research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

Crystal structures of the di­methyl sulfoxide solvate of 3,6-bis­­(indol-3-yl)-1,4-di­methyl­piperazine-2,5-dione and of the di­methyl sulfoxide and tetra­hydro­furan solvates of 1,4-di­methyl-3,6-bis­­(2-methyl­indol-3-yl)piperazine-2,5-dione

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aDepartment of Biochemistry, Chemistry and Physics, Georgia Southern University, Armstrong Campus, 11935 Abercorn Street Savannah GA 31419, USA, bCenter for Advanced Materials Science, Department of Biochemistry, Chemistry and Physics, Georgia Southern University, 11935 Abercorn Street, Savannah, GA 31419, USA, and cDepartment of Biochemistry, Chemistry and Physics, Georgia Southern University, Statesboro Campus, 1332 Southern Drive Statesboro, GA 30458, USA
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 23 September 2025; accepted 20 October 2025; online 28 October 2025)

The syntheses and structures of the dimethyl sulfoxide (DMSO) solvate of 3,6-bis­(indol-3-yl)-1,4-di­methyl­piperazine-2,5-dione, C11H10N2O (I), and of the dimethyl sulfoxide and tetra­hydro­furan (THF) solvates of 1,4-dimethyl-3,6-bis­(2-methyl­indol-3-yl)piperazine-2,5-dione, C12H12N2O, (II) and (III), respectively, are reported. The asymmetric units of (I) and (II) each contain two crystallographically independent half-mol­ecules that are completed by inversion symmetry, whereas (III) contains one independent half-mol­ecule. In all three structures, the piperazine-2,5-dione core is essentially planar and the overall mol­ecular non-planarity arises from rotations of the indole substituents: ranging between 58 and 63° in (I), approximately 72° for both independent mol­ecules in (II) and approximately 62° in (III). In the crystal of (I), mol­ecules are linked by two N—H⋯O hydrogen bonds to form C(18) chains; (II) features a single N—H⋯O contact giving C(8) chains; and (III) exhibits N—H⋯O inter­actions that generate C(7) chains assembling into sheets lying parallel to (100). No significant ππ stacking is present in any of these structures. All three structures contain regions of disordered solvent (DMSO or THF) that were treated with a solvent mask during refinement.

1. Chemical context

The bis­indolyl piperazine-2,5-dione motif has attracted considerable inter­est as a precursor to the dragmacidin family of marine natural products (Garg et al., 2002View full citation). These alkaloids, isolated from deep-sea sponges and tunicates, are distinguished by a piperazine core bearing indole units at the 3- and 6-positions (Kawasaki et al., 2002View full citation, 2003View full citation). Members of the dragmacidin series have been reported to display anti­cancer, anti­viral, anti-inflammatory and anti­bacterial activity (Cutignano et al., 2000View full citation; Feldman & Ngernmeesri, 2011View full citation; Morris & Andersen, 1990View full citation; Wright et al., 1992View full citation). Notably, dragmacidin, the first reported member, exhibits in vitro cytotoxic activity in A-549 (human lung), HCT-8 (human colon), P388 (murine leukemia) and MDA-MB (human mammary) cell lines (Kohmoto et al., 1988View full citation).

3,6-Bis(indol-3-yl)-1,4-di­methyl­piperazine-2,5-dione and 1,4-dimethyl-3,6-bis­(2-methyl­indol-3-yl)piperazine-2,5-dione were prepared during efforts to access new dragmacidin derivatives (Crooke & Whitlock, 2012View full citation). In addition to a one-pot route, a reproducible two-step procedure was used: sarcosine anhydride was brominated, and the resulting precipitate was reacted with the appropriate indole in di­methyl­formamide (DMF) to afford the bis­indolyl products. As part of our work in this area, we now describe the syntheses and structures of the title compounds, each of which contain disordered solvent regions.

[Scheme 1]

2. Structural commentary

Compound (I) crystallizes in the monoclinic space group C2/c and its mol­ecular structure is shown in Fig. 1[link]. The asymmetric unit contains two independent mol­ecular halves with each complete C22H20N4O2 mol­ecule generated by crystallographic inversion symmetry. Each indole ring shows an r.m.s. deviation of 0.004 Å. The indole ring containing N1 is rotated by 57.9 (2)° (C10—C9—C7—C6) relative to the piperazine-2,5-dione ring (r.m.s. deviation = 0.037 Å). Similarly, the indole ring containing N3 is rotated by 63.3 (3)° (C21—C20—C18—C17) relative to the piperazine-2,5-dione ring (r.m.s. deviation = 0.072 Å). These rotations are the principal contributors to the overall nonplanarity of the mol­ecule. The carbonyl C=O distances are normal at 1.234 (2) Å for C10=O1 and 1.230 (4) Å for C21=O2.

[Figure 1]
Figure 1
The mol­ecular structure of (I) with displacement ellipsoids drawn at the 50% probability level. The unlabelled atoms in the C1 mol­ecule are generated by the symmetry operation −x + Mathematical equation, −y + Mathematical equation, −z + 1 and those in the C12 mol­ecule by −x + 1, −y, −z + 1.

The mol­ecular structure of compound (II) (triclinic, space group PMathematical equation) is shown in Fig. 2[link]. The asymmetric unit also contains two independent mol­ecular halves completed by inversion symmetry to form C24H24N4O2 mol­ecules. The indole rings show r.m.s. deviations of 0.019 and 0.021 Å for the rings containing N1 and N3, respectively. The indole ring containing N1 is rotated by 71.4 (2)° (C10—C9—C7—C6) relative to the piperazine-2,5-dione ring (r.m.s. deviation = 0.037 Å). Similarly, the indole ring containing N3 is rotated by −72.7 (3)° (C22—C21—C19—C18) relative to the piperazine-2,5-dione ring (r.m.s. deviation = 0.046 Å). These rotations are the principal contributors to the overall nonplanarity of the mol­ecule. The carbonyl C=O distances are 1.232 (3) Å (C10=O1) and 1.226 (3) Å (C22=O2).

[Figure 2]
Figure 2
The mol­ecular structure of (II) with displacement ellipsoids drawn at the 50% probability level. The unlabelled atoms in the C1 mol­ecule are generated by the symmetry operation −x + 2, −y + 1, −z + 1 and those in the C13 mol­ecule by −x, −y, −z.

Compound (III) crystallizes in the monoclinic space group P21/c and its mol­ecular structure is shown in Fig. 3[link]. The asymmetric unit contains a half mol­ecule, which is completed by inversion symmetry to generate a C24H24N4O2 mol­ecule. The indole ring shows an r.m.s. deviation of 0.010 Å. The indole ring is rotated by −62.4 (3)° (C1—C2—C3—C4) relative to the piperazine-2,5-dione ring (r.m.s. deviation = 0.031 Å) and the carbonyl C1=O1 distance is 1.231 (2) Å.

[Figure 3]
Figure 3
The mol­ecular structure of (III) with displacement ellipsoids drawn at the 50% probability level. The unlabelled atoms are generated by the symmetry operation –x + 1, –y + 1, –z + 1.

All three structures contain disordered solvent regions that were masked (see Refinement).

3. Supra­molecular features

In the crystal of (I), the mol­ecules are linked by two N—H⋯O hydrogen bonds (Table 1[link], Fig. 4[link]): N1—H1⋯O2, which generates chains parallel to [1Mathematical equation0] with graph-set motif C22(18), and N3—H3⋯O1, forming chains along [130] with graph-set motif C22(18). Together, the hydrogen bonds generate (001) sheets. No significant aromatic ππ stacking is observed.

Table 1
Hydrogen-bond geometry (Å, °) for (I)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O2i 0.89 (3) 2.10 (3) 2.828 (2) 138 (2)
N3—H3A⋯O1 0.95 (3) 1.86 (3) 2.730 (2) 151 (3)
Symmetry code: (i) Mathematical equation.
[Figure 4]
Figure 4
A view along the b-axis direction of the crystal packing of (I) with close contacts shown as red dashed lines.

In the crystal of (II), mol­ecules are linked by an N1—H1⋯O2 hydrogen bond (Table 2[link], Fig. 5[link]), which generates chains running parallel to [100] with graph-set motif C11(8). The second mol­ecule (containing N3) is not involved in hydrogen bonding. No significant ππ stacking is observed.

Table 2
Hydrogen-bond geometry (Å, °) for (II)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O1i 0.85 (3) 2.11 (3) 2.950 (2) 168 (3)
Symmetry code: (i) Mathematical equation.
[Figure 5]
Figure 5
A view along the c-axis direction of the crystal packing of (II) with close contacts shown as red dashed lines.

In the crystal of (III), mol­ecules are linked by an N2—H2⋯O1 hydrogen bond (Table 3[link], Fig. 6[link]), which generates chains of N—H⋯O hydrogen bonds [graph-set motif C11(7)] that form sheets parallel to the (100) plane. No significant ππ stacking is observed.

Table 3
Hydrogen-bond geometry (Å, °) for (III)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H2⋯O1i 0.91 (3) 1.89 (3) 2.787 (2) 168 (3)
Symmetry code: (i) Mathematical equation.
[Figure 6]
Figure 6
A view along the a-axis direction of the crystal packing of (III) with close contacts shown as red dashed lines.

4. Database survey

A search of the Cambridge Structural Database ((CSD; website, accessed on August, 2025; Groom et al., 2016View full citation) for 1,4-dimethyl-3,6-dioxopiperazine (diketopiperazine) frameworks bearing 2,6-substitution returned 13 structures. Seven entries feature simple alkyl groups; methyl (CSD refcode RMNALA10; Benedetti et al., 1976View full citation) and isopropyl (NMLVAL10; Benedetti et al., 1976View full citation), a mixed meth­yl/isopropyl pair (MOJTUB; Wang et al., 2008View full citation), and 1,1,1-tri­fluoro­isopropyl (LAKGAF; Su et al., 1993View full citation). Five entries carry benzylic/aromatic groups, including benzyl (NMLPHE11; Ge et al., 2019View full citation) and (4-hy­droxy­phen­yl)methyl (NIPBIB; Croft et al., 2004View full citation). One structure bears a carboxyl­ate protecting group, tert-but­oxy­carbonyl (EZESIO; Yang, 2021View full citation).

5. Synthesis and crystallization

To prepare compound (I), 0.0117 g of 3,6-bis­(indol-3-yl)-1,4-di­methyl­piperazine-2,5-dione (Miles & Whitlock, 2009View full citation) were dissolved in ∼10 ml of di­methyl­sulfoxide (DMSO) and heated to ∼423 K in a 50 ml beaker. The beaker was placed in a fume hood to allow slow evaporation for approximately 1 week, after which X-ray quality crystals began to form.

Compound (II): a 0.0079-g sample of 1,4-dimethyl-3,6-bis­(2-methyl­indol-3-yl)piperazine-2,5-dione (Miles & Whitlock, 2009View full citation) was dissolved in ∼5 ml of DMSO and heated to near boiling (∼423 K) in a 50 ml beaker. The beaker was placed in a fume hood to allow slow evaporation for approximately 1 week, after which X-ray quality crystals began to form.

Compound (III) was prepared by the same procedure as (II) except that 0.050 g of 1,4-dimethyl-3,6-bis­(2-methyl­indol-3-yl)piperazine-2,5-dione (0.05 g) (Miles & Whitlock, 2009View full citation) was dissolved in ∼50 ml of tetra­hydro­furan (THF) in a 100 ml beaker. The solution was allowed to slowly evaporate for approximately 1 week, after which X-ray quality crystals began to form.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 4[link]. In all three structures, disordered solvent regions were treated using the built-in solvent-mask routine in OLEX2. Solvent-accessible voids were located in each unit cell with the following characteristics: for compound (I), a total cavity volume of 520 Å3 per unit cell containing 172 electrons (consistent with one C2H6OS mol­ecule per asymmetric unit, 168 electrons per cell); for compound (II), a 312 Å3 void with 85 electrons (one C2H6OS per asymmetric unit, 84 electrons per cell); and for compound (III), a 404 Å3 cavity holding 90 electrons (one C4H8O per asymmetric unit, 80 electrons per cell). All disordered solvent electron density was subsequently removed via the solvent-mask procedure.

Table 4
Experimental details

  (I) (II) (III)
Crystal data
Chemical formula C22H20N4O2·0.5C2H6OS C24H24N4O2·C2H6SO C24H24N4O2·C4H8O
Mr 411.48 478.60 472.57
Crystal system, space group Monoclinic, C2/c Triclinic, PMathematical equation Monoclinic, P21/c
Temperature (K) 100 298 293
a, b, c (Å) 31.2994 (4), 7.3881 (1), 17.9817 (2) 9.3137 (2), 12.3332 (2), 12.3873 (2) 8.5276 (9), 8.9357 (7), 17.4883 (13)
α, β, γ (°) 90, 102.023 (1), 90 117.110 (2), 93.520 (1), 97.399 (2) 90, 96.731 (8), 90
V3) 4066.93 (9) 1244.35 (4) 1323.4 (2)
Z 8 2 2
Radiation type Cu Kα Cu Kα Mo Kα
μ (mm−1) 1.18 1.44 0.08
Crystal size (mm) 0.10 × 0.06 × 0.04 0.36 × 0.11 × 0.07 0.4 × 0.4 × 0.3
 
Data collection
Diffractometer XtaLAB Synergy, Single source at home/near, HyPix3000 XtaLAB Synergy, Single source at home/near, HyPix3000 XtaLAB Mini (ROW)
Absorption correction Gaussian (CrysAlis PRO; Rigaku OD, 2023View full citation) Multi-scan (CrysAlis PRO; Rigaku OD, 2023View full citation) Multi-scan (CrysAlis PRO; Rigaku OD, 2023View full citation)
Tmin, Tmax 0.927, 1.000 0.436, 1.000 0.968, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 12151, 3716, 3134 25135, 4560, 4029 6423, 2420, 1519
Rint 0.027 0.039 0.031
(sin θ/λ)max−1) 0.602 0.602 0.602
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.046, 0.120, 1.05 0.058, 0.177, 1.06 0.053, 0.178, 1.02
No. of reflections 3716 4560 2420
No. of parameters 263 283 143
H-atom treatment H atoms treated by a mixture of independent and constrained refinement H atoms treated by a mixture of independent and constrained refinement H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.21, −0.36 0.60, −0.21 0.26, −0.15
Computer programs: CrysAlis PRO (Rigaku OD, 2023View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2018/3 (Sheldrick, 2015bView full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

3,6-Bis(indol-3-yl)-1,4-dimethylpiperazine-2,5-dione dimethyl sulfoxide hemihydrate (I) top
Crystal data top
C22H20N4O2·0.5C2H6OSF(000) = 1736
Mr = 411.48Dx = 1.344 Mg m3
Monoclinic, C2/cCu Kα radiation, λ = 1.54184 Å
a = 31.2994 (4) ÅCell parameters from 6717 reflections
b = 7.3881 (1) Åθ = 2.9–69.6°
c = 17.9817 (2) ŵ = 1.18 mm1
β = 102.023 (1)°T = 100 K
V = 4066.93 (9) Å3Block, clear colourless
Z = 80.10 × 0.06 × 0.04 mm
Data collection top
XtaLAB Synergy, Single source at home/near, HyPix3000
diffractometer
3716 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source3134 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.027
Detector resolution: 10.0000 pixels mm-1θmax = 68.3°, θmin = 2.9°
ω scansh = 3737
Absorption correction: gaussian
(CrysAlisPro; Rigaku OD, 2023)
k = 88
Tmin = 0.927, Tmax = 1.000l = 2119
12151 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.046H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.120 w = 1/[σ2(Fo2) + (0.0451P)2 + 5.8441P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
3716 reflectionsΔρmax = 0.21 e Å3
263 parametersΔρmin = 0.36 e Å3
0 restraints
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.69198 (5)0.5128 (2)0.42587 (8)0.0444 (4)
N20.76249 (5)0.5922 (2)0.46638 (8)0.0308 (4)
N10.87085 (5)0.8346 (3)0.37106 (9)0.0344 (4)
O20.53832 (5)0.2656 (3)0.59204 (13)0.0703 (6)
C60.80197 (6)0.9116 (2)0.37659 (9)0.0220 (4)
N30.61216 (6)0.3788 (3)0.43637 (13)0.0474 (5)
N40.53359 (5)0.0338 (3)0.56374 (12)0.0489 (5)
C10.83537 (6)0.9333 (3)0.33524 (10)0.0264 (4)
C50.76208 (6)1.0008 (2)0.35093 (9)0.0250 (4)
H50.7391300.9891270.3778370.030*
C70.81931 (6)0.7946 (3)0.43927 (9)0.0258 (4)
C90.79628 (6)0.7240 (3)0.49886 (10)0.0296 (4)
H90.8185330.6583160.5374300.035*
C100.71973 (7)0.6176 (3)0.46083 (10)0.0314 (4)
C40.75654 (6)1.1058 (3)0.28604 (10)0.0299 (4)
H40.7296781.1672590.2684470.036*
C160.56976 (6)0.0656 (3)0.39021 (11)0.0303 (4)
H160.5468530.1379520.4015550.036*
C80.86087 (6)0.7530 (3)0.43377 (10)0.0329 (4)
H80.8802000.6782460.4684200.040*
C30.79030 (7)1.1224 (3)0.24595 (10)0.0325 (4)
H30.7856031.1939380.2010930.039*
C170.57703 (6)0.1098 (3)0.42017 (12)0.0334 (4)
C150.59634 (6)0.1316 (3)0.34402 (11)0.0315 (4)
H150.5917170.2507340.3240460.038*
C20.82979 (6)1.0385 (3)0.26952 (10)0.0315 (4)
H20.8525231.0514940.2421830.038*
C140.63015 (6)0.0256 (3)0.32604 (11)0.0324 (4)
H140.6476790.0740180.2935960.039*
C120.61152 (6)0.2127 (3)0.40155 (12)0.0346 (5)
C130.63833 (6)0.1467 (3)0.35452 (11)0.0338 (4)
H130.6612860.2179650.3426680.041*
C110.77761 (8)0.4289 (3)0.43354 (12)0.0408 (5)
H11A0.7835410.4572430.3834220.061*
H11B0.7550100.3351990.4282750.061*
H11C0.8044090.3848380.4669720.061*
C180.55721 (6)0.2240 (3)0.46845 (14)0.0447 (6)
C210.52059 (7)0.1388 (4)0.55313 (16)0.0543 (7)
C200.52044 (7)0.1779 (4)0.50718 (15)0.0515 (7)
H200.5143820.2883440.5354250.062*
C190.57983 (7)0.3831 (3)0.47672 (16)0.0540 (7)
H190.5738920.4826840.5064050.065*
C220.56984 (7)0.0801 (4)0.62727 (16)0.0614 (8)
H22A0.5704090.0055830.6690880.092*
H22B0.5656940.2030790.6448820.092*
H22C0.5975360.0734260.6101210.092*
H10.8970 (9)0.837 (4)0.3587 (14)0.054 (7)*
H3A0.6357 (10)0.461 (4)0.4377 (17)0.076 (9)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0531 (9)0.0501 (9)0.0362 (7)0.0279 (8)0.0232 (7)0.0200 (7)
N20.0444 (10)0.0248 (8)0.0255 (8)0.0095 (7)0.0124 (7)0.0039 (6)
N10.0252 (8)0.0467 (10)0.0321 (8)0.0051 (8)0.0080 (7)0.0045 (8)
O20.0217 (8)0.0698 (13)0.1167 (17)0.0058 (9)0.0079 (9)0.0323 (12)
C60.0252 (8)0.0206 (8)0.0209 (8)0.0030 (7)0.0067 (6)0.0032 (7)
N30.0293 (9)0.0349 (10)0.0782 (14)0.0068 (8)0.0118 (9)0.0178 (10)
N40.0218 (8)0.0628 (14)0.0636 (12)0.0095 (9)0.0121 (8)0.0367 (11)
C10.0258 (9)0.0288 (10)0.0253 (9)0.0001 (8)0.0065 (7)0.0057 (7)
C50.0263 (9)0.0259 (9)0.0243 (8)0.0006 (7)0.0088 (7)0.0022 (7)
C70.0292 (9)0.0256 (9)0.0218 (8)0.0011 (8)0.0037 (7)0.0022 (7)
C90.0392 (10)0.0282 (10)0.0203 (8)0.0052 (8)0.0039 (7)0.0005 (7)
C100.0474 (11)0.0303 (10)0.0194 (8)0.0143 (9)0.0139 (8)0.0034 (7)
C40.0338 (10)0.0279 (10)0.0276 (9)0.0063 (8)0.0056 (7)0.0005 (8)
C160.0225 (9)0.0314 (10)0.0364 (10)0.0024 (8)0.0052 (7)0.0047 (8)
C80.0328 (10)0.0354 (11)0.0282 (9)0.0062 (9)0.0006 (7)0.0025 (8)
C30.0440 (11)0.0303 (10)0.0250 (9)0.0000 (9)0.0108 (8)0.0038 (8)
C170.0186 (8)0.0348 (11)0.0453 (11)0.0003 (8)0.0031 (8)0.0109 (9)
C150.0301 (9)0.0308 (10)0.0325 (10)0.0011 (8)0.0042 (8)0.0048 (8)
C20.0358 (10)0.0354 (11)0.0275 (9)0.0046 (9)0.0164 (8)0.0011 (8)
C140.0265 (9)0.0398 (11)0.0309 (9)0.0049 (8)0.0058 (7)0.0010 (9)
C120.0220 (9)0.0316 (11)0.0478 (11)0.0011 (8)0.0015 (8)0.0056 (9)
C130.0230 (9)0.0381 (11)0.0397 (10)0.0015 (8)0.0048 (8)0.0036 (9)
C110.0601 (14)0.0277 (11)0.0393 (11)0.0066 (10)0.0208 (10)0.0081 (9)
C180.0201 (9)0.0458 (13)0.0677 (15)0.0031 (9)0.0082 (9)0.0293 (12)
C210.0170 (10)0.0634 (17)0.0854 (18)0.0041 (11)0.0175 (11)0.0408 (15)
C200.0218 (10)0.0555 (15)0.0787 (17)0.0048 (10)0.0141 (10)0.0425 (14)
C190.0269 (10)0.0444 (14)0.0899 (19)0.0028 (10)0.0104 (11)0.0347 (13)
C220.0233 (10)0.081 (2)0.0773 (17)0.0086 (12)0.0056 (11)0.0446 (16)
Geometric parameters (Å, º) top
O1—C101.234 (2)C16—H160.9500
N2—C91.466 (2)C16—C171.404 (3)
N2—C101.335 (3)C16—C151.381 (3)
N2—C111.465 (3)C8—H80.9500
N1—C11.372 (2)C3—H30.9500
N1—C81.371 (3)C3—C21.369 (3)
N1—H10.89 (3)C17—C121.417 (3)
O2—C211.230 (4)C17—C181.440 (3)
C6—C11.413 (2)C15—H150.9500
C6—C51.402 (2)C15—C141.407 (3)
C6—C71.434 (2)C2—H20.9500
N3—C121.376 (3)C14—H140.9500
N3—C191.363 (3)C14—C131.377 (3)
N3—H3A0.95 (3)C12—C131.397 (3)
N4—C211.340 (3)C13—H130.9500
N4—C201.471 (4)C11—H11A0.9800
N4—C221.473 (3)C11—H11B0.9800
C1—C21.395 (3)C11—H11C0.9800
C5—H50.9500C18—C201.503 (3)
C5—C41.382 (3)C18—C191.364 (3)
C7—C91.504 (2)C21—C20ii1.526 (3)
C7—C81.360 (3)C20—H201.0000
C9—H91.0000C19—H190.9500
C9—C10i1.516 (3)C22—H22A0.9800
C4—H40.9500C22—H22B0.9800
C4—C31.403 (3)C22—H22C0.9800
C10—N2—C9124.44 (17)C16—C17—C12118.38 (18)
C10—N2—C11119.27 (17)C16—C17—C18135.76 (19)
C11—N2—C9116.15 (17)C12—C17—C18105.86 (18)
C1—N1—H1124.6 (17)C16—C15—H15119.4
C8—N1—C1108.59 (16)C16—C15—C14121.16 (19)
C8—N1—H1126.3 (17)C14—C15—H15119.4
C1—C6—C7106.35 (15)C1—C2—H2121.3
C5—C6—C1118.65 (16)C3—C2—C1117.39 (17)
C5—C6—C7135.01 (16)C3—C2—H2121.3
C12—N3—H3A121.3 (19)C15—C14—H14119.3
C19—N3—C12108.71 (19)C13—C14—C15121.33 (18)
C19—N3—H3A129.0 (19)C13—C14—H14119.3
C21—N4—C20123.9 (2)N3—C12—C17108.09 (18)
C21—N4—C22119.5 (3)N3—C12—C13129.3 (2)
C20—N4—C22115.3 (2)C13—C12—C17122.63 (19)
N1—C1—C6107.95 (16)C14—C13—C12117.34 (18)
N1—C1—C2129.81 (17)C14—C13—H13121.3
C2—C1—C6122.24 (17)C12—C13—H13121.3
C6—C5—H5120.4N2—C11—H11A109.5
C4—C5—C6119.23 (16)N2—C11—H11B109.5
C4—C5—H5120.4N2—C11—H11C109.5
C6—C7—C9127.58 (16)H11A—C11—H11B109.5
C8—C7—C6106.87 (16)H11A—C11—H11C109.5
C8—C7—C9125.51 (17)H11B—C11—H11C109.5
N2—C9—C7111.08 (14)C17—C18—C20127.9 (2)
N2—C9—H9107.1C19—C18—C17106.9 (2)
N2—C9—C10i114.85 (16)C19—C18—C20125.1 (2)
C7—C9—H9107.1O2—C21—N4123.8 (2)
C7—C9—C10i109.13 (15)O2—C21—C20ii118.3 (2)
C10i—C9—H9107.1N4—C21—C20ii117.8 (3)
O1—C10—N2122.59 (19)N4—C20—C18110.70 (18)
O1—C10—C9i117.43 (18)N4—C20—C21ii115.3 (2)
N2—C10—C9i119.93 (17)N4—C20—H20107.1
C5—C4—H4119.8C18—C20—C21ii109.0 (2)
C5—C4—C3120.49 (17)C18—C20—H20107.1
C3—C4—H4119.8C21ii—C20—H20107.1
C17—C16—H16120.4N3—C19—C18110.4 (2)
C15—C16—H16120.4N3—C19—H19124.8
C15—C16—C17119.16 (18)C18—C19—H19124.8
N1—C8—H8124.9N4—C22—H22A109.5
C7—C8—N1110.24 (17)N4—C22—H22B109.5
C7—C8—H8124.9N4—C22—H22C109.5
C4—C3—H3119.0H22A—C22—H22B109.5
C2—C3—C4121.99 (17)H22A—C22—H22C109.5
C2—C3—H3119.0H22B—C22—H22C109.5
N1—C1—C2—C3179.52 (19)C8—C7—C9—N2107.9 (2)
C6—C1—C2—C30.2 (3)C8—C7—C9—C10i124.5 (2)
C6—C5—C4—C30.4 (3)C17—C16—C15—C140.6 (3)
C6—C7—C9—N269.8 (2)C17—C12—C13—C140.1 (3)
C6—C7—C9—C10i57.9 (2)C17—C18—C20—N464.5 (3)
C6—C7—C8—N10.7 (2)C17—C18—C20—C21ii63.3 (3)
N3—C12—C13—C14179.1 (2)C17—C18—C19—N30.8 (3)
C1—N1—C8—C70.7 (2)C15—C16—C17—C120.1 (3)
C1—C6—C5—C40.4 (3)C15—C16—C17—C18179.7 (2)
C1—C6—C7—C9177.64 (17)C15—C14—C13—C120.4 (3)
C1—C6—C7—C80.4 (2)C12—N3—C19—C181.0 (3)
C5—C6—C1—N1179.87 (16)C12—C17—C18—C20176.9 (2)
C5—C6—C1—C20.7 (3)C12—C17—C18—C190.3 (3)
C5—C6—C7—C92.6 (3)C11—N2—C9—C761.3 (2)
C5—C6—C7—C8179.4 (2)C11—N2—C9—C10i174.29 (16)
C5—C4—C3—C20.9 (3)C11—N2—C10—O13.5 (3)
C7—C6—C1—N10.1 (2)C11—N2—C10—C9i173.93 (16)
C7—C6—C1—C2179.48 (17)C18—C17—C12—N30.2 (2)
C7—C6—C5—C4179.87 (19)C18—C17—C12—C13179.45 (19)
C9—N2—C10—O1171.94 (17)C21—N4—C20—C18104.3 (2)
C9—N2—C10—C9i10.6 (3)C21—N4—C20—C21ii20.0 (3)
C9—C7—C8—N1177.38 (17)C20—N4—C21—O2163.8 (2)
C10—N2—C9—C7114.30 (19)C20—N4—C21—C20ii20.5 (3)
C10—N2—C9—C10i10.1 (3)C20—C18—C19—N3177.5 (2)
C4—C3—C2—C10.6 (3)C19—N3—C12—C170.7 (3)
C16—C17—C12—N3179.44 (18)C19—N3—C12—C13179.9 (2)
C16—C17—C12—C130.2 (3)C19—C18—C20—N4111.5 (3)
C16—C17—C18—C203.5 (4)C19—C18—C20—C21ii120.6 (3)
C16—C17—C18—C19179.9 (2)C22—N4—C21—O22.9 (3)
C16—C15—C14—C130.8 (3)C22—N4—C21—C20ii172.8 (2)
C8—N1—C1—C60.5 (2)C22—N4—C20—C1862.9 (2)
C8—N1—C1—C2179.8 (2)C22—N4—C20—C21ii172.75 (18)
Symmetry codes: (i) x+3/2, y+3/2, z+1; (ii) x+1, y, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O2iii0.89 (3)2.10 (3)2.828 (2)138 (2)
N3—H3A···O10.95 (3)1.86 (3)2.730 (2)151 (3)
Symmetry code: (iii) x+3/2, y+1/2, z+1.
1,4-Dimethyl-3,6-bis(2-methylindol-3-yl)piperazine-2,5-dione dimethyl sulfoxide monosolvate (II) top
Crystal data top
C24H24N4O2·C2H6SOZ = 2
Mr = 478.60F(000) = 508
Triclinic, P1Dx = 1.277 Mg m3
a = 9.3137 (2) ÅCu Kα radiation, λ = 1.54184 Å
b = 12.3332 (2) ÅCell parameters from 17902 reflections
c = 12.3873 (2) Åθ = 4.0–69.7°
α = 117.110 (2)°µ = 1.44 mm1
β = 93.520 (1)°T = 298 K
γ = 97.399 (2)°Block, clear colourless
V = 1244.35 (4) Å30.36 × 0.11 × 0.07 mm
Data collection top
XtaLAB Synergy, Single source at home/near, HyPix3000
diffractometer
4560 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source4029 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.039
Detector resolution: 10.0000 pixels mm-1θmax = 68.2°, θmin = 4.1°
ω scansh = 1111
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2023)
k = 1414
Tmin = 0.436, Tmax = 1.000l = 1414
25135 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.058H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.177 w = 1/[σ2(Fo2) + (0.0886P)2 + 0.6913P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
4560 reflectionsΔρmax = 0.60 e Å3
283 parametersΔρmin = 0.21 e Å3
0 restraints
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O11.20329 (17)0.40135 (17)0.56994 (18)0.0588 (5)
O20.1008 (2)0.24272 (15)0.12756 (17)0.0649 (5)
N20.99719 (17)0.48117 (16)0.60324 (16)0.0397 (4)
N40.14924 (19)0.05031 (16)0.02277 (16)0.0428 (4)
N10.50383 (19)0.35296 (18)0.53767 (18)0.0472 (5)
C60.7058 (2)0.30236 (18)0.44973 (18)0.0358 (4)
C101.1103 (2)0.44957 (18)0.5413 (2)0.0398 (5)
C70.7330 (2)0.43181 (18)0.53668 (18)0.0372 (4)
N30.2971 (3)0.2443 (2)0.1043 (2)0.0638 (6)
C90.87168 (19)0.52304 (18)0.56525 (19)0.0373 (4)
H90.8599900.6004490.6353770.045*
C10.5593 (2)0.2567 (2)0.4515 (2)0.0411 (5)
C80.6080 (2)0.4585 (2)0.58912 (19)0.0416 (5)
C50.7883 (2)0.21910 (19)0.37191 (19)0.0419 (5)
H50.8853990.2457950.3692110.050*
C190.1706 (2)0.1339 (2)0.04553 (19)0.0421 (5)
C220.0582 (2)0.13100 (19)0.06521 (19)0.0430 (5)
C180.1568 (2)0.0974 (2)0.1717 (2)0.0465 (5)
C210.1057 (2)0.08458 (19)0.03270 (18)0.0403 (4)
H210.1476040.1197040.1096160.048*
C40.7237 (2)0.0973 (2)0.2995 (2)0.0486 (5)
H40.7786440.0416460.2488340.058*
C200.2590 (2)0.2212 (2)0.0089 (2)0.0511 (5)
C20.4933 (2)0.1344 (2)0.3766 (2)0.0519 (6)
H20.3959960.1067830.3778100.062*
C30.5770 (3)0.0556 (2)0.3007 (2)0.0546 (6)
H30.5355110.0267340.2492620.065*
C130.2377 (3)0.1687 (2)0.2053 (3)0.0569 (6)
C230.3070 (2)0.0969 (2)0.0516 (3)0.0577 (6)
H23A0.3270200.1742780.0496410.087*
H23B0.3565630.0380750.0077080.087*
H23C0.3406830.1089090.1317210.087*
C120.5754 (3)0.5746 (2)0.6888 (2)0.0556 (6)
H12A0.5658300.5648510.7607640.083*
H12B0.4857800.5921620.6631200.083*
H12C0.6535630.6417710.7068800.083*
C170.0903 (3)0.0086 (3)0.2608 (2)0.0586 (6)
H170.0372600.0405760.2413260.070*
C110.9833 (3)0.4598 (3)0.7088 (2)0.0563 (6)
H11A1.0784640.4626400.7454630.084*
H11B0.9246900.3800240.6830060.084*
H11C0.9374610.5226710.7675420.084*
C160.1048 (3)0.0049 (4)0.3782 (3)0.0756 (9)
H160.0615350.0640590.4381130.091*
C240.3164 (3)0.2864 (3)0.1101 (3)0.0691 (8)
H24A0.4095810.3062740.0956690.104*
H24B0.3271940.2335790.1479590.104*
H24C0.2491990.3611110.1630520.104*
C140.2508 (3)0.1543 (3)0.3241 (3)0.0760 (9)
H140.3043500.2020740.3453460.091*
C150.1829 (4)0.0684 (4)0.4080 (3)0.0858 (11)
H150.1890890.0586110.4872130.103*
H10.414 (4)0.357 (3)0.548 (3)0.073 (9)*
H3A0.375 (4)0.280 (3)0.111 (3)0.095 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0336 (8)0.0773 (12)0.0873 (12)0.0219 (8)0.0136 (8)0.0533 (10)
O20.0573 (10)0.0392 (9)0.0720 (12)0.0033 (7)0.0119 (9)0.0077 (8)
N20.0262 (8)0.0467 (9)0.0451 (9)0.0066 (7)0.0039 (7)0.0205 (8)
N40.0352 (9)0.0410 (9)0.0461 (10)0.0036 (7)0.0004 (7)0.0165 (8)
N10.0245 (8)0.0544 (11)0.0559 (11)0.0062 (7)0.0117 (7)0.0194 (9)
C60.0272 (9)0.0402 (10)0.0395 (10)0.0052 (7)0.0041 (7)0.0185 (8)
C100.0227 (9)0.0392 (10)0.0544 (12)0.0045 (7)0.0017 (8)0.0200 (9)
C70.0243 (9)0.0418 (10)0.0408 (10)0.0060 (7)0.0050 (7)0.0153 (9)
N30.0533 (12)0.0568 (13)0.0852 (16)0.0139 (10)0.0035 (11)0.0370 (12)
C90.0247 (9)0.0357 (10)0.0441 (10)0.0069 (7)0.0048 (7)0.0121 (8)
C10.0293 (9)0.0456 (11)0.0474 (11)0.0055 (8)0.0061 (8)0.0212 (9)
C80.0287 (9)0.0475 (11)0.0436 (11)0.0082 (8)0.0068 (8)0.0165 (9)
C50.0325 (10)0.0434 (11)0.0480 (12)0.0080 (8)0.0093 (8)0.0189 (9)
C190.0359 (10)0.0442 (11)0.0437 (11)0.0075 (8)0.0044 (8)0.0185 (9)
C220.0432 (11)0.0401 (11)0.0371 (10)0.0048 (9)0.0028 (8)0.0123 (9)
C180.0331 (10)0.0582 (13)0.0500 (12)0.0017 (9)0.0023 (9)0.0289 (11)
C210.0404 (11)0.0399 (11)0.0342 (10)0.0091 (8)0.0059 (8)0.0112 (8)
C40.0473 (12)0.0426 (11)0.0514 (13)0.0120 (9)0.0115 (10)0.0166 (10)
C200.0419 (12)0.0436 (12)0.0617 (14)0.0084 (9)0.0021 (10)0.0197 (11)
C20.0343 (11)0.0515 (13)0.0618 (14)0.0041 (9)0.0031 (10)0.0229 (11)
C30.0509 (13)0.0411 (12)0.0599 (14)0.0003 (10)0.0036 (11)0.0163 (11)
C130.0442 (12)0.0642 (15)0.0688 (16)0.0034 (11)0.0046 (11)0.0415 (13)
C230.0367 (12)0.0583 (14)0.0704 (16)0.0011 (10)0.0013 (11)0.0266 (13)
C120.0387 (11)0.0606 (14)0.0535 (13)0.0165 (10)0.0133 (10)0.0121 (11)
C170.0415 (12)0.0866 (18)0.0497 (13)0.0120 (12)0.0113 (10)0.0327 (13)
C110.0424 (12)0.0770 (17)0.0587 (14)0.0101 (11)0.0062 (10)0.0399 (13)
C160.0521 (15)0.123 (3)0.0509 (15)0.0039 (16)0.0127 (12)0.0420 (17)
C240.0587 (15)0.0563 (15)0.0728 (18)0.0226 (12)0.0116 (13)0.0102 (13)
C140.0594 (16)0.101 (2)0.087 (2)0.0105 (16)0.0146 (15)0.071 (2)
C150.0646 (18)0.140 (3)0.0644 (18)0.014 (2)0.0007 (15)0.067 (2)
Geometric parameters (Å, º) top
O1—C101.232 (3)C18—C131.407 (3)
O2—C221.226 (3)C18—C171.400 (4)
N2—C101.336 (3)C21—H210.9800
N2—C91.471 (2)C4—H40.9300
N2—C111.457 (3)C4—C31.400 (3)
N4—C221.334 (3)C20—C241.494 (4)
N4—C211.468 (3)C2—H20.9300
N4—C231.465 (3)C2—C31.374 (3)
N1—C11.373 (3)C3—H30.9300
N1—C81.373 (3)C13—C141.395 (4)
N1—H10.85 (3)C23—H23A0.9600
C6—C71.438 (3)C23—H23B0.9600
C6—C11.414 (3)C23—H23C0.9600
C6—C51.402 (3)C12—H12A0.9600
C10—C9i1.517 (3)C12—H12B0.9600
C7—C91.506 (3)C12—H12C0.9600
C7—C81.371 (3)C17—H170.9300
N3—C201.372 (3)C17—C161.382 (4)
N3—C131.377 (4)C11—H11A0.9600
N3—H3A0.92 (4)C11—H11B0.9600
C9—H90.9800C11—H11C0.9600
C1—C21.389 (3)C16—H160.9300
C8—C121.488 (3)C16—C151.387 (5)
C5—H50.9300C24—H24A0.9600
C5—C41.377 (3)C24—H24B0.9600
C19—C181.435 (3)C24—H24C0.9600
C19—C211.495 (3)C14—H140.9300
C19—C201.368 (3)C14—C151.361 (5)
C22—C21ii1.520 (3)C15—H150.9300
C10—N2—C9125.04 (18)C5—C4—H4119.3
C10—N2—C11119.54 (18)C5—C4—C3121.4 (2)
C11—N2—C9114.98 (17)C3—C4—H4119.3
C22—N4—C21124.73 (18)N3—C20—C24120.2 (2)
C22—N4—C23118.72 (19)C19—C20—N3109.0 (2)
C23—N4—C21115.63 (18)C19—C20—C24130.7 (2)
C1—N1—C8109.87 (17)C1—C2—H2121.2
C1—N1—H1128 (2)C3—C2—C1117.7 (2)
C8—N1—H1121 (2)C3—C2—H2121.2
C1—C6—C7106.30 (17)C4—C3—H3119.5
C5—C6—C7135.52 (18)C2—C3—C4121.0 (2)
C5—C6—C1118.17 (18)C2—C3—H3119.5
O1—C10—N2121.9 (2)N3—C13—C18107.6 (2)
O1—C10—C9i118.61 (18)N3—C13—C14130.6 (3)
N2—C10—C9i119.49 (17)C14—C13—C18121.7 (3)
C6—C7—C9126.94 (17)N4—C23—H23A109.5
C8—C7—C6107.46 (17)N4—C23—H23B109.5
C8—C7—C9125.59 (18)N4—C23—H23C109.5
C20—N3—C13109.4 (2)H23A—C23—H23B109.5
C20—N3—H3A125 (2)H23A—C23—H23C109.5
C13—N3—H3A122 (2)H23B—C23—H23C109.5
N2—C9—C10i114.68 (16)C8—C12—H12A109.5
N2—C9—C7110.94 (16)C8—C12—H12B109.5
N2—C9—H9107.0C8—C12—H12C109.5
C10i—C9—H9107.0H12A—C12—H12B109.5
C7—C9—C10i109.76 (16)H12A—C12—H12C109.5
C7—C9—H9107.0H12B—C12—H12C109.5
N1—C1—C6107.51 (18)C18—C17—H17120.6
N1—C1—C2129.92 (19)C16—C17—C18118.9 (3)
C2—C1—C6122.56 (19)C16—C17—H17120.6
N1—C8—C12119.88 (18)N2—C11—H11A109.5
C7—C8—N1108.82 (18)N2—C11—H11B109.5
C7—C8—C12131.2 (2)N2—C11—H11C109.5
C6—C5—H5120.4H11A—C11—H11B109.5
C4—C5—C6119.18 (19)H11A—C11—H11C109.5
C4—C5—H5120.4H11B—C11—H11C109.5
C18—C19—C21127.36 (19)C17—C16—H16119.5
C20—C19—C18107.4 (2)C17—C16—C15121.0 (3)
C20—C19—C21125.2 (2)C15—C16—H16119.5
O2—C22—N4122.9 (2)C20—C24—H24A109.5
O2—C22—C21ii117.74 (19)C20—C24—H24B109.5
N4—C22—C21ii119.35 (18)C20—C24—H24C109.5
C13—C18—C19106.5 (2)H24A—C24—H24B109.5
C17—C18—C19134.7 (2)H24A—C24—H24C109.5
C17—C18—C13118.8 (2)H24B—C24—H24C109.5
N4—C21—C19111.20 (17)C13—C14—H14121.0
N4—C21—C22ii114.68 (17)C15—C14—C13118.0 (3)
N4—C21—H21106.7C15—C14—H14121.0
C19—C21—C22ii110.40 (17)C16—C15—H15119.2
C19—C21—H21106.7C14—C15—C16121.6 (3)
C22ii—C21—H21106.7C14—C15—H15119.2
N1—C1—C2—C3177.7 (2)C22—N4—C21—C19113.3 (2)
C6—C7—C9—N256.4 (3)C22—N4—C21—C22ii12.9 (3)
C6—C7—C9—C10i71.4 (2)C18—C19—C21—N455.7 (3)
C6—C7—C8—N11.1 (2)C18—C19—C21—C22ii72.7 (3)
C6—C7—C8—C12176.2 (2)C18—C19—C20—N32.1 (3)
C6—C1—C2—C31.6 (4)C18—C19—C20—C24176.6 (2)
C6—C5—C4—C31.1 (3)C18—C13—C14—C150.1 (4)
C10—N2—C9—C10i10.2 (3)C18—C17—C16—C150.4 (4)
C10—N2—C9—C7114.8 (2)C21—N4—C22—O2168.4 (2)
C7—C6—C1—N11.8 (2)C21—N4—C22—C21ii13.4 (3)
C7—C6—C1—C2178.7 (2)C21—C19—C18—C13179.5 (2)
C7—C6—C5—C4179.5 (2)C21—C19—C18—C172.8 (4)
N3—C13—C14—C15177.8 (3)C21—C19—C20—N3179.7 (2)
C9—N2—C10—O1171.18 (19)C21—C19—C20—C241.6 (4)
C9—N2—C10—C9i10.7 (3)C20—N3—C13—C181.3 (3)
C9—C7—C8—N1178.31 (19)C20—N3—C13—C14176.9 (3)
C9—C7—C8—C124.3 (4)C20—C19—C18—C131.3 (2)
C1—N1—C8—C70.0 (3)C20—C19—C18—C17175.3 (3)
C1—N1—C8—C12177.7 (2)C20—C19—C21—N4122.1 (2)
C1—C6—C7—C9177.62 (19)C20—C19—C21—C22ii109.4 (2)
C1—C6—C7—C81.8 (2)C13—N3—C20—C192.1 (3)
C1—C6—C5—C40.8 (3)C13—N3—C20—C24176.7 (2)
C1—C2—C3—C40.3 (4)C13—C18—C17—C160.8 (4)
C8—N1—C1—C61.2 (2)C13—C14—C15—C161.1 (4)
C8—N1—C1—C2179.4 (2)C23—N4—C22—O20.1 (3)
C8—C7—C9—N2124.3 (2)C23—N4—C22—C21ii178.1 (2)
C8—C7—C9—C10i108.0 (2)C23—N4—C21—C1955.6 (2)
C5—C6—C7—C93.5 (4)C23—N4—C21—C22ii178.29 (19)
C5—C6—C7—C8177.0 (2)C17—C18—C13—N3177.2 (2)
C5—C6—C1—N1177.29 (19)C17—C18—C13—C141.1 (4)
C5—C6—C1—C22.2 (3)C17—C16—C15—C141.4 (5)
C5—C4—C3—C21.6 (4)C11—N2—C10—O10.8 (3)
C19—C18—C13—N30.0 (2)C11—N2—C10—C9i177.35 (19)
C19—C18—C13—C14178.4 (2)C11—N2—C9—C10i177.48 (18)
C19—C18—C17—C16177.1 (3)C11—N2—C9—C757.5 (2)
Symmetry codes: (i) x+2, y+1, z+1; (ii) x, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O1iii0.85 (3)2.11 (3)2.950 (2)168 (3)
Symmetry code: (iii) x1, y, z.
1,4-Dimethyl-3,6-bis(2-methylindol-3-yl)piperazine-2,5-dione tetrahydrofuran monosolvate (III) top
Crystal data top
C24H24N4O2·C4H8OF(000) = 504
Mr = 472.57Dx = 1.186 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.5276 (9) ÅCell parameters from 1124 reflections
b = 8.9357 (7) Åθ = 2.4–21.3°
c = 17.4883 (13) ŵ = 0.08 mm1
β = 96.731 (8)°T = 293 K
V = 1323.4 (2) Å3Irregular, clear light red
Z = 20.4 × 0.4 × 0.3 mm
Data collection top
XtaLAB Mini (ROW)
diffractometer
2420 independent reflections
Radiation source: fine-focus sealed X-ray tube, Rigaku (Mo) X-ray Source1519 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
ω scansθmax = 25.4°, θmin = 2.4°
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2023)
h = 910
Tmin = 0.968, Tmax = 1.000k = 109
6423 measured reflectionsl = 2120
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.053 w = 1/[σ2(Fo2) + (0.0989P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.178(Δ/σ)max < 0.001
S = 1.02Δρmax = 0.26 e Å3
2420 reflectionsΔρmin = 0.15 e Å3
143 parametersExtinction correction: SHELXL-2018/3 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.019 (4)
Primary atom site location: dual
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.6513 (2)0.59725 (19)0.63282 (8)0.0738 (6)
N10.5240 (2)0.65140 (17)0.51655 (9)0.0552 (5)
N20.6285 (3)0.7814 (2)0.27788 (12)0.0705 (6)
C10.5781 (3)0.5565 (2)0.57146 (10)0.0493 (6)
C40.7086 (3)0.6138 (2)0.36953 (11)0.0516 (6)
C20.4530 (3)0.6105 (2)0.43922 (10)0.0499 (6)
H2A0.3509210.6617280.4300190.060*
C30.5519 (3)0.6631 (2)0.37871 (11)0.0550 (6)
C90.7526 (3)0.6901 (2)0.30495 (11)0.0587 (6)
C100.5065 (3)0.7634 (3)0.32147 (12)0.0648 (7)
C50.8164 (3)0.5138 (3)0.40716 (12)0.0623 (6)
H50.7914630.4620540.4502700.075*
C80.8974 (3)0.6686 (3)0.27802 (14)0.0700 (7)
H80.9242700.7203850.2353090.084*
C70.9994 (3)0.5686 (3)0.31634 (15)0.0779 (8)
H71.0970930.5516450.2992090.094*
C60.9599 (3)0.4919 (3)0.38035 (15)0.0759 (7)
H61.0315070.4246060.4054950.091*
C120.5442 (5)0.8121 (3)0.53101 (16)0.0991 (11)
H12A0.4659450.8664660.4981280.149*
H12B0.6475940.8422220.5205250.149*
H12C0.5321830.8330180.5838570.149*
C110.3572 (4)0.8489 (3)0.30298 (16)0.0923 (10)
H11A0.3798180.9541650.3045570.138*
H11B0.2862360.8256030.3400350.138*
H11C0.3092820.8220710.2524270.138*
H20.622 (3)0.825 (3)0.2308 (16)0.092 (9)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0805 (12)0.0974 (13)0.0430 (8)0.0108 (10)0.0060 (8)0.0230 (8)
N10.0905 (15)0.0337 (9)0.0431 (9)0.0042 (9)0.0150 (9)0.0044 (7)
N20.0864 (16)0.0763 (13)0.0498 (11)0.0047 (12)0.0129 (11)0.0245 (10)
C10.0623 (14)0.0549 (12)0.0330 (10)0.0011 (10)0.0157 (9)0.0048 (9)
C40.0645 (15)0.0517 (12)0.0394 (11)0.0034 (10)0.0100 (10)0.0024 (9)
C20.0643 (14)0.0462 (12)0.0406 (11)0.0089 (10)0.0117 (10)0.0061 (9)
C30.0722 (16)0.0516 (12)0.0423 (11)0.0043 (11)0.0115 (10)0.0119 (9)
C90.0748 (17)0.0593 (13)0.0430 (11)0.0088 (12)0.0111 (11)0.0041 (10)
C100.0811 (18)0.0644 (14)0.0491 (12)0.0045 (13)0.0083 (12)0.0189 (10)
C50.0703 (17)0.0625 (14)0.0560 (12)0.0033 (12)0.0144 (12)0.0089 (11)
C80.0795 (19)0.0754 (16)0.0594 (14)0.0175 (14)0.0261 (13)0.0032 (12)
C70.0702 (18)0.0842 (18)0.0833 (18)0.0055 (15)0.0254 (15)0.0084 (15)
C60.0714 (19)0.0778 (17)0.0798 (16)0.0058 (14)0.0143 (14)0.0063 (14)
C120.168 (3)0.0423 (13)0.093 (2)0.0147 (16)0.038 (2)0.0148 (13)
C110.098 (2)0.092 (2)0.0856 (19)0.0211 (17)0.0080 (17)0.0409 (16)
Geometric parameters (Å, º) top
O1—C11.231 (2)C10—C111.487 (4)
N1—C11.323 (3)C5—H50.9300
N1—C21.462 (3)C5—C61.375 (3)
N1—C121.465 (3)C8—H80.9300
N2—C91.376 (3)C8—C71.366 (4)
N2—C101.369 (3)C7—H70.9300
N2—H20.91 (3)C7—C61.387 (3)
C1—C2i1.524 (3)C6—H60.9300
C4—C31.434 (3)C12—H12A0.9600
C4—C91.408 (3)C12—H12B0.9600
C4—C51.391 (3)C12—H12C0.9600
C2—H2A0.9800C11—H11A0.9600
C2—C31.504 (3)C11—H11B0.9600
C3—C101.365 (3)C11—H11C0.9600
C9—C81.386 (4)
C1—N1—C2125.65 (16)C3—C10—C11131.2 (2)
C1—N1—C12118.62 (19)C4—C5—H5120.2
C2—N1—C12115.62 (18)C6—C5—C4119.7 (2)
C9—N2—H2122.0 (18)C6—C5—H5120.2
C10—N2—C9110.06 (18)C9—C8—H8121.1
C10—N2—H2125.8 (18)C7—C8—C9117.8 (2)
O1—C1—N1122.78 (19)C7—C8—H8121.1
O1—C1—C2i117.35 (19)C8—C7—H7119.4
N1—C1—C2i119.85 (18)C8—C7—C6121.2 (2)
C9—C4—C3106.31 (19)C6—C7—H7119.4
C5—C4—C3135.82 (19)C5—C6—C7121.0 (3)
C5—C4—C9117.9 (2)C5—C6—H6119.5
N1—C2—C1i113.94 (15)C7—C6—H6119.5
N1—C2—H2A107.4N1—C12—H12A109.5
N1—C2—C3111.53 (18)N1—C12—H12B109.5
C1i—C2—H2A107.4N1—C12—H12C109.5
C3—C2—C1i108.90 (15)H12A—C12—H12B109.5
C3—C2—H2A107.4H12A—C12—H12C109.5
C4—C3—C2126.14 (17)H12B—C12—H12C109.5
C10—C3—C4107.89 (19)C10—C11—H11A109.5
C10—C3—C2126.0 (2)C10—C11—H11B109.5
N2—C9—C4107.2 (2)C10—C11—H11C109.5
N2—C9—C8130.2 (2)H11A—C11—H11B109.5
C8—C9—C4122.5 (2)H11A—C11—H11C109.5
N2—C10—C11120.36 (19)H11B—C11—H11C109.5
C3—C10—N2108.5 (2)
N1—C2—C3—C464.2 (3)C9—N2—C10—C31.6 (3)
N1—C2—C3—C10117.7 (2)C9—N2—C10—C11179.2 (2)
N2—C9—C8—C7179.5 (2)C9—C4—C3—C2178.71 (19)
C1—N1—C2—C1i8.7 (3)C9—C4—C3—C100.3 (2)
C1—N1—C2—C3115.1 (2)C9—C4—C5—C60.5 (3)
C1i—C2—C3—C462.4 (3)C9—C8—C7—C60.4 (4)
C1i—C2—C3—C10115.7 (2)C10—N2—C9—C41.4 (3)
C4—C3—C10—N21.2 (3)C10—N2—C9—C8178.3 (2)
C4—C3—C10—C11179.8 (3)C5—C4—C3—C20.4 (4)
C4—C9—C8—C70.2 (4)C5—C4—C3—C10178.8 (2)
C4—C5—C6—C70.3 (4)C5—C4—C9—N2180.0 (2)
C2—N1—C1—O1172.4 (2)C5—C4—C9—C80.3 (3)
C2—N1—C1—C2i9.1 (4)C8—C7—C6—C50.2 (4)
C2—C3—C10—N2179.6 (2)C12—N1—C1—O13.5 (3)
C2—C3—C10—C111.4 (4)C12—N1—C1—C2i174.9 (2)
C3—C4—C9—N20.7 (2)C12—N1—C2—C1i175.3 (2)
C3—C4—C9—C8179.1 (2)C12—N1—C2—C360.9 (3)
C3—C4—C5—C6178.6 (2)
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···O1ii0.91 (3)1.89 (3)2.787 (2)168 (3)
Symmetry code: (ii) x, y+3/2, z1/2.
 

Acknowledgements

The authors thank the Center for Advanced Materials Science, located within the Department of Biochemistry, Chemistry, and Physics at Georgia Southern University for the financial support of this work and the National Science Foundation Major Research Instrumentation fund for the purchase of the X-ray diffractometer.

Funding information

Funding for this research was provided by: National Science Foundation, Directorate for Mathematical and Physical Sciences, MRI (grant No. 2215812).

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