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In the ortho­rhom­bic crystalline phase of the title compound, C20H11I2NO2, all the benzene rings are parallel, whereas the acridine systems are either parallel or perpendicular to each other; this generates a herring-bone pattern. The acridine systems and benzene rings are inclined at an angle of 45.5 (1)° to each other, and the acridine systems and carboxyl­ate groups are inclined at an angle of 54.2 (1)°. Oppositely oriented consecutive mol­ecules, with π–π inter­actions between their acridine systems and I...I and I...N contacts, are aligned in stacks along the a axis. These stacks, inter­acting through π–π contacts between benzene rings, are arranged in layers.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805038729/cf2003sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805038729/cf2003Isup2.hkl
Contains datablock I

CCDC reference: 293848

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.038
  • wR factor = 0.095
  • Data-to-parameter ratio = 18.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.92 PLAT213_ALERT_2_C Atom C19 has ADP max/min Ratio ............. 3.30 prolat
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 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 2 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: CrysAlis CCD (Oxford Diffraction, 2003); cell refinement: CrysAlis RED (Oxford Diffraction, 2003); data reduction: CrysAlis RED; 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: SHELXL97 and PLATON (Spek, 2003).

2,5-diiodophenyl acridine-9-carboxylate top
Crystal data top
C20H11I2NO2F(000) = 2080
Mr = 551.10Dx = 2.065 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 15550 reflections
a = 9.297 (3) Åθ = 3.1–27.8°
b = 15.673 (5) ŵ = 3.56 mm1
c = 24.329 (9) ÅT = 100 K
V = 3545 (2) Å3Plate, yellow
Z = 80.50 × 0.40 × 0.08 mm
Data collection top
Kuma KM-4-CCD
diffractometer
4128 independent reflections
Radiation source: fine-focus sealed tube2824 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.063
ω scansθmax = 27.8°, θmin = 3.1°
Absorption correction: analytical
(CrysAlis RED; Oxford Diffraction, 2003)
h = 1211
Tmin = 0.194, Tmax = 0.752k = 2020
24568 measured reflectionsl = 3128
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0484P)2]
where P = (Fo2 + 2Fc2)/3
4128 reflections(Δ/σ)max = 0.001
226 parametersΔρmax = 2.10 e Å3
0 restraintsΔρmin = 0.72 e Å3
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
C10.4245 (4)0.2819 (3)0.3176 (2)0.0255 (11)
H10.41390.29200.35580.031*
C20.3432 (5)0.3252 (3)0.2814 (2)0.0262 (11)
H20.27430.36500.29470.031*
C30.3578 (5)0.3130 (3)0.2240 (2)0.0277 (12)
H30.29940.34470.19940.033*
C40.4541 (5)0.2566 (3)0.2042 (2)0.0257 (11)
H40.46350.24940.16560.031*
C50.8137 (5)0.0440 (3)0.2280 (2)0.0252 (11)
H50.81940.03970.18910.030*
C60.8995 (4)0.0056 (3)0.2602 (2)0.0277 (11)
H60.96430.04470.24360.033*
C70.8932 (5)0.0002 (3)0.3178 (2)0.0278 (12)
H70.95470.03450.33960.033*
C80.8003 (4)0.0549 (3)0.3429 (2)0.0249 (11)
H80.79700.05780.38190.030*
C90.6118 (4)0.1692 (3)0.33342 (19)0.0204 (10)
N100.6349 (3)0.1505 (2)0.21782 (17)0.0230 (9)
C110.5279 (4)0.2201 (3)0.2985 (2)0.0217 (11)
C120.5424 (5)0.2071 (3)0.2406 (2)0.0229 (10)
C130.7072 (5)0.1083 (3)0.3108 (2)0.0237 (10)
C140.7151 (5)0.1028 (3)0.2526 (2)0.0228 (10)
C150.6008 (4)0.1837 (3)0.3937 (2)0.0220 (10)
O160.5719 (3)0.10875 (18)0.42094 (13)0.0212 (7)
O170.6092 (3)0.25119 (19)0.41681 (14)0.0285 (8)
C180.5311 (5)0.1136 (3)0.4762 (2)0.0243 (10)
C190.6310 (5)0.1125 (3)0.5176 (2)0.0260 (11)
C200.5849 (6)0.1054 (3)0.5718 (2)0.0335 (12)
H200.65400.10230.60050.040*
C210.4411 (6)0.1027 (3)0.5843 (2)0.0325 (12)
H210.41180.09690.62160.039*
C220.3381 (6)0.1082 (3)0.5431 (2)0.0318 (12)
H220.23840.10730.55180.038*
C230.3842 (5)0.1152 (3)0.4887 (2)0.0239 (11)
I240.85223 (3)0.11763 (2)0.501604 (16)0.03345 (12)
I250.23482 (3)0.128043 (19)0.424114 (15)0.03119 (11)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.017 (2)0.017 (2)0.042 (3)0.0030 (18)0.006 (2)0.001 (2)
C20.018 (2)0.019 (2)0.041 (3)0.0020 (18)0.001 (2)0.004 (2)
C30.021 (2)0.020 (3)0.042 (3)0.0044 (19)0.005 (2)0.008 (2)
C40.022 (2)0.023 (2)0.032 (3)0.0068 (19)0.001 (2)0.008 (2)
C50.022 (2)0.021 (2)0.032 (3)0.0058 (19)0.001 (2)0.005 (2)
C60.022 (2)0.018 (2)0.044 (3)0.0031 (19)0.005 (2)0.004 (2)
C70.022 (2)0.021 (3)0.040 (3)0.0033 (18)0.000 (2)0.003 (2)
C80.018 (2)0.021 (2)0.036 (3)0.0039 (18)0.000 (2)0.000 (2)
C90.012 (2)0.021 (2)0.027 (3)0.0027 (17)0.0015 (18)0.002 (2)
N100.0155 (18)0.0202 (19)0.033 (2)0.0072 (15)0.0006 (17)0.0040 (18)
C110.014 (2)0.014 (2)0.037 (3)0.0044 (16)0.0020 (19)0.001 (2)
C120.018 (2)0.018 (2)0.033 (3)0.0043 (18)0.001 (2)0.001 (2)
C130.014 (2)0.020 (2)0.037 (3)0.0057 (17)0.000 (2)0.001 (2)
C140.016 (2)0.019 (2)0.033 (3)0.0066 (18)0.006 (2)0.001 (2)
C150.012 (2)0.021 (2)0.033 (3)0.0000 (17)0.0023 (19)0.003 (2)
O160.0197 (15)0.0210 (16)0.0230 (19)0.0020 (12)0.0016 (13)0.0001 (14)
O170.0261 (17)0.0220 (18)0.038 (2)0.0023 (13)0.0003 (15)0.0031 (16)
C180.024 (2)0.017 (2)0.032 (3)0.0038 (18)0.005 (2)0.001 (2)
C190.021 (2)0.026 (3)0.030 (3)0.0019 (18)0.001 (2)0.023 (2)
C200.043 (3)0.027 (3)0.030 (3)0.004 (2)0.002 (2)0.004 (2)
C210.043 (3)0.030 (3)0.025 (3)0.003 (2)0.003 (2)0.010 (2)
C220.032 (3)0.025 (3)0.038 (3)0.000 (2)0.017 (2)0.008 (2)
C230.022 (2)0.018 (2)0.032 (3)0.0008 (17)0.0047 (19)0.006 (2)
I240.02268 (17)0.0368 (2)0.0409 (2)0.00353 (13)0.00691 (14)0.00059 (18)
I250.01820 (16)0.03018 (19)0.0452 (2)0.00071 (12)0.00057 (14)0.00198 (16)
Geometric parameters (Å, º) top
C1—C21.344 (6)C9—C151.488 (6)
C1—C111.441 (6)N10—C121.353 (6)
C1—H10.950N10—C141.354 (6)
C2—C31.416 (7)C11—C121.430 (6)
C2—H20.950C13—C141.420 (7)
C3—C41.347 (6)C15—O161.375 (5)
C3—H30.950C15—O171.200 (5)
C4—C121.435 (6)O16—C181.399 (6)
C4—H40.950C18—C191.370 (7)
C5—C61.362 (7)C18—C231.399 (6)
C5—C141.431 (6)C19—C201.389 (7)
C5—H50.950C19—I242.095 (5)
C6—C71.406 (7)C20—C211.372 (7)
C6—H60.950C20—H200.950
C7—C81.362 (6)C21—C221.390 (7)
C7—H70.950C21—H210.950
C8—C131.435 (6)C22—C231.396 (7)
C8—H80.950C22—H220.950
C9—C111.404 (6)C23—I252.107 (5)
C9—C131.414 (6)
C2—C1—C11120.3 (5)N10—C12—C11123.8 (4)
C2—C1—H1119.9N10—C12—C4117.8 (4)
C11—C1—H1119.9C11—C12—C4118.4 (4)
C1—C2—C3121.5 (5)C9—C13—C14117.5 (4)
C1—C2—H2119.3C9—C13—C8124.1 (5)
C3—C2—H2119.3C14—C13—C8118.4 (4)
C4—C3—C2120.4 (5)N10—C14—C13124.2 (4)
C4—C3—H3119.8N10—C14—C5116.5 (5)
C2—C3—H3119.8C13—C14—C5119.3 (4)
C3—C4—C12121.0 (5)O17—C15—O16122.7 (4)
C3—C4—H4119.5C9—C15—O17126.3 (4)
C12—C4—H4119.5C9—C15—O16111.0 (4)
C6—C5—C14120.1 (5)C15—O16—C18118.0 (3)
C6—C5—H5119.9C19—C18—C23120.1 (5)
C14—C5—H5119.9C19—C18—O16121.5 (4)
C5—C6—C7120.8 (5)C23—C18—O16118.3 (4)
C5—C6—H6119.6C18—C19—C20119.3 (5)
C7—C6—H6119.6C18—C19—I24121.9 (4)
C8—C7—C6120.9 (5)C20—C19—I24118.8 (4)
C8—C7—H7119.5C21—C20—C19120.9 (5)
C6—C7—H7119.5C21—C20—H20119.5
C7—C8—C13120.4 (5)C19—C20—H20119.5
C7—C8—H8119.8C20—C21—C22120.6 (5)
C13—C8—H8119.8C20—C21—H21119.7
C11—C9—C13119.8 (4)C22—C21—H21119.7
C11—C9—C15118.2 (4)C21—C22—C23118.5 (5)
C13—C9—C15122.0 (4)C21—C22—H22120.7
C12—N10—C14117.1 (4)C23—C22—H22120.7
C9—C11—C12117.6 (4)C22—C23—C18120.3 (5)
C9—C11—C1123.9 (5)C22—C23—I25120.8 (4)
C12—C11—C1118.5 (4)C18—C23—I25118.9 (4)
C11—C1—C2—C31.1 (6)C9—C13—C14—N101.6 (6)
C1—C2—C3—C40.4 (7)C8—C13—C14—N10178.9 (4)
C2—C3—C4—C120.7 (6)C9—C13—C14—C5177.9 (4)
C14—C5—C6—C70.3 (7)C8—C13—C14—C50.6 (6)
C5—C6—C7—C80.7 (7)C6—C5—C14—N10179.2 (4)
C6—C7—C8—C130.4 (7)C6—C5—C14—C130.3 (6)
C13—C9—C11—C120.5 (6)C11—C9—C15—O1749.6 (6)
C15—C9—C11—C12178.3 (4)C13—C9—C15—O17128.2 (5)
C13—C9—C11—C1178.0 (4)C11—C9—C15—O16127.4 (4)
C15—C9—C11—C14.2 (6)C13—C9—C15—O1654.8 (5)
C2—C1—C11—C9176.7 (4)O17—C15—O16—C189.2 (6)
C2—C1—C11—C120.7 (6)C9—C15—O16—C18168.0 (3)
C14—N10—C12—C111.5 (6)C15—O16—C18—C1989.1 (5)
C14—N10—C12—C4178.4 (4)C15—O16—C18—C2394.2 (5)
C9—C11—C12—N101.9 (6)C23—C18—C19—C205.6 (7)
C1—C11—C12—N10179.5 (4)O16—C18—C19—C20171.0 (4)
C9—C11—C12—C4178.0 (4)C23—C18—C19—I24176.2 (3)
C1—C11—C12—C40.4 (6)O16—C18—C19—I247.2 (6)
C3—C4—C12—N10178.8 (4)C18—C19—C20—C212.4 (7)
C3—C4—C12—C111.1 (6)I24—C19—C20—C21179.3 (4)
C11—C9—C13—C141.1 (6)C19—C20—C21—C220.9 (7)
C15—C9—C13—C14176.6 (4)C20—C21—C22—C231.0 (7)
C11—C9—C13—C8178.3 (4)C21—C22—C23—C182.2 (6)
C15—C9—C13—C80.5 (7)C21—C22—C23—I25178.0 (3)
C7—C8—C13—C9177.4 (4)C19—C18—C23—C225.6 (7)
C7—C8—C13—C140.2 (6)O16—C18—C23—C22171.2 (4)
C12—N10—C14—C130.3 (6)C19—C18—C23—I25174.6 (3)
C12—N10—C14—C5179.2 (4)O16—C18—C23—I258.7 (5)
Table 2. ππ interactions (Å,°). Cg represents the centroids of the rings, as follows: Cg1 ring C9/C11/C12/N10/C14/C13, Cg2 ring C1/C2/C3/C4/C12/C11, Cg3 ring C5/C6/C7/C8/C13/C14 and Cg4 ring C18/C19/C20/C21/C22/C23 (Fig. 1). top
CgICgJCg···CgDihedral angleInterplanar dist.Offset
12i3.522 (3)3.53.243 (3)1.374 (3)
13ii3.725 (3)2.33.312 (3)1.705 (3)
21ii3.522 (3)3.53.319 (3)1.178 (3)
23ii3.796 (3)2.63.322 (3)1.837 (3)
31i3.725 (2)2.33.290 (3)1.747 (3)
32i3.797 (3)2.63.279 (3)1.915 (3)
44iii3.748 (3)0.03.531 (3)1.257 (3)
Notes: Cg···Cg is the distance between ring centroids. The dihedral angle is that between the planes of the rings CgI and CgJ. The interplanar distance is the perpendicular distance of CgI from ring J. The offset is the perpendicular distance of ring I from ring J. Symmetry codes: (i) 1/2+x, y, 1/2-z; (ii) -1/2+x, y, 1/2-z; (iii) 1-x, -y, 1-z.
I···I and N···I contacts (Å, °) in (I). top
XIJI···JX-I···J
C19I24I25iv4.029 (5)162.8 (2)
C23I25I24v4.029 (5)103.3 (2)
C23I25N10ii3.593 (4)153.7 (2)
Symmetry codes: (ii) x-1/2, y, 1/2-z; (iv) 1+x, y, z; (v) -1+x, y, z.
 

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