Skip to main content
Physics LibreTexts

9.3: Bonding in Crystalline Solids

  • Page ID
    4543
  • [ "article:topic", "authorname:openstax", "body-centered cubic (BCC)", "face-centered cubic (FCC)", "lattice", "repulsion constant", "simple cubic", "license:ccby" ]

    Beginning in this section, we study crystalline solids, which consist of atoms arranged in an extended regular pattern called a lattice. Solids that do not or are unable to form crystals are classified as amorphous solids. Although amorphous solids (like glass) have a variety of interesting technological applications, the focus of this chapter will be on crystalline solids.

    Atoms arrange themselves in a lattice to form a crystal because of a net attractive force between their constituent electrons and atomic nuclei. The crystals formed by the bonding of atoms belong to one of three categories, classified by their bonding: ionic, covalent, and metallic. Molecules can also bond together to form crystals; these bonds, not discussed here, are classified as molecular. Early in the twentieth century, the atomic model of a solid was speculative. We now have direct evidence of atoms in solids (Figure).

    Figure shows a 3 dimensional wavy structure with peaks and troughs.

    Figure \(\PageIndex{1}\): An image made with a scanning tunneling microscope of the surface of graphite. The peaks represent the atoms, which are arranged in hexagons. The scale is in angstroms.

    Ionic Bonding in Solids

    Many solids form by ionic bonding. A prototypical example is the sodium chloride crystal, as we discussed earlier. Electrons transfer from sodium atoms to adjacent chlorine atoms, since the valence electrons in sodium are loosely bound and chlorine has a large electron affinity. The positively charged sodium ions and negatively charged chlorine (chloride) ions organize into an extended regular array of atoms (Figure).

    Figure shows a crystal lattice structure with alternately placed small red spheres labeled sodium ions and bigger green spheres labeled chloride ions.

    Figure \(\PageIndex{2}\): Structure of the sodium chloride crystal. The sodium and chloride ions are arranged in a face-centered cubic (FCC) structure.

    The charge distributions of the sodium and chloride ions are spherically symmetric, and the chloride ion is about two times the diameter of the sodium ion. The lowest energy arrangement of these ions is called the face-centered cubic (FCC) structure. In this structure, each ion is closest to six ions of the other species. The unit cell is a cube—an atom occupies the center and corners of each “face” of the cube. The attractive potential energy of the \(Na^+\) ion due to the fields of these six \(Cl^-\) ions is written

    \[U_1 = -6\frac{e^2}{4\pi \epsilon_0 r}\]

    where the minus sign designates an attractive potential (and we identify \(k = 1/4 \pi \epsilon_0\)). At a distance \(\sqrt{2r}\) are its next-nearest neighbors: twelve \(Na^+\) ions of the same charge. The total repulsive potential energy associated with these ions is

    \[U_2 = 12\frac{e^2}{4\pi \epsilon_0\sqrt{2}r}.\]

    Next closest are eight \(Cl^-\) ions a distance 3√r3r from the \(Na^+\) ion. The potential energy of the \(Na^+\) ion in the field of these eight ions is

    \[U_3 = -8\frac{e^2}{4\pi \epsilon_0 \sqrt{3}r}.\]

    Continuing in the same manner with alternate sets of \(Cl^-\) and \(Na^+\) ions, we find that the net attractive potential energy \(U_A\) of the single \(Na^+\) ion can be written as

    \[U_{coul} = - \alpha \frac{e^2}{4\pi \epsilon_0 r}\]

    where \(\alpha\) is the Madelung constant, introduced earlier. From this analysis, we can see that this constant is the infinite converging sum

    \[\alpha = 6 - \frac{12}{sqrt{2}} + \frac{8}{\sqrt{3}} + . . .\]

    Distant ions make a significant contribution to this sum, so it converges slowly, and many terms must be used to calculate αα accurately. For all FCC ionic solids, αα is approximately 1.75.

    Other possible packing arrangements of atoms in solids include simple cubic and body-centered cubic (BCC). These three different packing structures of solids are compared in Figure. The first row represents the location, but not the size, of the ions; the second row indicates the unit cells of each structure or lattice; and the third row represents the location and size of the ions. The BCC structure has eight nearest neighbors, with a Madelung constant of about 1.76—only slightly different from that for the FCC structure. Determining the Madelung constant for specific solids is difficult work and the subject of current research.

    There are nine figures in three rows and three columns. The columns are labeled: a, simple cubic, b, body-centered cubic or BCC, and c, face-centered cubic or FCC.  In row one, the first figure shows a cube with small red spheres in all eight corners. The second one shows the same arrangement with an additional green sphere in the center. The third cube has eight red spheres in the corners and six green spheres, one on each surface of the cube. The row is labeled locations of ions in unit cells. The second row has three cubes similar to the first row, but the spheres are bigger and cut off at the surfaces. This row is labeled sizes of ions and parts allotted to each cell. The third row has the same three cubes as the two previous rows, but with additional cells of the lattice surrounding the cubes. This row is labeled unit cells within the overall lattice.

    Figure \(\PageIndex{3}\): Packing structures for solids from left to right: (a) simple cubic, (b) body-centered cubic (BCC), and (c) face-centered cubic (FCC). Each crystal structure minimizes the energy of the system.

    The energy of the sodium ions is not entirely due to attractive forces between oppositely charged ions. If the ions are bought too close together, the wave functions of core electrons of the ions overlap, and the electrons repel due to the exclusion principle. The total potential energy of the \(Na^+\) ion is therefore the sum of the attractive Coulomb potential (\(U_{coul}\)) and the repulsive potential associated with the exclusion principle (\(U_{ex}\)). Calculating this repulsive potential requires powerful computers. Fortunately, however, this energy can be described accurately by a simple formula that contains adjustable parameters:

    \[U_{ex} = \frac{A}{r^n}\]

    where the parameters A and n are chosen to give predictions consistent with experimental data. For the problem at the end of this chapter, the parameter n is referred to as the repulsion constant. The total potential energy of the \(Na^+\) ion is therefore

    \[U = -\alpha\frac{e^2}{4\pi \epsilon_0 r} + \frac{A}{r^n}.\]

    At equilibrium, there is no net force on the ion, so the distance between neighboring \(Na^+\) and \(Cl^-\) ions must be the value \(r_0\) for which U is a minimum. Setting \(\frac{dU}{dr} = 0\), we have

    \[0 = \frac{\alpha e^2}{4\pi \epsilon_0 r_0^2} - \frac{nA}{r_0^{n+1}}.\]

    Thus,

    \[A = \frac{\alpha e^2 r_0^{n-1}}{4\pi \epsilon_0 n}.\]

    Inserting this expression into the expression for the total potential energy, we have

    \[U = - \frac{\alpha e^2}{4\pi \epsilon_0 r_0} \left[\frac{r_0}{r} - \frac{1}{n}\left(\frac{r_0}{r}\right)^n \right].\]

    Notice that the total potential energy now has only one adjustable parameter, n. The parameter A has been replaced by a function involving r0r0, the equilibrium separation distance, which can be measured by a diffraction experiment (you learned about diffraction in a previous chapter). The total potential energy is plotted in Figure for \(n = 0\), the approximate value of n for NaCl.

    Graph of potential energy versus r by r subscript 0. There are three curves on the graph. A curve labeled U subscript R drops down in an almost vertical line to a y value of 0 and an x value of roughly 1. Here, it turns and extends in a horizontal line to the right. A curve labeled U, similarly drops down till it reaches a y value below zero. From here, it rises up slightly and evens out to a y value below zero. The third curve, labeled U subscript A is along the second branch of the curve U. It separates from U at an x value of roughly 1, which is the lowest point of curve U. From here, UA goes down and right.

    Figure \(\PageIndex{4}\): The potential energy of a sodium ion in a NaCl crystal for \(n = 8\). The equilibrium bond length occurs when the energy is a minimized.

    As long as \(n > 1\), the curve for U has the same general shape: U approaches infinity as \(r \rightarrow 0\) and U approaches zero as \(r \rightarrow \infty\). The minimum value of the potential energy is given by

    \[U_{min} (r = r_0) = -\alpha \frac{fe^2}{r_0}\left( 1 - \frac{1}{n}\right).\]

    The energy per ion pair needed to separate the crystal into ions is therefore

    \[U_{diss} = \alpha \frac{ke^2}{r_0}\left(1 - \frac{1}{n}\right).\]

    This is the dissociation energy of the solid. The dissociation energy can also be used to describe the total energy needed to break a mole of a solid into its constituent ions, often expressed in kJ/mole. The dissociation energy can be determined experimentally using the latent heat of vaporization. Sample values are given in the following table.

    Lattice Energy for Alkali Metal Halides
      \(F^-\) \(Cl^-\) \(Br^-\) \(I^-\)
    \(Li^+\) 1036 853 807 757
    \(Na^+\) 923 787 747 704
    \(K^+\) 821 715 682 649
    \(Rb^+\) 785 689 660 630
    \(Cs^+\) 740 659 631 604

    Thus, we can determine the Madelung constant from the crystal structure and n from the lattice energy. For NaCl, we have \(r_0 = 2.81 A\), \(n \approx 8\), and \(U_{diss} = 7.84 \space eV/ion \space pair\). This dissociation energy is relatively large. The most energetic photon from the visible spectrum, for example, has an energy of approximately

    \[hf = (4.14 \times 10^{-15} eV \cdot s)(7.5 \times 10^{14} Hz) = 3.1 \space eV.\]

    Because the ions in crystals are so tightly bound, ionic crystals have the following general characteristics:

    1. They are fairly hard and stable.
    2. They vaporize at relatively high temperatures (1000 to 2000 K).
    3. They are transparent to visible radiation, because photons in the visible portion of the spectrum are not energetic enough to excite an electron from its ground state to an excited state.
    4. They are poor electrical conductors, because they contain effectively no free electrons.
    5. They are usually soluble in water, because the water molecule has a large dipole moment whose electric field is strong enough to break the electrostatic bonds between the ions.

    Example

    The Dissociation Energy of Salt

    Determine the dissociation energy of sodium chloride (NaCl) in kJ/mol. (Hint: The repulsion constant n of NaCl is approximately 8.)

    Strategy

    A sodium chloride crystal has an equilibrium separation of 0.282 nm. (Compare this value with 0.236 nm for a free diatomic unit of NaCl.) The dissociation energy depends on the separation distance, repulsion constant, and Madelung constant for an FCC structure. The separation distance depends in turn on the molar mass and measured density. We can determine the separation distance, and then use this value to determine the dissociation energy for one mole of the solid.

    Solution

    The atomic masses of Na and Cl are 23.0 u and 58.4 u, so the molar mass of NaCl is 58.4 g/mol. The density of NaCl is \(2.16 \space g/cm^3\). The relationship between these quantities is

    \[\rho = \frac{M}{V} = \frac{M}{2N_A r_0^3},\]

    where M is the mass of one mole of salt, NANA is Avogadro’s number, and r0r0 is the equilibrium separation distance. The factor 2 is needed since both the sodium and chloride ions represent a cubic volume \(r_0^3\). Solving for the distance, we get

    \[r_0^3 = \frac{M}{2N_A \rho} = \frac{58.4 \space g/mol}{2(6.03 \times 10^{23})(2.160 \space g/cm^3)} = 2.23 \times 10^{-23} \space cm^3,\] or

    \[r_0 = 2.80 \times 10^{-8} cm = 0.280 \space nm.\]

    The potential energy of one ion pair (\(Na^+ Cl^-\)) is

    \[U = -\alpha \frac{ke^2}{r_0} \left(1 - \frac{1}{n}\right),\]

    where \(\alpha\) is the Madelung constant, \(r_0\) is the equilibrium separation distance, and n is the repulsion constant. NaCl is FCC, so the Madelung constant is \(\alpha = 1.7476\). Substituting these values, we get

    \[U = -1.75 \frac{1.44 \space eV \cdot nm}{0.280 \space nm} \left(1 - \frac{1}{8}\right) = - 7.88 \frac{eV}{ion \space pair}.\]

    The dissociation energy of one mole of sodium chloride is therefore

    \[D = \left(\frac{7.88 \space eV}{ion \space pair}\right)\left( \frac{\frac{23.052 \space kcal}{1 \space mol}}{\frac{1 \space eV}{ion \space pair}}\right) = 182 \space kcal/mol = 760 \space kJ/mol.\]

    Significance

    This theoretical value of the dissociation energy of 766 kJ/mol is close to the accepted experimental value of 787 kJ/mol. Notice that for larger density, the equilibrium separation distance between ion pairs is smaller, as expected. This small separation distance drives up the force between ions and therefore the dissociation energy. The conversion at the end of the equation took advantage of the conversion factor \(1 \space kJ = 0.239 \space kcal\).

    Check Your Understanding If the dissociation energy were larger, would that make it easier or more difficult to break the solid apart?

    [Hide Solution]

    more difficult

    Covalent Bonding in Solids

    Crystals can also be formed by covalent bonding. For example, covalent bonds are responsible for holding carbon atoms together in diamond crystals. The electron configuration of the carbon atom is \(1s^22s^22p^2\) - a He core plus four valence electrons. This electron configuration is four electrons short of a full shell, so by sharing these four electrons with other carbon atoms in a covalent bond, the shells of all carbon atoms are filled. Diamond has a more complicated structure than most ionic crystals (Figure). Each carbon atom is the center of a regular tetrahedron, and the angle between the bonds is 110°.110°. This angle is a direct consequence of the directionality of the p orbitals of carbon atoms.

    Figure a shows a crystal lattice. A cube formed by dotted lines marks an area in the lattice. There are four light blue spheres, one on each diagonally opposite corner of the cube. There is a dark blue sphere in the center of the cube. All spheres are connected to each other by lines of the same length. This length is 0.154 nm. Figure b is the photograph of a diamond.

    Figure \(\PageIndex{5}\): Structure of the diamond crystal. (a) The single carbon atom represented by the dark blue sphere is covalently bonded to the four carbon atoms represented by the light blue spheres. (b) Gem-quality diamonds can be cleaved along smooth planes, which gives a large number of angles that cause total internal reflection of incident light, and thus gives diamonds their prized brilliance.

    Covalently bonded crystals are not as uniform as ionic crystals but are reasonably hard, difficult to melt, and are insoluble in water. For example, diamond has an extremely high melting temperature (4000 K) and is transparent to visible light. In comparison, covalently bonded tin (also known as alpha-tin, which is nonmetallic) is relatively soft, melts at 600 K, and reflects visible light. Two other important examples of covalently bonded crystals are silicon and germanium. Both of these solids are used extensively in the manufacture of diodes, transistors, and integrated circuits. We will return to these materials later in our discussion of semiconductors.

    Metallic Bonding in Solids

    As the name implies, metallic bonding is responsible for the formation of metallic crystals. The valence electrons are essentially free of the atoms and are able to move relatively easily throughout the metallic crystal. Bonding is due to the attractive forces between the positive ions and the conduction electrons. Metallic bonds are weaker than ionic or covalent bonds, with dissociation energies in the range \(1 - 3 \space eV\).

    Contributors

    Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a Creative Commons Attribution License (by 4.0).