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Crystals of commercial iodic(V) acid, HIO3, were investigated using single-crystal and powder X-ray diffraction. The crystals turned out to be HI3O8 or HIO3·I2O5 [iodic acid-diiodine penta­oxide (1/1)] instead, whose structure has been determined previously [Feikema & Vos (1966). Acta Cryst. 20, 769-777]. Redetermination of the structure gave higher precision and allowed the location of the H atom.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805037037/wm6113sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805037037/wm6113Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 299 K
  • Mean [sigma](I-O) = 0.002 Å
  • R factor = 0.020
  • wR factor = 0.044
  • Data-to-parameter ratio = 18.9

checkCIF/PLATON results

No syntax errors found



Alert level A PLAT431_ALERT_2_A Short Inter HL..A Contact I1 .. O7 .. 2.58 Ang. PLAT431_ALERT_2_A Short Inter HL..A Contact I1 .. O8 .. 2.64 Ang. PLAT431_ALERT_2_A Short Inter HL..A Contact I2 .. O8 .. 2.57 Ang. PLAT431_ALERT_2_A Short Inter HL..A Contact I3 .. O3 .. 2.55 Ang. PLAT431_ALERT_2_A Short Inter HL..A Contact I3 .. O4 .. 2.59 Ang.
Alert level B PLAT430_ALERT_2_B Short Inter D...A Contact O4 .. O7 .. 2.84 Ang. PLAT430_ALERT_2_B Short Inter D...A Contact O5 .. O8 .. 2.78 Ang.
Alert level C PLAT431_ALERT_2_C Short Inter HL..A Contact I3 .. O1 .. 3.37 Ang.
5 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 8 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: COLLECT (Nonius, 1999); cell refinement: DIRAX/LSQ (Duisenberg et al., 2003); data reduction: EVALCCD (Duisenberg, 1992); program(s) used to solve structure: coordinates taken from previous determination; program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2005); software used to prepare material for publication: maXus (Mackay et al., 1999).

Iodic acid–diiodine pentaoxide (1/1) top
Crystal data top
HIO3·I2O5F(000) = 896
Mr = 509.71Dx = 5.120 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 108 reflections
a = 7.5529 (4) Åθ = 5.6–23.0°
b = 7.6961 (4) ŵ = 14.18 mm1
c = 11.3787 (5) ÅT = 299 K
β = 90.178 (4)°Fragment, colourless
V = 661.42 (6) Å30.23 × 0.17 × 0.16 mm
Z = 4
Data collection top
Nonius KappaCCD area-detector
diffractometer
1847 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.042
φ and ω scansθmax = 30.0°, θmin = 5.2°
Absorption correction: numerical
(HABITUS; Herrendorf & Bärnighausen, 1997)
h = 1010
Tmin = 0.189, Tmax = 0.355k = 1010
12999 measured reflectionsl = 1516
1913 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.020 w = 1/[σ2(Fo2) + (0.0157P)2 + 1.6864P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.044(Δ/σ)max = 0.001
S = 1.27Δρmax = 0.78 e Å3
1913 reflectionsΔρmin = 1.49 e Å3
101 parametersExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0185 (4)
Primary atom site location: structure-invariant direct methods
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
I10.24144 (3)0.22767 (3)0.095268 (19)0.00977 (7)
I20.33769 (3)0.73614 (3)0.103605 (19)0.00941 (7)
I30.75579 (3)0.04724 (3)0.191590 (19)0.01001 (7)
O10.4572 (3)0.3010 (4)0.0539 (2)0.0162 (5)
O20.1298 (4)0.4313 (4)0.0870 (3)0.0162 (5)
O30.1711 (3)0.8224 (4)0.0080 (2)0.0154 (5)
O40.4408 (4)0.9407 (4)0.1359 (3)0.0154 (5)
O50.1833 (3)0.7451 (4)0.2407 (2)0.0125 (5)
O60.7837 (4)0.4546 (4)0.1579 (3)0.0174 (6)
O70.8028 (4)0.8423 (4)0.1242 (2)0.0165 (5)
O80.9774 (3)0.1143 (4)0.2253 (2)0.0153 (5)
H60.87310.46530.12130.021*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.00976 (11)0.01153 (12)0.00803 (11)0.00084 (7)0.00119 (8)0.00027 (7)
I20.01121 (11)0.00968 (12)0.00734 (11)0.00024 (7)0.00018 (8)0.00038 (7)
I30.00851 (11)0.01091 (12)0.01060 (11)0.00110 (7)0.00052 (7)0.00053 (7)
O10.0124 (12)0.0228 (14)0.0134 (12)0.0058 (11)0.0054 (10)0.0027 (11)
O20.0171 (12)0.0124 (13)0.0191 (13)0.0036 (10)0.0014 (10)0.0019 (10)
O30.0147 (12)0.0217 (14)0.0098 (11)0.0032 (10)0.0022 (9)0.0049 (10)
O40.0138 (12)0.0119 (13)0.0203 (13)0.0036 (9)0.0017 (10)0.0019 (10)
O50.0111 (12)0.0190 (14)0.0076 (12)0.0016 (9)0.0012 (10)0.0007 (9)
O60.0170 (13)0.0220 (15)0.0133 (12)0.0013 (10)0.0032 (10)0.0049 (10)
O70.0197 (13)0.0124 (13)0.0175 (13)0.0020 (10)0.0005 (10)0.0052 (10)
O80.0108 (11)0.0207 (14)0.0145 (12)0.0042 (10)0.0028 (9)0.0010 (10)
Geometric parameters (Å, º) top
I1—O21.782 (3)I2—O1ii2.390 (2)
I1—O11.789 (3)I2—O8v2.569 (3)
I1—O5i1.953 (3)I2—O22.829 (3)
I1—O7ii2.575 (2)I3—O7iv1.790 (3)
I1—O8iii2.636 (2)I3—O81.792 (3)
I1—O4iv2.712 (3)I3—O6vi1.880 (3)
I2—O31.788 (3)I3—O3ii2.545 (3)
I2—O41.794 (3)I3—O4iv2.593 (3)
I2—O51.952 (2)O6—H60.7988
O2—I1—O198.06 (14)O5—I2—O1ii173.70 (11)
O2—I1—O5i97.27 (12)O7iv—I3—O899.15 (13)
O1—I1—O5i88.11 (12)O7iv—I3—O6vi95.06 (13)
O3—I2—O495.92 (13)O8—I3—O6vi93.75 (12)
O3—I2—O592.96 (11)I1—O1—I2ii138.85 (15)
O4—I2—O593.76 (12)I2—O5—I1vii126.02 (14)
O3—I2—O1ii92.58 (11)I3v—O6—H6124.9
O4—I2—O1ii88.64 (11)
Symmetry codes: (i) x+1/2, y1/2, z+1/2; (ii) x+1, y+1, z; (iii) x1, y, z; (iv) x, y1, z; (v) x+3/2, y+1/2, z+1/2; (vi) x+3/2, y1/2, z+1/2; (vii) x+1/2, y+1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O6—H6···O2viii0.802.002.744 (4)156
Symmetry code: (viii) x+1, y, z.
 

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