CRYSTAL STRUCTURE OF POTASSIUM BICHROMATE K₂Cr₂O₇ (LOPEZITE)
CRYSTALLOGRAPHY
Submitted 1967-01-01 | SovietRxiv: ru-196701.61935 | Translated from Russian

Abstract Generated abstract

The paper reports an X-ray crystallographic determination of the triclinic structure of potassium bichromate, K2Cr2O7, lopezite, using single-crystal diffraction data and three-dimensional Patterson and electron-density syntheses. The structure is refined in the centrosymmetric space group P1bar, with four independent chromium and four independent potassium positions, and consists of paired CrO4 tetrahedra forming Cr2O7 diortho groups together with potassium coordination polyhedra of varying coordination numbers. The authors describe two types of quadrupoles of potassium polyhedra linked through chromium tetrahedra into a three-dimensional framework, and argue that lopezite represents a chromate analogue of diorthosilicate structural motifs. They also note that the X-ray centrosymmetry contrasts with reported morphological asymmetry, interpreting this as a case of lower macroscopic than microscopic symmetry.

Full Text

UDC 548.736

CRYSTALLOGRAPHY

E. A. KUZ’MIN, V. V. ILYUKHIN, Academician N. V. BELOV

CRYSTAL STRUCTURE OF POTASSIUM BICHROMATE K₂Cr₂O₇ (LOPEZITE)

Single crystals of chrompik—the triclinic modification of K₂Cr₂O₇—were isolated from solution and kindly placed at our disposal by E. N. Slavnova. The unit-cell parameters \((a = 7.52;\ b = 13.40;\ c = 7.40\ \text{Å};\ \alpha = 98^\circ,\ \beta = 90^\circ 50',\ \gamma = 96^\circ 10';\ Z = 4)\) are in agreement with those previously reported for natural lopezite \((^1)\). The good solubility of potassium bichromate in water made it possible without difficulty to obtain specimens of almost spherical shape. The experimental material for the X-ray structural analysis consisted of 2600 nonzero reflections \(hk0—hk8\) and \(0kl—3kl\) (MoK\(_\alpha\) radiation, \(\max \sin \vartheta/\lambda = 0.85\ \text{Å}^{-1}\)).

A detailed analysis of the three-dimensional Patterson synthesis (together with the well-established absence of a piezoelectric effect) made it possible to carry out the analysis under the assumption of a centrosymmetric variant of the structure. In interpreting the three-dimensional Patterson function, the most effective proved to be the “method of combining points of a vector system into \(n\) identical \(n\)-gons” \((^{2,8})\), which made it possible to localize the Cr and K atoms. Further refinement of the structure proceeded at the stage of electron-density syntheses \(\rho(xyz)\). At this stage (an isotropic thermal correction, averaged over groups of atoms, was introduced: \(B_{\mathrm{Cr}} \approx 1.1\ \text{Å}^2,\ B_{\mathrm{K}} \approx 1.4\ \text{Å}^2,\ B_{\mathrm{O}} \approx 1.7\ \text{Å}^2\)) the discrepancy factor \(R_{hkl}\) over the entire volume of the sphere of reflections is equal to 16.1%*. The coordinates of the basis atoms at the achieved value of the \(R\)-factor are given in Table 1. The centrosymmetric structure (space group \(P\bar{1}\)) is characterized by 66 parameters.

Table 1

Coordinates of the basis atoms in the structure of K₂Cr₂O₇

Atoms \(x/a\) \(y/b\) \(z/c\) Atoms \(x/a\) \(y/b\) \(z/c\)
Cr₁ 0.192 0.086 0.207 O₄ 0.299 0.160 0.358
Cr₂ 0.768 0.108 0.592 O₅ 0.387 0.849 0.291
Cr₃ 0.846 0.583 0.188 O₆ 0.095 0.804 0.450
Cr₄ 0.574 0.387 0.182 O₇ 0.327 0.954 0.583
K₁ 0.668 0.139 0.104 O₈ 0.697 0.476 0.067
K₂ 0.232 0.152 0.751 O₉ 0.483 0.301 0.047
K₃ 0.344 0.636 0.302 O₁₀ 0.705 0.332 0.301
K₄ 0.084 0.341 0.340 O₁₁ 0.416 0.434 0.306
O₁ 0.325 0.057 0.030 O₁₂ 0.005 0.543 0.313
O₂ 0.025 0.135 0.136 O₁₃ 0.721 0.650 0.324
O₃ 0.107 0.978 0.290 O₁₄ 0.933 0.645 0.037

Each of the four crystallographically independent chromium atoms is surrounded by four oxygen atoms in a tetrahedron. The Cr tetrahedra are joined in pairs into diortho groups Cr₂O₇. Among the Cr—O distances in each diortho group, two elongated ones stand out (Cr₁—O₃ and Cr₂—O₃, Cr₃—O₈ and Cr₄—O₈, respectively) to the common atom O in the diortho group at

* The noncentrosymmetric variant of the structure, differing from the selected one only by a small displacement of the light atoms, did not give a substantial improvement of the \(R\)-factor (15.8%), but led to a sharp worsening of the interatomic distances.

against the background of the other six:

\[ \begin{gathered} \text{Dichromate group I }(\mathrm{Cr}_1-\mathrm{Cr}_2):\quad \mathrm{Cr}_1-\mathrm{O}_3 = 1.72_5\ \text{\AA} \\ \mathrm{Cr}_2-\mathrm{O}_3 = 1.85_6\ \text{\AA} \\ \text{with the remaining } \mathrm{Cr}_1,\ \mathrm{Cr}_2-\mathrm{O}=1.53\text{--}1.68\ \text{\AA}, \\ \text{Dichromate group II }(\mathrm{Cr}_3-\mathrm{Cr}_4):\quad \mathrm{Cr}_3-\mathrm{O}_8 = 1.84_2\ \text{\AA} \\ \mathrm{Cr}_4-\mathrm{O}_8 = 1.74_5\ \text{\AA} \\ \text{with the remaining } \mathrm{Cr}_3,\ \mathrm{Cr}_4-\mathrm{O}=1.51\text{--}1.63\ \text{\AA}, \\ \text{Angles: }(\mathrm{I})\ \mathrm{Cr}_1-\mathrm{O}_3-\mathrm{Cr}_2 = 127^\circ \\ (\mathrm{II})\ \mathrm{Cr}_3-\mathrm{O}_8-\mathrm{Cr}_4 = 122^\circ . \end{gathered} \]

The O—O distances in the tetrahedra are: 2.58–2.79 Å (Cr₁ tetrahedron), 2.48–2.87 Å (Cr₂ tetrahedron), 2.45–2.84 Å (Cr₃ tetrahedron), 2.67–2.90 Å (Cr₄ tetrahedron).

The large K cations also occupy 4 independent crystallographic positions and, as usual, have an ill-defined environment: K₁ and K₂ in seven-vertex polyhedra, which occur more frequently for moderately large

Fig. 1. K-bichromate K₂Cr₂O₇. Arrangement of K cations in the yz projection. A quadrupole of 4 seven-vertex polyhedra around K is highlighted. Common edges are marked by triple lines

Fig. 1. K bichromate $\mathrm{K}_2\mathrm{Cr}_2\mathrm{O}_7$. Arrangement of K cations in the $yz$ projection. A quadrupole of 4 seven-vertex polyhedra around K is highlighted. Common edges are marked by triple lines

($r_i = 0.97$–0.99 Å) Na and Ca cations: this is a combination of a trigonal prism and a semioctahedron “attached” to one of the rectangular faces of the prism. If the K₁ polyhedron is sufficiently compact: 6 distances K₁—O are 2.67–2.78 Å (with an average of 2.73 Å) and one anion is removed to 2.97 Å, then the K₂ polyhedron may be characterized as very loose: 6 neighbors are removed to distances of 2.78–3.00 Å (average 2.91 Å), and only one distance is much shorter and almost equal to the sum of the ionic radii: 2.69 Å.

The coordination of K₃ is sixfold, which for such a large cation is a rather rare case. The coordination polyhedron is a flattened octahedron, noted earlier for the still larger Rb ($^4,^5$). The distances K₃—O = 2.73–2.93 Å, with an average of 2.84 Å (anions more than 3.10 Å away were not included in the coordination sphere). Finally, K₄ is located in the eight-vertex polyhedron already described by us ($^6$), encountered in compounds of the type $\mathrm{M}_n\mathrm{BX}_4$, where $\mathrm{M}=\mathrm{K}, \mathrm{Rb}, \mathrm{Cs}, \mathrm{NH}_4, \mathrm{Ba}$; $\mathrm{B}=\mathrm{S}, \mathrm{Be}, \mathrm{Cr}, \mathrm{P}$ and $\mathrm{X}=\mathrm{F}, \mathrm{O}$. Seven distances K₄—O vary within the narrow interval 2.82–2.95 Å around an average of 2.88 Å, and again one (the eighth) is substantially shorter: 2.69 Å.

In the structural motif of $K_2Cr_2O_7$ (lopezite) one can distinguish two quadrupoles of K-polyhedra. The first quadrupole is composed of two pairs of hemivertex polyhedra: $K_1$ and $K_2^{**}$, $K_2$ and $K_1^{**}$*, situated (each pair) at approximately the same height (along the $a$ axis):

$$ K_1^{**}=0.20,\qquad K_2=0.14,\qquad K_2^{**}=0.46,\qquad K_1=0.40 \qquad (\text{Fig. 1}). $$

The hemivertex polyhedra are joined along a common edge into pairs, which condense into foursomes also along edges. At the midpoint of the edge common to $K_1$ and

Fig. 2. K-bichromate K2Cr2O7. Second quadrupole of K-polyhedra: two octahedra and two octads in the same yz projection. Common edges are marked by triple lines

Fig. 2. K-bichromate $K_2Cr_2O_7$. The second quadrupole of K-polyhedra: two octads and two octahedra in the same $yz$ projection. Common edges are marked by triple lines.

$K_1^{**}$ there is a center of symmetry; $K_1$ has common edges with $K_2$ and $K_2^{**}$; analogously $K_1^{**}$ has common edges with $K_2$ and $K_2^{**}$, but $K_2$ and $K_2^{**}$ are not directly connected to one another. The planar quadrupole (the plane of the quadrupole $\sim(\bar{1}12)$) of $K_1—K_2$ hemivertex polyhedra is connected with translationally identical ones not directly, but through Cr-tetrahedra: (the $Cr_1$ tetrahedron in the direction $a[100]$ and $Cr_2$ in the direction $c[001]$).

In the quadrupole of $(2K_3+2K_4)$-polyhedra the four K cations: $K_3$, $K_3^{**}$, $K_4$ and $K_4^{**}$ are situated almost in the plane $(1\bar{1}1)$. The polyhedra are combined into a quadrupole as follows: $K_4$ has common edges with $K_3$ and $K_3^{**}$, and likewise $K_4^{**}$ with $K_3$ and $K_3^{**}$; however, if $K_3$ and $K_3^{**}$ have no common elements, then $K_4$ and $K_4^{**}$ have an additional bond—a common edge passing through the center of symmetry (Fig. 2). As in the case of the first quadrupole, the second quartet of K-polyhedra is not connected with translationally identical ones directly. Here too the Cr-tetrahedra ($Cr_3$ and $Cr_4$ tetrahedra) act as the linking elements.

When the quadrupoles of both kinds are joined into a three-dimensional framework, the $K_3$ octahedron from the second quartet has only one common edge with the $K_2$ hemivertex polyhedron of the first quadrupole, whereas the $K_4$ octad is connected (also by one edge) with the $K_1$ hemivertex polyhedron, but already of a quadrupole translationally identical to the first.

In the space filled with bulky polyhedra, the remaining voids are occupied by $Cr_2O_7$ diortho groups (encountered in chromates for the first time). It may be noted that in the structure of lopezite (K-bichromate) the relationship between K and Cr $(CrO_4)$ repeats that which is characteristic of Ca(Na) and Si$(SiO_4)$

* Here and below, $K_n^{**}$ denotes an atom related to the basic $K_n$ by reflection in a center of symmetry.

in silicates: the relative sizes of the K- and Cr-polyhedra are such that not a single Cr-tetrahedron, but the diortho group \(\mathrm{Cr_2O_7}\) (Fig. 3), is stretched over the edge of a large seven-vertex polyhedron around K, and K bichromate may be regarded as the first deciphered analogue of the diorthosilicates of Chapter II of crystal chemistry, not only of silicates,* but also of chromates, and in general of compounds with the complex anion \(\mathrm{BX_4}\).

Fig. 3. \(\mathrm{K_2Cr_2O_7}\). \(yz\) projection with separated diortho groups \([\mathrm{Cr_2O_7}]\)

Fig. 3. \(\mathrm{K_2Cr_2O_7}\). \(yz\) projection with separated diortho groups \([\mathrm{Cr_2O_7}]\)

In a number of works the “morphological” absence of a center of symmetry in \(\mathrm{K_2Cr_2O_7}\) is emphasized, in contradiction to the purely dry result of the X-ray investigation. Apparently, K bichromate is yet another example of the manifestation in a macrocrystal of lower symmetry in comparison with the microsymmetry established by X-ray structural analysis (hypomorphy, hyposymmetry according to Kleber \((^{9,10})\)).

Institute of Crystallography
Academy of Sciences of the USSR

Received
6 I 1967

REFERENCES

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\(^10\) W. Kleber, Wissenschaftliche Zs. d. Humboldt Universität zu Berlin, 5, No. 1 (1956).

* Cf. also the crystal-chemical similarity and analogy with silicates of Chapter II of phosphates (\(^7\)), borates (\(^8\)), fluoroberyllates (\(^{3,6}\)).

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CRYSTAL STRUCTURE OF POTASSIUM BICHROMATE K₂Cr₂O₇ (LOPEZITE)