences be ween he
p edic ed and ac ual alues o he ou pu .
The e alua ion o co ela ion and linea eg ession indica es whe he wo pa ame e s
ha e a e y high, high, mode a e, low, o no dependence. These nume ically ob ained
linea co ela ion cu es we e aced wi h he no ma i e cu e o he Schmid hamme used.
The cu es ob ained we e also desc ibed using he equa ion and he s a is ical pa ame e s
desc ibed abo e.
3. Resul s and Discussion
DT and NDT in es iga ions we e ca ied ou on h ee di e en g ades o conc e es,
namely, C30, C35, and C40, o es ima e comp essi e s eng h wi h a good app oxima ion.
Tables 2and 3p esen he a e age o 25 comp essi e s eng h measu es in MPa and
25 ebound numbe s in e ical and ho izon al hamme posi ions o conc e e cu ed o
7 and 28 days, espec i ely. Acco ding o he esul s, he comp essi e s eng h inc eased
wi h inc easing conc e e g ade; wi h espec o samples cu ed o 7 days, he comp essi e
s eng h inc eased om 31.7 MPa (C30) o 38.9 MPa (C40). Fu he mo e, o samples cu ed
o 28 days, he comp essi e s eng h inc eased om 42.9 MPa (C30) o 51.1 MPa (C40).
The e o e, by compa ing he esul s, i is ob ious ha inc easing he numbe o days ha
conc e e samples we e cu ed in wa e led o an inc ease in comp essi e s eng h. Mo eo e ,
i can be unde s ood om Tables 2and 3 ha i he hamme posi ion changes om a
ho izon al di ec ion o a e ical di ec ion, he ebound numbe dec eases.
These obse a ions do no de ia e om he expec a ions and in o ma ion a ailable
in he li e a u e [
8
,
11
,
18
]. E alua ion o he s anda d de ia ion shows ha in all cases he
numbe s a e less han 10% o he mean, which co esponds o he es ic ion ha no esul
had o be excluded om he s a is ical se .
In as uc u es 2023,8, 155 5 o 14
Table 2.
A e age comp essi e s eng hs in MPa and ebound numbe o di e en conc e e cu ed o
7 days.
Age Class Tes Mean STD
7 days
C30
Comp essi e S eng h 31.7 MPa 3.19
Rebound numbe (ho izon al) 28.5 2.81
Rebound numbe ( e ical) 23.1 1.22
C35
Comp essi e S eng h 37.5 MPa 2.74
Rebound numbe (ho izon al) 30.1 2.48
Rebound numbe ( e ical) 24.5 2.25
C40
Comp essi e S eng h 38.9 MPa 4.22
Rebound numbe (ho izon al) 33.2 2.14
Rebound numbe ( e ical) 26 1.75
Table 3.
A e age comp essi e s eng h in MPa and ebound numbe o di e en conc e e cu ed o
28 days.
Age Class Tes Mean STD
28 days
C30
Comp essi e S eng h 42.9 MPa 4.82
Rebound numbe (ho izon al) 34.1 2.19
Rebound numbe ( e ical) 25.9 1.73
C35
Comp essi e S eng h 47.1 MPa 4.36
Rebound numbe (ho izon al) 35.5 1.19
Rebound numbe ( e ical) 28.6 2.36
C40
Comp essi e S eng h 51.1 MPa 3.68
Rebound numbe (ho izon al) 36.1 1.55
Rebound numbe ( e ical) 30.7 3.15
A compa ison be ween he s anda d de ia ion o he hyd aulic p ess measu emen
and he s anda d de ia ion o he ebound es shows ha in his applica ion he ebound
esul s ha e less a iance. This was obse ed o all h ee ypes o conc e e.
To ind he co ela ion be ween Schmid ebound numbe and comp essi e s eng h,
he c ushing conc e e s eng h in MPa e sus ebound numbe s is plo ed o 7-day-old
conc e e and in ho izon al hamme posi ion o conc e e C30 (see Figu e 2), C35 (see
Figu e 3), and C40 (Figu e 4). Simila ly, da a om e ical measu emen s a 7 days a e
conc e ing we e analyzed. The esul s a e p esen ed oge he wi h he eg ession cu e in
Figu es 5–7. Fu he mo e, da a a 28 days o all conc e es in he ho izon al di ec ion (see
Figu es 8–10) and he e ical di ec ion o he hamme measu emen (see Figu es 11–13)
a e p esen ed.
Fi s , an e alua ion o he esul s measu ed 7 days a e he conc e e. The co ela ion
be ween he ho izon al ebound hamme measu emen and he hyd aulic comp essi e
s eng h o conc e e C30 shown in Figu e 2shows a PCC o 95%, demons a ing high
ag eemen . E en he g aphical e alua ion o he linea co ela ion has a de e mina ion
alue o o e 0.9. On he o he hand, in Figu e 3, whe e he same pai is co ela ed bu o
C35 conc e e, a sligh ly highe PCC is seen, bu he linea eg ession has a be e i in his
case. The equa ion o he cu e has a di e en basis bu a e y simila slope. Figu e 4 hen
shows he conc e e C40, o which he co ela ion eg ession cu e has a nega i e in e cep
alue on he y-axis, and so i can be seen ha he cu e is signi ican ly di e en . Unlike he
i s wo conc e es (C30 and C35), he C40 conc e e has a no ma i e ins umen cu e wi h
almos he same slope as he esul ing co ela ion cu e om he nume ical e alua ion.
Figu e 5shows he co ela ion o he e ical ebound es expe imen and he com-
p essi e s eng h o he p ess o C30 conc e e. The co ela ion o he esul s is a a e y
high le el and he cu e de e mina ion is also e y high. The slope o he cu e does no
co espond o he no ma i e cu e. Figu e 6 hen shows he same es s, bu o C35 conc e e.
Again, we see high co ela ion coe icien numbe s and high ag eemen . Figu e 7shows

In as uc u es 2023,8, 155 6 o 14
he same o C40 conc e e. Again, o his conc e e, he slope o he eg ession cu e is e y
simila o he no ma i e cu e.
In as uc u es 2023, 8, x FOR PEER REVIEW 6 o 14
Figu e 2. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7
days o conc e e C30.
Figu e 3. Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 7
days o conc e e C35.
Figu e 2.
Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7 days
o conc e e C30.
In as uc u es 2023, 8, x FOR PEER REVIEW 6 o 14
Figu e 2. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7
days o conc e e C30.
Figu e 3. Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 7
days o conc e e C35.
Figu e 3.
Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 7
days o conc e e C35.
In as uc u es 2023,8, 155 7 o 14
In as uc u es 2023, 8, x FOR PEER REVIEW 7 o 14
Figu e 4. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7
days o conc e e C40.
Figu e 5. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days
o conc e e C30.
Figu e 4.
Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7 days
o conc e e C40.
In as uc u es 2023, 8, x FOR PEER REVIEW 7 o 14
Figu e 4. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 7
days o conc e e C40.
Figu e 5. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days
o conc e e C30.
Figu e 5.
Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C30.
In as uc u es 2023,8, 155 8 o 14
In as uc u es 2023, 8, x FOR PEER REVIEW 8 o 14
Figu e 6. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C35.
Figu e 7. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C40.
PCC = 0.958
y = 2.4942x − 25.191
R² = 0.918
0
10
20
30
40
50
60
70
0 102030405060
Comp essi e S eng h [MPa] (DT)
Schmid Rebound Numbe [-] (NDT)
C35 - day 7 - e ical
Expe imen s
No ma i e Schmid cu e
Linea - expe imen
Figu e 6.
Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C35.
In as uc u es 2023, 8, x FOR PEER REVIEW 8 o 14
Figu e 6. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C35.
Figu e 7. Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C40.
PCC = 0.958
y = 2.4942x − 25.191
R² = 0.918
0
10
20
30
40
50
60
70
0 102030405060
Comp essi e S eng h [MPa] (DT)
Schmid Rebound Numbe [-] (NDT)
C35 - day 7 - e ical
Expe imen s
No ma i e Schmid cu e
Linea - expe imen
Figu e 7.
Co ela ion o he ebound index o he e ical es and comp essi e s eng h a 7 days o
conc e e C40.
In as uc u es 2023,8, 155 9 o 14
In as uc u es 2023, 8, x FOR PEER REVIEW 9 o 14
Figu e 8. Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 28
days o conc e e C30.
Figu e 9. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 28 days
o conc e e C35.
Figu e 8.
Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 28
days o conc e e C30.
In as uc u es 2023, 8, x FOR PEER REVIEW 9 o 14
Figu e 8. Co ela ion o he ebound index om he ho izon al es and comp essi e s eng h a 28
days o conc e e C30.
Figu e 9. Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 28 days
o conc e e C35.
Figu e 9.
Co ela ion o he ebound index o he ho izon al es and comp essi e s eng h a 28 days
o conc e e C35.