EENS 2110 |
Mineralogy |
Tulane University |
Prof. Stephen A. Nelson |
Crystal Chemistry |
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As we have been discussing for the last several weeks, crystals, and thus minerals, are made up of a 3-dimensional array of atoms arranged in an orderly fashion. Now we explore what these atoms are and how they interact with one another to determine the physical and structural properties of crystals. So, first we explore the properties of the atom. |
Atoms Atoms make up the chemical elements. Each chemical element has nearly identical atoms. An atom is composed of three different particles:
In a neutrally charged atom, each element has the same number of protons and the same number of electrons.
Isotopes are atoms of the same element with differing numbers of neutrons. i.e. the number of neutrons may vary within atoms of the same element. Some isotopes are unstable which results in radioactivity.
It is the electrons in the atoms that are responsible for the chemical properties of atoms. The electronic configuration determines the types of atoms that can be bound to one another, the strength of the bonds, and the types of bonds. Thus, we need to look closely at the electrons and the electronic configuration of atoms. |
Bohr Atom Electrons orbit around the nucleus in different shells, labeled from the innermost shell as K, L, M, N, etc. Each shell can have a certain number of electrons. The K-shell can have 2 Electrons, the L-shell, 8, the M-shell 18, N-shell 32. Each shell is associated with a principal quantum number, n, where nK = 1, nL = 2, nM = 3, nN = 4, etc. The number of electrons in each shell is controlled by this principal quantum number by the following relationship: # electrons = 2n2 Thus, the K-shell can contain 2 electrons, the L-shell, 8 electrons, the M-shell, 18 electrons, and the N-shell, 32 electrons. |
Planck found that the energy released in the electronic transitions is only released in distinct packets, which he called "quanta", and that these packets of energy are related to a constant (now called Planck's constant, and the frequency or wavelength of the radiation released. E = hν = hc/λ where
This led to the quantum mechanical view of the atom.
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Quantum Mechanical View of the Atom
The quantum mechanical view of the atom suggests that the electrons are located within specific regions of probability. These probability regions are described by the azimuthal quantum number or orbital shape quantum number, l. A maximum of 2 electrons can be found in each probability region, each electron have a spin quantum number with a value of either +½ or -½. The orbital shape quantum number has the following values and designations for the shape of the probability region in which the electrons are most probably to be found. |
Value of l 1 2 3 4 Sub-shell designation s p d f
The sub-shell designations stand for sharp, principal, diffuse, and fundamental. The probability regions described by these sub-shells are as follows: |
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Since 2 electrons can occur in each of the different p orbitals, a maximum of 6 electrons are associated with p-orbitals in each principal shell. |
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The Pauli Exclusion Principal states that no 2
electrons in an atom can have the same quantum numbers, thus each of the
sub-orbitals described above can have a maximum of 2 electrons, and each
of these will have opposite values of the spin quantum number.
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As the atomic number (number of protons) in an atom increases, the
shells and sub-shells with lower energy are filled first. The drawing
at the right illustrates qualitatively the energy relationships between
the various shells and sub-shells of atoms. Thus 1s sub-shells with
the lowest energy are filled first. These are followed by 2s orbitals,
then 2p orbitals. As the principal quantum number increases to 3,
the 3s, 3p, and 3d orbitals are filled. But, beginning with n = 4,
there is overlap between the energies of s and d orbitals, and thus the 4s
orbital is filled before the 3d orbitals, and
the 4p orbitals do not contain electrons until the 3d orbitals are filled. This overlap continues in a similar way for higher
principle quantum number shells.
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Electronic Structure of the Atom and the Periodic Table of the Elements Based on the energy levels of the various sub-shells, we can begin filling in the electronic structure of atoms as shown in the following table. Note that this table only goes up to atomic number 36. A complete table can found in Klein and Dutrow on pages 44-46. |
At. # Elem. K L M N 1s 2s 2p 3s 3p 3d 4s 4p 4d 4f 1 H 1 <------- K-shell completely filled 2 He 2 3 Li 2 1 4 Be 2 2 5 B 2 2 1 <----L-shell completely filled 6 C 2 2 2 7 N 2 2 3 8 O 2 2 4 9 F 2 2 5 10 Ne 2 2 6 11 Na 2 2 6 1 12 Mg 2 2 6 2 13 Al 2 2 6 2 1 <----3p-orbitals completely filled 14 Si 2 2 6 2 2 15 P 2 2 6 2 3 16 S 2 2 6 2 4 17 Cl 2 2 6 2 5 18 Ar 2 2 6 2 6 19 K 2 2 6 2 6 1 20 Ca 2 2 6 2 6 2 21 Sc 2 2 6 2 6 1 2 22 Ti 2 2 6 2 6 2 2 23 V 2 2 6 2 6 3 2 24 Cr 2 2 6 2 6 5 1 25 Mn 2 2 6 2 6 5 2 26 Fe 2 2 6 2 6 6 2 27 Co 2 2 6 2 6 7 2 28 Ni 2 2 6 2 6 8 2 29 Cu 2 2 6 2 6 10 1 30 Zn 2 2 6 2 6 10 2 31 Ga 2 2 6 2 6 10 2 1 <- 4p orbitals filled 32 Ge 2 2 6 2 6 10 2 2 33 As 2 2 6 2 6 10 2 3 34 Se 2 2 6 2 6 10 2 4 35 Br 2 2 6 2 6 10 2 5 36 Kr 2 2 6 2 6 10 2 6
This periodic filling of shells and sub-shells forms the basis of the
periodic table of the elements. Elements with similar configurations
of outer shell electrons (called valence electrons) have
similar chemical properties. The rows in the table, labeled 1, 2,
3, 4, 5, 6, & 7, correspond to the principal quantum number.
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The Ion
In a neutral atom, the number of protons and the number of electrons are equal, thus the number of positive charges is the same as the number of negative charges and the atom has no charge. However, some elements in the Periodic Table tend to loose electrons to become positively charged and some elements tend to gain electrons to become negatively charged. Atoms with an electrical charge are called ions. Elements that tend to loose electrons are called metals, while those that tend to gain electrons are non-metals. Metals thus tend to form positively charged ions called cations, while non-metals tend to form negatively charged ions called anions.
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Ionization Potential
When electrons are either removed or gained by an atom there is a transfer of energy. The amount of energy required to remove an electron is called the ionization potential. The version of the periodic table shown below gives value of the first ionization potential. Note that elements with high ionization potential do not like to give up electrons, while those with low ionization potential can give up electrons more readily and tend to become cations. We can make the following observations: |
To summarize, the common valence states of the common elements are
listed in the table below for quick reference.
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Valence States of the Common Elements |
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H+1 |
Transition Elements |
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Li+1 | Be+2 | B+3 | C+4 | N+5 | O-2 | F-1 | ||||||||||
Na+1 | Mg+2 | Al+3 | Si+4 | P+5 | S-2 S+6 |
Cl-1 | ||||||||||
K+1 | Ca+2 | Sc+3 | Ti+4 | V+5 | Cr+3 | Mn+2 Mn+3 Mn+4 |
Fe+2 Fe+3 |
Co+2 | Ni+2 | Cu+2 | Zn+2 | Ga+3 | Ge+4 | As+3 As+5 |
Br-1 | |
Th+4 REE +3, except Eu sometimes +2 U+4 |
Electronegativity Another way of looking at the tendency to gain or lose electrons is based on the electronegativity. Electronegativity is defined as the ability of an atom in a crystal structure or molecule to attract electrons into its outer shell. Elements with low values of electronegativity are electron donors, and those with high values are electron acceptors. The Noble gases have electronegativity values of zero, because they neither accept or donate electrons. As we will see in our later discussion, electronegativity difference between atoms plays an important role in determining they type of chemical bond that forms between elements.
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The chemical and physical properties of crystals depend almost entirely on the forces that bind the atoms together in a crystal structure. These forces are known collectively as chemical bonds. Chemical bonding depends on the electronic structure of the atoms involved, in particular the valence electrons in the outermost shells, and on the size of the ion or atom. In general we recognize 4 different types of chemical bonds, although as we will see, all bond types are transitional from one type to another. |
Ionic Bonds
As we have seen, there is a tendency for atoms to lose or gain electrons and become ions in order to achieve the stable electronic configuration with completely filled outer electron shells. Positively charged ions are called cations and negatively charged ions are called anions. These ions can achieve various values of electronic charge depending on the number of electrons gained or lost.
When atoms become charged ions the force of attraction between oppositely charged ions results in an ionic bond. |
For example, Na has one electron in its outermost shell. It will tend to give up this electron to become Na+1 ion. Similarly, Cl has 7 electrons in its outermost shell and would like to gain an electron to become Cl-1 ion. Once these atoms become Na+1 and Cl-1, the force of attraction between the oppositely charged ions results in an ionic bond. |
Ionic bonds are non-directional in nature, that is the attractive forces occur form all directions. Crystals made of ionically bonded atoms tend to have the following properties: |
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Covalent Bonds
Covalent bonds can also be thought of as shared electron bonds. Covalent bonds develop when atoms can achieve the a stable outer shell electron configuration by sharing electrons with another atom. This results in each of the atoms having a stable electronic configuration part of the time. |
For example, Oxygen has six electrons in its outer shell, 2 are in s-orbitals and 4 are in p-orbitals. If it can gain two more electrons to fill its p-orbital shells, it would have the stable electronic configuration of a Noble gas. A second Oxygen atom also needs 2 more electrons to achieve the stable configuration. If the two Oxygens each share 2 electrons with each other, then each Oxygen has the stable electronic configuration part of the time. The covalent bond thus formed is a very strong bond. Thus we find oxygen gas is composed of O2 molecules. Similarly, F2 and Cl2 gases are composed of covalently bonded F and Cl pairs. |
Covalent bonds are very strong directional bonds, that is they occur
along the zone where they electrons are shared. Covalently bonded
crystals have the following properties:
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Elements near the right hand side of the periodic table tend to bond to each other by covalent bonds to form molecules that are found in crystal structures. For example Si and O form an SiO4-4 molecule that can bind to other atoms or molecules either covalently or ionically. Carbon has four electrons in its outer shell and needs 4 more to achieve the stable electronic configuration. So a Carbon atom can share electrons with 4 other Carbon atoms to form covalent bonds. This results in compounds like diamond or graphite that are held together by strong covalent bonds between Carbon atoms.
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For example, consultation of electronegativity chart above shows Cl with
a value of 3.16 and Na with a value of 0.93. The electronegativity
difference is 2.3, suggesting that only 80% of the bonding in NaCl is
ionic. Even looking a larger electronegativity difference like for
NaF, the bonding would by only about 90% ionic. Bonding between
Oxygen atoms or between Carbon atoms, where the electronegativity
difference is 0, would result in pure covalent bonds.
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Metallic Bonds
None of the bond types discussed so far result in materials that can easily conduct electricity. Pure metals however do conduct electricity easily and therefore must be bonded in a different way. |
This is the metallic bond, where positively charge atomic nuclei share electrons in their electron clouds freely. In a sense, each atom is sharing electrons freely with other atoms, and some of the electrons are free to move from atom to atom. Since some of the electrons are free to move, metallically bonded materials have high electrical conductivity. |
Pure metals appear to bind in this way. When crystals are formed
with metallic bonds they have the following properties:
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Residual Bonds
Residual bonds are weak bonds that involve the attraction of partially charged atoms or molecules. These partial charges are created when electrons become concentrated on one side of an atom or molecule to satisfy ionic or covalent bonds. This sometimes creates a polar atom or molecule which has a concentration of negative charges on one side and a concentration of positive charges on the other side. When residual bonds occur in a crystal structure, they generally form planes or zones of easy cleavage because of the weakness of the residual bond.
Two special cases are discussed here. |
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Mixture of Bonds in Crystals Since most crystals are complex mixtures of atoms, there will likely be more than one bond type in complex crystals. Thus, except in very simple compounds properties such as hardness, cleavage, solution rate, and growth rate may be directional, as discussed in a previous lecture. |
Examples of questions on this material that could be asked on an exam
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