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The structure of the title compound, pentane-1,5-di­ammonium aluminium(III) hydrogen bis(phosphate), (C5H16N2)[AlP2O8H], obtained solvothermally at 473 K, has been determined by single-crystal X-ray diffraction. It consists of one-dimensional [AlP2O8H]2- macroanions, connected to each other by pentane­di­ammonium cations. Contrary to similar compounds with P/Al = 2, the three-dimensional structure is mainly obtained via a network of hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100008532/gs1096sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100008532/gs1096Isup2.hkl
Contains datablock I

CCDC reference: 150759

Computing details top

Data collection: SMART (Siemens, 1996a); cell refinement: SMART; data reduction: SHELXTL96 (Siemens, 1996b); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: DIAMOND (Bergerhoff, 1996); software used to prepare material for publication: SHELXTL.

(I) top
Crystal data top
(C5H16N2)[AlHP2O8]F(000) = 672
Mr = 322.13Dx = 1.621 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.8783 (2) ÅCell parameters from 5007 reflections
b = 10.4689 (1) Åθ = 2.3–29.8°
c = 16.0680 (4) ŵ = 0.43 mm1
β = 95.147 (1)°T = 296 K
V = 1319.90 (5) Å3Parallelepiped, colorless
Z = 40.12 × 0.06 × 0.05 mm
Data collection top
Siemens SMART
diffractometer
3421 independent reflections
Radiation source: fine-focus sealed tube1901 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
ω scansθmax = 29.8°, θmin = 2.3°
Absorption correction: semi-empirical (using intensity measurements)
SADABS (Sheldrick, 1996)
h = 1010
Tmin = 0.844, Tmax = 0.978k = 1413
8939 measured reflectionsl = 219
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.136Calculated w = 1/[σ2(Fo2) + (0.0573P)2 + 3.0698P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
2521 reflectionsΔρmax = 1.36 e Å3
167 parametersΔρmin = 0.60 e Å3
4 restraintsExtinction correction: SHELXL93 (Sheldrick, 1993), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0130 (77)
Special details top

Experimental. 'Blessing, Acta Cryst. (1995) A51 33–38'

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 on F2 for ALL reflections except for 900 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating R-factor-obs 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
P10.55909 (13)0.78402 (9)0.02396 (7)0.0280 (3)
P20.09646 (13)1.05563 (11)0.13485 (6)0.0290 (3)
Al10.24723 (13)0.95928 (11)0.02995 (7)0.0246 (4)
O10.1684 (4)0.9724 (3)0.0667 (2)0.0379 (7)
O20.6564 (4)0.7078 (3)0.0386 (2)0.0373 (7)
H20.71230.75710.06490.056*
O30.0882 (4)0.9116 (3)0.1048 (2)0.0381 (7)
O40.1982 (4)1.1793 (3)0.1459 (2)0.0467 (9)
O50.4005 (4)0.8408 (3)0.0252 (2)0.0435 (8)
O60.5116 (4)0.6993 (3)0.0927 (2)0.0466 (8)
O70.1067 (5)0.9814 (4)0.2149 (2)0.0521 (9)
O80.6701 (4)0.8956 (3)0.0585 (2)0.0398 (8)
N10.5653 (6)0.4525 (4)0.1464 (2)0.0438 (10)
H1A0.49340.40530.11330.066*
H1B0.57040.53090.12540.066*
H1C0.52880.45650.19720.066*
C10.7372 (9)0.3936 (7)0.1518 (5)0.077 (2)
H1D0.78400.40380.09840.092*
H1E0.72580.30280.16180.092*
C20.8618 (10)0.4488 (8)0.2194 (5)0.088 (2)
H2A0.82250.42710.27320.105*
H2B0.97090.40710.21620.105*
C30.8903 (13)0.5913 (9)0.2175 (5)0.110 (3)
H3A0.79120.62900.23950.132*
H3B0.98550.60770.25870.132*
C40.9232 (15)0.6711 (14)0.1428 (8)0.153 (5)
H4A0.85020.64110.09500.184*
H4B0.89170.75870.15340.184*
C51.1025 (11)0.6688 (10)0.1213 (5)0.099 (3)
H5A1.13630.58020.11620.118*
H5B1.10620.70810.06690.118*
N21.2290 (5)0.7318 (4)0.1793 (3)0.0439 (9)
H2C1.33010.72960.15860.066*
H2D1.23570.69160.22830.066*
H2E1.19840.81270.18630.066*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
P10.0276 (5)0.0230 (5)0.0341 (6)0.0016 (4)0.0063 (4)0.0016 (4)
P20.0259 (5)0.0418 (6)0.0193 (5)0.0018 (4)0.0019 (4)0.0034 (4)
Al10.0218 (6)0.0289 (6)0.0233 (6)0.0004 (4)0.0024 (4)0.0027 (4)
O10.041 (2)0.048 (2)0.0262 (15)0.0047 (14)0.0096 (12)0.0020 (13)
O20.036 (2)0.0285 (15)0.049 (2)0.0033 (12)0.0141 (13)0.0019 (13)
O30.0279 (15)0.049 (2)0.037 (2)0.0003 (13)0.0009 (12)0.0117 (13)
O40.042 (2)0.060 (2)0.039 (2)0.019 (2)0.0100 (14)0.016 (2)
O50.036 (2)0.046 (2)0.047 (2)0.0153 (14)0.0034 (14)0.0090 (14)
O60.055 (2)0.032 (2)0.056 (2)0.0010 (14)0.022 (2)0.0116 (14)
O70.060 (2)0.073 (2)0.024 (2)0.015 (2)0.0098 (14)0.0063 (15)
O80.045 (2)0.036 (2)0.038 (2)0.0117 (14)0.0052 (13)0.0015 (13)
N10.067 (3)0.030 (2)0.037 (2)0.006 (2)0.016 (2)0.003 (2)
C10.080 (4)0.070 (4)0.080 (5)0.012 (3)0.000 (4)0.026 (3)
C20.073 (4)0.123 (7)0.067 (4)0.002 (4)0.008 (3)0.005 (4)
C30.097 (6)0.158 (10)0.077 (5)0.056 (6)0.015 (4)0.002 (6)
C40.169 (13)0.130 (10)0.153 (12)0.019 (9)0.024 (10)0.010 (8)
C50.099 (6)0.134 (7)0.063 (4)0.075 (5)0.004 (4)0.007 (4)
N20.041 (2)0.052 (2)0.039 (2)0.002 (2)0.006 (2)0.012 (2)
Geometric parameters (Å, º) top
P1—O61.490 (3)C1—C21.512 (8)
P1—O81.533 (3)C1—H1D0.97
P1—O51.537 (3)C1—H1E0.97
P1—O21.539 (3)C2—C31.509 (9)
P2—O71.499 (3)C2—H2A0.97
P2—O41.525 (3)C2—H2B0.97
P2—O3i1.530 (3)C3—C41.503 (9)
P2—O11.546 (3)C3—H3A0.97
Al1—O51.727 (3)C3—H3B0.97
Al1—O11.729 (3)C4—C51.484 (9)
Al1—O8ii1.731 (3)C4—H4A0.97
Al1—O31.731 (3)C4—H4B0.97
O2—H20.82C5—N21.459 (8)
O3—P2i1.530 (3)C5—H5A0.97
O8—Al1ii1.731 (3)C5—H5B0.97
N1—C11.483 (8)N2—H2C0.89
N1—H1A0.89N2—H2D0.89
N1—H1B0.89N2—H2E0.89
N1—H1C0.89
O6—P1—O8111.0 (2)C2—C1—H1E108.6 (5)
O6—P1—O5111.4 (2)H1D—C1—H1E107.6
O8—P1—O5107.6 (2)C3—C2—C1116.8 (7)
O6—P1—O2110.4 (2)C3—C2—H2A108.1 (5)
O8—P1—O2109.3 (2)C1—C2—H2A108.1 (5)
O5—P1—O2107.1 (2)C3—C2—H2B108.1 (5)
O7—P2—O4110.6 (2)C1—C2—H2B108.1 (4)
O7—P2—O3i111.3 (2)H2A—C2—H2B107.3
O4—P2—O3i108.8 (2)C4—C3—C2127.0 (9)
O7—P2—O1108.7 (2)C4—C3—H3A105.6 (7)
O4—P2—O1109.8 (2)C2—C3—H3A105.6 (5)
O3i—P2—O1107.6 (2)C4—C3—H3B105.6 (6)
O5—Al1—O1108.9 (2)C2—C3—H3B105.6 (5)
O5—Al1—O8ii111.3 (2)H3A—C3—H3B106.1
O1—Al1—O8ii110.0 (2)C5—C4—C3114.4 (9)
O5—Al1—O3106.4 (2)C5—C4—H4A108.7 (7)
O1—Al1—O3110.6 (2)C3—C4—H4A108.7 (7)
O8ii—Al1—O3109.6 (2)C5—C4—H4B108.7 (7)
P2—O1—Al1149.8 (2)C3—C4—H4B108.7 (7)
P1—O2—H2109.47 (12)H4A—C4—H4B107.6
P2i—O3—Al1139.7 (2)N2—C5—C4117.0 (9)
P1—O5—Al1146.4 (2)N2—C5—H5A108.0 (5)
P1—O8—Al1ii142.0 (2)C4—C5—H5A108.0 (7)
C1—N1—H1A109.5 (3)N2—C5—H5B108.0 (4)
C1—N1—H1B109.5 (4)C4—C5—H5B108.0 (6)
H1A—N1—H1B109.5H5A—C5—H5B107.3
C1—N1—H1C109.5 (3)C5—N2—H2C109.5 (4)
H1A—N1—H1C109.5C5—N2—H2D109.5 (4)
H1B—N1—H1C109.5H2C—N2—H2D109.5
N1—C1—C2114.5 (5)C5—N2—H2E109.5 (5)
N1—C1—H1D108.6 (4)H2C—N2—H2E109.5
C2—C1—H1D108.6 (4)H2D—N2—H2E109.5
N1—C1—H1E108.6 (3)
Symmetry codes: (i) x, y+2, z; (ii) x+1, y+2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···O4ii0.821.672.457 (4)159
N1—H1A···O2iii0.892.002.885 (5)177
N1—H1B···O60.891.892.745 (5)162
N1—H1C···O7iv0.891.862.727 (5)163
N2—H2C···O6v0.891.882.750 (5)165
N2—H2D···O4vi0.892.052.869 (5)153
N2—H2E···O7v0.891.982.861 (6)171
Symmetry codes: (ii) x+1, y+2, z; (iii) x+1, y+1, z; (iv) x+1/2, y1/2, z+1/2; (v) x+1, y, z; (vi) x+3/2, y1/2, z+1/2.
 

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