NCERT Solutions Class 12 Chemistry Chapter 1: The Solid State – Complete Guide

Chapter 1 of Class 12 Chemistry deals with The Solid State, a fundamental topic that explores the structure and properties of solids. This chapter is crucial for both board exams and competitive examinations like JEE and NEET. Let’s explore the key concepts, important formulas, and problem-solving approaches.
Introduction to Solid State
Solids are characterized by definite shape, definite volume, high density, incompressibility, and rigidity. The constituent particles (atoms, molecules, or ions) are held together by strong interparticle forces and have fixed positions, though they can oscillate about their mean positions.
Classification of Solids
Based on Arrangement of Particles
Crystalline Solids:
- Regular and orderly arrangement of constituent particles
- Sharp melting point
- Anisotropic (different properties in different directions)
- True solids
- Examples: NaCl, Diamond, Quartz
Amorphous Solids:
- Irregular arrangement of particles
- Melt over a range of temperatures
- Isotropic (same properties in all directions)
- Pseudo solids or supercooled liquids
- Examples: Glass, Rubber, Plastics
Types of Crystalline Solids
| Type | Constituent Particles | Bonding | Properties | Examples |
|---|---|---|---|---|
| Ionic | Cations & Anions | Electrostatic | High MP, Brittle, Conduct when molten | NaCl, MgO |
| Covalent | Atoms | Covalent bonds | Very high MP, Hard, Poor conductors | Diamond, SiC |
| Molecular | Molecules | Dispersion/Dipole/H-bond | Low MP, Soft, Non-conductors | Ice, I₂ |
| Metallic | Metal atoms | Metallic bond | Variable MP, Malleable, Good conductors | Fe, Cu, Au |
Crystal Lattice and Unit Cell
Crystal Lattice
A three-dimensional arrangement of points representing the positions of constituent particles in a crystal is called a crystal lattice or space lattice. Each point is called a lattice point.
Unit Cell
The smallest repeating unit in a crystal lattice that represents the complete crystal structure is called a unit cell. There are seven crystal systems based on unit cell dimensions.
Types of Unit Cells
- Primitive (Simple): Particles only at corners
- Body-Centered: Particles at corners + one at body center
- Face-Centered: Particles at corners + one at each face center
- End-Centered: Particles at corners + one at two opposite face centers
Number of Atoms in Different Unit Cells
Contribution of Atoms at Different Positions
- Corner atom: 1/8 (shared by 8 unit cells)
- Face-centered atom: 1/2 (shared by 2 unit cells)
- Body-centered atom: 1 (belongs to one unit cell)
- Edge-centered atom: 1/4 (shared by 4 unit cells)
Atoms per Unit Cell
- Simple Cubic (SC): 8 × 1/8 = 1 atom
- Body-Centered Cubic (BCC): (8 × 1/8) + 1 = 2 atoms
- Face-Centered Cubic (FCC): (8 × 1/8) + (6 × 1/2) = 4 atoms
Close Packing Structures
Close Packing in Two Dimensions
- Square Close Packing: Coordination number = 4
- Hexagonal Close Packing: Coordination number = 6
Close Packing in Three Dimensions
- Hexagonal Close Packing (HCP): ABAB… pattern, coordination number = 12
- Cubic Close Packing (CCP/FCC): ABCABC… pattern, coordination number = 12
Packing Efficiency
Packing efficiency = (Volume occupied by atoms / Total volume of unit cell) × 100
Packing Efficiency Values
- Simple Cubic: 52.4%
- Body-Centered Cubic: 68%
- Face-Centered Cubic: 74%
- HCP: 74%
Voids in Close Packing
Tetrahedral Voids
Formed when a sphere of second layer is above the void of first layer. Number of tetrahedral voids = 2 × number of spheres
Octahedral Voids
Formed when triangular voids of first and second layers do not overlap. Number of octahedral voids = number of spheres
Density Calculations
The density of a crystalline solid can be calculated using:
ρ = (Z × M) / (a³ × Nₐ)
Where:
- ρ = Density
- Z = Number of atoms per unit cell
- M = Molar mass
- a = Edge length of unit cell
- Nₐ = Avogadro’s number
Defects in Crystals
Point Defects
Stoichiometric Defects (Intrinsic):
- Vacancy Defect: Missing atoms from lattice sites. Decreases density.
- Interstitial Defect: Extra atoms in interstitial sites. Increases density.
- Schottky Defect: Equal vacancies of cations and anions. Common in ionic compounds with similar cation and anion sizes (NaCl, KCl).
- Frenkel Defect: Smaller ion displaced to interstitial site. Common when there’s large size difference (AgCl, ZnS).
Non-Stoichiometric Defects:
- Metal Excess Defect: Due to anionic vacancies or extra cations in interstitial sites
- Metal Deficiency Defect: Due to cationic vacancies
Impurity Defects
Foreign atoms occupy lattice positions. Example: Doping of Si with As (n-type) or B (p-type) semiconductors.
Important Formulas Summary
- Relation between r and a for SC: a = 2r
- Relation between r and a for BCC: a = 4r/√3
- Relation between r and a for FCC: a = 2√2r
- Density: ρ = ZM/a³Nₐ
Conclusion
The Solid State chapter forms the foundation for understanding material properties and their applications. Focus on understanding the concepts of unit cells, packing efficiency, and defects. Practice numerical problems on density calculations and relationship between atomic radius and edge length. This chapter carries significant weightage in both board exams and competitive examinations.
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