Insights Into the Caso4–H2O System: a Raman-Spectroscopic Study

Insights Into the Caso4–H2O System: a Raman-Spectroscopic Study

minerals Article Insights into the CaSO4–H2O System: A Raman-Spectroscopic Study Thomas Schmid 1,2,* , Robert Jungnickel 1 and Petra Dariz 2,3 1 Bundesanstalt für Materialforschung und -prüfung, Richard-Willstätter-Str. 11, 12489 Berlin, Germany; [email protected] 2 School of Analytical Sciences Adlershof (SALSA), Humboldt-Universität zu Berlin, Unter den Linden 6, 10099 Berlin, Germany; [email protected] 3 Bern University of Applied Sciences, Bern University of the Arts, Conservation-Restoration, Fellerstr. 11, 3027 Bern, Switzerland * Correspondence: [email protected] or [email protected] Received: 20 December 2019; Accepted: 22 January 2020; Published: 29 January 2020 Abstract: Even though being the subject of natural scientific research for many decades, the system CaSO4–H2O, consisting of the five crystalline phases gypsum, bassanite, and the anhydrites III, II, and I, has left many open questions for research. Raman spectroscopy was used because of its structural sensitivity and in situ measurement capability to obtain further insight by studying phase transitions in both ex situ and in situ experiments. The findings include significant contributions to the completeness and understanding of Raman spectroscopic data of the system. The dehydration path gypsum–bassanite–anhydrite III was shown to have strong parallels to a physical drying process, which depends on many parameters beyond the burning temperature. Raman band width determination was demonstrated to enable the quantitative discrimination of α-bassanite and β-bassanite as well as the postulated three sub-forms of anhydrite II (AII), which are all based on differences in crystallinity. In the latter case, the observed continuous structural variations over increasing burning temperatures were elucidated as a combination of decreasing surface areas and healing of crystal lattice defects. We propose an only two-fold sub-division of AII into reactive “disordered AII” and much less reactive “crystalline AII” with a transition temperature of 650 C ◦ ± 50 K. Keywords: gypsum; bassanite; hemihydrate; anhydrite; dehydration; rehydration; phase transition; crystal defects; in situ Raman spectroscopy; Raman band width 1. Introduction In the course of the 19th century, gypsum increasingly became a subject of natural scientific investigations and the sentence written by Eugene W. Posnjak about 80 years ago is still currently relevant: “It seemed very surprising that, considering the relative simplicity of the system CaSO4–H2O, and its accessibility for study, it could remain over a period of so many years the subject of so much controversy.” [1] (p. 248). To mention only the most significant milestones in research history, Henry Le Chatelier published his doctoral thesis on “Recherches expérimentales sur la constitution des mortiers hydrauliques” (experimental research on the constitution of hydraulic mortars) in 1887, recognising plaster of Paris as calcium sulphate hemihydrate (and not as anhydrite as supposed by Antoine Laurent de Lavoisier in 1765) and its setting as a rehydration process leading to the formation of gypsum again. He observed the partial dehydration of calcium sulphate dihydrate into the hemihydrate bassanite and the subsequent transformation into the anhydrous salt at 128 ◦C and 163 ◦C, respectively [2,3]. In 1903, Jacobus Henricus van’t Hoff and his co-workers gave a transition Minerals 2020, 10, 115; doi:10.3390/min10020115 www.mdpi.com/journal/minerals Minerals 2020, 10, 115 2 of 35 temperatureMinerals 2020, 10 for, 115 the gypsum–hemihydrate reaction of 107 ◦C and proposed the existence of a soluble2 of 34 anhydrite form in the wrong assumption of a direct dehydration of gypsum without the intermediate hemihydrate step at 93 ◦°CC[ [4],4], which was was confirmed confirmed and and revised, revised, respectively, respectively, in independent studies by W. A.A. DavisDavis [[5],5], HarryHarry B. Weiser etet al.al. [[6],6], andand EugeneEugene W. PosnjakPosnjak [[1].1]. In 1913, Werner GrahmannGrahmann foundfound (optical)(optical) indicationsindications for for a a high-temperature high-temperature form form of of anhydrite anhydrite and and reported reported a transitiona transition point point at approximatelyat approximately 1194 1194◦C[ °C7 ].[7]. Evidence Evidence for for the the actual actual conversion conversion of of anhydrite anhydrite IIII intointo anhydriteanhydrite II isis basedbased on an endothermic peakpeak onon thethe heatingheating curvecurve ofof gypsumgypsum atat approximatelyapproximately 1180–12301180–1230 ◦°CC[ [8–13].8–13]. After decades of controversy regarding the number of phases in the CaSO4–H2O system, there After decades of controversy regarding the number of phases in the CaSO4–H2O system, there isis agreementagreement onon fourfour phasesphases stablestable (or(or metastable,metastable, respectively)respectively) atat roomroom temperature—gypsumtemperature—gypsum CaSO4∙2H2H2OO (dihydrate), (dihydrate), bassanite bassanite CaSO CaSO4∙½H2O1 H(hemihydrate),O (hemihydrate), anhydrite anhydrite III CaSO III4 (soluble CaSO anhydrite,(soluble 4· 2 4· 2 2 4 γ-CaSO4), and anhydrite II CaSO4 (insoluble anhydrite or natural anhydrite, β-CaSO4). Several of anhydrite, γ-CaSO4), and anhydrite II CaSO4 (insoluble anhydrite or natural anhydrite, β-CaSO4). Severalthose are of thosedescribed are described with more with than more one than structural one structural model. model. The excerpt The excerpt of the of thecrystal crystal structure structure of ofgypsum gypsum in inFigure Figure 1 1shows shows the the view view along along the the [001] direction, which revealsreveals chainschains ofof alternatingalternating calcium and sulphate ions that are building blocks of all phases of the CaSO4–H2O system. calcium and sulphate ions that are building blocks of all phases of the CaSO4–H2O system. Figure 1. Crystal structures of the four main phases of the CaSO4–H2O system, which are stable atFigure room 1. temperature.Crystal structures The of graphical the four representationsmain phases of werethe CaSO designed4–H2O bysystem, employing which theare softwarestable at VESTAroom temperature. (Visualisation The for graphical Electronic representations and STructural were Analysis) designed [14 by] andemploying structural the datasoftware available VESTA in References(Visualisation [15 –for18 ].Electronic and STructural Analysis) [14] and structural data available in References [15–18]. In gypsum, they are arranged as double layers interconnected by the hydrogen bonds of waterIn layers. gypsum, Gypsum, they are which arranged forms as monoclinicdouble layers prismatic interconnected crystals by (space the hydrogen group C2 /bondsc)[15], of cleaves water predominantlylayers. Gypsum, along which these forms layers. monoclinic Conversion prismatic of the crystals dihydrate (space into hemihydrategroup C2/c) (bassanite)[15], cleaves is predominantly along these layers. Conversion of the dihydrate into hemihydrate2+ (bassanite)2 is accompanied by clear structural changes, which leads to the arrangement of six Ca –SO4 − chains aroundaccompanied approximately by clear 0.4-nmstructural wide changes, channels which hosting leads the to crystal the arrangement water. Figure of1 showssix Ca2+ the–SO view42− chains onto thearound (001) approximately plane of bassanite, 0.4-nm which wide channels crystallises hosting in the the monoclinic crystal water. space Figure group 1 showsI2 [16]. the Only view slight onto the (001) plane of bassanite, which crystallises in the monoclinic space group I2 [16]. Only slight rearrangements of the Ca2+–SO42− chains lead to orthorhombic anhydrite III (C222) [17], which is mainly characterised by empty channels due to the loss of crystal water. Lastly, anhydrite II consists of regularly arranged Ca2+–SO42− chains in an orthorhombic (Amma) crystal lattice [18]. Since the high- Minerals 2020, 10, 115 3 of 35 2+ 2 rearrangements of the Ca –SO4 − chains lead to orthorhombic anhydrite III (C222) [17], which is mainly characterised by empty channels due to the loss of crystal water. Lastly, anhydrite II consists 2+ 2 of regularly arranged Ca –SO4 − chains in an orthorhombic (Amma) crystal lattice [18]. Since the high-temperature phase anhydrite I (α-CaSO4) is not stable at room temperature, only X-ray diffraction conducted in heating chambers was able to provide structural insight, which revealed a cubic crystal lattice in analogy to sodium chloride with calcium ions coordinated by 12 oxygen atoms (in gypsum and anhydrite II, the coordination number is 8) [11]. Research proceeds regarding structural differences and properties of the phases constituting the CaSO4–H2O system, which allow their qualitative and quantitative identification, such as the two forms of hemihydrate and the three proposed sub-phases of anhydrite II (AII). The AII sub-phases exhibit different macroscopic characteristics (e.g., morphology, hydration reactivity, etc.) as a function of increasing calcination temperature. Sparingly soluble AII-s is produced at 300–500 ◦C, insoluble AII-u at 500–700 ◦C, and estrich gypsum AII-E at 700–1180 ◦C[19,20]. The first successful analytical approach to AII sub-phases was achieved recently in 2017, which demonstrated that, over the burning temperature range from 500 to 900 ◦C, the specific surface area of anhydrite II decreases due to an increase of crystallite size, while an overall increase of crystallinity can be traced by quantitatively evaluating the widths of room-temperature Raman bands, which get sharper

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