The Solid State - Class 12 Chemistry Notes

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General Characteristics of Solid State

The following are the characteristic properties of the solid state:

(i) They have definite mass, volume and shape.

(ii) Intermolecular distances are short.

(iii) Intermolecular forces are strong.

(iv) Their constituent particles (atoms, molecules or ions) have fixed positions and can only oscillate about their mean positions.

(v) They are incompressible and rigid.

Amorphous and Crystalline Solids

Solids can be broken down into two major categories: crystalline solids and amorphous solids.

Amorphous solids, such as glass, are those solids that do not have any underlining order in their molecular structure. On the other hand, crystalline solids are those solids that have a well defined order in their structure.

Crystalline solids can be further broken down into four groups: ionic solids, molecular solids, network solids and metallic solids. Ionic solids are those solids in which the individual atoms form bonds as a result of positive and negative charges on the atoms.

Classification of Crystalline Solids

Crystalline substances can be described by the types of particles in them and the types of chemical bonding that takes place between the particles.

There are four types of crystals:

(1) Ionic: An ionic crystal is a crystalline ionic compound. They are solids consisting of ions bound together by their electrostatic attraction into a regular lattice. Examples of such crystals are the alkali halides, including potassium fluoride, potassium chloride, potassium bromide, potassium iodide, sodium fluoride.

(2) Metallic: Metallic crystals consist of metal cations surrounded by a "sea" of mobile valence electrons. Covalent crystals are composed of atoms which are covalently bonded to one another. Molecular crystals are held together by weak intermolecular forces.

(3) Covalent or network: A network solid or covalent network solid (also called atomic crystalline solids) is a chemical compound (or element) in which the atoms are bonded by covalent bonds in a continuous network extending throughout the material.

(4) Molecular: Molecular crystals are substances that have relatively weak intermolecular binding, such as dry ice (solidified carbon dioxide), solid forms of the noble gases (e.g., argon, krypton, and xenon), and crystals of numerous organic compounds.

Crystal Lattices and Unit Cells

The crystal lattice is the symmetrical three-dimensional structural arrangements of atoms, ions or molecules (constituent particle) inside a crystalline solid as points. It can be defined as the geometrical arrangement of the atoms, ions or molecules of the crystalline solid as points in space.

Characteristics of Crystal Lattice

  • In a crystal lattice, each atom, molecule or ions (constituent particle) is represented by a single point.
  • These points are called lattice site or lattice point.
  • Lattice sites or points are together joined by a straight line in a crystal lattice.
  • When we connect these straight lines we can get a three-dimensional view of the structure. This 3D arrangement is called Crystal Lattice also known as Bravais Lattices.

Primitive and Centred Unit Cells

Primitive Unit Cell: When particles in unit cell are present only at the corners, it is called the primitive unit cell.

Centred Unit Cells: When particles are present at other positions in addition to those at corners in a unit cell, it is called a Centred Unit Cell. There are 3 types of Centred Unit Cells:

  • Body Centred: When the constituent particle at the centre of the body, it is known as Body Centred Unit cell.
  • Face Centred: When the constituent particle present at the centre of each face, it is known as Face Centred Unit cell.
  • End Centred: When the constituent particle present at the centre of two opposite faces, it is known as an End Centred Unit cell.

Number of Atoms in a Unit Cell

(1) The number of atoms contained in one simple cubic unit cell of monoatomic substance is 1. 8 atoms are present at 8 corners of a simple cubic unit cell. Each atom contributes one eigth to the unit cell. Total contribution =8×81=1

(2) The number of atoms contained in one face-centred cubic unit cell of monoatomic substance is 4. 8 atoms are present at 8 corners of a fcc unit cell. Each atom contributes one eigth to the unit cell. Total contribution =8×81=1. 6 atoms are present at 6 corners of a fcc unit cell. Each atom contributes one half to the unit cell. Total contribution =6×21=3. Total number of atoms in one fcc unit cell =1+3=4.

(3) The number of atoms contained in one body-centred cubic unit cell of monoatomic substance is 2. 8 atoms are present at 8 corners of a bcc unit cell. Each atom contributes one eigth to the unit cell. Total contribution =8×81=1. 1 atom is present at body centre of a bcc unit cell. The atom contributes fully to the unit cell. Total contribution =1×11=1. Total number of atoms in one fcc unit cell =1+1=2.

Close Packed Structures

The term "closest packed structures" refers to the most tightly packed or space-efficient composition of crystal structures (lattices). To maximize the efficiency of packing and minimize the volume of unfilled space, the spheres must be arranged as close as possible to each other.

(a) Close Packing in One Dimension

In one dimension close packing, spheres are arranged in a row such that adjacent atoms are in contact with each other. Coordination number is defined as the no. of the nearest neighbour particles. In case of one dimension close packing, coordination number is equal to two.

(b) Close Packing in Two Dimensions

In two-dimensional close packing, a row of closed packed spheres are stacked to obtain a two-dimensional pattern. This stacking is done in two ways: Square close packing: The second row can be placed exactly below the first row in a close packing.

(c) Close Packing in Three Dimensions

Formation of three-dimensional close packing can be done by placing the second square closed packing exactly above the first one. In this close packing, the spheres are aligned properly in horizontally and vertically. Similarly, by placing more layers one above the other, we can obtain a simple cubic lattice.

Formula of a Compound and Number of Voids Filled

Number of octahedral voids = Number of close-packed particles

Number of tetrahedral voids = 2 × Number of close-packed particles

In ionic solids, the bigger ions (usually anions) form the close-packed structure and the smaller ions (usually cations) occupy the voids.

If the latter ion is small enough, then it occupies the tetrahedral void, and if bigger, then it occupies the octahedral void.

Not all the voids are occupied. Only a fraction of the octahedral or tetrahedral voids are occupied.

The fraction of the octahedral or tetrahedral voids that are occupied depends on the chemical formula of the compound.

Packing Efficiency

Packing efficiency is defined as the percentage of space occupied by constituent particles packed inside the lattice. It can be calculated with the help of geometry in three structures namely: HCP and CCP structures, Body-Centred Cubic Structures.

Packing efficiency can be written as below, Packing efficiency = Volume occupied by 6 spheres ×100 / Total volume of unit cells. Examples are Magnesium, Titanium, Beryllium etc. In body-centered cubic structures, the three atoms are arranged diagonally.

Packing Efficiency in hcp and ccp Structures

Both ccp and hcp are highly efficient lattice; in terms of packing. The packing efficiency of both types of close packed structure is 74%, i.e. 74% of the space in hcp and ccp is filled. The hcp and ccp structure are equally efficient; in terms of packing. The packing efficiency of simple cubic lattice is 52.4%.

Packing Efficiency Body-Centred Cubic Structures

In body-centred cubic unit cell (BCC) has atoms at each corner of the cube and an atom at the centre of the structure. The packing efficiency of the BCC lattice is 68%.

Packing Efficiency in Simple Cubic Lattice

In a simple cubic lattice, the atoms are located only on the corners of the cube. Since a simple cubic unit cell contains only 1 atom. The packing efficiency of the simple cubic cell is 52.4 %. Thus 47.6 % volume is empty space (void space) i.e. almost half the space is empty.

Calculations Involving Unit Cell Dimensions

Edge length of a unit cell of a cubic crystal = a,

Density of the solid substance = d

Molar mass = M

Volume of a unit cell = a3

Mass of the unit cell = number of atoms in unit cell × mass of each atom = number of atoms present in one unit cell (z) × mass of a single atom (m)

Class 12 Chemistry Notes

Imperfections in Solids

Any irregularity in the pattern of crystal arrangement in a solid lattice is called imperfection in solids. The occurrence of defects takes place when crystallization (the process of formation of crystals) occurs at a very fast or at an intermediate rate. This is because particles don’t get enough time to arrange themselves in a regular pattern. Basically, defects fall out in two forms:

Point Defect: Point Defect occurs when an atom is missing or is irregularly arranged in a crystal lattice. In other words, the deviations and irregularities observed around an atom or a point are known as a Point Defect. Point Defects are classified into two defects, namely:

  • Stoichiometric Defects: The defects due to which the stoichiometry of solids remains undisturbed are called stoichiometric Defects. After stoichiometric defect, the ratio of cation and anions remain same in a solid. They are also known as intrinsic or thermodynamic defects. Stoichiometric Defects are further classified into two defects: Vacancy Defect, Interstitial Defect, Schottky Defect and Frenkel Defect.
  • Nonstoichiometric Defects: The defect in which the ratio of cation and anion in an ionic lattice is variable is known as a non-stoichiometric defect. They are of two types, namely: Metal Excess Defect and Metal Deficiency Defect.

Line Defect: Line defects, or dislocations, are lines along which whole rows of atoms in a solid are arranged anomalously. The resulting irregularity in spacing is most severe along a line called the line of dislocation. Line defects can weaken or strengthen solids.

Electrical Properties

Electrical properties are their ability to conduct electrical current. Various electrical properties are resistivity, Electrical conductivity, temperature coefficient of resistance, dielectric strength and thermoelectricity.

Conduction of Electricity in Metals

Electrical conductivity in metals is a result of the movement of electrically charged particles. It is these "free electrons" that allow metals to conduct an electric current. Because valence electrons are free to move, they can travel through the lattice that forms the physical structure of a metal.

Conduction of Electricity in Semi-conductors

Electrical conductivity of semiconductors increases with increase in temperature, since more electrons can jump to the conduction band due to small gap between the valence band and conduction band. Silicon and germanium exhibit this behavior and are called intrinsic semiconductors.

  • Electron – rich impurities: Silicon and germanium belong to group 14 of the periodic table and have four valence electrons each.
  • Electron – deficit impurities: Silicon or germanium can also be doped with a group 13 element like B, Al or Ga which contains only three valence electrons.

Magnetic Properties

Anything that is magnetic, like a bar magnet or a loop of electric current, has a magnetic moment. A magnetic moment is a vector quantity, with a magnitude and a direction. An electron has an electron magnetic dipole moment, generated by the electron's intrinsic spin property, making it an electric charge in motion.

On the basis of their magnetic properties, substances can be classified into five categories: (i) paramagnetic (ii) diamagnetic (iii) ferromagnetic (iv) antiferromagnetic and (v) ferrimagnetic.

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