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The previously unknown crystal structure of magnesium perchlorate anhydrate, determined and refined from laboratory X-ray powder diffraction data, represents a new structure type. The title compound was obtained by heating magnesium perchlorate hexahydrate at 523 K for 2 h under vacuum and it crystallizes in the monoclinic space group
P2
1/
c. The asymmetric unit contains one Mg (site symmetry
on special position 2
a), one Cl and four O sites (on general positions 4
e). The structure consists of a three-dimensional network resulting from the corner-sharing of MgO
6 octahedra and ClO
4 tetrahedra. Each MgO
6 octahedron share corners with six ClO
4 tetrahedra. Each ClO
4 tetrahedron shares corners with three MgO
6 octahedra, with one O-atom corner dangling. The ClO
4 tetrahedra are oriented in such a way that one-dimensional channels parallel to [100] are formed between the dangling O atoms.
Supporting information
Data collection: COMMANDER (Bruker, 2003); cell refinement: GSAS (Larson & Von Dreele, 2000); data reduction: EVA (Bruker, 2003); 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).
Magnesium bis(perchlorate)
top
Crystal data top
Mg(ClO4)2 | Z = 2 |
Mr = 223.20 | F(000) = 222.58 |
Monoclinic, P21/c | Dx = 2.628 Mg m−3 |
Hall symbol: -P 2ybc | Cu Kα1 radiation, λ = 1.5405 Å |
a = 4.85705 (10) Å | T = 296 K |
b = 8.41719 (16) Å | white |
c = 7.87301 (16) Å | flat_sheet, 20 × 20 mm |
β = 118.7704 (11)° | Specimen preparation: Prepared at 296 K |
V = 282.14 (1) Å3 | |
Data collection top
Bruker D8 Advance diffractometer | Data collection mode: reflection |
Radiation source: sealed X-ray tube, Bruker Cu Ceramic X-ray tube | Scan method: step |
Ge 111 monochromator | 2θmin = 15.0°, 2θmax = 129.989°, 2θstep = 0.017° |
Specimen mounting: packed powder | |
Refinement top
Least-squares matrix: full | Profile function: CW Profile function number 4 with 21 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) = 14.783 #2(GV) = 23.166 #3(GW) = 12.718
#4(GP) = 1.024 #5(LX) = 5.292 #6(ptec) = 0.00
#7(trns) = 0.00 #8(shft) = -1.9997 #9(sfec) = 0.00
#10(S/L) = 0.0517 #11(H/L) = 0.0011 #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
#19(S301 ) = 0.0E+00 #20(S103 ) = 0.0E+00 #21(S121 ) = 0.0E+00
Peak tails are ignored where the intensity is below 0.0010 times the peak
Aniso. broadening axis 0.0 0.0 1.0 |
Rp = 0.102 | 32 parameters |
Rwp = 0.145 | 0 restraints |
Rexp = 0.107 | 0 constraints |
RBragg = 0.087 | Weighting scheme based on measured s.u.'s |
R(F2) = 0.0875 | (Δ/σ)max = 0.04 |
6894 data points | Background function: GSAS Background function number 1 with 18 terms.
Shifted Chebyshev function of 1st kind
1: 48.1453 2: -38.0385 3: 35.2720 4: -29.0981
5: 26.3053 6: -21.8255 7: 18.1473 8: -13.0811
9: 9.91226 10: -7.27175 11: 4.02413 12: -0.768059
13: -0.560606 14: 2.20823 15: -2.95237 16: 3.09518
17: -1.89111 18: 2.06051 |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Mg1 | 0.0 | 0.0 | 0.0 | 0.0144 (10)* | |
Cl1 | 0.3101 (5) | 0.3330 (2) | 0.2442 (3) | 0.0164 (4)* | |
O1 | 0.2717 (10) | 0.1649 (5) | 0.2119 (6) | 0.0131 (12)* | |
O2 | 0.0640 (10) | 0.3853 (5) | 0.2817 (7) | 0.0220 (16)* | |
O3 | 0.6143 (9) | 0.3493 (5) | 0.4192 (6) | 0.0219 (15)* | |
O4 | 0.3005 (10) | 0.4203 (5) | 0.0882 (6) | 0.0184 (15)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
? | ? | ? | ? | ? | ? | ? |
Geometric parameters (Å, º) top
Mg1—Cl1 | 3.322 (2) | Cl1—Mg1vii | 3.281 (2) |
Mg1—Cl1i | 3.350 (2) | Cl1—O1 | 1.434 (4) |
Mg1—Cl1ii | 3.281 (2) | Cl1—O2 | 1.431 (4) |
Mg1—Cl1iii | 3.322 (2) | Cl1—O3 | 1.463 (4) |
Mg1—Cl1iv | 3.281 (2) | Cl1—O4 | 1.412 (5) |
Mg1—Cl1v | 3.350 (2) | O1—Mg1 | 2.081 (4) |
Mg1—O1 | 2.081 (4) | O1—Cl1 | 1.434 (4) |
Mg1—O1iii | 2.081 (4) | O2—Mg1vi | 2.121 (5) |
Mg1—O2i | 2.121 (5) | O2—Cl1 | 1.431 (4) |
Mg1—O2v | 2.121 (5) | O3—Mg1vii | 2.092 (4) |
Mg1—O3ii | 2.092 (4) | O3—Cl1 | 1.463 (4) |
Mg1—O3iv | 2.092 (4) | O4—Cl1 | 1.412 (5) |
Cl1—Mg1 | 3.322 (2) | O4—O4viii | 2.889 (8) |
Cl1—Mg1vi | 3.350 (2) | O4—O4ix | 3.175 (9) |
| | | |
O1—Mg1—O1iii | 180.0 | O2x—Mg1—O3ii | 93.63 (16) |
O1—Mg1—O2i | 86.43 (16) | O2x—Mg1—O3xi | 86.37 (16) |
O1—Mg1—O2x | 93.57 (16) | O3ii—Mg1—O3xi | 180.0 |
O1—Mg1—O3ii | 91.78 (17) | O1—Cl1—O2 | 106.9 (3) |
O1—Mg1—O3xi | 88.22 (17) | O1—Cl1—O3 | 104.2 (3) |
O1iii—Mg1—O2i | 93.57 (16) | O1—Cl1—O4 | 114.3 (3) |
O1iii—Mg1—O2x | 86.43 (16) | O2—Cl1—O3 | 110.0 (3) |
O1iii—Mg1—O3ii | 88.22 (17) | O2—Cl1—O4 | 109.8 (3) |
O1iii—Mg1—O3xi | 91.78 (17) | O3—Cl1—O4 | 111.5 (3) |
O2i—Mg1—O2x | 179.9657 | Mg1—O1—Cl1 | 141.1 (3) |
O2i—Mg1—O3ii | 86.37 (16) | Mg1vi—O2—Cl1 | 140.3 (3) |
O2i—Mg1—O3xi | 93.63 (16) | Mg1vii—O3—Cl1 | 133.9 (3) |
Symmetry codes: (i) −x, y−1/2, −z+1/2; (ii) −x+1, y−1/2, −z+1/2; (iii) −x, −y, −z; (iv) x−1, −y+1/2, z−1/2; (v) x, −y+1/2, z−1/2; (vi) −x, y+1/2, −z+1/2; (vii) −x+1, y+1/2, −z+1/2; (viii) −x, −y+1, −z; (ix) −x+1, −y+1, −z; (x) x, −y+3/2, z+1/2; (xi) x−1, −y+3/2, z+1/2. |
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