research communications
of trirubidium citrate from laboratory X-ray powder diffraction data and DFT comparison
aAtlantic International University, Honolulu HI, USA, and bIllinois Institute of Technology, Chicago IL, USA
*Correspondence e-mail: kaduk@polycrystallography.com
The +·C6H5O73−, has been solved and refined using laboratory X-ray powder diffraction data, and optimized using density functional techniques. The two independent Rb+ cations are seven- and eight-coordinate, with bond-valence sums of 0.99 and 0.92 valence units. The coordination polyhedra share edges and corners to form a three-dimensional framework. The only hydrogen bond is an intramolecular one between the hydroxy group and the central carboxylate, with graph set S(5). The hydrophobic methylene groups lie in pockets in the framework.
of trirubidium citrate, 3RbKeywords: crystal structure; powder diffraction; density functional theory; citrate; rubidium.
1. Chemical context
In the course of a systematic study of the crystal structures of Group 1 (alkali metal) citrate salts to understand the anion's conformational flexibility, ionization, coordination tendencies, and hydrogen bonding, we have determined several new crystal structures. Most of the new structures were solved using X-ray powder diffraction data (laboratory and/or synchrotron), but single crystals were used where available. The general trends and conclusions about the sixteen new compounds and twelve previously characterized structures are being reported separately (Rammohan & Kaduk, 2017a). Eight of the new structures – NaKHC6H5O7, NaK2C6H5O7, Na3C6H5O7, NaH2C6H5O7, Na2HC6H5O7, K3C6H5O7, Rb2HC6H5O7, and Rb3C6H5O7(H2O) – have been published recently (Rammohan & Kaduk, 2016a,b,c,d,e, 2017b,c; Rammohan et al., 2016), and two additional structures – KH2C6H5O7 and KH2C6H5O7(H2O)2 – have been communicated to the CSD (Kaduk & Stern, 2016a,b).
2. Structural commentary
The . The root-mean-square deviation of the non-hydrogen atoms in the Rietveld-refined and DFT-optimized structures is 0.052 Å (Fig. 2). The largest difference is 0.086 Å, at C1. The excellent agreement between the two structures is strong evidence that the experimental structure is correct (van de Streek & Neumann, 2014). This discussion uses the DFT-optimized structure. Most of the bond lengths, bond angles, and torsion angles fall within the normal ranges indicated by a Mercury Mogul geometry check (Macrae et al., 2008). The C3—C2—C1 angle of 116.5° is flagged as unusual [Z-score = 2.3; average = 112.7 (16)°]. The C2—C3—C2 angle of 106.0° is also flagged as unusual [Z-score = 2.5; average = 109.6 (14)°]. This hygroscopic compound was measured in situ, so perhaps slightly unusual geometry could be expected.
of the title compound is shown in Fig. 1The citrate anion occurs in the trans,trans-conformation, which is one of the two low-energy conformations of an isolated citrate. The central carboxylate group and the hydroxy group lie on a mirror plane. The terminal carboxylate O11 atom and the central carboxylate O15 atom chelate to Rb19, O11 and the central carboxylate O16 atom chelate to a second Rb19, and the terminal carboxylate O12 atom and the O17 hydroxy group chelate to a third Rb19. The terminal O11–C1–C12 carboxylate group acts as a bidentate ligand to Rb20. The Mulliken overlap populations and atomic charges indicate that the metal-oxygen bonding is ionic.
The Bravais–Friedel–Donnay–Harker (Bravais, 1866; Friedel, 1907; Donnay & Harker, 1937) morphology suggests that we might expect blocky morphology for trirubidium citrate, with {011} as the principal faces. A 4th-order spherical harmonic texture model was included in the The texture index was 1.001, indicating that was not significant for this rotated flat-plate specimen.
3. Supramolecular features
The two independent Rb+ cations, Rb19 and Rb20, are seven- and eight-coordinate, with bond-valence sums of 0.99 and 0.92 valence units, respectively. The coordination polyhedra share edges and corners to form a three-dimensional network (Fig. 3). The only hydrogen bond is an intramolecular one (Table 1) between the hydroxy group and the central carboxylate, with graph set S(5). The Mulliken overlap population indicates, by the correlation in Rammohan & Kaduk (2017a), that this hydrogen bond contributes 12.6 kcal mol−1 to the crystal energy.
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4. Database survey
Details of the comprehensive literature search for citrate structures are presented in Rammohan & Kaduk (2017a). A search of the cell of trirubidium citrate monohydrate in the Cambridge Structural Database (Groom et al., 2016) (increasing the default tolerance from 1.5 to 2.0%) yielded 221 hits, but combining the cell search with the elements C, H, O, and Rb only yielded no hits.
5. Synthesis and crystallization
A portion of Rb3(C6H5O7)(H2O)1 (Rammohan & Kaduk, 2017c) was heated at 14 K min−1 to 463 K and held at that temperature for 10 min. The white solid was immediately transferred to a glass vial to cool.
6. Refinement
Crystal data, data collection and structure . Diffraction data are displayed in Fig. 4. The white solid was ground in a mortar and pestle, blended with NIST 640b Si internal standard in order to verify the calibrated goniometer zero error, packed into a standard Bruker D2 sample cell and protected from the atmosphere by an 8 µm thick Kapton window attached to the cell with Vaseline. The powder pattern indicated that the sample was still hydrated, so the blend was re-heated at 17 K min−1 to 483 (10) K and held for 10 min. Re-measuring the powder pattern indicated that a new phase had formed.
details are summarized in Table 2The pattern was indexed using DICVOL06 (Louër & Boultif, 2007) on a primitive orthorhombic cell having a = 7.904, b = 12.701, c = 10.773 Å, and V = 1081.8 Å3. These lattice parameters are 2.6, 1.8, and 3.3% larger than those of K3C6H5O7 (Rammohan & Kaduk, 2016e), and the volume is 7.9% larger. The compound was assumed to be isostructural to the K analogue (space group Pna21), and the coordinates of tripotassium citrate were used as the initial model for the Rietveld refinement.
Pseudo-Voigt profile coefficients were as parameterized in Thompson et al. (1987) with profile coefficients for Simpson's rule integration of the pseudo-Voigt function according to Howard (1982). The asymmetry correction of Finger et al. (1994) was applied, and microstrain broadening by Stephens (1999). The structure was refined by the using GSAS/EXPGUI (Larson & Von Dreele, 2004; Toby, 2001). All C—C and C—O bond lengths were restrained, as were all bond angles. The hydrogen atoms were included at fixed positions, which were recalculated during the course of the using Materials Studio (Dassault Systèmes, 2014). The Uiso value of the C atom in the central part of the citrate anion, and the C and O atoms on the exterior, were constrained to be equal, and the Uiso valuess of the hydrogen atoms were constrained to be 1.3 times those of the atoms to which they are attached.
The structure refined satisfactorily (Rwp = 0.0301 and reduced χ2 = 1.828 for 69 variables) in Pna21 (the of the K analogue), but both the ADDSYM module of PLATON (Spek, 2009) and the Find Symmetry module of Materials Studio (Dassault Systèmes, 2014) suggested the presence of an additional centre of symmetry, and that the was Pnma (with a transformation of axes). The tolerance on the search was 0.12 Å. Because lower residuals were obtained with fewer parameters, we believe that Pnma is the correct space group.
7. DFT calculations
After the CRYSTAL14 (Dovesi et al., 2014). The basis sets for the C, H, and O atoms were those of Peintinger et al. (2012), and the basis set for Rb was that of Schoenes et al. (2008). The calculation was run on eight 2.1 GHz Xeon cores (each with 6 Gb RAM) of a 304-core Dell Linux cluster at IIT, used 8 k-points and the B3LYP functional, and took about seven h. The Uiso values from the were assigned to the optimized fractional coordinates.
a density functional geometry optimization (fixed experimental unit cell) was carried out usingSupporting information
https://doi.org/10.1107/S2056989017001086/vn2123sup1.cif
contains datablocks RAMM077C_publ, ramm077c_DFT, RAMM077C_overall, RAMM077C_phase_1, RAMM077C_phase_2, RAMM077C_p_01. DOI:Supporting information file. DOI: https://doi.org/10.1107/S2056989017001086/vn2123RAMM077C_phase_1sup2.cml
Supporting information file. DOI: https://doi.org/10.1107/S2056989017001086/vn2123RAMM077C_phase_2sup3.cml
Data collection: DIFFRAC.Measurement (Bruker, 2009) for RAMM077C_phase_1. Molecular graphics: DIAMOND (Crystal Impact, 2015) for RAMM077C_phase_1. Software used to prepare material for publication: publCIF (Westrip, 2010) for RAMM077C_phase_1.
3Rb+·C6H5O73− | c = 12.6986 (3) Å |
Mr = 445.50 | V = 1082.08 (7) Å3 |
Orthorhombic, Pnma | Z = 4 |
Hall symbol: -P 2ac 2n | Dx = 2.735 Mg m−3 |
a = 7.9096 (2) Å | T = 300 K |
b = 10.7733 (3) Å |
x | y | z | Uiso*/Ueq | ||
C1 | 0.8481 (8) | 0.5192 (4) | 0.1236 (8) | 0.0129 (18)* | |
C2 | 0.9284 (10) | 0.6373 (4) | 0.0836 (8) | 0.028 (5)* | |
C3 | 0.8129 (13) | 0.75 | 0.1037 (8) | 0.028 (5)* | |
C6 | 0.6630 (17) | 0.75 | 0.0251 (11) | 0.0129 (18)* | |
H7 | 1.03549 | 0.6517 | 0.12302 | 0.036 (6)* | |
H8 | 0.9452 | 0.62963 | −0.00257 | 0.036 (6)* | |
O11 | 0.6988 (9) | 0.4914 (7) | 0.0961 (6) | 0.0129 (18)* | |
O12 | 0.9397 (9) | 0.4386 (5) | 0.1695 (6) | 0.0129 (18)* | |
O15 | 0.6865 (17) | 0.75 | −0.0763 (10) | 0.0129 (18)* | |
O16 | 0.5218 (18) | 0.75 | 0.0658 (10) | 0.0129 (18)* | |
O17 | 0.7506 (12) | 0.75 | 0.2090 (9) | 0.0129 (18)* | |
H18 | 0.61955 | 0.75 | 0.19313 | 0.017 (2)* | |
Rb19 | 0.3442 (2) | 0.97103 (16) | 0.12323 (13) | 0.0255 (6)* | |
Rb20 | 0.1377 (4) | 0.25 | 0.29027 (16) | 0.0255 (6)* |
C1—C2 | 1.5102 (11) | O15—Rb20viii | 3.074 (13) |
C1—O11 | 1.267 (3) | O15—Rb20ix | 3.053 (14) |
C1—O12 | 1.272 (3) | O16—C6 | 1.231 (19) |
C2—C1 | 1.5102 (11) | O16—Rb19 | 2.859 (8) |
C2—C3 | 1.5410 (11) | O16—Rb19i | 2.859 (8) |
C2—H7 | 0.996 (9) | O16—Rb20viii | 3.719 (13) |
C2—H8 | 1.105 (10) | O17—C3 | 1.425 (3) |
C3—C2 | 1.5410 (11) | O17—H18 | 1.056 (9) |
C3—C2i | 1.5410 (11) | O17—Rb19ii | 3.280 (8) |
C3—C6 | 1.5502 (11) | O17—Rb19x | 3.280 (8) |
C3—O17 | 1.425 (3) | H18—O17 | 1.056 (9) |
C6—C3 | 1.5502 (11) | Rb19—O11i | 2.855 (7) |
C6—O15 | 1.300 (16) | Rb19—O11xi | 3.766 (7) |
C6—O16 | 1.231 (19) | Rb19—O11xii | 2.815 (8) |
H7—C2 | 0.996 (9) | Rb19—O12xiii | 3.395 (7) |
H8—C2 | 1.105 (10) | Rb19—O12xi | 2.906 (7) |
O11—C1 | 1.267 (3) | Rb19—O15vii | 3.074 (3) |
O11—Rb19i | 2.855 (7) | Rb19—O16 | 2.859 (8) |
O11—Rb19ii | 3.766 (7) | Rb19—O17xi | 3.280 (8) |
O11—Rb19iii | 2.815 (8) | Rb20—O11xiv | 3.013 (7) |
O11—Rb20iv | 3.013 (7) | Rb20—O11xv | 3.013 (7) |
O12—C1 | 1.272 (3) | Rb20—O12xvi | 2.989 (6) |
O12—Rb19v | 3.395 (7) | Rb20—O12xvii | 2.989 (6) |
O12—Rb19ii | 2.906 (7) | Rb20—O12xiv | 3.178 (7) |
O12—Rb20vi | 2.989 (6) | Rb20—O12xv | 3.178 (7) |
O12—Rb20iv | 3.178 (7) | Rb20—O15xviii | 3.074 (13) |
O15—C6 | 1.300 (16) | Rb20—O15ix | 3.053 (14) |
O15—Rb19vii | 3.074 (3) | Rb20—O16xviii | 3.719 (13) |
O15—Rb19iii | 3.074 (3) | ||
C2—C1—O11 | 119.9 (3) | Rb19xix—O17—Rb19xxi | 93.1 (3) |
C2—C1—O12 | 119.3 (3) | O11i—Rb19—O11xxii | 89.3 (2) |
C2—C1—Rb19xix | 108.2 (5) | O11i—Rb19—O12xiii | 155.0 (2) |
O11—C1—O12 | 119.7 (3) | O11i—Rb19—O12xxiii | 78.8 (2) |
C1—C2—C3 | 111.0 (3) | O11i—Rb19—O15vii | 85.2 (3) |
C1—C2—H7 | 108.7 (5) | O11i—Rb19—O16 | 66.7 (3) |
C1—C2—H8 | 108.7 (7) | O11i—Rb19—O17xxiii | 113.8 (3) |
C3—C2—H7 | 107.3 (6) | O11xxii—Rb19—O12xiii | 92.01 (17) |
C3—C2—H8 | 107.1 (5) | O11xxii—Rb19—O12xxiii | 154.38 (18) |
H7—C2—H8 | 114.0 (8) | O11xxii—Rb19—O15vii | 73.9 (3) |
C2—C3—C2i | 104.0 (6) | O11xxii—Rb19—O16 | 82.6 (3) |
C2—C3—C6 | 110.3 (3) | O11xxii—Rb19—O17xxiii | 132.2 (2) |
C2—C3—O17 | 111.2 (3) | O12xiii—Rb19—O12xxiii | 89.55 (15) |
C2i—C3—C6 | 110.3 (3) | O12xiii—Rb19—O15vii | 71.3 (3) |
C2i—C3—O17 | 111.2 (3) | O12xiii—Rb19—O16 | 138.2 (3) |
C6—C3—O17 | 109.9 (3) | O12xiii—Rb19—O17xxiii | 83.3 (2) |
C3—C6—O15 | 121.9 (10) | O12xxiii—Rb19—O15vii | 82.5 (3) |
C3—C6—O16 | 115.1 (10) | O12xxiii—Rb19—O16 | 112.5 (3) |
O15—C6—O16 | 123.0 (11) | O12xxiii—Rb19—O17xxiii | 73.4 (2) |
C1—O11—Rb19i | 148.1 (7) | O15vii—Rb19—O16 | 143.5 (3) |
C1—O11—Rb19xii | 113.8 (6) | O15vii—Rb19—O17xxiii | 144.9 (3) |
C1—O11—Rb20xx | 102.8 (3) | O16—Rb19—O17xxiii | 70.9 (3) |
Rb19i—O11—Rb19xii | 90.7 (2) | O11xxiv—Rb20—O11xxv | 119.3 (3) |
Rb19i—O11—Rb20xx | 84.7 (2) | O11xxiv—Rb20—O12xvi | 156.4 (3) |
Rb19xii—O11—Rb20xx | 112.8 (3) | O11xxiv—Rb20—O12xvii | 75.1 (2) |
C1—O12—Rb19v | 105.2 (4) | O11xxiv—Rb20—O12xxiv | 41.44 (11) |
C1—O12—Rb19xix | 92.2 (6) | O11xxiv—Rb20—O12xxv | 110.8 (2) |
C1—O12—Rb20vi | 175.9 (6) | O11xxiv—Rb20—O15xviii | 82.52 (19) |
C1—O12—Rb20xx | 94.7 (3) | O11xxiv—Rb20—O15ix | 110.68 (17) |
Rb19v—O12—Rb19xix | 107.8 (2) | O11xxv—Rb20—O12xvi | 75.1 (2) |
Rb19v—O12—Rb20vi | 77.87 (16) | O11xxv—Rb20—O12xvii | 156.4 (3) |
Rb19v—O12—Rb20xx | 156.85 (19) | O11xxv—Rb20—O12xxiv | 110.8 (2) |
Rb19xix—O12—Rb20vi | 84.22 (19) | O11xxv—Rb20—O12xxv | 41.44 (11) |
Rb19xix—O12—Rb20xx | 82.72 (18) | O11xxv—Rb20—O15xviii | 82.52 (19) |
Rb20vi—O12—Rb20xx | 82.91 (15) | O11xxv—Rb20—O15ix | 110.68 (17) |
C6—O15—Rb19vii | 100.4 (3) | O12xvi—Rb20—O12xvii | 85.7 (3) |
C6—O15—Rb19xii | 100.4 (3) | O12xvi—Rb20—O12xxiv | 155.67 (15) |
C6—O15—Rb20viii | 115.2 (9) | O12xvi—Rb20—O12xxv | 92.37 (19) |
C6—O15—Rb20ix | 161.1 (10) | O12xvi—Rb20—O15xviii | 81.1 (2) |
Rb19vii—O15—Rb19xii | 155.8 (5) | O12xvi—Rb20—O15ix | 77.4 (2) |
Rb19vii—O15—Rb20viii | 80.0 (2) | O12xvii—Rb20—O12xxiv | 92.37 (19) |
Rb19vii—O15—Rb20ix | 82.1 (3) | O12xvii—Rb20—O12xxv | 155.67 (15) |
Rb19xii—O15—Rb20viii | 80.0 (2) | O12xvii—Rb20—O15xviii | 81.1 (2) |
Rb19xii—O15—Rb20ix | 82.1 (3) | O12xvii—Rb20—O15ix | 77.4 (2) |
Rb20viii—O15—Rb20ix | 83.6 (3) | O12xxiv—Rb20—O12xxv | 79.5 (2) |
C6—O16—Rb19 | 123.6 (2) | O12xxiv—Rb20—O15xviii | 122.6 (2) |
C6—O16—Rb19i | 123.6 (2) | O12xxiv—Rb20—O15ix | 78.5 (2) |
Rb19—O16—Rb19i | 112.8 (5) | O12xxv—Rb20—O15xviii | 122.6 (2) |
C3—O17—H18 | 99.2 (8) | O12xxv—Rb20—O15ix | 78.5 (2) |
C3—O17—Rb19xix | 122.1 (3) | O15xviii—Rb20—O15ix | 150.6 (4) |
C3—O17—Rb19xxi | 122.1 (3) |
Symmetry codes: (i) x, −y+3/2, z; (ii) x+1/2, −y+3/2, −z+1/2; (iii) −x+1, y−1/2, −z; (iv) x+1/2, −y+1/2, −z+1/2; (v) x+1, −y+3/2, z; (vi) x+1, y, z; (vii) −x+1, −y+2, −z; (viii) −x+1/2, y+1/2, z−1/2; (ix) −x+1, −y+1, −z; (x) x+1/2, y, −z+1/2; (xi) x−1/2, −y+3/2, −z+1/2; (xii) −x+1, y+1/2, −z; (xiii) x−1, −y+3/2, z; (xiv) x−1/2, −y+1/2, −z+1/2; (xv) x−1/2, y, −z+1/2; (xvi) x−1, y, z; (xvii) x−1, −y+1/2, z; (xviii) −x+1/2, y−1/2, z+1/2; (xix) x+3/2, −y+5/2, −z+3/2; (xx) x+3/2, −y+3/2, −z+3/2; (xxi) x+3/2, y, −z+3/2; (xxii) −x+1, y+3/2, −z; (xxiii) x+1/2, −y+5/2, −z+3/2; (xxiv) x+1/2, −y+3/2, −z+3/2; (xxv) x+1/2, y, −z+3/2. |
Si | V = 160.20 Å3 |
Mr = 28.09 | Z = 8 |
Cubic, Fd3m | Dx = 2.329 Mg m−3 |
Hall symbol: -F 4vw 2vw | T = 300 K |
a = 5.43105 Å |
x | y | z | Uiso*/Ueq | ||
Si1 | 0.125 | 0.125 | 0.125 | 0.01* |
Si1—Si1i | 2.3517 | Si1—Si1iii | 2.3517 |
Si1—Si1ii | 2.3517 | Si1—Si1iv | 2.3517 |
Si1i—Si1—Si1ii | 109.4712 | Si1ii—Si1—Si1iii | 109.4712 |
Si1i—Si1—Si1iii | 109.4712 | Si1ii—Si1—Si1iv | 109.4712 |
Si1i—Si1—Si1iv | 109.4712 | Si1iii—Si1—Si1iv | 109.4712 |
Symmetry codes: (i) x+1/4, y+1/4, −z; (ii) −z, x+1/4, y+1/4; (iii) y+1/4, −z, x+1/4; (iv) −x, −y, −z. |
C6H5O7Rb3 | b = 10.7733 Å |
Mr = 445.50 | c = 12.6986 Å |
Orthorhombic, Pnma | V = 1082.08 Å3 |
a = 7.9096 Å | Z = 4 |
x | y | z | Uiso*/Ueq | ||
C1 | 0.85652 | 0.51237 | 0.11762 | 0.01290* | |
C2 | 0.92710 | 0.63666 | 0.08156 | 0.02780* | |
H7 | 1.04404 | 0.65330 | 0.12425 | 0.03610* | |
H8 | 0.95879 | 0.63156 | −0.00199 | 0.03610* | |
O11 | 0.70573 | 0.48606 | 0.09469 | 0.01290* | |
O12 | 0.95620 | 0.44175 | 0.16822 | 0.01290* | |
Rb19 | 0.34329 | 0.97183 | 0.12807 | 0.02550* | |
C3 | 0.81408 | 0.75000 | 0.09868 | 0.02780* | |
C6 | 0.65846 | 0.75000 | 0.02369 | 0.01290* | |
O15 | 0.68502 | 0.75000 | −0.07431 | 0.01290* | |
O16 | 0.51559 | 0.75000 | 0.06782 | 0.01290* | |
O17 | 0.75259 | 0.75000 | 0.20645 | 0.01290* | |
H18 | 0.62975 | 0.75000 | 0.19609 | 0.01680* | |
Rb20 | 0.14960 | 0.25000 | 0.29368 | 0.02550* |
C1—C2 | 1.521 | C3—C2i | 1.529 |
C1—O11 | 1.260 | C3—C6 | 1.556 |
C1—O12 | 1.270 | C3—O17 | 1.452 |
C2—C3 | 1.529 | C6—O15 | 1.262 |
C2—H7 | 1.087 | C6—O16 | 1.261 |
C2—H8 | 1.092 | O17—H18 | 0.981 |
Symmetry code: (i) x, −y+3/2, z. |
Acknowledgements
We thank Andrey Rogachev for the use of computing resources at IIT.
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