organic compounds
Cylopentylamine monohydrate
aSchool of Chemistry, The University of Edinburgh, King's Buildings, West Mains Road, Edinburgh EH9 3JJ, Scotland
*Correspondence e-mail: d.r.allan@ed.ac.uk
The 5H11N·H2O, is composed of molecular chains of alternating cyclopentylamine and water molecules which are linked by O—H⋯O and O—H⋯N hydrogen bonds. These chains are parallel to the monoclinic b axis and they are bridged by weaker O⋯H—N contacts, forming hydrogen-bonded layers of molecules parallel to (100).
of cylopentylamine monohydrate, CComment
The , was determined at 205 K (just below the ∼215 K melting point) as part of a series of studies on the structural behaviour of prototypical hydrogen-bonded molecular systems at conditions of either non-ambient temperature or pressure. It crystallizes in the monoclinic P21/c with one cyclopentylamine molecule and a single water molecule in the (Fig. 1).
of cylopentylamine monohydrate, (I)The water molecules are linked by O—H⋯O hydrogen bonds, forming the backbone of molecular chains which run parallel to the b axis, while O—H⋯N hydrogen bonds link the cyclopentylamine molecules to this backbone in an alternating sequence (Fig. 2 and Table 1). The lengths of these hydrogen bonds are fairly similar, while the weaker O—H⋯N hydrogen bond is correspondingly less linear. Significantly weaker O⋯H—N contacts bridge neighbouring molecular chains, forming slabs of molecules parallel to (100) (Fig. 3). One of these O⋯N distances is marginal.
Experimental
The sample of cyclopentylamine monohydrate was prepared from anhydrous starting material (of 99% purity, as received from Aldrich) and placed in a sealed glass capillary tube with an internal diameter of ca 0.2 mm. The sample was cooled using an Oxford Cryosystems low-temperature device (Cosier & Glazer, 1986) until crystallization was observed. The temperature was then cycled between 180 and 215 K, and the capillary successively translated through the gas stream, so that the sample was partially remelted and the number of crystallites reduced. The final sample, at 205 K, was composed of a small number of crystals and the reflections from the largest of these were indexed and their intensities subsequently used for structure solution.
Crystal data
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Refinement
H atoms attached to C atoms were placed in idealized positions (C—H = 0.96–1.00 Å) and allowed to ride on their parent atoms. H atoms attached to N and O atoms were located in a difference map and restrained to idealized distances and angles [N—H = 0.90 (1) Å, O—H = 0.82 (1) Å and O—H—O = 104 (1)°]. All H atoms were constrained so that Uiso(H) values were equal to 1.2Ueq of their respective parent atoms.
Data collection: SMART (Bruker, 2001); cell SAINT; data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: CAMERON (Watkin et al., 1996); software used to prepare material for publication: CRYSTALS and PLATON (Spek, 2003).
Supporting information
https://doi.org/10.1107/S1600536806005198/jh6043sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536806005198/jh6043Isup2.hkl
Data collection: SMART (Bruker, 2001); cell
SAINT; data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: CAMERON (Watkin et al., 1996); software used to prepare material for publication: CRYSTALS and PLATON (Spek, 2003).C5H11N·H2O | F(000) = 232 |
Mr = 103.16 | Dx = 1.044 Mg m−3 |
Monoclinic, P21/c | Synchrotron radiation, λ = 0.68130 Å |
Hall symbol: -P 2ybc | Cell parameters from 445 reflections |
a = 12.969 (4) Å | θ = 8–43° |
b = 4.7125 (13) Å | µ = 0.07 mm−1 |
c = 11.005 (3) Å | T = 205 K |
β = 102.614 (17)° | Cylinder, colourless |
V = 656.4 (3) Å3 | 0.20 × 0.10 × 0.10 × 0.10 (radius) mm |
Z = 4 |
Bruker SMART diffractometer | 875 reflections with I > 2σ(I) |
Curved silicon monochromator | Rint = 0.051 |
φ and ω scans | θmax = 27.5°, θmin = 4.3° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2004) | h = −17→17 |
Tmin = 0.35, Tmax = 0.99 | k = −6→6 |
5211 measured reflections | l = −14→14 |
1573 independent reflections |
Refinement on F | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.056 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.054 | Modified Chebychev polynomial (Watkin, 1994; Prince, 1982) with the coefficients 2.88, -1.06, 1.90 |
S = 1.13 | (Δ/σ)max = 0.001 |
875 reflections | Δρmax = 0.25 e Å−3 |
76 parameters | Δρmin = −0.16 e Å−3 |
5 restraints |
x | y | z | Uiso*/Ueq | ||
O1 | 1.01039 (11) | 0.1644 (3) | 0.82203 (12) | 0.0497 | |
N1 | 0.87797 (12) | 0.2930 (4) | 0.98670 (14) | 0.0473 | |
C2 | 0.76853 (14) | 0.3412 (4) | 0.92430 (17) | 0.0473 | |
C3 | 0.75593 (15) | 0.5310 (5) | 0.81296 (17) | 0.0552 | |
C6 | 0.69733 (15) | 0.4823 (6) | 1.00014 (19) | 0.0638 | |
C4 | 0.63976 (15) | 0.6122 (6) | 0.78280 (19) | 0.0630 | |
C5 | 0.60449 (16) | 0.5968 (6) | 0.9053 (2) | 0.0678 | |
H21 | 0.7390 | 0.1534 | 0.8947 | 0.0574* | |
H32 | 0.7998 | 0.7044 | 0.8354 | 0.0677* | |
H31 | 0.7771 | 0.4371 | 0.7433 | 0.0675* | |
H62 | 0.7337 | 0.6375 | 1.0504 | 0.0798* | |
H61 | 0.6744 | 0.3489 | 1.0547 | 0.0796* | |
H42 | 0.6295 | 0.8019 | 0.7461 | 0.0731* | |
H41 | 0.5999 | 0.4774 | 0.7238 | 0.0730* | |
H52 | 0.5840 | 0.7785 | 0.9321 | 0.0824* | |
H51 | 0.5454 | 0.4708 | 0.9009 | 0.0827* | |
H1 | 0.9678 (15) | 0.188 (5) | 0.8667 (18) | 0.0777* | |
H12 | 0.9016 (16) | 0.454 (3) | 1.0256 (19) | 0.0630* | |
H2 | 1.0062 (19) | 0.311 (3) | 0.7810 (19) | 0.0780* | |
H11 | 0.8823 (17) | 0.155 (4) | 1.0422 (16) | 0.0627* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0579 (8) | 0.0455 (8) | 0.0482 (8) | 0.0092 (7) | 0.0172 (6) | 0.0043 (6) |
N1 | 0.0446 (9) | 0.0530 (11) | 0.0420 (8) | 0.0072 (8) | 0.0044 (7) | 0.0023 (8) |
C2 | 0.0442 (10) | 0.0479 (11) | 0.0474 (10) | 0.0012 (9) | 0.0046 (8) | −0.0010 (9) |
C3 | 0.0486 (10) | 0.0762 (15) | 0.0403 (10) | 0.0097 (11) | 0.0089 (8) | 0.0055 (10) |
C6 | 0.0542 (12) | 0.0909 (17) | 0.0500 (11) | 0.0145 (12) | 0.0194 (9) | 0.0110 (12) |
C4 | 0.0465 (11) | 0.0831 (17) | 0.0536 (12) | 0.0070 (11) | −0.0021 (9) | 0.0056 (11) |
C5 | 0.0438 (11) | 0.0847 (17) | 0.0756 (15) | 0.0073 (11) | 0.0148 (10) | 0.0102 (13) |
O1—H1 | 0.823 (9) | C3—H31 | 0.975 |
O1—H2 | 0.822 (9) | C6—C5 | 1.510 (3) |
N1—C2 | 1.453 (2) | C6—H62 | 0.975 |
N1—H12 | 0.894 (9) | C6—H61 | 0.960 |
N1—H11 | 0.887 (9) | C4—C5 | 1.517 (3) |
C2—C3 | 1.497 (3) | C4—H42 | 0.978 |
C2—C6 | 1.526 (3) | C4—H41 | 0.973 |
C2—H21 | 0.991 | C5—H52 | 0.961 |
C3—C4 | 1.519 (3) | C5—H51 | 0.962 |
C3—H32 | 0.995 | ||
H1—O1—H2 | 103.9 (9) | C2—C6—H62 | 111.3 |
C2—N1—H12 | 106.9 (14) | C5—C6—H62 | 109.7 |
C2—N1—H11 | 110.4 (14) | C2—C6—H61 | 111.4 |
H12—N1—H11 | 109.4 (19) | C5—C6—H61 | 110.9 |
N1—C2—C3 | 113.65 (16) | H62—C6—H61 | 108.3 |
N1—C2—C6 | 117.06 (16) | C3—C4—C5 | 105.72 (16) |
C3—C2—C6 | 102.50 (17) | C3—C4—H42 | 111.0 |
N1—C2—H21 | 106.4 | C5—C4—H42 | 111.8 |
C3—C2—H21 | 107.4 | C3—C4—H41 | 109.8 |
C6—C2—H21 | 109.4 | C5—C4—H41 | 110.0 |
C2—C3—C4 | 104.77 (17) | H42—C4—H41 | 108.4 |
C2—C3—H32 | 109.5 | C4—C5—C6 | 106.34 (16) |
C4—C3—H32 | 109.5 | C4—C5—H52 | 112.7 |
C2—C3—H31 | 111.9 | C6—C5—H52 | 109.8 |
C4—C3—H31 | 112.3 | C4—C5—H51 | 112.1 |
H32—C3—H31 | 108.9 | C6—C5—H51 | 108.7 |
C2—C6—C5 | 105.32 (17) | H52—C5—H51 | 107.2 |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···N1 | 0.82 (1) | 2.01 (1) | 2.821 (2) | 172 (2) |
O1—H2···O1i | 0.82 (1) | 2.00 (1) | 2.820 (1) | 178 (3) |
N1—H11···O1ii | 0.89 (1) | 2.35 (1) | 3.137 (2) | 148 (2) |
N1—H12···O1iii | 0.89 (1) | 2.55 (1) | 3.426 (2) | 166 (2) |
Symmetry codes: (i) −x+2, y+1/2, −z+3/2; (ii) −x+2, −y, −z+2; (iii) −x+2, −y+1, −z+2. |
Acknowledgements
We thank Dr T. Prior of Daresbury Laboratory for his help during the experiment on station 9.8 at SRS. We also thank the EPSRC for funding both this project and DRA's Advanced Research Fellowship.
References
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