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In the crystal structure of the title salt, C8H12NO+·C6H2N3O7-, the aromatic rings of the anions and cations are stacked alternately to form one-dimensional columns. These columns are linked to each other via hydrogen bonds, making a three-dimensional network.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802007286/bt6141sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802007286/bt6141Isup2.hkl
Contains datablock I

CCDC reference: 185809

Key indicators

  • Single-crystal X-ray study
  • T = 250 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.049
  • wR factor = 0.143
  • Data-to-parameter ratio = 11.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
REFLT_03 From the CIF: _diffrn_reflns_theta_max 75.00 From the CIF: _reflns_number_total 3050 TEST2: Reflns within _diffrn_reflns_theta_max Count of symmetry unique reflns 3217 Completeness (_total/calc) 94.81% Alert C: < 95% complete
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

Solid-state photoreactivities of some donor–acceptor crystals have been investigated by one of the authors (YI) (Ito et al., 1998). The structure of (I) has been determined to study the packing mode of the molecules in the crystal.

The title crystal, (I), consists of ammonium cations and phenolate anions (Fig. 1 and Table 1). The aromatic rings of the anions and cations are stacked alternatively along c to form one-dimensional columns (Fig. 2). The columns are linked with each other by N—H···O and O—H···O hydrogen bonds (Table 2), forming a three-dimensional network.

Experimental top

Crystals of (I) were grown by slow evaporation from an aqueous methanol solution of a mixture of 2-(4-hydroxyphenyl)ethylamine and picric acid (1:1).

Refinement top

The relatively low completeness of data collection (0.948 for θmax = 75°) is a result of the blind region of the low-temperature apparatus. There is a rotational disorder of one of the nitro groups. It was assumed that nitro-O atoms are disordered over two sites, the O7/O8 and O9/O10 atoms, with 50% probabilities each. The hydroxyl and ammonium H atoms were located from difference syntheses and refined isotropically. The O—H bond length is 0.78 (3) Å, and the N—H lengths 0.89 (2)–0.93 (3) Å. The other H atoms were positioned geometrically and fixed with Uiso(H) = 1.2Ueq(parent atom).

Computing details top

Data collection: WinAFC Diffractometer Control Software (Rigaku, 1999); cell refinement: WinAFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPII (Johnson, 1976); software used to prepare material for publication: TEXSAN.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), with displacement ellipsoids at the 50% probability level. The disordered O9/O10 atoms bonded to N14 have been omitted for clarity.
[Figure 2] Fig. 2. The projection of the crystal structure of (I) along c.
(I) top
Crystal data top
C8H12NO+·C6H2N3O7Z = 2
Mr = 366.29F(000) = 380
Triclinic, P1Dx = 1.556 Mg m3
a = 8.9692 (6) ÅCu Kα radiation, λ = 1.5418 Å
b = 12.312 (1) ÅCell parameters from 25 reflections
c = 7.3832 (6) Åθ = 25.4–29.6°
α = 104.391 (6)°µ = 1.13 mm1
β = 96.502 (6)°T = 250 K
γ = 83.654 (6)°Plate, yellow
V = 781.8 (1) Å30.5 × 0.4 × 0.2 mm
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.047
θ–2θ scansθmax = 75.0°, θmin = 2.5°
Absorption correction: integration
(Coppens et al., 1965)
h = 1111
Tmin = 0.626, Tmax = 0.809k = 1515
3422 measured reflectionsl = 90
3050 independent reflections3 standard reflections every 150 reflections
2939 reflections with I > 2σ(I) intensity decay: none
Refinement top
Refinement on F2 w = 1/[σ2(Fo2) + (0.0858P)2 + 0.2511P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.049(Δ/σ)max = 0.001
wR(F2) = 0.143Δρmax = 0.34 e Å3
S = 1.08Δρmin = 0.24 e Å3
3050 reflectionsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
270 parametersExtinction coefficient: 0.020 (2)
H atoms treated by a mixture of independent and constrained refinement
Crystal data top
C8H12NO+·C6H2N3O7γ = 83.654 (6)°
Mr = 366.29V = 781.8 (1) Å3
Triclinic, P1Z = 2
a = 8.9692 (6) ÅCu Kα radiation
b = 12.312 (1) ŵ = 1.13 mm1
c = 7.3832 (6) ÅT = 250 K
α = 104.391 (6)°0.5 × 0.4 × 0.2 mm
β = 96.502 (6)°
Data collection top
Rigaku AFC-7R
diffractometer
2939 reflections with I > 2σ(I)
Absorption correction: integration
(Coppens et al., 1965)
Rint = 0.047
Tmin = 0.626, Tmax = 0.8093 standard reflections every 150 reflections
3422 measured reflections intensity decay: none
3050 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.049270 parameters
wR(F2) = 0.143H atoms treated by a mixture of independent and constrained refinement
S = 1.08Δρmax = 0.34 e Å3
3050 reflectionsΔρmin = 0.24 e Å3
Special details top

Refinement. Refinement was based on F2 against all reflections. The weighted R-factor (wR) and goodness of fit (S) were based on F2, and conventional R-factor (R) was calculated on F, with F set to zero for negative F2. The threshold expression of I > 2σ(I) was used only for calculating R-factor(gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.9168 (1)1.3109 (1)0.5128 (2)0.0544 (4)
O20.3729 (1)0.89420 (9)0.2564 (2)0.0409 (3)
O30.6149 (2)0.7937 (1)0.0780 (2)0.0586 (4)
O40.6160 (2)0.6138 (1)0.0171 (3)0.0743 (5)
O50.1662 (2)0.4609 (1)0.3155 (2)0.0674 (4)
O60.0469 (2)0.5304 (1)0.2084 (2)0.0627 (4)
O70.0798 (9)0.895 (1)0.195 (2)0.077 (3)0.50
O80.0967 (3)1.0013 (2)0.2337 (7)0.077 (1)0.50
O90.095 (1)0.9054 (10)0.159 (1)0.068 (2)0.50
O100.0857 (4)0.9643 (3)0.3591 (6)0.074 (1)0.50
N110.3180 (2)1.0848 (1)0.5540 (2)0.0380 (3)
N120.5501 (2)0.7071 (1)0.0343 (2)0.0443 (4)
N130.0895 (2)0.5334 (1)0.2113 (2)0.0473 (4)
N140.0451 (2)0.9035 (1)0.2023 (2)0.0535 (4)
C150.5876 (2)1.1617 (1)0.3102 (2)0.0423 (4)
C160.7369 (2)1.1865 (1)0.3571 (2)0.0420 (4)
C170.7689 (2)1.2892 (1)0.4755 (2)0.0398 (4)
C180.6534 (2)1.3660 (1)0.5497 (2)0.0427 (4)
C190.5052 (2)1.3396 (1)0.5029 (3)0.0446 (4)
C200.4701 (2)1.2373 (1)0.3827 (2)0.0415 (4)
C210.3076 (2)1.2105 (2)0.3360 (3)0.0512 (4)
C220.2384 (2)1.1864 (1)0.4982 (3)0.0437 (4)
C230.3080 (2)0.8150 (1)0.1459 (2)0.0348 (3)
C240.3867 (2)0.7152 (1)0.0351 (2)0.0359 (3)
C250.3173 (2)0.6250 (1)0.0759 (2)0.0390 (4)
C260.1617 (2)0.6270 (1)0.0888 (2)0.0393 (4)
C270.0751 (2)0.7186 (1)0.0055 (2)0.0389 (4)
C280.1455 (2)0.8096 (1)0.1154 (2)0.0375 (4)
H10.914 (4)1.371 (3)0.579 (5)0.1052 (1)*
H11A0.410 (3)1.099 (2)0.608 (3)0.06100 (8)*
H11B0.320 (2)1.025 (2)0.454 (3)0.04512 (6)*
H11C0.263 (2)1.069 (2)0.642 (3)0.04951 (7)*
H150.56581.09190.22710.0507*
H160.81621.13330.30820.0503*
H180.67551.43610.63180.0512*
H190.42621.39220.55390.0535*
H21A0.25061.27300.30080.0613*
H21B0.30281.14630.23360.0613*
H22A0.24531.24950.60240.0525*
H22B0.13561.17380.46170.0525*
H250.37530.56160.14340.0467*
H270.03160.71910.00520.0466*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0380 (7)0.0483 (8)0.0704 (9)0.0052 (5)0.0008 (6)0.0034 (7)
O20.0396 (6)0.0350 (6)0.0417 (6)0.0063 (4)0.0030 (4)0.0037 (5)
O30.0447 (7)0.0721 (9)0.0493 (7)0.0193 (6)0.0102 (5)0.0124 (6)
O40.0477 (8)0.0597 (9)0.110 (1)0.0138 (7)0.0133 (8)0.0156 (9)
O50.0649 (9)0.0429 (7)0.0745 (10)0.0019 (6)0.0057 (7)0.0220 (7)
O60.0534 (8)0.0525 (8)0.0719 (10)0.0179 (6)0.0052 (7)0.0105 (7)
O70.036 (3)0.071 (4)0.116 (6)0.006 (3)0.042 (4)0.010 (4)
O80.044 (2)0.034 (1)0.132 (3)0.001 (1)0.002 (2)0.015 (2)
O90.044 (3)0.059 (3)0.076 (3)0.003 (2)0.008 (2)0.023 (3)
O100.050 (2)0.062 (2)0.078 (2)0.002 (1)0.001 (2)0.037 (2)
N110.0354 (7)0.0309 (7)0.0425 (7)0.0012 (5)0.0061 (6)0.0013 (6)
N120.0394 (7)0.0531 (9)0.0366 (7)0.0000 (6)0.0041 (5)0.0051 (6)
N130.0507 (9)0.0353 (7)0.0492 (8)0.0074 (6)0.0013 (6)0.0029 (6)
N140.0402 (9)0.0437 (8)0.0605 (10)0.0001 (6)0.0005 (7)0.0144 (7)
C150.0501 (9)0.0327 (8)0.0428 (9)0.0073 (7)0.0002 (7)0.0065 (6)
C160.0461 (9)0.0334 (8)0.0448 (9)0.0012 (6)0.0052 (7)0.0075 (7)
C170.0386 (8)0.0361 (8)0.0442 (9)0.0037 (6)0.0007 (6)0.0099 (7)
C180.0464 (9)0.0325 (8)0.0460 (9)0.0040 (6)0.0031 (7)0.0036 (6)
C190.0429 (9)0.0389 (9)0.0504 (9)0.0019 (7)0.0073 (7)0.0085 (7)
C200.0415 (9)0.0405 (8)0.0441 (9)0.0055 (7)0.0001 (7)0.0141 (7)
C210.0436 (9)0.055 (1)0.057 (1)0.0097 (8)0.0076 (8)0.0193 (9)
C220.0347 (8)0.0347 (8)0.0570 (10)0.0014 (6)0.0044 (7)0.0037 (7)
C230.0395 (8)0.0318 (7)0.0317 (7)0.0049 (6)0.0037 (6)0.0037 (6)
C240.0372 (8)0.0356 (8)0.0327 (7)0.0022 (6)0.0038 (6)0.0044 (6)
C250.0442 (9)0.0327 (8)0.0359 (8)0.0005 (6)0.0051 (6)0.0013 (6)
C260.0460 (9)0.0308 (8)0.0373 (8)0.0074 (6)0.0030 (6)0.0005 (6)
C270.0386 (8)0.0378 (8)0.0379 (8)0.0072 (6)0.0047 (6)0.0023 (6)
C280.0390 (8)0.0323 (8)0.0365 (8)0.0023 (6)0.0056 (6)0.0013 (6)
Geometric parameters (Å, º) top
O1—C171.366 (2)C16—C171.386 (2)
O1—H10.78 (3)C16—H160.950
O2—C231.256 (2)C17—C181.386 (2)
O3—N121.226 (2)C18—C191.388 (3)
O4—N121.223 (2)C18—H180.950
O5—N131.227 (2)C19—C201.393 (2)
O6—N131.231 (2)C19—H190.950
O7—N141.131 (8)C20—C211.513 (3)
O8—N141.296 (4)C21—C221.514 (3)
O9—N141.259 (9)C21—H21A0.950
O10—N141.252 (4)C21—H21B0.950
N11—C221.495 (2)C22—H22A0.950
N11—H11A0.89 (2)C22—H22B0.950
N11—H11B0.90 (2)C23—C241.455 (2)
N11—H11C0.93 (3)C23—C281.456 (2)
N12—C241.458 (2)C24—C251.371 (2)
N13—C261.442 (2)C25—C261.386 (2)
N14—C281.445 (2)C25—H250.950
C15—C161.392 (3)C26—C271.378 (2)
C15—C201.388 (2)C27—C281.379 (2)
C15—H150.950C27—H270.950
C17—O1—H1103 (3)C15—C20—C19118.2 (2)
C22—N11—H11A110 (2)C15—C20—C21121.7 (1)
C22—N11—H11B110 (1)C19—C20—C21120.1 (1)
C22—N11—H11C107 (1)C20—C21—C22113.3 (2)
H11A—N11—H11B112 (2)C20—C21—H21A108.5
H11A—N11—H11C108 (2)C20—C21—H21B108.5
H11B—N11—H11C108 (2)C22—C21—H21A108.5
O3—N12—O4122.8 (2)C22—C21—H21B108.5
O3—N12—C24118.9 (1)H21A—C21—H21B109.5
O4—N12—C24118.2 (1)N11—C22—C21111.2 (1)
O5—N13—O6122.8 (1)N11—C22—H22A109.0
O5—N13—C26118.6 (2)N11—C22—H22B109.0
O6—N13—C26118.6 (1)C21—C22—H22A109.0
O7—N14—O8121.1 (6)C21—C22—H22B109.0
O7—N14—C28120.4 (6)H22A—C22—H22B109.5
O8—N14—C28115.1 (2)O2—C23—C24124.0 (1)
O9—N14—O10115.6 (5)O2—C23—C28124.7 (1)
O9—N14—C28121.0 (5)C24—C23—C28111.3 (1)
O10—N14—C28119.5 (2)N12—C24—C23120.3 (1)
C16—C15—C20121.2 (1)N12—C24—C25115.3 (1)
C16—C15—H15119.4C23—C24—C25124.4 (1)
C20—C15—H15119.4C24—C25—C26119.4 (1)
C15—C16—C17119.5 (1)C24—C25—H25120.3
C15—C16—H16120.2C26—C25—H25120.3
C17—C16—H16120.2N13—C26—C25118.9 (1)
O1—C17—C16117.3 (1)N13—C26—C27119.6 (1)
O1—C17—C18122.4 (1)C25—C26—C27121.4 (1)
C16—C17—C18120.3 (2)C26—C27—C28119.0 (1)
C17—C18—C19119.4 (1)C26—C27—H27120.5
C17—C18—H18120.3C28—C27—H27120.5
C19—C18—H18120.3N14—C28—C23120.6 (1)
C18—C19—C20121.3 (1)N14—C28—C27114.9 (1)
C18—C19—H19119.3C23—C28—C27124.5 (1)
C20—C19—H19119.3
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O5i0.78 (3)2.59 (4)3.022 (2)117 (2)
O1—H1···O6i0.78 (3)2.22 (3)2.988 (2)168 (3)
N11—H11B···O20.90 (2)1.94 (2)2.829 (2)167 (2)
N11—H11A···O2ii0.89 (2)2.08 (2)2.969 (2)170 (2)
N11—H11A···O3ii0.89 (2)2.39 (2)2.791 (2)108 (2)
N11—H11C···O7iii0.93 (3)2.09 (2)2.93 (1)151 (2)
N11—H11B···O80.90 (2)2.42 (2)2.961 (4)118 (2)
N11—H11C···O9iii0.93 (3)2.16 (3)3.05 (1)158 (2)
N11—H11B···O100.90 (2)2.28 (2)2.748 (4)112 (2)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y+2, z+1; (iii) x, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC8H12NO+·C6H2N3O7
Mr366.29
Crystal system, space groupTriclinic, P1
Temperature (K)250
a, b, c (Å)8.9692 (6), 12.312 (1), 7.3832 (6)
α, β, γ (°)104.391 (6), 96.502 (6), 83.654 (6)
V3)781.8 (1)
Z2
Radiation typeCu Kα
µ (mm1)1.13
Crystal size (mm)0.5 × 0.4 × 0.2
Data collection
DiffractometerRigaku AFC-7R
diffractometer
Absorption correctionIntegration
(Coppens et al., 1965)
Tmin, Tmax0.626, 0.809
No. of measured, independent and
observed [I > 2σ(I)] reflections
3422, 3050, 2939
Rint0.047
(sin θ/λ)max1)0.626
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.143, 1.08
No. of reflections3050
No. of parameters270
No. of restraints?
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.34, 0.24

Computer programs: WinAFC Diffractometer Control Software (Rigaku, 1999), WinAFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation, 1999), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEPII (Johnson, 1976), TEXSAN.

Selected bond lengths (Å) top
O1—C171.366 (2)O2—C231.256 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O5i0.78 (3)2.59 (4)3.022 (2)117 (2)
O1—H1···O6i0.78 (3)2.22 (3)2.988 (2)168 (3)
N11—H11B···O20.90 (2)1.94 (2)2.829 (2)167 (2)
N11—H11A···O2ii0.89 (2)2.08 (2)2.969 (2)170 (2)
N11—H11A···O3ii0.89 (2)2.39 (2)2.791 (2)108 (2)
N11—H11C···O7iii0.93 (3)2.09 (2)2.93 (1)151 (2)
N11—H11B···O80.90 (2)2.42 (2)2.961 (4)118 (2)
N11—H11C···O9iii0.93 (3)2.16 (3)3.05 (1)158 (2)
N11—H11B···O100.90 (2)2.28 (2)2.748 (4)112 (2)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y+2, z+1; (iii) x, y+2, z+1.
 

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