organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2414-3146

2-Methyl-N-[(E)-4-nitro­ben­zyl­i­dene]pro­pan-2-am­ine

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aNelson Mandela University, Summerstrand Campus, Department of Chemistry, University Way, Summerstrand, PO Box 77000, Port Elizabeth, 6031, South Africa
*Correspondence e-mail: [email protected]

Edited by M. Bolte, Goethe-Universität Frankfurt, Germany (Received 1 December 2025; accepted 16 December 2025; online 24 December 2025)

The title compound, C11H14N2O2, is a Schiff base derived from tert-butyl­amine and para-nitro­benzaldehyde. All atoms except the methyl groups are located on a mirror plane. Thus, there is only half a mol­ecule in the asymmetric unit. The tert-butyl group shows rotational disorder over four positions. The mol­ecule is E-configured. In the extended structure, C—H⋯O contacts connect the mol­ecules into chains along [010] in the crystal structure.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

Imines – also known as Schiff bases – are the condensation products between a primary amine and a carbonyl compound and, thus, have found application as protection group for either one of the two compounds during classical organic multi-step synthesis procedures (Becker et al., 2000View full citation; Greene & Wuts, 2007View full citation). They have also found use as ligands in transition-metal chemistry for transition metals such as rhenium (Mukiza et al., 2020View full citation; Yumata et al., 2011bView full citation; Habarurema et al., 2014aView full citation,bView full citation,cView full citation, 2015aView full citation,bView full citation; Potgieter et al., 2013View full citation; Gerber et al., 2011View full citation, 2012View full citation) or rare-earth metals (Abrahams et al., 2017View full citation) and, in a structural variation, also play a role in carbohydrate chemistry in the shape of hydrazones that, in turn, give rise to osazones (Lindhorst, 2007View full citation). In a continuation of our inter­est in structural aspects of Schiff bases (Potgieter et al., 2011View full citation; Booysen et al., 2011aView full citation,bView full citation; Mohamed et al., 2023View full citation; Schmitt et al., 2011View full citation, 2014View full citation, 2015aView full citation,bView full citation; Yumata et al., 2011aView full citation; Habarurema et al., 2014aView full citation,bView full citation; Madanhire et al., 2015aView full citation,bView full citation) we initiated a study around the metrical parameters of Schiff bases derived from aromatic aldehydes and the influence of coordination towards transition metals on these values. An intriguing family of compounds are derivatives featuring strongly deactivating nitro groups on the aromatic aldehyde core such as the series of mono­nitro-substituted benzaldehydes. The literature abounds in structural information around Schiff bases derived from ortho-nitro­benzladehyde (e.g. Cueno-Cabezas et al., 2025View full citation; Shan et al., 2004View full citation; Duggin et al., 2024View full citation) and some derived coordination compounds with mercury (Sheikh et al., 2025View full citation) and manganese (Mansour et al., 2024View full citation) as well as meta-nitro­benzaldehyde (e.g. Priyadharshini et al., 2025View full citation; Glidewell et al., 2005View full citation; Akkurt et al., 2008View full citation) and some derived coordination compounds with tin (Cui et al., 2022View full citation) and anti­mony (Artemeva et al., 2019View full citation) and para-nitro­benzaldehyde (e.g. Rogalewicz et al., 2025View full citation; Chuskit et al., 2025View full citation; Watson et al., 1984View full citation) and some derived coordination compounds with nickel, copper, zinc and palladium (Rogalewicz et al., 2025View full citation).

The structure solution shows the presence of a Schiff base derived from 4-nitro­benzaldehyde and tert-butyl­amine. The C=N double bond is (E)-configured (C2—N1—C1— C11 = 180 and N1—C1—C11—C12 = 0°]) (Fig. 1[link]). The tert-butyl group shows rotational disorder. Except for the methyl groups, the mol­ecule is exactly planar. Intra­cyclic C—C—C angles cover a range of 118.48 (19)–122.28 (18)° with the largest angle located on the carbon atom bearing the nitro group and the smallest angle on one of the CH groups directly adjacent to the latter carbon atom. All other bond lengths and angles are in good agreement with comparable values reported for other Schiff bases whose mol­ecular and crystal structures have been determined on grounds of diffraction studies carried out on single crystals and whose metrical parameters have been deposited with the Cambridge Structural Database (Groom et al., 2016View full citation).

[Figure 1]
Figure 1
The mol­ecular structure of the title compound, with atom labels and anisotropic displacement ellipsoids (drawn at 50% probability level). Only one of the four positions of the disordered methyl groups is shown.

In the crystal, C—H⋯O contacts (Table 1[link]) whose range falls by more than 0.1 Å below the sum of the van der Waals radii of the atoms participating in them are observed. These are established between one hydrogen atom each of two methyl groups as donors and one of the nitro group's oxygen atoms as acceptor. In terms of graph-set analysis (Etter et al., 1990View full citation; Bernstein et al., 1995View full citation), the descriptor for these contacts is C11(11). π-Stacking is not a prominent consolidating feature in the crystal structure of the title compound, with the shortest inter­centroid distance in between two centers of gravity measured at 4.0640 (6) Å.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C5—H5B⋯O1i 0.98 2.53 3.41 (3) 149
C6—H6C⋯O1ii 0.98 2.58 3.459 (19) 149
C7—H7B⋯O1i 0.98 2.56 3.35 (2) 138
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.

Synthesis and crystallization

The compound was obtained following a standard procedure by reacting para-nitro­benzaldehyde with tert-butyl­amine (Becker et al., 2000View full citation). Crystals suitable for the diffraction study were obtained straight from the solidified isolated product.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C11H14N2O2
Mr 206.24
Crystal system, space group Orthorhombic, Pnma
Temperature (K) 200
a, b, c (Å) 9.5110 (4), 7.2400 (3), 16.2386 (7)
V3) 1118.18 (8)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.09
Crystal size (mm) 0.39 × 0.25 × 0.14
 
Data collection
Diffractometer Bruker APEXII CCD
Absorption correction Numerical (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.951, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 38579, 1388, 1087
Rint 0.027
(sin θ/λ)max−1) 0.649
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.168, 1.17
No. of reflections 1388
No. of parameters 127
No. of restraints 30
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.14, −0.28
Computer programs: APEX2 and SAINT (Bruker, 2014View full citation), SHELXS97 (Sheldrick 2008View full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation), Mercury (Macrae et al., 2020View full citation), SHELXL2019/3 (Sheldrick, 2015View full citation) and PLATON (Spek, 2020View full citation).

Structural data


Computing details top

2-Methyl-N-[(E)-4-nitrobenzylidene]propan-2-amine top
Crystal data top
C11H14N2O2Dx = 1.225 Mg m3
Mr = 206.24Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PnmaCell parameters from 9822 reflections
a = 9.5110 (4) Åθ = 2.5–27.5°
b = 7.2400 (3) ŵ = 0.09 mm1
c = 16.2386 (7) ÅT = 200 K
V = 1118.18 (8) Å3Block, colourless
Z = 40.39 × 0.25 × 0.14 mm
F(000) = 440
Data collection top
Bruker APEXII CCD
diffractometer
1087 reflections with I > 2σ(I)
φ and ω scansRint = 0.027
Absorption correction: numerical
(SADABS; Krause et al., 2015)
θmax = 27.5°, θmin = 2.5°
Tmin = 0.951, Tmax = 1.000h = 1212
38579 measured reflectionsk = 99
1388 independent reflectionsl = 2121
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)] = 0.051Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.168H-atom parameters constrained
S = 1.17 w = 1/[σ2(Fo2) + (0.0741P)2 + 0.2341P]
where P = (Fo2 + 2Fc2)/3
1388 reflections(Δ/σ)max < 0.001
127 parametersΔρmax = 0.14 e Å3
30 restraintsΔρmin = 0.28 e Å3
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.

Refinement. H atoms were placed in calculated positions (C–H 0.95 Å for aromatic and vinylic carbon atoms, C–H 0.98 Å for the methyl groups) and were included in the refinement in the riding model approximation, with U(H) set to 1.2Ueq(C) (aromatic and vinylic carbon atoms) and U(H) set to 1.5Ueq(C) (methyl carbon atoms).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.80982 (18)0.2500000.41353 (13)0.0882 (6)
O20.7034 (2)0.2500000.29689 (12)0.0958 (7)
N10.16773 (16)0.2500000.61550 (10)0.0528 (4)
N20.7029 (2)0.2500000.37195 (13)0.0682 (6)
C10.1760 (2)0.2500000.53874 (12)0.0519 (5)
H10.0918860.2500000.5071960.062*
C20.0296 (2)0.2500000.65746 (12)0.0536 (5)
C110.31255 (19)0.2500000.49559 (12)0.0484 (5)
C120.4375 (2)0.2500000.53988 (13)0.0542 (5)
H120.4351450.2500000.5983630.065*
C130.5655 (2)0.2500000.49924 (14)0.0574 (5)
H130.6511080.2500000.5293400.069*
C140.5664 (2)0.2500000.41468 (13)0.0539 (5)
C150.4456 (2)0.2500000.36931 (13)0.0611 (6)
H150.4489690.2500000.3108390.073*
C160.3178 (2)0.2500000.41056 (13)0.0591 (5)
H160.2327160.2500000.3798980.071*
C30.0973 (5)0.265 (4)0.6039 (3)0.068 (3)0.25
H3A0.1820030.2639140.6382660.102*0.25
H3B0.0933430.3812360.5728470.102*0.25
H3C0.0998060.1609660.5655490.102*0.25
C40.031 (2)0.409 (3)0.7219 (14)0.065 (5)0.25
H4A0.0599070.4120070.7507370.098*0.25
H4B0.1062520.3875950.7618110.098*0.25
H4C0.0461140.5269410.6939010.098*0.25
C50.025 (2)0.067 (3)0.7079 (13)0.059 (4)0.25
H5A0.0646230.0588910.7373980.089*0.25
H5B0.0343190.0382760.6704860.089*0.25
H5C0.1026420.0659270.7476390.089*0.25
C60.062 (2)0.4163 (17)0.6252 (12)0.056 (3)0.25
H6A0.0825750.3983700.5666620.084*0.25
H6B0.1497160.4223500.6563920.084*0.25
H6C0.0093760.5318630.6324790.084*0.25
C70.047 (2)0.073 (2)0.6354 (16)0.100 (8)0.25
H7A0.0625910.0693050.5758250.150*0.25
H7B0.0102650.0329420.6520700.150*0.25
H7C0.1373430.0696670.6641170.150*0.25
C80.0610 (8)0.276 (4)0.7447 (4)0.120 (7)0.25
H8A0.0268680.2777210.7762070.180*0.25
H8B0.1207410.1751170.7641600.180*0.25
H8C0.1102220.3941100.7522810.180*0.25
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0537 (10)0.1050 (15)0.1060 (15)0.0000.0215 (9)0.000
O20.0840 (13)0.1273 (18)0.0762 (12)0.0000.0377 (10)0.000
N10.0448 (8)0.0618 (10)0.0518 (9)0.0000.0050 (7)0.000
N20.0630 (11)0.0611 (11)0.0805 (14)0.0000.0266 (10)0.000
C10.0457 (9)0.0615 (11)0.0486 (10)0.0000.0014 (7)0.000
C20.0440 (9)0.0643 (12)0.0525 (10)0.0000.0078 (8)0.000
C110.0477 (10)0.0472 (10)0.0502 (10)0.0000.0060 (7)0.000
C120.0513 (11)0.0587 (12)0.0526 (10)0.0000.0061 (8)0.000
C130.0489 (10)0.0589 (12)0.0644 (12)0.0000.0055 (8)0.000
C140.0523 (10)0.0449 (10)0.0645 (12)0.0000.0183 (9)0.000
C150.0657 (12)0.0674 (13)0.0502 (11)0.0000.0120 (9)0.000
C160.0531 (11)0.0740 (14)0.0502 (10)0.0000.0036 (8)0.000
C30.049 (2)0.095 (9)0.060 (3)0.013 (7)0.0064 (19)0.024 (7)
C40.079 (8)0.060 (6)0.057 (7)0.014 (5)0.011 (5)0.006 (5)
C50.057 (5)0.064 (7)0.057 (7)0.004 (5)0.020 (5)0.008 (7)
C60.045 (4)0.045 (5)0.079 (6)0.010 (4)0.012 (4)0.001 (4)
C70.067 (9)0.109 (13)0.124 (16)0.003 (7)0.040 (9)0.017 (9)
C80.084 (5)0.23 (2)0.049 (3)0.065 (12)0.017 (3)0.017 (10)
Geometric parameters (Å, º) top
O1—N21.221 (3)C15—H150.9500
O2—N21.219 (3)C16—H160.9500
N1—C11.249 (2)C3—H3A0.9800
N1—C21.480 (2)C3—H3B0.9800
N2—C141.472 (2)C3—H3C0.9800
C1—C111.476 (2)C4—H4A0.9800
C1—H10.9500C4—H4B0.9800
C2—C81.460 (7)C4—H4C0.9800
C2—C31.491 (5)C5—H5A0.9800
C2—C71.513 (11)C5—H5B0.9800
C2—C41.555 (11)C5—H5C0.9800
C2—C51.557 (10)C6—H6A0.9800
C2—C61.574 (8)C6—H6B0.9800
C11—C161.382 (3)C6—H6C0.9800
C11—C121.389 (3)C7—H7A0.9800
C12—C131.384 (3)C7—H7B0.9800
C12—H120.9500C7—H7C0.9800
C13—C141.373 (3)C8—H8A0.9800
C13—H130.9500C8—H8B0.9800
C14—C151.365 (3)C8—H8C0.9800
C15—C161.388 (3)
C1—N1—C2121.03 (17)C2—C3—H3A109.5
O2—N2—O1123.4 (2)C2—C3—H3B109.5
O2—N2—C14118.4 (2)H3A—C3—H3B109.5
O1—N2—C14118.3 (2)C2—C3—H3C109.5
N1—C1—C11121.96 (18)H3A—C3—H3C109.5
N1—C1—H1119.0H3B—C3—H3C109.5
C11—C1—H1119.0C2—C4—H4A109.5
C8—C2—N1105.4 (3)C2—C4—H4B109.5
N1—C2—C3116.7 (3)H4A—C4—H4B109.5
C8—C2—C7116.0 (9)C2—C4—H4C109.5
N1—C2—C7108.5 (10)H4A—C4—H4C109.5
N1—C2—C4107.7 (9)H4B—C4—H4C109.5
C3—C2—C4110.0 (8)C2—C5—H5A109.5
N1—C2—C5105.5 (7)C2—C5—H5B109.5
C3—C2—C5110.3 (8)H5A—C5—H5B109.5
C4—C2—C5105.9 (5)C2—C5—H5C109.5
C8—C2—C6109.6 (8)H5A—C5—H5C109.5
N1—C2—C6109.6 (8)H5B—C5—H5C109.5
C7—C2—C6107.6 (5)C2—C6—H6A109.5
C16—C11—C12119.11 (17)C2—C6—H6B109.5
C16—C11—C1120.41 (18)H6A—C6—H6B109.5
C12—C11—C1120.48 (17)C2—C6—H6C109.5
C13—C12—C11120.36 (19)H6A—C6—H6C109.5
C13—C12—H12119.8H6B—C6—H6C109.5
C11—C12—H12119.8C2—C7—H7A109.5
C14—C13—C12118.9 (2)C2—C7—H7B109.5
C14—C13—H13120.6H7A—C7—H7B109.5
C12—C13—H13120.6C2—C7—H7C109.5
C15—C14—C13122.28 (18)H7A—C7—H7C109.5
C15—C14—N2119.19 (19)H7B—C7—H7C109.5
C13—C14—N2118.5 (2)C2—C8—H8A109.5
C14—C15—C16118.48 (19)C2—C8—H8B109.5
C14—C15—H15120.8H8A—C8—H8B109.5
C16—C15—H15120.8C2—C8—H8C109.5
C11—C16—C15120.91 (19)H8A—C8—H8C109.5
C11—C16—H16119.5H8B—C8—H8C109.5
C15—C16—H16119.5
C2—N1—C1—C11180.000 (1)C12—C13—C14—C150.000 (1)
C1—N1—C2—C8172.2 (12)C12—C13—C14—N2180.000 (1)
C1—N1—C2—C34.8 (12)O2—N2—C14—C150.000 (1)
C1—N1—C2—C763.0 (10)O1—N2—C14—C15180.000 (1)
C1—N1—C2—C4129.1 (11)O2—N2—C14—C13180.000 (1)
C1—N1—C2—C5118.1 (10)O1—N2—C14—C130.000 (1)
C1—N1—C2—C654.3 (8)C13—C14—C15—C160.000 (1)
N1—C1—C11—C16180.000 (1)N2—C14—C15—C16180.000 (1)
N1—C1—C11—C120.000 (1)C12—C11—C16—C150.000 (1)
C16—C11—C12—C130.000 (1)C1—C11—C16—C15180.000 (1)
C1—C11—C12—C13180.000 (1)C14—C15—C16—C110.000 (1)
C11—C12—C13—C140.000 (1)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5B···O1i0.982.533.41 (3)149
C6—H6C···O1ii0.982.583.459 (19)149
C7—H7B···O1i0.982.563.35 (2)138
Symmetry codes: (i) x+1, y, z+1; (ii) x+1, y+1, z+1.
 

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