Introduction

The term “geopolymer” as used by Davidovits [1] is hardly connected to the reaction of metakaolin with alkaline solutions forming amorphous to semi-crystalline three-dimensional networks by polycondensation [2]. It has been chosen because of its analogy to organic material, which react at ambient temperatures to solid polymers. The prefix “Geo” refers to the inorganic nature of the material.

Apart from metakaolin, several materials react in this way, for instance, thermally treated clays [3], ashes, natural pozzolanes or minerals [4] as well as different waste materials. They have to consist of a metastable or amorphous phase with a high energetic level. In detail, the whole reaction comprises two more or less parallel steps,

  1. 1.

    Activation by an alkaline solution to form reactive monomers or oligomers.

  2. 2.

    Polycondensation to form the aluminosilicate network (ASN).

Geopolymers are alkali-activated materials. Alkaline activation has been used successfully for the activation of blast furnace slag since for more than 40 years [5, 6]. The reaction products of alkali-activated blast furnace slag have been widely investigated and can be compared to calcium silicate hydrates (C-S-H) and calcium aluminate hydrates (C-A-H) from Portland cements, apart from incorporated tetrahedral aluminium into the dreierketten structure of the calcium silicate hydrates [7] and hydrotalcite if the slag contains magnesium [8, 9].

What makes an alkali activation of metakaolin and blast furnace slag so different? Blast furnace slag contains a reasonable amount of calcium inside the glassy phase. If alkali-activated slags do not belong to the group of geopolymers, what happens after mixing slag and metakaolin and then activating with alkaline solution? What kind of reaction product will be formed? It has been shown the possibility of a simultaneously formation of C-S-H and aluminosilicate phases in metakaolin/lime mixtures depends on the alkalinity of the system [10]. Yip and van Deventer [11] found in their investigation on metakaolin/slag blends that C-S-H phases and aluminosilicate gel coexist.

The question is whether there is a coexistence of the two types of reaction products? Will there be an interaction between the partners in the blend? Will different reaction products be formed or is there domination of one of the partners, instance e.g. calcium dominates the reaction of the blends and only C-S(A)-H/C-A-H phases will be formed. Are these geopolymers?

It is attempted to answer these questions in this paper by discussing metakaolin-slag blends activated using pure sodium hydroxide solutions.

Experimental

Materials, mixture design and sample preparation

Ground granulated blast furnace slag (S) and commercially available metakaolin Metastar 402 from Imerys GB (M) were used as raw materials. The chemical composition and physical properties are given in Tables 1 and 2. As can seen by the chemical phase compositions in Fig. 1, as well as 73 wt.% glass, the slag used in this work contains crystalline calcium silicate phases and a considerable amount of calcite. Beside the crystalline phases feldspar, quartz and muscovite, 84 wt.% of the metakaolin is amorphous attributed to dehydroxylated kaolinite.

Table 1 Chemical composition of the raw materials
Table 2 Physical properties of the raw materials
Fig. 1
figure 1

Mineral composition of the metakaolin and slag

These materials were activated with sodium hydroxide solution in such way that the concentration for the activation of the pure metakaolin was higher than for the pure slag in order to reach the same Na/Al value of 0.4. The water content was adjusted to give the same workability of the pastes; therefore the water content varies. The detailed mixtures are given in Table 3.

Table 3 Composition of alkali-activated blends

Samples measuring 1 × 1 × 6 cm³ were prepared and kept inside the moulds at 40°C for one day. After de-moulding the samples were stored in closed boxes over water at room temperature.

Strength measurements

Compressive strength and bending tensile strength were measured after 28 days of storage. The measurement of bending tensile strength was performed with three specimens (1 × 1 × 6 cm³) of each mixture using three-point bending. The compressive strength was measured on each of the resulting half’s of the specimens with a compression area of 1 × 2 cm2.

Solid state NMR spectroscopy

Solid state NMR experiments were performed with a Bruker Avance 300 spectrometer (magnetic field strength 7.0455 T, resonance frequency of 29Si and 27Al is 59.63 and 78.20 MHz, respectively). To measure the 29Si MAS NMR spectra, the samples were packed in 7 mm zirconia rotors and spun at 5 kHz at an angle of 54°44′. The chemical shifts were recorded relative to external tetramethylsilane (TMS). The single pulse technique was applied with a pulse width of 4 μs. According to the high paramagnetic portion of the samples, a short repetition time of 5 s was chosen [12] and a typical number of scans were 40,000. For the 27Al MAS NMR spectra the samples were packed in 4 mm zirconia rotors and spun at 15 kHz at an angle of 54°44′. The chemical shifts were recorded relative to external Al(H2O) 3+6 . The single pulse technique was used with a pulse width of 3 μs. The repetition time was 2 s and the number of scans was 1,000. Thirty Hertz line broadening was applied to all spectra prior to deconvolution. The signal patterns of the spectra were deconvoluted with the Bruker WINNMR software using Lorentz curve which led to the best result.

X-ray diffraction

To determine the X-ray diffraction pattern the hardened and dried material was mixed with a standard material (ZnO about 10% per weight) and ground under addition of isopropanol in a bar mill (McCrone-Micronizer, McCrone Ltd., UK) for about 1 min. This mill was used to avoid preferred orientation (texture) and the introduction of stress. CuKα radiation was used. Quantification was carried out using Rietveld refinement (Autoquant®).

Thermal analysis

Thermal analysis was determined in a Seteram Setsys 16/18 equipment under air using a heating rate of 10 K/min in the temperature range 30–1,000°C.

Scanning electron microscopy

Scanning electron microscopy was performed with a HITACHI S2700LB combined with EDS TRACOR Voyager 2100. The experiments were carried out on dried but freshly broken samples that were sputtered with carbon.

Results

Strength

The pure slag binder (AA-S) reached the maximal strength values whereas the pure metakaolin binder (AA-M) showed a low strength which was probably due to the low alkali concentration as can be seen in Fig. 2. The samples of the blends (AA-M50/S50 and AA-M25/S75) achieved similar strength to the pure slag binder. The results of the bending tensile strength follow almost the same trend. The compressive strength of the blend AA-M25/S75 seems to be a little lower than the strength of the blend AA-M50/S50.

Fig. 2
figure 2

Strength performance of the alkali-activated blends

Reaction products

XRD

The reacted binders consist, as expected, mostly of amorphous phases either from not reacted raw material or from non-crystalline reaction products (Fig. 3). The crystalline phases quartz, muscovite, feldspar and calcite are supplied by the raw materials. New formed crystalline phases can only be seen in the samples containing slag, instance e.g. hydrotalcite (especially in AA-S) that is commonly found in alkali-activated slags and slag blended cements [8, 9]. The pronounced humps around 30° and 50° 2θ indicate the formation of a small quantity of crystalline C-S-H-phases.

DTA

The results of the thermal analysis are shown in Fig. 4. In the temperature range 30 to 300°C the lost of the different bonded adsorptive water of the binders AA-M and AA-S made with the single powders metakaolin and slag, respectively can be observed. The curves for the blends (AA-M50/S50 and AA-M25/S75) are clearly due to a combination of the curves for the binders made with the single materials (AA-M and AA-S) without any other contributions.

Fig. 3
figure 3

X-ray diffraction pattern of the binders

Fig. 4
figure 4

Results of thermal analysis

NMR

The expected structure informations using 29Si NMR spectroscopy are described as follows:

  • Silicate tetrahedra which are bonded in silicate chains can either be situated at the chain ends (Q1; NMR signal at −78 ppm ± 2 ppm) or in the middle (Q2, NMR signal at −85 ppm ± 2 ppm). If aluminate tetrahedra are incorporated into the silicate chain as bridging tetrahedra, an additional NMR peak from the neighbouring Silicates will appear at −82 ppm ± 2 ppm (Q2(1Al)) [13].

  • Zeolites as well as geopolymers are a network of silicate and aluminate tetrahedra that connect over all four corners to other tetrahedra. Therefore five possible NMR peaks of silicate tetrahedra Q4, which are connected to zero, one, two, three or four aluminate tetrahedra might be detectable in the spectrum between −85 and −110 ppm [14].

Figure 5 presents the 29Si NMR spectra of the raw materials metakaolin (M) and slag (S) as well as the spectra of the alkali-activated materials (binders AA-M, AA-S, AA-M50/S50, AA-M25/S75). The spectrum of the metakaolin contains one predominant broad single peak with a maximum around −101 ppm from Q4(1Al). The alkali-activated metakaolin (AA-M) consist of unreacted metakaolin which can be seen on the broad peak at −101 ppm and reaction product which can be seen on several peaks mainly situated in the range between −80 and −93 ppm.

Fig. 5
figure 5

29Si NMR spectra of the raw materials and alkali-activated binders

The spectrum for the slag contains one broad peak centred around −74 ppm. The alkali-activated slag (AA-S) comprises still unreacted slag (broad peak at −74 ppm) and reaction product that can be seen as a broad peak in the range between −75 and −87 ppm. The alkali-activated blends (AA-M50/S50 and AA-M25/S75) show peaks of more or less unreacted slag and metakaolin and peaks of reaction products in the whole range between −75 and −93 ppm.

The 27Al NMR spectrum of a slag binder should show signals of four-coordinated aluminium created by the aluminate tetrahedra incorporated in the silicate chains of the C-S-H-phases [8] as well as signals of six-coordinated aluminium from magnesium or calcium aluminate hydrate phases [15]. The spectrum of the ASN should exhibit only one signal due to the four-coordinated aluminium [10]. Figure 6 shows the 27Al NMR spectra of the raw materials metakaolin (M) and slag (S) as well as the spectra of the alkali-activated materials (binders AA-M, AA-S, AA-M50/S50, AA-M25/S75). The spectrum for the metakaolin contains three overlapping peaks according to four-, five- and six-coordinated aluminium. The AA-M comprises unreacted metakaolin which can be seen by the small peak at 0 ppm (six-coordinated aluminium). The reaction product can be seen as the large peak centred on 60 ppm which comes from the four-coordinated aluminium bonded in the ASN.

Fig. 6
figure 6

27Al NMR spectra of the raw materials and alkali-activated binders

The spectrum of the slag shows several broad strongly overlapping peaks according to varying environments of four-, five- and six-coordinated aluminium. The AA-S comprises unreacted slag indicated by the asymmetric shape of the tetrahedral aluminium that overlaps the peak of tetrahedral aluminium inside the C-S-H-phases (around 70 ppm). Additionally a reaction product with six-coordinated aluminium is formed which can be seen as the sharp peak at about 10 ppm. Based on the results of X-ray diffraction this signal can be assigned to the hydrotalcite phase.

The alkali-activated blends (AA-M50/S50 and AA-M25/S75) show one dominant peak around 60 ppm, mainly from the tetrahedral aluminium of the ASN. The asymmetric shape indicates the overlapping with tetrahedral aluminium of different environments, for example in the unreacted slag and metakaolin and in the C-S-H-phases.

Quantifying of the reaction products

The NMR spectra were deconvoluted following the regime shown in Fig. 7. First the spectra of the raw materials were evaluated with the Bruker WINNMR Deconvolution software to obtain values for chemical shift, width and intensity of all signals. The peak position and its width were used as fixed values for the next step: The spectra of the alkali-activated binders made from the single materials were evaluated by using the fixed peak position and width from the raw materials to fit the unreacted material using the intensity. The literature data as described above were used to define the peak positions and fit the signals of the reaction product with the parameters width and intensity. The peak position and its width were used again as fixed values in the next step: By using the fixed peak positions and widths of the pure binder spectra and fitting only the peak intensity, the deconvolution of the spectra of the alkali-activated blends led to reasonable results.

Fig. 7
figure 7

Procedure for the deconvolution and interpretation of the alkali-activated binders

The results of the deconvolution are shown in Figs. 8, 9, 10, 11, 12.

Fig. 8
figure 8

29Si NMR spectrum and interpretation of the alkali-activated metakaolin (AA-M)

Fig. 9
figure 9

27Al NMR spectrum and interpretation of the alkali-activated metakaolin (AA-M)

Fig. 10
figure 10

29Si NMR spectrum and interpretation of the alkali-activated slag (AA-S)

Fig. 11
figure 11

27Al NMR spectrum and interpretation of the alkali-activated slag (AA-S)

Fig. 12
figure 12

29Si NMR spectrum and interpretation of the alkali-activated blend 50% metakaolin/50% slag (AA-M50/S50)

The intensity of the single peaks was used to calculate the amount G Qi of the different chemical environments of silicon and aluminium.

Difficulties occurred for the deconvolution of both the 29Si NMR and 27Al NMR spectra of the alkali-activated blends because of overlapping peaks at −85 ppm from Q2 of the C-S-H-phases and Q4(4Al) of the ASN as well as the overlapping peaks of tetrahedral aluminium in the C-S-H, the ASN and the raw materials. Few preliminary considerations have been made:

  • The intensity of the Q4(4Al)-signal will effect the Si/Al ratio of the ASN quite strongly. The aluminosilicate can not incorporate more aluminium into the network because of the molar value Si/Al is already about 1. It can also not give up any silicon for the same reason.

  • The intensity of the Q2-signal can reach at most the intensity of the Q2-signal of the pure slag binder. The intensity will decrease if more aluminium is included in the C-S-H-phases.

That means that the dominant peak should be the Q4(4Al)-signal from the ASN rather than the Q2-signal from the C-S-H phases. The calculation of the amounts of aluminosilicate and C-S-H are made by help of the fitting procedure with fixed position and width which has been taken out of the pure metakaolin and slag binder spectra, respectively, as described above. The different environments of tetrahedral aluminium of the alkali-activated blends could not be separated in this way. The results of the 29Si-NMR are in Table 4 and the results of the 27Al-NMR in Table 5.

Table 4 Results of 29Si NMR spectroscopy
Table 5 Results of 27Al NMR spectroscopy

Due to the large noticeable amount of unreacted raw materials the question on the degree of reaction (RD) arises. These values can be calculated using the amount of unreacted material metakaolin GM and slag GS given in Table 4. Therefore the silicon input from metakaolin X(Si)M and slag X(Si)S, respectively, which is known from chemical und mixture composition, has to be considered. Then the reaction degree of the metakaolin RDM and the slag RDS can be calculated as follows:

$$ RD_{{\text{M}}} = \frac{{X({\text{Si}})_{{\text{M}}} - G_{{\text{M}}} ( - 101\,{\text{ppm}})}} {{X({\text{Si}})_{{\text{M}}} }}\quad {\text{and}}\quad RD_{{\text{S}}} = \frac{{X({\text{Si)}}_{{\text{S}}} - G_{{\text{S}}} ( - 74\,{\text{ppm}})}} {{X({\text{Si)}}_{{\text{S}}} }} $$

In this case the reaction degree of each raw material in blends can be discussed separately. The overall reaction degree RDov can also be calculated directly by using the amount of the reaction products (RP):

$$ {\text{RD}}_{{{\text{ov}}}} {\text{(}}^{{{\text{29}}}} {\text{Si)}} = {\sum\limits_{i = 1}^4 {G_{{{\text{Q}}_{{\text{i}}} }} } }{\text{(RP}}) $$

The results are given in Table 6.

Table 6 Specification of the reaction products

Based on the quantification of each signal, the average chain length (CL) and the molar ratio silicon to aluminium of the C-S-H-phases (Si/AlC-S-H) as well as of the ASN (Si/AlASN) can be calculated:

$$ \overline{{{\text{CL}}}} = \frac{{G_{{{\text{Q}}_{{\text{1}}} }} + \frac{3} {2}G_{{{\text{Q}}_{{\text{2}}} {\text{(1Al}})}} + G_{{{\text{Q}}_{{\text{2}}} }} }} {{\frac{1} {2}G_{{{\text{Q}}_{{\text{1}}} }} }} $$
$$ {\text{Si/Al}}_{{{\text{CSH}}}} = \frac{{G_{{{\text{Q}}_{1} }} + G_{{{\text{Q}}_{{2(1Al)}} }} + G_{{{\text{Q}}_{{\text{2}}} }} }} {{\frac{1} {2}G_{{{\text{Q}}_{{\text{2}} }} (1{\text{Al}})}}} $$
$$ {\text{Si/Al}}_{{{\text{ASN}}}} = \frac{{{\sum\nolimits_{n = 0}^4 {G{\left[ {{\text{Q}}_{4} (n{\text{Al}})} \right]}} }}} {{{\sum\nolimits_{n = 0}^4 {\frac{n} {4}G{\left[ {{\text{Q}}_{4} (n{\text{Al}})} \right]}} }}} $$

The results are given in Table 7.

Table 7 Comparison of reaction degree, calculation from 29Si NMR spectroscopy

Discussion

The alkaline activated metakaolin (AA-M) reacted to form an ASN showing, as expected, only Q4-Signals in the 29Si NMR spectrum and four-coordinated aluminium in the 27Al NMR spectrum. The appearance of signals from structures other than the Q4(4Al) is generally not observed. This can be explained by the low activator concentration as was shown in [16]. The alkaline activated slag (AA-S) reacted to form C-S-H-phases (with incorporated aluminium), revealed as Q1 and Q2 in the 29Si NMR spectrum and four-coordinated aluminium in the 27Al NMR spectrum, as well as to hydrotalcite which was seen as six-coordinated aluminium in the 27Al NMR spectrum and confirmed by X-ray diffraction.

At the first, the reaction product of the alkali-activated blends (AA-M50/S50 and AA-M25/S75) seems to be only the sum of the single activated powders. This means no dominance of one partner could be found. Considering the low activator concentration chosen, the dominance of formation of C-S-H phases was expected according to the results of Palomo [10]. However, in this case both partners contributed independently. Even for the alkali-activated blend AA-M25/S75, with the lowest activator concentration of metakaolin in the mix, the reaction degree of the metakaolin is much higher than that of the pure activated metakaolin binder (AA-M). Contrary to the investigations of Palomo [10], both materials of the blend possess all ingredients necessary for reaction.

The reason for the essentially parallel reaction may be found in the different time and place of reaction. Metakaolin and the components of the slag may have different kinetics for their dissolution/precipitation. These reactions take place at a nanoscale around the grains.

The coexistence of the both types of reaction products can also be seen in the SEM image (Fig. 13). The SEM image for sample AA-M50/S50 shows a slag grain with reaction layer around it. The element composition is shown for two points, EDX1 from the unreacted grain and EDX2 from the reaction layer. Apart from the problem of the measured volume (contribution from deeper layers), the element composition of spot EDX2 might indicate a lower Si/Al than expected for slag and C-S-H but too high for the ASN.

Fig. 13
figure 13

SEM image and results from EDS measurement of the sample AA-M50/S50

A closer inspection reveals that there is in fact an interaction between the single powders. Slag incorporates aluminium from the metakaolin as can be seen from the change in molar ratio of silicon to aluminium which decreases from 6 (pure slag binder) to 2.8 (50/50 blend). This causes a longer average chain length which increases from 6 to 13. The simultaneous increase of the Si/Al ration of the ASN from 1.07 to about 1.2 underlines the consistency of the measurement and interpretation. The effect of elongation the silicate chains in C-S-H by increasing aluminium content was described by Andersen et al. [13] as well. Schneider et al. [17] mentioned the decrease of the molar ratio of silicon to aluminium affected by the increasing sodium hydroxide concentration. As proved in parallel investigation [18], both average chain length and Si/Al ratio remain unaffected by the change of alkaline concentration in a pure slag system. Only the reaction degree could be increased by a higher concentration.

Conclusions

Obviously both type of reaction products—C-S-H from slag and ASN from the metakaolin—are able to coexist. There is only a small interaction between the reacting systems which is probable due to different kinetics of the dissolution process and distribution of the reacting species. The interaction could be shown by the incorporation of additional aluminium into C-S-H phases so that their Si/Al decreased from 6 to 2.8 and their average chain length increased from 6 to 13.

The alkaline activation of metakaolin-slag mixes yields a binder blend containing calcium silicate hydrate system and geopolymer system and a mixture of both phases due to interaction at their contact surfaces. This results in a good overall strength performance.

Whether slag removes the aluminium or the metakaolin cannot retain it due to the low sodium content is not distinguishable. It could not be established whether the different reaction degree was affected by the reaction of the partner or by the change of alkali quantity. Therefore further measurements are in progress at higher and constant activator concentration. In an attempt to bridge the gap of quantification the reaction products from 27Al NMR spectroscopy additional techniques for instance 1H-27Al CP NMR and MQ 27Al NMR will be used.

The results show that the primary question is not “whether these blends are geopolymers or not”, but there are binder mixtures containing geopolymer and slag binder in different proportions depending on their composition.