Home Physical Sciences Synthesis, single-crystal structure determination and Raman spectra of the tricyanomelaminates NaA5[C6N9]2 · 4 H2O (A = Rb, Cs)
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Synthesis, single-crystal structure determination and Raman spectra of the tricyanomelaminates NaA5[C6N9]2 · 4 H2O (A = Rb, Cs)

  • Olaf Reckeweg EMAIL logo , Armin Schulz and Francis J. DiSalvo
Published/Copyright: March 4, 2016
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Abstract

Transparent colorless crystals of NaA5[C6N9]2 · 4 H2O (A = Rb, Cs) were obtained by blending aqueous solutions of Na3[C6N9] and RbF or CsF, respectively, and subsequent evaporation of the water under ambient conditions. Both compounds crystallize in the space group P21/m (no. 11) with the cell parameters a = 815.56(16), b = 1637.7(4) and c = 1036.4(3) pm, and β = 110.738(12)° for NaRb5[C6N9]2 · 4 H2O and a = 843.32(6), b = 1708.47(11) and c = 1052.42(7) pm, and β = 112.034(2)° for NaCs5[C6N9]2 · 4 H2O, respectively. Raman spectra of the title compounds complement our results.

1 Introduction

The compound Na3[C6N9] · 3 H2O, a water-soluble salt containing the tricyanomelaminate anion (called from now on [TCM]) has been known since 1938 [1]. Unfortunately, next to a short sketch of the synthesis (spontaneous trimerization of sodium dicyanamide (dca), Na[N(CN)2], in aqueous solution) only the lattice parameters, the symmetry and some thoughts concerning the possible crystallographic positions are given. Some 60 years later [2], Schnick et al. reported an alternative synthesis (heat induced trimerization of anhydrous Na[dca] and subsequent recrystallization in aqueous solution) and performed a complete structure analysis on single crystals. Additionally, IR spectra and DSC/TG data were collected. Based on these results, Schnick et al. expanded the knowledge about this class of compounds by synthesizing the anhydrous alkali metal salts A3[TCM] (A = Na [3], K and Rb [4]) and some of the hydrated species with the stoichiometries A3[TCM] · H2O (A = K and Rb) [5] and Rb[H2C6N9] · ½ H2O [6] which were also structurally characterized including a study of their thermal behavior. Li3[TCM] has been synthesized [7, 8], but no structural information is reported, while the cesium salt is only mentioned as unpublished results (ref. [6] in ref. [9]).

While attempting to synthesize Cs3[TCM] by a metathesis reactions in aqueous solution, we serendipitously found crystals of NaCs5[TCM]2 · 4 H2O. In follow-up experiments we were able to reproduce our results and to also synthesize NaRb5[TCM]2 · 4 H2O. We report here the results of the single-crystal structure determination and the Raman spectra of both compounds and compare them with literature data.

2 Experimental section

2.1 Synthesis

All manipulations were performed under normal atmospheric conditions. Na3[TCM] was obtained by sealing gram portions of Na[dca] (Alfa Aesar, 96 %) under vacuum in silica tubes and heating the container up to 500 °C with subsequent annealing at this temperature for 6 h. The thus obtained Na3[TCM] was dissolved with the respective alkali metal fluoride (Aldrich, 99 %) in a stoichiometric ratio of 2:5 (overall mass: 0.5 g) in 10 mL deionized, boiling water. The water was allowed to evaporate at r.t. leaving small cubes of NaF and brick-like cuboids of the title compounds behind.

An analog approach to synthesize NaK5[TCM]2 · 4 H2O or similar mixed alkali metal compounds has been unsuccessful so far.

2.2 Crystallographic studies

Crystals of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O were selected by their habit and immersed in polybutene oil (Aldrich, Mn ~ 320, isobutylene > 90 %) for single-crystal selection under a polarization microscope. Single crystals were mounted in a drop of polybutene sustained in a plastic loop, and placed onto the goniometer. A cold stream of nitrogen (T = 223(2) K) froze the polybutene oil, thus keeping the crystal stationary and protected from oxygen and moisture in the air. Intensity data were collected with a Bruker X8 Apex II diffractometer equipped with a 4 K CCD detector and graphite-monochromatized MoKα radiation (λ = 71.073 pm). The intensity data were manipulated with the program package [10] that came with the diffractometer. An empirical absorption correction was applied using sadabs [11]. The program shelxs-97 [12, 13] found the positions of the respective alkali metal(s) with the help of Direct Methods. The positions of the carbon and nitrogen atoms and of carbon, nitrogen and oxygen atoms, respectively, were apparent from the positions of the highest electron density on the difference Fourier maps resulting from the first refinement cycles by full-matrix least-squares calculations on F2 with shelxl-97 [14, 15]. The positions of the hydrogen atoms could not be found and refined reliably. Doing further refinement cycles with all atoms being refined unrestrained the refinement converged and resulted in stable models for the respective crystal structure. Crystallographic details are described in Table 1. Atomic coordinates and equivalent isotropic displacement coefficients are shown in Table 2 for NaRb5[TCM]2 · 4 H2O and in Table 3 for NaCs5[TCM]2 · 4 H2O. Table 4 displays selected interatomic distances and angles of the title compounds.

Table 1

Summary of single-crystal X-ray diffraction structure determination data of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O.

CompoundNaRb5[C6N9]2 · 4 H2ONaCs5[C6N9]2 · 4 H2O
Mr918.71155.9
Crystal colorTransparent colorlessTransparent colorless
Crystal shapeIrregular thin plateIrregular plate
Crystal size, mm30.07×0.06×0.030.12×0.10×0.07
Crystal systemMonoclinicMonoclinic
Space group (no.); ZP21/m (11); 2P21/m (11); 2
Lattice parameters:
a, pm815.56(16)843.32(6)
b, pm1637.4(4)1708.47(11)
c, pm1036.4(3)1052.42(7)
β, deg110.738(12)112.034(2)
V, Å31294.6(5)1405.56(16)
Dcalcd, g cm−32.362.73
F(000), e8681048
m, mm−19.56.5
DiffractometerBruker X8 Apex II equipped with a 4 K CCD

MoKα; 71.073; graphite

ϕ and ω scans; 223(2)
Radiation; l, pm; monochromator
Scan mode; T, K
Ranges
2 qmax, deg61.1166.31
h, k, l–11 → 10, –23 → 23, –14 → 13–12 → 11, –25 → 26, –15 → 16
Data correctionLp, sadabs [11]
Transmission: min./max.0.597/0.7460.566/0.747
Reflections: measured/unique15881/403321977/5498
Unique reflections: Fo > 4s (Fo)26314491
Rint/Rσ0.0566/0.06070.0327/0.0313
Refined parameters203203
R1a/wR2b/GoFc (all refl.)0.0729/0.0914/0.9720.0398/0.0712/1.022
Factors x/y (weighting scheme)b0.041/00.0359/0
Max. shift, esd, last refinement cycle<0.0001<0.0002
Δρfin (max, min), e Å−31.41 (97 pm to H11),

–0.93 (192 pm to N11)
2.53 (143 pm to H11),

–0.88 (145 pm to Cs4)
CSD number430375430376

aR1 = Σ ||Fo|–|Fc||/Σ |Fo|; bwR2 = [Σw(Fo2Fc2)2/Σ(wFo2)2]1/2; w = 1/[σ2(Fo2) + (xP)2 + yP], where P = [(Fo2) + 2Fc2]/3 and x and y are constants adjusted by the program; cGoF(S) = [Σw(Fo2Fc2)2/(np)]1/2, with n being the number of reflections and p being the number of refined parameters.

Table 2

Atomic coordinates and equivalent isotropic displacement parametersa of NaRb5[TCM]2 · 4 H2O.

AtomWyckoff sitexyzUeq (pm2)a
Rb12e0.47146(7)¼0.02090(6)286(1)
Rb22e0.14802(6)¼0.51012(6)273(1)
Rb32d½½0287(1)
Rb44f0.23267(4)0.50508(2)0.43935(4)270(1)
Na2e0.5963(3)¼0.4449(2)240(5)
N14f0.2295(4)0.6347(2)–0.0350(3)207(7)
N24f0.0782(4)0.3763(2)0.0804(3)249(7)
N34f0.1246(4)0.6261(2)0.1528(3)201(6)
C14f0.2537(4)0.6341(2)0.1006(4)190(7)
N114f0.5768(4)0.3565(2)–0.1834(3)234(7)
C124f0.4629(4)0.6408(2)0.3168(4)199(8)
N134f0.4863(4)0.3602(2)0.5618(3)259(7)
C24f0.0614(4)0.6291(2)–0.1212(4)206(8)
N214f–0.0244(4)0.3708(2)0.2603(3)257(7)
C224f–0.1617(5)0.3638(2)0.2973(3)228(8)
N234f0.2743(4)0.6436(2)0.6584(4)317(8)
C34f0.0392(4)0.3794(2)–0.0576(4)223(8)
N314f0.1801(4)0.3875(2)–0.0987(3)267(7)
C324f–0.1458(4)0.5996(2)0.2314(4)219(8)
N334f0.1313(4)0.4134(2)0.6550(4)295(8)
O12e–0.1307(5)¼0.6403(4)296(10)
H11b2e–0.195(10)¼0.559(9)740c
H12b2e–0.121(11)¼0.707(8)740c
O22e0.3204(5)¼0.2558(5)345(10)
H21b4f0.267(7)0.289(3)0.211(5)863c
O34f0.3998(4)0.4524(2)0.2407(3)356(8)
H31b4f0.466(8)0.419(4)0.272(6)891c
H32b4f0.284(7)0.428(4)0.182(6)891c

aUeq is defined as a third of the orthogonalized Uij tensors; bSite occupancy was restrained to 2/3; cThe isotropic displacement factor of the hydrogen atom was constrained to the equivalent displacement factor of oxygen as the last unconstrained atom as suggested in ref. [13].

Table 3

Atomic coordinates and equivalent isotropic displacement parametersa of NaCs5[TCM]2 · 4 H2O.

AtomWyckoff sitexyzUeq (pm2)a
Cs12e0.47125(3)¼0.02091(3)248(1)
Cs22e0.15772(3)¼0.52806(2)242(1)
Cs32d½½0278(1)
Cs44f0.23247(2)0.50395(1)0.44584(2)258(1)
Na2e0.6023(2)¼0.4503(2)246(3)
N14f0.2252(3)0.6367(1)–0.0386(2)202(5)
N24f0.0747(3)0.3731(1)0.0910(2)228(5)
N34f0.1215(3)0.6286(1)0.1433(2)186(4)
C14f0.2485(3)0.6364(2)0.0952(3)177(5)
N114f0.5853(3)0.3567(1)–0.1812(2)216(5)
C124f0.4507(3)0.6423(2)0.3141(3)183(5)
N134f0.5011(3)0.3574(1)0.5672(2)239(5)
C24f0.0616(4)0.6326(2)–0.1270(3)202(5)
N214f–0.0281(3)0.3660(1)0.2653(2)242(5)
C224f–0.1643(4)0.3578(2)0.2971(3)239(6)
N234f0.2728(4)0.6502(2)0.6616(3)334(6)
C34f0.0380(3)0.3767(2)–0.0458(3)195(5)
N314f0.1761(3)0.3855(2)–0.0828(2)257(5)
C324f–0.1453(3)0.6012(2)0.2125(3)224(5)
N334f0.1385(3)0.4133(2)0.6773(3)296(6)
O12e–0.1333(4)¼0.6521(3)283(7)
H11b2e–0.200(9)¼0.589(7)708c
H12b2e–0.114(10)¼0.710(7)708c
O22e0.3155(4)¼0.2700(3)304(7)
H21b4f0.269(6)0.280(2)0.233(4)761c
O34f0.4051(3)0.4446(2)0.2480(3)360(6)
H31b4f0.491(7)0.408(3)0.293(5)900c
H32b4f0.315(7)0.424(3)0.211(6)900c

aUeq is defined as a third of the orthogonalized Uij tensors; bSite occupancy was restrained to 2/3; cThe isotropic displacement factor of the hydrogen atom was constrained to the equivalent displacement factor of oxygen as the last unconstrained atom as suggested in ref. [13].

Table 4

Selected bond lengths (pm) and angles (deg) of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O.

NaRb5[TCM]2 · 4 H2ONaCs5[TCM]2 · 4 H2O
Rb1–N1 2×304.7(3)Cs1–N1 2×318.1(2)
N11 2×309.1(3)N11 2×327.7(12)
O2309.3(5)O2326.3(4)
N31 2×318.9(3)N31 2×327.7(2)
Rb2–O1302.7(4)Cs2–O1318.3(3)
N33 2×309.5(4)N33 2×323.5(3)
N21 2×316.5(3)N21 2×328.3(2)
N13 2×318.0(3)N13 2×332.0(3)
O2339.8(5)O2344.4(4)
Rb3–O3 2×299.1(3)Cs3–O3 2×314.9(3)
N1 2×304.9(3)N1 2×320.7(2)
N31 2×305.9(3)N31 2×320.4(3)
N11 2×322.0(3)N11 2×334.4(2)
Rb4–O3297.1(3)Cs4–O3312.3(3)
N33304.1(3)N33322.6(3)
N33308.1(3)N33322.9(3)
N13310.8(3)N13329.6(2)
N23314.1(4)N23330.7(3)
N21314.9(3)N21329.5(2)
N13318.4(4)N13330.3(3)
N3341.7(3)N3364.8(2)
Na–O2240.4(5)Na–O2245.1(4)
O1242.2(5)O1243.5(4)
N23 2×246.9(4)N23 2×251.7(3)
N13 2×251.1(4)N13 2×252.9(3)
N1–C1134.9(5)N1–C1134.7(3)
C2134.9(4)C2134.6(3)
N2–C2135.1(4)N2–C2134.2(4)
C3135.2(5)C3135.5(3)
N3–C1134.9(4)N3–C1135.3(3)
C3135.3(5)C3135.5(3)
C12–N11130.4(5)C12–N11131.6(3)
N13117.7(5)N13116.0(3)
C22–N21131.1(5)C22–N21132.0(4)
N23116.9(5)N23115.9(4)
C32–N31132.0(5)C32–N31131.0(4)
N33116.0(5)N33116.7(4)
C1–N1–C2115.4(3)C1–N1–C2115.6(2)
C2–N2–C3115.1(3)C2–N2–C3115.1(2)
C1–N3–C3115.1(3)C1–N3–C3115.1(2)
N11–C12–N13174.1(4)N11–C12–N13173.3(3)
N21–C22–N23174.2(4)N21–C22–N23173.2(3)
N31–C32–N33173.9(4)N31–C32–N33171.8(3)

Further details of the crystal structure investigation(s) may be obtained from FIZ Karlsruhe, 76344 Eggenstein-Leopoldshafen, Germany (fax: (+49)7247-808-666; E-mail: crysdata@fiz-karlsruhe.de, on quoting the deposition number CSD-430375 for NaRb5[TCM]2 · 4 H2O and CSD-430376 for NaCs5[TCM]2 · 4 H2O.

2.3 Raman spectroscopy

The single-crystals of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O were sealed in thin-walled glass capillaries. Raman spectroscopic investigations were performed on a microscope laser Raman spectrometer (Jobin Yvon, 4 mW, equipped with a HeNe laser with an excitation line at λ = 632.817 nm, 50× magnification, 8 × 240 s accumulation time). The results are displayed in Fig. 1, the exact frequencies and their assigned modes are shown in Table 5.

Fig. 1: Raman spectra of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O. On the vertical axis, Raman intensities are displayed in arbitrary units.
Fig. 1:

Raman spectra of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O. On the vertical axis, Raman intensities are displayed in arbitrary units.

Table 5

Raman and IR dataa of different [C6N9]3– compounds compared to Na3[TCM] · 3 H2O and Na3[TCM] (ref. [2]). Raman results are given as bold face numbers; all numbers are given in cm−1.

NaRb5[TCM]2 · 4 H2ONaCs5[TCM]2 · 4 H2ONa3[TCM] · 3 H2O (ref. [2])Rb3[TCM] · H2O (ref. [5])
329 m326
δas(ring-sub.)376 w374 w383.3376 w
δs(lattice)500 w499 w498 w
δs(N–C≡N)521 m519 s513.5519 w
νs(N–C≡N)538 m535 m570.8/589.4538 w
δs(ring)976 m973 m998.8980 w
νas(ring-N)1382 m1383 m1397.01386 w
νas(ring-N)1402 m1399 m1397.01395 vs
νs(ring-N)1486 m1477 m1517.51486 w, br
δ(H–O–H) + νas(O–H)1635 vw1629 vw1616.71626 m
νs(C≡N)2135 m2129 m2127 w
νs(C≡N)2164 vs2155 vs2193.12158 vs

as, Strong; vs, very strong; m, medium; w, weak; vw, very weak weak; br, broad.

3 Results and discussion

3.1 Raman spectra

The frequencies obtained from the Raman spectra of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O compare well to the vibrational frequencies reported in the literature for Na3[TCM] · 3 H2O [2] or Rb3 [TCM] · H2O [5] (Table 5) and confirm therefore the presence of the tricyanomelaminate anion.

3.2 The crystal structures of NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O

NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O are found to be isotypic. Generally speaking, the crystal structure is somewhat typical for [TCM] containing compounds. It is built up from layers of sodium and rubidium or cesium cations, respectively, and of the [TCM] anion. The tricyanomelaminate anion consists of a six-membered triazine ring with three N–C–N substituents each bound to a carbon atom of the triazine ring (Fig. 2). One of the nearly linear substituents is turned by 180°, thereby reducing the molecular symmetry of the anion from C3h to Cs – if one neglects the slight deviations from planarity. All C–N bond lengths and angles (Table 5) are in the expected range when compared to the lengths and angles of similar compounds. The sodium atom is coordinated in an octahedral fashion by four nitrogen and two trans-positioned water molecules. The four crystallographically independent Rb or Cs atoms, respectively, are eight-fold coordinated in an irregular fashion by nitrogen and/or oxygen atoms. The crystal water molecules are found both in the plane of the alkali metal cations, but also displaced from the cation layers (both up and down) completing the coordination sphere of the cations (Fig. 3).

Fig. 2: The [TCM] anion as found in NaA5[TCM]2 · 4 H2O (A = Rb or Cs).
Fig. 2:

The [TCM] anion as found in NaA5[TCM]2 · 4 H2O (A = Rb or Cs).

Fig. 3: Non-perspective view on the unit cell of NaA5[TCM]2 · 4 H2O parallel to the crystallographic c axis (C, black circles; N, white circles; O, black circles; H, white circles; Na, white ellipsoids; Rb or Cs, gray ellipsoids).
Fig. 3:

Non-perspective view on the unit cell of NaA5[TCM]2 · 4 H2O parallel to the crystallographic c axis (C, black circles; N, white circles; O, black circles; H, white circles; Na, white ellipsoids; Rb or Cs, gray ellipsoids).

4 Conclusion

The compounds NaRb5[TCM]2 · 4 H2O and NaCs5[TCM]2 · 4 H2O were synthesized, their crystal structures have been determined and the Raman spectra of both title compounds recorded. The Raman data as well as the crystal structure are similar to that of previously reported alkali metal tricyanomelaminate compounds such as A3[TCM] (A = Na [3], K and Rb [4]), A3[TCM] · H2O (A = K and Rb) [5] or Rb[H2C6N9] · ½ H2O [6]. Due to the employed synthesis, no pure product could be acquired so far, which prevented the acquirement of DSC/TG data as yet.


Corresponding author: Olaf Reckeweg, Baker Laboratory, Department of Chemistry and Chemical Biology, Cornell University, Ithaca, NY 14853-1301, USA, Fax: +1-607-255-4137, E-mail:

References

[1] J. L. Hoard, J. Am. Chem. Soc. 1938, 80, 1147.Search in Google Scholar

[2] B. Jürgens, W. Milius, P. Morys, W. Schnick, Z. Anorg. Allg. Chem. 1998, 624, 91.Search in Google Scholar

[3] B. Jürgens, E. Irran, J. Schneider, W. Schnick, Inorg. Chem. 2000, 39, 665.Search in Google Scholar

[4] E. Irran, B. Jürgens, W. Schnick, Chem. Eur. J. 2001, 7, 5372.Search in Google Scholar

[5] E. Irran, B. Jürgens, W. Schnick, Solid State Sci. 2002, 4, 1305.10.1016/S1293-2558(02)00012-2Search in Google Scholar

[6] B. Jürgens, H. Höppe, W. Schnick, Z. Anorg. Allg. Chem. 2004, 630, 35.10.1002/zaac.200300286Search in Google Scholar

[7] A. P. Purdy, E. Houser, C. F. George, Polyhedron1997, 16, 3671.10.1016/S0277-5387(97)00097-1Search in Google Scholar

[8] O. Reckeweg, F. J. DiSalvo, A. Schulz, B. Blaschkowski, S. Jagiella, Th. Schleid, Z. Anorg. Allg. Chem. 2014, 640, 851.10.1002/zaac.201300586Search in Google Scholar

[9] B. Jürgens, H. A. Höppe, E. Irran, J. Schneider, W. Schnick, Inorg. Chem. 2002, 41, 4849.10.1021/ic025800kSearch in Google Scholar

[10] apex2 (version 1.22), saint plus,xprep (version 6.14), Software for the CCD system, Bruker Analytical X-ray Instruments Inc., Madison, Wisconsin (USA) 2004.Search in Google Scholar

[11] G. M. Sheldrick, sadabs, Program for Empirical Absorption Correction of Area Detector Data, University of Göttingen, Göttingen (Germany) 2003.Search in Google Scholar

[12] G. M. Sheldrick, shelxs-97, Program for the Solution of Crystal Structures, University of Göttingen, Göttingen (Germany) 1997.Search in Google Scholar

[13] G. M. Sheldrick, Acta Crystallogr. 1990, A46, 467.10.1107/S0108767390000277Search in Google Scholar

[14] G. M. Sheldrick, shelxl-97, Program for the Refinement of Crystal Structures, University of Göttingen, Göttingen (Germany) 1997.Search in Google Scholar

[15] G. M. Sheldrick, Acta Crystallogr. 2008, A64, 112.10.1107/S0108767307043930Search in Google Scholar

Received: 2016-1-15
Accepted: 2016-1-26
Published Online: 2016-3-4
Published in Print: 2016-4-1

©2016 by De Gruyter

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