# Nanostructural Deformation Analysis of Calcium Silicate Hydrate in Portland Cement Paste by Atomic Pair Distribution Function

Authors: Hiroshi Suzuki; Sungchul Bae; Manabu Kanematsu
Journal: Advances in Materials Science and Engineering
 (2016)

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## Abstract

The deformation of nanostructure of calcium silicate hydrate (C-S-H) in Portland cement (PC) paste under compression was characterized by the atomic pair distribution function (PDF), measured using synchrotron X-ray diffraction. The PDF of the PC paste exhibited a unique deformation behavior for a short-range order below 2.0 nm, close to the size of the C-S-H globule, while the deformation for a long-range order was similar to that of a calcium hydroxide phase measured by Bragg peak shift. The compressive deformation of the C-S-H nanostructure was comprised of three stages with different interactions between globules. This behavior would originate from the granular nature of C-S-H, which deforms with increasing packing density by slipping the interfaces between globules, rearranging the overall C-S-H nanostructure. This new approach will lead to increasing applications of the PDF technique to understand the deformation mechanism of C-S-H in PC-based materials.


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## Body

## 1. Introduction

Portland cement (PC) paste is composed of various hydration products, such as calcium hydroxide (CH), ettringite, monosulphate, and calcium silicate hydrate (C-S-H), as well as several anhydrous PC clinker phases [1]. C-S-H, a primary binding phase in PC paste, has predominant influences on its mechanical and chemical properties. It is, therefore, crucial to understand the role of the C-S-H phase in the deformation behavior of PC paste.In previous studies, various discussions on the mesoscale structure of C-S-H have been made regarding the basis of physical properties such as specific surface area, pore size, and density measured by a number of observation techniques [2–4]. Jennings, accordingly, suggested that the basic model for the nanostructure of C-S-H to represent these physical parameters, which is a particle-packing model with nanoscale globules, is known as the colloid model [5, 6]. This is a useful model for understanding the physical and mechanical properties of C-S-H as in the case of Constantinides and Ulm [7] discovering the unique nanogranular behavior of C-S-H, driven by particle-to-particle contact forces, from the results of the mapping of the indentation modulus.Although there are various deformation studies on PC paste on the basis of CH phase behavior measured using neutron and X-ray diffraction techniques [8–10], there is a lack of studies on the deformation of C-S-H itself due to its unique nanostructure. Meanwhile, the atomic pair distribution function (PDF) technique is well known as a method to evaluate nanoscale structures of materials with no or less crystal periodicity. For instance, using the PDF technique, Skinner et al. suggested that the size of the C-S-H nanoparticle is estimated to be approximately 3.5 nm in diameter [11]. Furthermore, this technique has been successfully applied to quantitative evaluation of the deformation behavior of amorphous metallic glasses by directly measuring displacement between neighbor atoms [12]. In this study, the deformation behavior of the C-S-H phase in PC paste is discussed by applying the PDF technique to access a quantitative evaluation of the local strains occurring in the C-S-H nanostructure.


## 2. Material and Methods

PC for research containing fewer impurities was mixed with a water-to-cement ratio of 0.5. The paste was cured for a total of 73 days, that is, demolded after 24 hours, cured in water for 28 days, and stored for 45 days under ambient conditions at 20°C and 60% RH. The rectangular specimen, with a dimension of 5 × 5 × 10 mm3, was obtained from the PC paste with dimensions of 50 × 50 × 92 mm3.The X-ray diffraction experiments were carried out using high-energy X-rays of 69.8 keV at BL22XU in SPring-8, Japan [13]. The specimen mounted on the load frame was set on the diffractometer and was irradiated by an incident beam with a size of 0.3 × 0.3 mm2. The diffraction from the specimen was measured by an imaging plate (IP) with exposure time of 20 seconds. The pixel size of the IP was approximately 0.1 mm. The distances from the IP to the specimen were set to be 300 mm and 700 mm. Each distance was determined to obtain a longer Q-range for the PDF and higher angular resolution for the strain analysis by Bragg peak shift, respectively. A diffraction pattern in the loading direction was obtained by circumferentially integrating the range of ±30° of the diffraction ring. The compressive loadings were applied to the specimen with the constant displacement mode until approximately 40 MPa. Since the applied stress was gradually released due to creep while stopping the displacement, the average stress during measurement was defined to be applied stress. The scattering vector was parallel to the axis of the applied compressive load.


## 3. Results

Figure1(a) presents a diffraction pattern measured by the IP placed at 300 mm. A number of diffraction peaks can be observed, which are derived from hydration products and anhydrous clinker phases. Although most diffraction peaks are difficult to identify because of their complex crystal structures, CH peaks can be extracted from the diffraction pattern since it is a simple trigonal structure. In contrast, the C-S-H nanostructure might appear as a halo pattern overlapped with the diffraction pattern. Figure 1(b) shows the PDF produced by the PDFgetX3 program [14] with a Q-range of Fourier transformation from 14 to 140 nm−1. The radius, r, in the horizontal axis in Figure 1(b) is the distance from an average atom located at the origin. This is mixed nanostructural information of all composed phases, including C-S-H, weighted by the volume fraction, and shows similar trends regarding the PDF of the hydrated tricalcium silicate paste shown in the previous study [11].Figure 1
(a) X-ray diffraction pattern of PC paste measured at the detector position of 300 mm and (b) the PDF data derived from the diffraction pattern shown in (a).
(a)
(b)Figure2 shows a change in strains as a function of the applied stress, derived from the Bragg peak shift. The elastic strain, ε
b, is obtained by a change in the lattice spacing, d, for h
k
l reflection in the sample from reference lattice spacing, d
n
0, in an initial step of loading; ε
b
=
(
d
n
-
d
n
0
)
/
d
n
0. The deformation of the CH phase (hereafter “CH-strain”) was calculated by averaging strains of 36 reflections related to the CH phase using the following equation:(1)
ε
b
A
v
g
=
1
n
∑
ε
b
n
=
1
n
∑
d
n
-
d
n
0
d
n
0
,where n indicates the number of reflections used for the strain calculation. In contrast, the average deformation of other composed crystalline phases, that is, hydration products except C-S-H and CH phases, was calculated by averaging the strains of the remaining 22 reflections. The CH phase shows a linear deformation, but we can see a slight change in gradient at 14 MPa of compressive loading by carefully looking. Assuming it is linear, Young’s modulus of the CH phase is calculated to be approximately 32 GPa, which is smaller than that of other composed phases, approximately 52 GPa.Figure 2
Strain change of the CH phase and the average strain of the other composed phases as a function of the applied compressive stress. The strains are derived from the Bragg peak shift. The average error bars are±
3.4
×
10
-
5 and ±
2.1
×
10
-
4, respectively. The lineally approximated lines are presented in solid lines.The PDF shown in Figure1(b) represents a mixed atomic distribution derived from all composed phases including C-S-H, weighted by the volume fraction of each phase. It is, therefore, challenging to extract only C-S-H structural information from the measured PDF. In this study, we attempted to characterize the deformation behavior of C-S-H by using the feature that the intensity damping of the PDF is correlated to the damping of the structural coherence in the crystalline grain, meaning the grain size [15]. The PDF in the short range could be dominated by C-S-H since its volume fraction is typically known to be approximately 50% or more [16]. In contrast, the structural information of C-S-H in the PDF decreases with an increase of r since the discrete PDF derived from C-S-H with the size of a few nanometers might be damping immediately.In the PDF technique, the atomic strain,ε
a, is obtained by a change of the peak position, r, from a reference radius, r
n
0, in an initial step of loading; ε
a
=
(
r
n
-
r
n
0
)
/
r
n
0. Figure 3 shows the atomic strain behaviors that averaged at intervals of 0.5 nm or 1.0 nm in r, calculated by the following equation:(2)
ε
a
A
v
g
=
1
n
∑
ε
a
n
=
1
n
∑
r
n
-
r
n
0
r
n
0
,where n indicates the number of peaks used for the strain calculation. The change in the atomic strain in the short range below 1.0 nm shows the S-curve and shifts the trend to be linear gradually with an increase in r. With exceeding 2.0 nm in r, the atomic strains change linearly along the CH-strain measured by the Bragg peak shift but do not always agree with the CH-strain beyond 3.0 nm in r. According to the result shown in Figure 3, 2.0 nm in the PDF seems to be a critical size in the transition of deformation. Considering the typical globule size of C-S-H, ~5.0 nm, suggested by various techniques in previous studies [4–6, 11, 17], the deformation behavior below 2.0 nm in r might be predominantly characterized by the C-S-H nanostructure. Figure 4 shows a change in atomic strains averaged in the ranges from 0 nm to 2.0 nm and from 2.0 nm to 6.0 nm, compared with the CH-strain. In the local structural deformation below 2.0 nm in r, the plateau region can be observed from 14 to 24 MPa of applied stress in compression. On the other hand, the deformation in the longer range between 2.0 nm and 6.0 nm shows a slightly similar trend to the local structural deformation, but it rather corresponds to the CH-strain. This means that the deformation above 2.0 nm in r predominantly represents the deformation of the CH phase.Figure 3
The atomic strains that averaged at intervals of 0.5 nm or 1.0 nm inr, compared with the strain of the CH phase derived from the Bragg peak shift. The average error bars are ±
22
×
10
-
5 (r = 0-1 nm), ±
9.5
×
10
-
5 (r = 1–1.5 nm), ±
6.1
×
10
-
5 (r = 1.5–2 nm), ±
6.3
×
10
-
5 (r = 2–2.5 nm), ±
4.0
×
10
-
5 (r = 2.5–3 nm), ±
3.2
×
1
0
-
5 (r = 3-4 nm), ±
2.5
×
10
-
5 (r = 4-5 nm), and ±
1.8
×
10
-
5 (r = 5-6 nm).
(a)
(b)Figure 4
Change in the atomic strains that averaged in the ranges from 0 nm to 2.0 nm inr and from 2.0 nm to 6.0 nm in r, compared with a change in the strain of the CH phase derived from the Bragg peak shift. The average error bars are ±
1.0
×
10
-
4 and ±
1.5
×
10
-
5, respectively.


## 4. Discussion

As shown in Figure4, the deformation behavior of the short-range structure in the range from 0 nm to 2 nm would consist of three stages with different trends as follows. The linear deformation behavior with 10 GPa of Young’s modulus is observed first in Stage-I, and then the deformation becomes smaller in Stage-II. After that, the compressive strain linearly increases again with 37 GPa of Young’s modulus in Stage-III. Here, it is appropriate to apply the colloid model [5, 6] to explain the unique deformation behavior of the short-range structure within 2.0 nm in r on the basis of the nanogranular nature.Figure5 shows the schematic idea regarding the deformation mechanism of C-S-H under compression. Assuming that C-S-H acts as a granular material, the force transmission between globules follows the principle of the force chain network [18]. Considering an initial structure of C-S-H in Stage-I, low-density C-S-H with large gel pores decreases Young’s modulus since the small contact area, that is, the small load-bearing area, between globules enhances deformation in C-S-H. Furthermore, there would be no slip between globules in Stage-I. In Stage-II, on the other hand, the interface filled by cohesive water between globules might start to slip since shear stress exceeds the critical strength of the interface, resulting in an increase in the packing density in C-S-H and then starting inhomogeneous deformation. While increasing the packing density in Stage-II, Young’s modulus in C-S-H is physically increasing with an increase in the load-bearing area between globules, and the strain in C-S-H decreases by following Hooke’s law even if there is no change in the applied loading. This implies that the strain in C-S-H can be relaxed by physical increasing in Young’s modulus of C-S-H during deformation. In the first half of Stage-II, a partial slip occurs between globules in the C-S-H structure, and Young’s modulus slightly increases with an increase of the solid-phase density. Following an increase in the applied stress, a slip occurs all over the C-S-H structure, resulting in a large increase in Young’s modulus and apparently showing small increase in strain, a plateau, in the second half of Stage-II. After full packing of globules in C-S-H, the C-S-H phase deforms homogeneously in Stage-III with 37 GPa of Young’s modulus. The difference in Young’s modulus between Stage-I and Stage-II indicates changes in the nanostructure, with an increase in density and a decrease in gel pores in C-S-H by compressive deformation. In accordance with the reference [7], the self-consistent model indicates that the indentation modulus of C-S-H can also increase more than threefold by an increase in the packing density of about 20%. Therefore, it is no wonder that this large difference in Young’s modulus appears between Stage-I and Stage-III.Figure 5
Schematic illustration of the deformation mechanism of C-S-H under uniaxial compression. Arrows in the globules in Stage-II indicate an image of its movement.


## 5. Conclusions

In this study, the deformation behavior of the C-S-H nanostructure was quantitatively characterized by the PDF technique, taking the feature of intensity damping in the PDF, which is correlated to the damping of the structural coherence in the crystalline grain size. The compressive deformation of the C-S-H nanostructure would consist of three stages with different interactions between globules. It would originate from the granular nature of C-S-H which deforms with increasing the packing density by slipping the interlayer between globules, rearranging the overall C-S-H nanostructure. However, it is necessary to isolate specific atom-atom correlations due to the C-S-H nanostructure throughout PDF data, since the PDF data presented in this study contain the contribution of other hydrated and anhydrous crystalline phases. Careful modeling of PDF using a pure PC clinker phase paste could enable us to remove the effect of other phases on PDF data. This more detailed understanding enables the C-S-H deformation model in PC paste, as well as PC-based systems containing supplementary cementitious materials.



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*Source: 8936084-2016-04-18.xml*