Download citation
Download citation
link to html
In the title compound, [ZnCl3(C3H8NO2)]·H2O, the sarcosine ligand unexpectedly coordinates to the metal in the cationic form (CH3–NH2+–CH2–COOH). The Zn atom is found to have tetrahedral coordination. A head-to-tail N—H...O hydrogen bond between the screw-related mol­ecules is present. The water mol­ecule does not participate in metal coordination, but co-operates in the packing as a donor and acceptor in hydrogen bonds to a carboxyl O atom and as a donor to a Cl atom.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680100592X/na6068sup1.cif
Contains datablocks sarzn, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680100592X/na6068Isup2.hkl
Contains datablock I

CCDC reference: 165630

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.017
  • wR factor = 0.053
  • Data-to-parameter ratio = 9.2

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of expected to reported Tmax/Tmin(RR) is > 1.10 Tmin and Tmax reported: 0.812 0.993 Tmin and Tmax expected: 0.400 0.675 RR = 1.380 Please check that your absorption correction is appropriate. General Notes
ABSTM_02 When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.679 Tmax scaled 0.675 Tmin scaled 0.552 REFLT_03 From the CIF: _diffrn_reflns_theta_max 24.97 From the CIF: _reflns_number_total 933 Count of symmetry unique reflns 933 Completeness (_total/calc) 100.00% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present yes WARNING: Large fraction of Friedel related reflns may be needed to determine absolute structure
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

Sarcosine (N-methylglycine, CH3NH2+CH2COO-), an α-amino acid present in several biologically important compounds, forms a number of addition compounds with inorganic acids and salts besides forming metallic complexes. The crystal structure of sarcosine itself was determined earlier in our laboratory (Mostad & Natarajan, 1989). The present study reports the crystal structure of a complex of sarcosine with ZnCl2, namely trichloro(sarcosinio)zinc(II) monohydrate, (I).

The sarcosine molecule exists in the cationic form with a positively charged amino group and a protonated carboxylic acid group. In the cases of complexes with metallic salts, the amino acid normally remains as a zwitterion. The formation of the zinc complex observed in the crystals may be justified by a complex series of hydrolytic equilibria involving the solvent water molecules, the Cl- ions and the sarcosine zwitterion. In the three other crystal structures of amino acid complexes with ZnCl2 known so far, amino acid molecules exist as zwitterions in glycine with ZnCl2 (Hariharan et al., 1989) and L-proline with ZnCl2 (Yukawa et al., 1985) and adopts a cationic form in L-histidine with ZnCl2 (Foster et al., 1993).

In Fig. 1, the molecular structure and the atom-numbering scheme adopted is shown. The molecular main chain deviates from planarity, the C3—N1—C2—C1 torsion angle (Table 1) indicating that the C3—N1 bond is synclinal to C2—C1. Similar observations have been made in the structures of sarcosine cadmium chloride (Krishnakumar & Natarajan, 1996), sarcosine telluric acid adduct (Averbuch-pouchot, 1988) and sarcosinium tartrate (Krishnakumar et al., 2001). C3—N1 is antiperiplanar to C2—C1 in the crystal structure of sarcosine (Mostad & Natarajan, 1989), sarcosine barium chloride (Krishnakumar et al., 1995), sarcosine sucrose (Krishnakumar & Natarajan et al., 1995), sarcosine oxalic acid monohydrate (Krishnakumar et al., 1999) and diaquabis(sarcosinato)copper(II) (Krishnakumar et al., 1994). The value of the O1—C1—O2—H1 torsion angle is -85.6°. This unusual value observed may be justified by the fact that the position of the hydrogen (H1) is determined by the two hydrogen bonds O2—H1···O1Wi (intermolecular) and N1—H1B···O2 (intramolecular), in which O2 is involved [symmetry code: (i) x + 1, y, z]. It is important to notice that both these hydrogen bonds justify the cationic status of the coordinating amino-acid ligand (see Table 2). It is interesting to notice also that the C1—O1 bond distance is remarkably longer than C1—O2 (Δ/σ = 10.25) (see Table 1), when usually in carboxylic acids, the contrary is observed [sp2O = 1.214 (19) Å and Csp2—OH = 1.308 (19) Å; Allen et al., 1987] and is justified by the coordination of O1 to metal and the hydrogen bond O2 forms with the water molecule.

Zinc is known to have both tetrahedral and octahedral coordination in crystal structures (Cingi et al., 1972). Zinc in the present structure has a tetrahedral coordination with three chlorines and a carboxyl O atom of the amino acid taking part. The angles around the Zn atom range from 104.2 (1) to 115.4 (1)°. Fig. 2 shows the packing of the molecules viewed down the b axis. A head-to-tail N—H···O hydrogen bond between the screw-related molecules is present. One of the three chlorines participates in a C—H···Cl hydrogen bond (see Table 2). The N1—H1A···O1ii and N1—H1B···Cliii hydrogen bonds form a ring of R44(12) graph-set motif (Etter et al., 1990), while the O2—H1···O1Wi and O1W—H2W···Cl3 interactions form a C22(8) chain running along [100] [symmetry codes: (ii) 2 - x, y - 1/2, -z; (iii) x, y - 1, z].

Experimental top

Colourless single crystals of the title complex were grown as transparent needles from a saturated aqueous solution containing sarcosine and zinc chloride in a stoichiometric ratio.

Refinement top

H atoms were placed at calculated positions and were allowed to ride on their respective parent atoms using SHELXL97 (Sheldrick, 1997) defaults. The positions of the water H atoms were calculated using HYDROGEN (Nardelli, 1999), with O—H = 0.85 Å, H—O—H = 107° and U(H)eq= 1.2Ueq of the parent atoms, and were not included in the refinement.

Computing details top

Data collection: CAD-4 Software (Enraf-Nonius, 1989); cell refinement: CAD-4 Software; data reduction: CAD-4 Software; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 1999); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) with the atom-numbering scheme and 50% probability displacement ellipsoids.
[Figure 2] Fig. 2. Packing diagram of the molecules of (I) in the unit cell viewed down the b axis.
'Trichloro(sarcosinium) zinc(II) monohydrate' top
Crystal data top
[ZnCl3(C3H8NO2)]·H2OF(000) = 280
Mr = 279.84Dx = 1.894 Mg m3
Dm = 1.90 (3) Mg m3
Dm measured by floatation in a mixture of carbon tetrachloride and bromoform
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 6.6181 (12) ÅCell parameters from 1017 reflections
b = 7.4989 (11) Åθ = 6–15°
c = 9.900 (4) ŵ = 3.28 mm1
β = 92.62 (2)°T = 293 K
V = 490.8 (2) Å3Plates, colourless
Z = 20.38 × 0.24 × 0.12 mm
Data collection top
Enraf-Nonius sealed tube
diffractometer
913 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.008
Graphite monochromatorθmax = 25.0°, θmin = 2.1°
ω–2θ scansh = 07
Absorption correction: ψ scan
(North et al., 1968)
k = 08
Tmin = 0.812, Tmax = 0.993l = 1111
1017 measured reflections2 standard reflections every 200 reflections
933 independent reflections intensity decay: 0.1%
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.017 w = 1/[σ2(Fo2) + (0.0239P)2 + 0.1562P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.053(Δ/σ)max < 0.001
S = 1.28Δρmax = 0.30 e Å3
933 reflectionsΔρmin = 0.24 e Å3
101 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.051 (4)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983)
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.010 (18)
Crystal data top
[ZnCl3(C3H8NO2)]·H2OV = 490.8 (2) Å3
Mr = 279.84Z = 2
Monoclinic, P21Mo Kα radiation
a = 6.6181 (12) ŵ = 3.28 mm1
b = 7.4989 (11) ÅT = 293 K
c = 9.900 (4) Å0.38 × 0.24 × 0.12 mm
β = 92.62 (2)°
Data collection top
Enraf-Nonius sealed tube
diffractometer
913 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.008
Tmin = 0.812, Tmax = 0.9932 standard reflections every 200 reflections
1017 measured reflections intensity decay: 0.1%
933 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.017H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.053Δρmax = 0.30 e Å3
S = 1.28Δρmin = 0.24 e Å3
933 reflectionsAbsolute structure: Flack (1983)
101 parametersAbsolute structure parameter: 0.010 (18)
1 restraint
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
Zn10.67915 (6)0.40483 (7)0.26537 (4)0.02369 (18)
Cl10.86420 (18)0.66062 (16)0.26939 (12)0.0336 (3)
Cl20.37724 (17)0.45863 (16)0.15902 (13)0.0368 (3)
Cl30.64383 (18)0.30575 (18)0.47779 (12)0.0374 (3)
O10.8288 (5)0.2418 (4)0.1452 (3)0.0281 (7)
O21.0144 (5)0.1081 (5)0.3096 (3)0.0294 (7)
H11.10070.18150.33360.044*
N11.2102 (5)0.1049 (7)0.1347 (4)0.0318 (8)
H1A1.22840.18720.07030.038*
H1B1.15740.16110.20530.038*
C10.9639 (6)0.1327 (6)0.1911 (4)0.0213 (9)
C21.0611 (7)0.0262 (7)0.0814 (5)0.0318 (11)
H2A0.95620.03600.02840.038*
H2B1.12750.10760.02160.038*
C31.4107 (7)0.0335 (7)0.1794 (6)0.0383 (12)
H3A1.46550.03410.10720.057*
H3B1.50010.13040.20320.057*
H3C1.39660.04230.25650.057*
O1W0.1661 (4)0.4117 (6)0.4685 (3)0.0297 (6)
H1W0.09810.37890.53490.036*
H2W0.20620.51860.48510.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.0218 (3)0.0221 (3)0.0272 (3)0.0014 (2)0.00139 (16)0.0002 (2)
Cl10.0324 (6)0.0266 (6)0.0423 (6)0.0071 (5)0.0061 (5)0.0030 (5)
Cl20.0278 (6)0.0390 (8)0.0426 (6)0.0047 (4)0.0079 (5)0.0031 (5)
Cl30.0374 (6)0.0450 (8)0.0305 (6)0.0116 (6)0.0085 (5)0.0086 (5)
O10.0320 (17)0.0245 (16)0.0280 (16)0.0076 (14)0.0032 (13)0.0010 (14)
O20.0337 (18)0.0299 (17)0.0250 (17)0.0040 (14)0.0031 (13)0.0014 (14)
N10.0332 (19)0.0196 (18)0.043 (2)0.003 (2)0.0091 (15)0.002 (2)
C10.022 (2)0.018 (2)0.025 (2)0.0030 (17)0.0043 (16)0.0023 (17)
C20.035 (2)0.032 (3)0.028 (2)0.010 (2)0.0010 (19)0.007 (2)
C30.028 (2)0.041 (3)0.046 (3)0.002 (2)0.005 (2)0.002 (2)
O1W0.0319 (15)0.0305 (15)0.0268 (14)0.0015 (18)0.0032 (11)0.0016 (18)
Geometric parameters (Å, º) top
Zn1—O11.999 (3)N1—H1B0.9000
Zn1—Cl22.2519 (13)C1—C21.515 (6)
Zn1—Cl32.2525 (14)C2—H2A0.9700
Zn1—Cl12.2751 (13)C2—H2B0.9700
O1—C11.280 (5)C3—H3A0.9600
O2—C11.219 (5)C3—H3B0.9600
O2—H10.8200C3—H3C0.9600
N1—C21.473 (6)O1W—H1W0.850 (3)
N1—C31.480 (6)O1W—H2W0.857 (4)
N1—H1A0.9000
O1—Zn1—Cl2106.53 (10)O2—C1—C2120.2 (4)
O1—Zn1—Cl3115.41 (10)O1—C1—C2113.3 (4)
Cl2—Zn1—Cl3111.58 (5)N1—C2—C1113.2 (4)
O1—Zn1—Cl1104.18 (10)N1—C2—H2A108.9
Cl2—Zn1—Cl1108.82 (5)C1—C2—H2A108.9
Cl3—Zn1—Cl1109.91 (5)N1—C2—H2B108.9
C1—O1—Zn1122.5 (3)C1—C2—H2B108.9
C1—O2—H1109.5H2A—C2—H2B107.7
C2—N1—C3116.3 (4)N1—C3—H3A109.5
C2—N1—H1A108.2N1—C3—H3B109.5
C3—N1—H1A108.2H3A—C3—H3B109.5
C2—N1—H1B108.2N1—C3—H3C109.5
C3—N1—H1B108.2H3A—C3—H3C109.5
H1A—N1—H1B107.4H3B—C3—H3C109.5
O2—C1—O1126.5 (4)H1W—O1W—H2W107.0 (3)
Cl2—Zn1—O1—C1152.6 (3)Zn1—O1—C1—C2178.5 (3)
Cl3—Zn1—O1—C128.2 (3)C3—N1—C2—C177.7 (5)
Cl1—Zn1—O1—C192.4 (3)O2—C1—C2—N11.4 (6)
Zn1—O1—C1—O22.7 (6)O1—C1—C2—N1177.5 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1···O1Wi0.822.212.919 (5)144
N1—H1A···O1ii0.902.213.001 (5)146
N1—H1B···O20.902.482.726 (5)96
N1—H1B···Cl1iii0.902.463.224 (4)142
O1W—H1W···O2iv0.852.452.943 (5)118
O1W—H1W···Cl1v0.852.543.220 (4)138
O1W—H2W···Cl3iv0.862.393.246 (4)173
C2—H2A···Cl2vi0.972.823.702 (5)152
Symmetry codes: (i) x+1, y, z; (ii) x+2, y1/2, z; (iii) x, y1, z; (iv) x+1, y+1/2, z+1; (v) x+1, y1/2, z+1; (vi) x+1, y1/2, z.

Experimental details

Crystal data
Chemical formula[ZnCl3(C3H8NO2)]·H2O
Mr279.84
Crystal system, space groupMonoclinic, P21
Temperature (K)293
a, b, c (Å)6.6181 (12), 7.4989 (11), 9.900 (4)
β (°) 92.62 (2)
V3)490.8 (2)
Z2
Radiation typeMo Kα
µ (mm1)3.28
Crystal size (mm)0.38 × 0.24 × 0.12
Data collection
DiffractometerEnraf-Nonius sealed tube
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.812, 0.993
No. of measured, independent and
observed [I > 2σ(I)] reflections
1017, 933, 913
Rint0.008
(sin θ/λ)max1)0.594
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.017, 0.053, 1.28
No. of reflections933
No. of parameters101
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.30, 0.24
Absolute structureFlack (1983)
Absolute structure parameter0.010 (18)

Computer programs: CAD-4 Software (Enraf-Nonius, 1989), CAD-4 Software, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 1999), SHELXL97.

Selected bond and torsion angles (º) top
O1—Zn1—Cl2106.53 (10)C2—N1—C3116.3 (4)
O1—Zn1—Cl3115.41 (10)O2—C1—O1126.5 (4)
Cl2—Zn1—Cl3111.58 (5)O2—C1—C2120.2 (4)
O1—Zn1—Cl1104.18 (10)O1—C1—C2113.3 (4)
Cl2—Zn1—Cl1108.82 (5)N1—C2—C1113.2 (4)
Cl3—Zn1—Cl1109.91 (5)
C3—N1—C2—C177.7 (5)O1—C1—C2—N1177.5 (4)
O2—C1—C2—N11.4 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1···O1Wi0.822.212.919 (5)144
N1—H1A···O1ii0.902.213.001 (5)146
N1—H1B···O20.902.482.726 (5)96
N1—H1B···Cl1iii0.902.463.224 (4)142
O1W—H1W···O2iv0.852.452.943 (5)118
O1W—H1W···Cl1v0.852.543.220 (4)138
O1W—H2W···Cl3iv0.862.393.246 (4)173
C2—H2A···Cl2vi0.972.823.702 (5)152
Symmetry codes: (i) x+1, y, z; (ii) x+2, y1/2, z; (iii) x, y1, z; (iv) x+1, y+1/2, z+1; (v) x+1, y1/2, z+1; (vi) x+1, y1/2, z.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds