Sodium chloride, also known as salt or halite, is an ionic compound with the chemical formula NaCl, representing a 1:1 ratio of sodium and chloride ions. With molar masses of 22.99 and 35.45 g/mol respectively, 100 g of NaCl contain 39.34 g Na and 60.66 g Cl.
The salient features of its structure are:
- Chloride ions are ccp type of arrangement, i.e., it contains chloride ions at the corners and at the center of each face of the cube.
- Sodium ions are so located that there are six chloride ions around it. This equivalent to saying that sodium ions occupy all the octahedral sites.
- As there is only one octahedral site for every chloride ion, the stoichiometry is 1 : 1.
- It is obvious from the diagram that each chloride ion is surrounded by six sodium ions which are disposed towards the corners of a regular octahedron. We may say that cations and anions are present in equivalent positions and the structure has 6 : 6 coordination.
- The structure of sodium chloride consists of eight ions a unit cell, four are Na+ ions and the other four are Cl– ions.
In this structure, each corner ion is shared between eight unit cells, each ion a face of the cell by two cells, each ion on a edge by four cells and the ion inside the cell belongs entirely to that unit cell.
So the positions of the ions are the followings (with Na at the center of axis) :
Na+ (0 0 0) (1/2 1/2 0) (1/2 0 1/2) (0 1/2 1/2)
Cl– (0 1/2 0) (1/2 0 0) (0 0 1/2) (1/2 1/2 1/2)
With this information we can compute the Structure Factor Fhkl, assuming the scattering factors of Na and Cl are expressed by fNa and fCl, respectively. The structure factors determines the amplitude and the phase of the diffracted beams. The intensity (measured value) is linked to the squared module of the Structure Factor.
Ihkl ∝ | Fhkl|2
For a perfect crystal the lattice gives the reciprocal lattice, which determines the positions (angles) of diffracted beams, and the basis gives the structure factor which determines the amplitude and phase of the diffracted beams for the (hkl) crystal plane.
where the sum is over all atoms in the unit cell, are the positional coordinates of the jth atom, and is the scattering factor of the jth atom. The coordinates have the directions and dimensions of the lattice vectors . That is, (0,0,0) is at the lattice point, the origin of position in the unit cell; (1,0,0) is at the next lattice point along and (1/2, 1/2, 1/2) is at the body center of the unit cell. defines a reciprocal lattice point at which corresponds to the real-space plane defined by the Miller indices.
Face-centered cubic (FCC)
The FCC lattice is a Bravais lattice, and its Fourier transform is a body-centered cubic lattice. However to obtain without this shortcut, consider an FCC crystal with one atom at each lattice point as a primitive or simple cubic with a basis of 4 atoms, at the origin (0, 0, 0) and at the three adjacent face centers, (1/2,1/2,0), (0,1/2,1/2) and (1/2,0,1/2). Equation becomes
with the result
The most intense diffraction peak from a material that crystallizes in the FCC structure is typically the (111). Films of FCC materials like gold tend to grow in a (111) orientation with a triangular surface symmetry. A zero diffracted intensity for a group of diffracted beams (here, of mixed parity) is called a systematic absence.
NaCl is composed by the Na+ FCC unit cell plus the displace Cl– FCC unit cell, thus the calculation of is similar to the pure FCC case and becomes the following :
Fhkl = [1 + (-1)h+k + (-1)k+l + (-1)h+l][fNa + (-1)hfCl]
that can be tabulated for each hkl triplet :
It can be noted that the main peaks are the reflections from 200 and 220 planes, whilst the reflection from the plane 111 is present but it is weak because it arises from the scattering difference from the two types of ion.
Most of the alkali halides, alkaline earth oxides, and sulphides exhibit this type of structure.
The first test performed was the complete 10° to 120° scan of the crystal, using the non-filtered tube emission, configured at 30 KV and 80 μA. The result is shown in the graph below, in which the Bragg reflections for the Kα and Kβ lines of the copper are present. The reflections were highlighted for the order n = 1, n = 2 and n = 3.
For the crystallographic analysis of sodium chloride we used the Nickel filter to have monochromatic emission in correspondence only to the Kα line of the copper at 0.1542 nm. We examined the NaCl crystal in the two orientations allowed by our protractor, corresponding to the crystal orientations (200) and (020). The images below show the setup of the measurements and the Bragg peaks obtained, both at about 31° 30′. Having obtained the same results, within the experimental error, is the demonstration that we are dealing with a crystal of cubic structure.
By rotating by 45° the crystal, together with the crystal holder, with respect to the movable arm, we sought the presence of reflections corresponding to the planes (nn0), the graph below shows the result obtained with the Bragg peak corresponding to the plane (220).
Further experimental investigations can be made by diffraction from powders or with the Laue technique having a small thickness single crystal available, but at the moment we have to settle for what we have already obtained and proceed to the “resolution” of the crystal with the available data.
“Solving” the Crystal Structure
From the checks made, described above, it has been established that the sodium chloride crystal has a cubic structure. The variants of the cubic lattice are the followings :
- Primitive cubic
- Body-centered cubic (bcc)
- Face-centered cubic (fcc)
- Diamond (or Zincblende)
each of these is characterized by a specific pattern of reflections. We verify that the experimentally obtained Bragg peaks are compatible with the fcc structure. Meanwhile for a cubic crystal with lattice constant a, the distance d between adjacent lattice planes (hkl) is computed as follows:
By combining the Bragg condition for the reflections with the above written equation we get :
From which we deduce that, for the diffraction peaks, the ratio remains constant and this allows to verify the type of cubic structure and to determine the lattice constant a, if the wavelength λ of the X-rays is known. For the measured Bragg reflections we can compile the following table for which we hypothesize an fcc structure, using the following formulas:
- λ = 0.1542 nm
- d = λ / 2senθ
- a = d x √(h2+k2+l2)
The values of a obtained are congruent with each other, a sign of the correctness of the initial hypotheses. They are also close to the correct value which turns out to be 0.564 nm.