research communications
4)2, from laboratory powder X-ray diffraction data
of calcium perchlorate anhydrate, Ca(ClOaDaegu Gyeongbuk Institute of Science and Technology (DGIST), Daegu 42988, Republic of Korea
*Correspondence e-mail: st.hong@dgist.ac.kr
The 4)2·xH2O] at 623 K in air for 12 h. It crystallizes in the orthorhombic Pbca and is isotypic with Ca(AlD4)2. The contains one Ca, two Cl and eight O sites, all on general sites (Wyckoff position 8c). The consists of isolated ClO4− tetrahedra and Ca2+ cations. The Ca2+ cation is coordinated by eight O atoms of eight symmetry-related ClO4− tetrahedra within a distorted square-antiprismatic environment.
of calcium perchlorate anhydrate was determined from laboratory X-ray powder diffraction data. The title compound was obtained by heating hydrated calcium perchlorate [Ca(ClOKeywords: crystal structure; powder X-ray diffraction; calcium perchlorate anhydrate; Ca(ClO4)2; isotypism.
CCDC reference: 1827999
1. Chemical context
Recently, the alkaline earth metals, in particular magnesium and calcium, have received attention because of their incorporation in multivalent-ion batteries that can replace Li-ion batteries (Wang et al., 2013; Datta et al., 2014; Amatucci et al., 2001). Calcium has several merits, such as low cost and abundance in nature (Padigi et al., 2015; Rogosic et al., 2014). In addition, the standard reduction potential of the calcium electrode is −2.87 V, which is only about 0.18 V higher than that of lithium (Muldoon et al., 2014). Thus, calcium perchlorate is mainly used as a salt next to organic electrolytes in Ca-ion batteries (Hayashi et al., 2003). Nevertheless, the of anhydrous calcium perchlorate was unknown until now (Pearse & Pflaum, 1959) because of the lack of single crystals. Calcium perchlorate is strongly hygroscopic, and growing single crystals of a size sufficient for X-ray structure analysis has not been successful up to date. On the other hand, the crystal structures of the perchlorates of magnesium, barium and other alkaline earth metals have been determined for both hydrated and anhydrous phases (Gallucci & Gerkin, 1988; Lee et al., 2015; Lim et al., 2011; Robertson & Bish, 2010). However, for calcium perchlorate only the hydrated forms were structurally determined (Hennings et al., 2014).
of calcium perchlorate anhydrate, using laboratory powder X-ray diffraction (PXRD) data (Fig. 12. Structural commentary
The 4)2, is isotypic with that of Ca(AlD4)2 (Sato et al., 2009), but is different from barium or magnesium perchlorates (Lee et al., 2015; Lim et al., 2011). Different viewing directions of the of Ca(ClO4)2 are presented in Fig. 2, using ClO4− tetrahedra and Ca2+ cations. The contains one Ca (on general positions 8c), two Cl (8c), and eight O (8c) sites. The ClO4− tetrahedra are slightly distorted [mean Cl—O distance 1.43 (2) Å, angular range 103.5 (4)–114.6 (4)°] and isolated from each other. The local environment around the Ca2+ cation is presented in Fig. 3. It is coordinated by eight isolated ClO4− tetrahedra with an apex oxygen atom of each tetrahedron bonded to the Ca2+ cation. The resulting coordination sphere can be considered as a distorted square antiprism. The average Ca—O distance is 2.476 Å (Table 1), which is intermediate between those of comparable Mg—O (2.098 Å) and Ba—O (2.989 Å) polyhedra (Lee et al., 2015; Lim et al., 2011), and consistent with the sum of the ionic radii of the alkaline earth metals and oxygen (Shannon, 1976). The of the Mg2+, Ca2+, and Ba2+ cations in the anhydrous perchlorates increases from 6, 8, and to 12, respectively.
of anhydrous calcium perchlorate, Ca(ClO3. Synthesis and crystallization
In order to prepare calcium perchlorate anhydrate, Ca(ClO4)2·xH2O (reagent grade, Alfa Aesar) was placed in 75 ml glass vials. The vials were placed into a box furnace, heated at 623 K for 12 h with a heating rate of 3 K min−1, cooled down to 423 K, and transferred to a under an Ar atmosphere. The exposed time in a normal atmosphere during the transfer was about 10 s. The sample was ground using an agate mortar, and placed in a dome-type PXRD sample holder that was sealed tightly to prevent atmospheric exposure during the data collection.
4. details
Crystal data, data collection and structure . The powder XRD data of anhydrous calcium perchlorate were collected using a Bragg–Brentano diffractometer (PANalytical Empyrean) with Cu Kα1 radiation (λ = 1.5406 Å) at 40 kV and 30 mA, using a graphite monochromator and a Pixcel3D 2×2 detector. X-ray intensities were measured for 12 h at 0.013° intervals in the angular range of 5° ≤ 2θ ≤ 140°. X-ray diffraction data were indexed by the TREOR90 algorithm (Werner, 1990) in the CRYSFIRE program suite (Shirley, 2002), with 22 indexed reflections starting from the smallest angle. An orthorhombic was revealed suggesting Pbca as the most probable Based on these results, the process was performed using the GSAS program (Larson & Von Dreele, 2000) and the CRYSTALS program (Betteridge et al., 2003). The process was started with the assumption that there is one dummy atom at an arbitrary position. Then were applied to calculate the initial solution of the using SHELXS97 (Sheldrick, 2008), which yielded a Ca site as a starting postition. The initial model was then replaced with the partial model, and this data was used for a LeBail fit in GSAS. Then, improved structure factors were calculated, which were used for the in CRYSTALS. These processes were repeated until a complete and sufficient structural model converged. Based on these results, the MCE programme (Rohlíček & Hušák, 2007) was used to draw the calculated Fourier-density map in three dimensions. For the final with GSAS, an overall displacement parameter was used, and Cl—O bond lengths were restrained with a tolerance value of 25% from the distances determined from CRYSTALS, where the distances matched well with Shannon's radii sum. Pseudovoigt profile coefficients as parameterized in Thompson et al. (1987), asymmetry correction of Finger et al. (1994) and microstrain broadening of Stephens (1999).
details are summarized in Table 2
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Supporting information
CCDC reference: 1827999
https://doi.org/10.1107/S2056989018003936/wm5437sup1.cif
contains datablock I. DOI:Supporting information file. DOI: https://doi.org/10.1107/S2056989018003936/wm5437Isup2.cml
Data collection: X'Pert Data Collector (PANalytical, 2011); cell
GSAS (Larson & Von Dreele, 2000); data reduction: X'Pert HighScore Plus (PANalytical, 2011); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008) and CRYSTALS (Betteridge et al., 2003); program(s) used to refine structure: GSAS (Larson & Von Dreele, 2000); molecular graphics: ATOMS (Dowty, 2000); software used to prepare material for publication: GSAS (Larson & Von Dreele, 2000).Ca(ClO4)2 | Z = 8 |
Mr = 238.98 | F(000) = 944.0 |
Orthorhombic, Pbca | Dx = 2.680 Mg m−3 |
Hall symbol: -P_2ac_2ab | Cu Kα1 radiation, λ = 1.5405 Å |
a = 13.75102 (8) Å | T = 295 K |
b = 9.50887 (5) Å | white |
c = 9.06168 (5) Å | flat_sheet, 24.9 × 24.9 mm |
V = 1184.88 (1) Å3 | Specimen preparation: Prepared at 295 K |
PANalytical Empyrean diffractometer | Data collection mode: reflection |
Radiation source: sealed X-ray tube, PANalytical Cu Ceramic X-ray tube | Scan method: step |
Specimen mounting: packed powder | 2θmin = 5.001°, 2θmax = 139.993°, 2θstep = 0.013° |
Least-squares matrix: full | Excluded region(s): 5 to 12.5 degrees are excluded due to background scattering at low angles, in addition there are no peaks in this region. |
Rp = 0.068 | Profile function: CW Profile function number 4 with 18 terms Pseudovoigt profile coefficients as parameterized in P. Thompson, D.E. Cox & J.B. Hastings (1987). J. Appl. Cryst.,20,79-83. Asymmetry correction of L.W. Finger, D.E. Cox & A. P. Jephcoat (1994). J. Appl. Cryst.,27,892-900. Microstrain broadening by P.W. Stephens, (1999). J. Appl. Cryst.,32,281-289. #1(GU) = 9.638 #2(GV) = -11.095 #3(GW) = 2.275 #4(GP) = 4.393 #5(LX) = 0.935 #6(ptec) = 0.00 #7(trns) = 0.00 #8(shft) = -4.2154 #9(sfec) = 0.00 #10(S/L) = 0.0005 #11(H/L) = 0.0005 #12(eta) = 0.7500 #13(S400 ) = 0.0E+00 #14(S040 ) = 0.0E+00 #15(S004 ) = 0.0E+00 #16(S220 ) = 0.0E+00 #17(S202 ) = 0.0E+00 #18(S022 ) = 0.0E+00 Peak tails are ignored where the intensity is below 0.0100 times the peak Aniso. broadening axis 0.0 0.0 1.0 |
Rwp = 0.104 | 44 parameters |
Rexp = 0.055 | 0 restraints |
R(F2) = 0.15096 | (Δ/σ)max = 0.04 |
10385 data points | Background function: GSAS Background function number 1 with 36 terms. Shifted Chebyshev function of 1st kind 1: 396.859 2: -606.961 3: 459.581 4: -240.760 5: 60.9683 6: 66.1787 7: -127.055 8: 123.403 9: -80.0454 10: 22.9955 11: 31.6319 12: -68.9521 13: 82.3967 14: -74.9306 15: 52.4628 16: -22.9755 17: -7.07207 18: 29.6007 19: -41.2483 20: 39.7866 21: -28.2300 22: 12.3296 23: 2.74056 24: -14.4441 25: 20.2978 26: -20.5325 27: 15.0728 28: -6.57858 29: -1.96745 30: 7.61710 31: -10.5263 32: 10.4139 33: -6.95249 34: 2.74624 35: 0.930279 36: -1.93129 |
x | y | z | Uiso*/Ueq | ||
Ca1 | 0.39788 (14) | 0.5357 (2) | 0.7164 (2) | 0.0110 (2)* | |
Cl1 | 0.34080 (17) | 0.6066 (3) | 0.3157 (3) | 0.0110 (2)* | |
Cl2 | 0.55928 (18) | 0.7776 (3) | 0.4961 (3) | 0.0110 (2)* | |
O1 | 0.6154 (4) | 0.7025 (6) | 0.3850 (6) | 0.0110 (2)* | |
O2 | 0.3176 (4) | 0.7464 (6) | 0.2773 (6) | 0.0110 (2)* | |
O3 | 0.5240 (4) | 0.6775 (7) | 0.5973 (7) | 0.0110 (2)* | |
O4 | 0.6137 (4) | 0.8834 (6) | 0.5773 (6) | 0.0110 (2)* | |
O5 | 0.4842 (4) | 0.8546 (7) | 0.4199 (6) | 0.0110 (2)* | |
O6 | 0.2815 (4) | 0.5078 (6) | 0.2414 (6) | 0.0110 (2)* | |
O7 | 0.4359 (4) | 0.5744 (6) | 0.2647 (7) | 0.0110 (2)* | |
O8 | 0.3387 (4) | 0.5833 (6) | 0.4708 (7) | 0.0110 (2)* |
Ca1—Cl1 | 3.776 (3) | Cl2—Ca1 | 3.769 (3) |
Ca1—Cl1i | 3.605 (3) | Cl2—Ca1v | 3.808 (3) |
Ca1—Cl1ii | 3.662 (3) | Cl2—Ca1iii | 3.596 (3) |
Ca1—Cl1iii | 3.851 (3) | Cl2—Ca1vii | 3.627 (3) |
Ca1—Cl2 | 3.769 (3) | Cl2—O1 | 1.456 (6) |
Ca1—Cl2i | 3.808 (3) | Cl2—O3 | 1.408 (6) |
Ca1—Cl2iii | 3.596 (3) | Cl2—O4 | 1.453 (6) |
Ca1—Cl2iv | 3.627 (3) | Cl2—O5 | 1.442 (6) |
Ca1—O1iii | 2.451 (6) | O1—Ca1iii | 2.451 (6) |
Ca1—O2i | 2.412 (6) | O1—Cl2 | 1.456 (6) |
Ca1—O3 | 2.448 (6) | O2—Ca1v | 2.412 (6) |
Ca1—O4iv | 2.370 (6) | O2—Cl1 | 1.411 (6) |
Ca1—O5i | 2.429 (6) | O3—Ca1 | 2.448 (6) |
Ca1—O6ii | 2.512 (6) | O3—Cl2 | 1.408 (6) |
Ca1—O7iii | 2.519 (6) | O4—Ca1vii | 2.370 (6) |
Ca1—O8 | 2.413 (6) | O4—Cl2 | 1.453 (6) |
Cl1—Ca1 | 3.776 (3) | O5—Ca1v | 2.429 (6) |
Cl1—Ca1v | 3.605 (3) | O5—Cl2 | 1.442 (6) |
Cl1—Ca1vi | 3.662 (3) | O6—Ca1vi | 2.512 (6) |
Cl1—Ca1iii | 3.851 (3) | O6—Cl1 | 1.414 (6) |
Cl1—O2 | 1.411 (6) | O7—Ca1iii | 2.519 (6) |
Cl1—O6 | 1.414 (6) | O7—Cl1 | 1.421 (6) |
Cl1—O7 | 1.421 (6) | O8—Ca1 | 2.413 (6) |
Cl1—O8 | 1.423 (6) | O8—Cl1 | 1.423 (6) |
O1iii—Ca1—O2i | 147.7 (2) | O6ii—Ca1—O8 | 77.5 (2) |
O1iii—Ca1—O3 | 113.4 (2) | O7iii—Ca1—O8 | 116.53 (2) |
O1iii—Ca1—O5i | 135.9 (2) | O2—Cl1—O6 | 112.2 (4) |
O1iii—Ca1—O6ii | 79.0 (2) | O2—Cl1—O7 | 109.4 (4) |
O1iii—Ca1—O7iii | 73.10 (19) | O2—Cl1—O8 | 112.7 (4) |
O1iii—Ca1—O8 | 78.62 (18) | O6—Cl1—O7 | 103.5 (4) |
O2i—Ca1—O3 | 87.3 (2) | O6—Cl1—O8 | 110.8 (4) |
O2i—Ca1—O5i | 71.4 (2) | O7—Cl1—O8 | 107.8 (4) |
O2i—Ca1—O6ii | 70.80 (19) | O1—Cl2—O3 | 107.6 (4) |
O2i—Ca1—O7iii | 139.2 (2) | O1—Cl2—O4 | 114.6 (4) |
O2i—Ca1—O8 | 84.0 (2) | O1—Cl2—O5 | 107.3 (4) |
O3—Ca1—O5i | 75.6 (2) | O3—Cl2—O4 | 108.4 (4) |
O3—Ca1—O6ii | 145.7 (2) | O3—Cl2—O5 | 114.1 (4) |
O3—Ca1—O7iii | 67.4 (2) | Ca1iii—O1—Cl2 | 132.3 (4) |
O3—Ca1—O8 | 74.3 (2) | Ca1v—O2—Cl1 | 139.7 (4) |
O5i—Ca1—O6ii | 118.8 (2) | Ca1—O3—Cl2 | 154.6 (4) |
O5i—Ca1—O7iii | 71.6 (2) | Ca1v—O5—Cl2 | 158.7 (4) |
O5i—Ca1—O8 | 141.7 (2) | Ca1vi—O6—Cl1 | 135.9 (4) |
O6ii—Ca1—O7iii | 144.7 (2) | Ca1iii—O7—Cl1 | 154.5 (4) |
Symmetry codes: (i) x, −y+3/2, z+1/2; (ii) −x+1/2, −y+1, z+1/2; (iii) −x+1, −y+1, −z+1; (iv) −x+1, y−1/2, −z+3/2; (v) x, −y+3/2, z−1/2; (vi) −x+1/2, −y+1, z−1/2; (vii) −x+1, y+1/2, −z+3/2. |
Funding information
This work was supported by Samsung Research Funding & Incubation Center of Samsung Electronics under Project No. SRFC-MA1601–04.
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