🔬 CHEMISTRY — CLASS 12
SOLID STATE
CHAPTER — 1
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📌 Topics Covered:
🔹 General
Characteristics of Solid State
🔹 Amorphous
& Crystalline Solids
🔹 Crystal
Lattice & Unit Cell
🔹 Types of Cubic
Unit Cells (SC, BCC, FCC)
🔹 Packing
Efficiency & Density Calculations
🔹 Voids
(Tetrahedral & Octahedral)
🔹 Imperfections
in Solids (Point Defects)
🔹 Electrical
& Magnetic Properties
✅ Simple Language
| 📊 Tables &
Charts |
🎯 Exam-Ready Notes
1. Introduction to Solid State
The solid state is one of
the three fundamental states of matter. In solids, particles (atoms, ions, or
molecules) are tightly packed and held together by strong intermolecular
forces. Unlike liquids or gases, solids have a definite shape and volume.
|
🌟 Why is Solid State Important? |
|
• Most materials we use daily — metals, glass, ceramics,
salt — are solids. |
|
• Understanding solids helps in designing semiconductors,
medicines, and new materials. |
|
• Solid-state chemistry is the foundation of electronics
and materials science. |
1.1 General Characteristics of Solids
All solids share some
common properties. These characteristics arise due to the strong attractive
forces between particles and their fixed positions.
|
Property |
Description |
|
Definite Shape |
Solids do not change their
shape on their own. |
|
Definite Volume |
Volume remains fixed
regardless of container. |
|
Incompressibility |
Cannot be compressed easily
(closely packed). |
|
Rigidity |
Particles cannot move
freely; they vibrate in place. |
|
High Density |
Particles are very close to
each other. |
|
Low Diffusion |
Particles cannot mix easily
with other solids. |
2. Types of Solids
Solids are broadly
classified into two types based on the arrangement of their constituent
particles:
2.1 Amorphous Solids (Greek: Amorphos = No Form)
In amorphous solids,
particles are arranged in a random, irregular pattern. There is no long-range
order. These are also called pseudo-solids or supercooled liquids.
|
📌 Key Features of Amorphous
Solids |
|
• No definite melting point — they soften over a range of
temperature. |
|
• Not true solids — they behave like liquids over very long
time scales. |
|
• Isotropic — same properties in all directions. |
|
• Examples: Glass, Rubber, Plastics, Wax, Tar, Fibre Glass. |
|
• Glass flows slowly over centuries — old cathedral windows
are thicker at bottom! |
2.2 Crystalline Solids (True Solids)
In crystalline solids,
particles are arranged in a perfectly ordered, repeating 3D pattern called a
crystal lattice. They have long-range order throughout the structure.
|
📌 Key Features of Crystalline
Solids |
|
• Sharp melting point — they melt at an exact temperature. |
|
• Anisotropic — properties differ in different directions. |
|
• True solids — rigid and maintain shape permanently. |
|
• Examples: NaCl (Table salt), Diamond, Quartz, Sugar, Ice. |
|
• They have flat faces, sharp edges, and characteristic
angles. |
2.3 Comparison: Amorphous vs Crystalline
|
Property |
Amorphous |
Crystalline |
Example |
|
Arrangement |
Irregular |
Regular/Ordered |
— |
|
Melting Point |
Not sharp |
Sharp & fixed |
— |
|
Shape |
Irregular |
Definite geometry |
— |
|
Isotropy |
Isotropic |
Anisotropic |
— |
|
Cleavage |
Irregular break |
Clean, flat cleavage |
— |
|
True Solid? |
No (pseudo) |
Yes |
— |
|
Example |
Glass, Rubber |
NaCl, Diamond |
— |
3. Classification of Crystalline Solids
Crystalline solids are
classified into four types based on the nature of particles and the forces
holding them together:
3.1 Ionic Solids
Ions (positive &
negative) are arranged alternately in a crystal lattice and held by strong
electrostatic forces.
✦ Particles: Cations (+) and Anions (−)
✦ Binding Force: Electrostatic (ionic)
force
✦ Melting Point: Very HIGH (e.g., NaCl
melts at 801°C)
✦ Hardness: Very hard and brittle
✦ Conductivity: Insulator in solid
state; conductor when molten or dissolved
✦ Examples: NaCl, KCl, MgO, ZnS, CaF₂
3.2 Covalent / Network Solids
Atoms are connected by a
continuous network of covalent bonds throughout the crystal — like a giant
molecule.
✦ Particles: Atoms
✦ Binding Force: Covalent bonds
✦ Melting Point: Very HIGH (diamond
> 3500°C)
✦ Hardness: Extremely hard (Diamond is
hardest natural substance)
✦ Conductivity: Insulators (except
Graphite — conductor due to free π electrons)
✦ Examples: Diamond, SiO₂ (Quartz),
SiC, AlN
|
💡 Diamond vs Graphite — Same
Element, Different Properties! |
|
Diamond: Each carbon bonded to 4 others in tetrahedral
arrangement → hardest solid, insulator. |
|
Graphite: Each carbon bonded to 3 others in layers → soft
(layers slide), good conductor. |
|
This is called ALLOTROPY — same element, different
crystalline forms. |
3.3 Molecular Solids
Molecules are held
together by weak intermolecular forces (van der Waals forces, dipole-dipole, or
hydrogen bonds).
|
Sub-type |
Details & Examples |
|
Non-polar Molecular |
Held by weak London
dispersion forces. Very low MP. Examples: H₂, O₂, Cl₂, I₂, CO₂, CH₄, noble
gases (Ar, Ne) |
|
Polar Molecular |
Held by dipole-dipole
forces. Slightly higher MP. Examples: HCl, SO₂, H₂S |
|
Hydrogen-bonded |
Held by strong H-bonds.
Highest MP among molecular. Examples: H₂O (ice), NH₃, HF |
3.4 Metallic Solids
Metal atoms are arranged
in a lattice and held together by a 'sea of delocalized electrons' — called the
metallic bond.
✦ Particles: Positive metal ions
(kernels) + free electrons
✦ Binding Force: Metallic bond
(delocalized electron cloud)
✦ Melting Point: Variable (Hg = −39°C;
W = 3422°C)
✦ Hardness: Variable (soft Na to hard
Fe)
✦ Conductivity: Excellent — free
electrons carry current
✦ Examples: Fe, Cu, Al, Ag, Au, Zn
|
🔑 Quick Summary — 4 Types of
Crystalline Solids |
|
1. Ionic Solids
→ Ions →
Electrostatic → Hard, Brittle, High
MP → NaCl |
|
2. Covalent Solids
→ Atoms → Covalent bonds
→ Very Hard, Very High MP → Diamond |
|
3. Molecular Solids
→ Molecules → Weak
forces → Soft, Low MP → Ice |
|
4. Metallic Solids
→ Atoms+e⁻ → Metallic
bond → Variable, Conductor → Copper |
4. Crystal Lattice and Unit Cell
The three-dimensional
arrangement of particles (atoms/ions/molecules) in a crystal is called a
Crystal Lattice or Space Lattice. It is a regular, repeating pattern extending
in all three dimensions.
|
📖 Important Definitions |
|
🔹 Lattice Point: The position in the lattice where
a particle is located. |
|
🔹 Crystal Lattice: The 3D arrangement of all
lattice points. |
|
🔹 Unit Cell: The smallest repeating portion of the
crystal lattice. |
|
🔹 Bravais Lattices: 14 types of unit cells
classified into 7 crystal systems. |
4.1 The 7 Crystal Systems
Based on the length of
axes (a, b, c) and angles (α, β, γ) between them, all crystals fall into 7
systems:
|
Crystal System |
Axial Lengths & Angles | Example |
|
Cubic |
a = b = c, α = β = γ = 90°
| NaCl, Diamond, KCl |
|
Tetragonal |
a = b ≠ c, α = β = γ = 90°
| SnO₂, TiO₂ |
|
Orthorhombic |
a ≠ b ≠ c, α = β = γ = 90°
| KNO₃, BaSO₄ |
|
Hexagonal |
a = b ≠ c, α = β = 90°, γ =
120° | Mg, ZnO, Graphite |
|
Rhombohedral |
a = b = c, α = β = γ ≠ 90°
| Calcite, Quartz |
|
Monoclinic |
a ≠ b ≠ c, α = γ = 90°, β ≠
90° | Na₂SO₄·10H₂O |
|
Triclinic |
a ≠ b ≠ c, α ≠ β ≠ γ ≠ 90°
| K₂Cr₂O₇, H₃BO₃ |
5. Types of Cubic Unit Cells
The cubic system is the
most important and common in chemistry. There are three types of cubic unit
cells:
5.1 Simple Cubic (SC) / Primitive Cubic
Atoms are present only at
the 8 corners of the cube. Each corner atom is shared among 8 unit cells.
✦ Atoms per unit cell = 8 × (1/8) = 1
✦ Coordination Number = 6
✦ Packing Efficiency = 52.4%
✦ Example: Polonium (Po) — only metal
with SC structure
5.2 Body-Centred Cubic (BCC)
One atom at each corner +
one atom at the body centre of the cube.
✦ Atoms per unit cell = 8 × (1/8) + 1 =
1 + 1 = 2
✦ Coordination Number = 8
✦ Packing Efficiency = 68%
✦ Examples: Na, K, Cr, W, Mo, α-Fe, Ba
5.3 Face-Centred Cubic (FCC) / Cubic Close-Packing (CCP / ABCABC)
One atom at each corner +
one atom at the centre of each face (6 faces). FCC is same as CCP structure.
✦ Atoms per unit cell = 8 × (1/8) + 6 ×
(1/2) = 1 + 3 = 4
✦ Coordination Number = 12
✦ Packing Efficiency = 74% (Most
efficient cubic packing)
✦ Examples: Cu, Ag, Au, Al, Ni, NaCl
(ionic), diamond cubic
|
📊 Comparison of Cubic Unit Cells |
|
Property |
Simple Cubic (SC) | BCC | FCC/CCP |
|
───────────────────────────────────────────────────────────────────────── |
|
Atoms/Unit Cell |
1 | 2 | 4 |
|
Coord. Number |
6 | 8 | 12 |
|
Packing Eff. |
52.4% | 68% | 74% |
|
Void Space |
47.6% | 32% | 26% |
|
Example |
Polonium | Na, Fe, Cr | Cu, Ag, Au |
6. Close Packing of Spheres
In a crystal, particles
pack as closely as possible to minimize empty space. There are two important
close-packed structures:
6.1 Hexagonal Close Packing (HCP) — ABAB pattern
In HCP, the second layer
(B) is placed in the hollows of the first layer (A). The third layer is placed
directly above the first layer (A). Pattern: ABABAB...
✦ Coordination Number = 12
✦ Packing Efficiency = 74%
✦ Examples: Mg, Zn, Ti, Be, Cd
6.2 Cubic Close Packing (CCP / FCC) — ABCABC pattern
The third layer (C) is
placed differently from both A and B. Pattern: ABCABC...
✦ Coordination Number = 12
✦ Packing Efficiency = 74% (same as
HCP)
✦ Examples: Cu, Ag, Au, Al, Ni
|
💡 Key Insight: HCP vs CCP |
|
Both HCP and CCP have the SAME packing efficiency (74%) and
coordination number (12). |
|
They differ only in the stacking sequence of layers. |
|
HCP: ABABAB...
(hexagonal symmetry) |
|
CCP: ABCABC...
(cubic symmetry = FCC) |
6.3 Voids in Close-Packed Structures
When spheres pack
together, empty spaces (voids/holes) are left. These voids are very important
because smaller atoms/ions can fit into them.
|
Type of Void |
Description |
|
Tetrahedral Void |
Formed when a sphere of
second layer is above the triangular void of first layer. Surrounded by 4
spheres. Smaller size — radius ratio = 0.225r. |
|
Octahedral Void |
Formed between 3 spheres of
layer A and 3 of layer B. Surrounded by 6 spheres. Larger size — radius ratio
= 0.414r. |
|
📌 Number of Voids Formula |
|
If 'n' = number of close-packed spheres in a unit cell: |
|
🔹 Number of
Tetrahedral Voids = 2n |
|
🔹 Number of
Octahedral Voids = n |
|
So: For FCC (n = 4):
Tetrahedral voids = 8,
Octahedral voids = 4 |
7. Density of Unit Cell
One of the most important
numerical calculations in Solid State Chemistry is finding the density of a
crystal using unit cell parameters.
|
🔢 DENSITY FORMULA |
|
|
|
Z × M |
|
d =
───────── |
|
NA × a³ |
|
|
|
Where: |
|
d = density of the crystal (g/cm³) |
|
Z = number of atoms per unit cell (SC=1, BCC=2, FCC=4) |
|
M = molar mass of the element (g/mol) |
|
NA = Avogadro's
number = 6.022 × 10²³ mol⁻¹ |
|
a = edge length of the unit cell (in cm) |
|
a³ = volume of the
unit cell |
Solved Example
|
✏️ Example Problem |
|
Q: An element has BCC structure with edge length a = 287
pm. Molar mass = 56 g/mol. |
|
Calculate the
density of the element. |
|
|
|
Solution: |
|
Z = 2 (BCC), M = 56
g/mol, a = 287 pm = 287 × 10⁻¹⁰ cm |
|
NA = 6.022 × 10²³
mol⁻¹ |
|
|
|
d = (Z × M) / (NA ×
a³) |
|
= (2 × 56) /
(6.022 × 10²³ × (287 × 10⁻¹⁰)³) |
|
= 112 / (6.022 ×
10²³ × 2.364 × 10⁻²³) |
|
= 112 / 14.23 |
|
≈ 7.87 g/cm³ |
|
|
|
Answer: Density ≈ 7.87 g/cm³ (This element is Iron — Fe!) |
8. Imperfections / Defects in Solids
A perfect crystal would
have all particles in their correct positions at 0 K. In reality, all crystals
have some imperfections. These are called Crystal Defects.
|
📌 Types of Defects |
|
1. Point Defects — Missing, extra, or misplaced atoms at
lattice points. |
|
2. Line Defects — Defects along a row of atoms. |
|
3. Planar Defects — Defects at grain boundaries. |
|
In Class 12, we mainly study POINT DEFECTS. |
8.1 Stoichiometric Defects (No change in composition)
|
Defect |
Description, Occurs In & Effect |
|
Vacancy Defect |
Some lattice sites are
empty. Occurs in non-ionic solids when heated. Decreases density. |
|
Interstitial Defect |
Extra atoms occupy
interstitial spaces. Occurs in non-ionic solids. Increases density. |
|
Schottky Defect |
Equal number of cations and
anions are missing. Occurs in ionic solids with similar sized ions. Decreases
density. Example: NaCl, KCl, AgBr. |
|
Frenkel Defect |
Smaller ions leave lattice
and occupy interstitial spaces. No change in density. Occurs in ionic solids
with large size difference. Example: ZnS, AgCl, AgBr, AgI. |
|
🔑 Schottky vs Frenkel — Quick
Difference |
|
Schottky Defect:
Ions are MISSING → Density DECREASES
→ NaCl (equal sized ions) |
|
Frenkel Defect:
Ions DISPLACED → Density
UNCHANGED → ZnS, AgCl (unequal sized
ions) |
|
AgBr shows BOTH Schottky and Frenkel defects — used in
photographic films! |
8.2 Non-Stoichiometric Defects (Change in composition ratio)
|
Defect |
Description & Example |
|
Metal Excess Defect
(F-Centre) |
Extra cations occupy
interstitial spaces, electrons fill anion vacancies. These electrons absorb
visible light → crystal appears coloured. Example: NaCl heated in Na vapour
turns yellow; KCl turns violet/lilac. |
|
Metal Deficiency Defect |
Fewer cations than anions.
Some metal ions exist in higher oxidation states. Example: FeO — always
Fe₀.₉₅O instead of FeO; some Fe³⁺ present. |
|
💡 F-Centre (Farbe = Colour) |
|
When NaCl crystals are heated in Na vapour → Na atoms
deposit on surface → extra Na⁺ ions |
|
enter lattice → Cl⁻ vacancies are filled by electrons →
these electrons are called F-centres. |
|
F-centres absorb light and make the crystal appear
coloured. |
|
NaCl + Na vapour → Yellow crystal |
|
KCl + K vapour → Violet/Lilac crystal |
8.3 Impurity Defects
When a foreign atom/ion
enters the crystal lattice, it creates an impurity defect.
✦ Substitutional Impurity: Foreign ion
replaces host ion. Example: SrCl₂ added to NaCl → Sr²⁺ replaces Na⁺. Each Sr²⁺
creates one cation vacancy to maintain electrical neutrality.
✦ Interstitial Impurity: Foreign atom
occupies void. Example: Carbon in iron (steel formation).
9. Electrical Properties of Solids
Solids can be classified
based on their ability to conduct electricity. This depends on the band
structure — the arrangement of energy levels (bands) in a solid.
9.1 Band Theory of Solids
In isolated atoms,
electrons occupy discrete energy levels. When atoms come together in a crystal,
these levels broaden into energy BANDS.
✦ Valence Band (VB): Filled with
valence electrons.
✦ Conduction Band (CB): Empty or
partially filled band where electrons can move freely.
✦ Forbidden Gap (Band Gap): Energy gap
between VB and CB.
|
Type of Solid |
Band Structure & Conductivity |
|
Conductors (Metals) |
VB and CB overlap OR CB is
partially filled. No band gap. Conductivity: 10⁴ – 10⁷ S/m. Examples: Cu, Ag,
Al, Fe |
|
Insulators |
Large band gap (> 3 eV).
Electrons cannot jump to CB. Conductivity: < 10⁻²⁰ S/m. Examples: Diamond,
Wood, Plastic, Glass |
|
Semiconductors |
Small band gap (~1 eV).
Electrons can jump at room temperature or by heating/doping. Conductivity:
10⁻⁶ to 10⁴ S/m. Examples: Si, Ge, GaAs |
9.2 Types of Semiconductors
|
🔬 Intrinsic Semiconductors |
|
Pure semiconductors with small band gap. |
|
Conductivity is due to thermal excitation of electrons. |
|
Examples: Pure Silicon (Si), Pure Germanium (Ge) |
|
At 0 K → insulator. At room temperature → slight
conductivity. |
|
🔬 Extrinsic Semiconductors
(Doped) |
|
Conductivity is increased by adding impurities (doping). |
|
|
|
n-type Semiconductor: |
|
• Doped with Group
15 element (P, As, Sb) into Group 14 (Si, Ge) |
|
• Extra electron
available → electrons are majority charge carriers |
|
• Example: Si doped
with Phosphorus (P) |
|
|
|
p-type Semiconductor: |
|
• Doped with Group
13 element (B, Al, Ga) into Group 14 (Si, Ge) |
|
• One electron less
→ hole is created → holes are majority charge carriers |
|
• Example: Si doped
with Boron (B) |
10. Magnetic Properties of Solids
The magnetic behaviour of
a substance depends on the number of unpaired electrons in its atoms or ions.
Paired electrons create opposing magnetic moments that cancel, while unpaired
electrons create net magnetic moments.
|
Type |
Description & Examples |
|
Diamagnetic |
All electrons are PAIRED.
Weakly REPELLED by magnetic field. Very weak effect. Examples: NaCl, TiO₂,
Cu, Zn, H₂O, Benzene |
|
Paramagnetic |
Has UNPAIRED electrons.
Weakly ATTRACTED by magnetic field. Effect lost when field is removed.
Examples: O₂, Cu²⁺, Fe³⁺, CuO, TiO |
|
Ferromagnetic |
Unpaired electrons
spontaneously align parallel in same direction — magnetic domains form.
Strongly attracted. Retain magnetism permanently. Examples: Fe, Co, Ni, CrO₂
(used in audio tapes) |
|
Antiferromagnetic |
Magnetic moments alternate
— cancel each other. Net magnetism = 0. Examples: MnO, MnO₂, Cr₂O₃, V₂O₃ |
|
Ferrimagnetic |
Unequal number of parallel
and anti-parallel magnetic moments. Net magnetism is small but non-zero.
Examples: Fe₃O₄ (magnetite), ZnFe₂O₄, MgFe₂O₄ |
|
💡 Easy Memory Trick for Magnetic
Properties |
|
DIA → Dull,
Indifferent, Away from magnet (repelled)
→ ALL paired electrons |
|
PARA → Partially attracted (weak) → Some unpaired electrons |
|
FERRO→ Strongly pulled
→ Large domains aligned → Fe,
Co, Ni |
|
FERRI→ FERRIte (mixed oxides) → Unequal anti-parallel moments → Fe₃O₄ |
|
ANTI → Anti = cancel each other → Equal anti-parallel
moments → MnO |
11. Important Formulae & Quick Revision
|
📐 All Important Formulae at a
Glance |
|
1. DENSITY: d = (Z ×
M) / (NA × a³) |
|
|
|
2. PACKING EFFICIENCY = (Volume occupied by atoms in unit
cell / Total volume) × 100 |
|
SC = (π/6)
= 52.4% |
|
BCC = (π√3/8) =
68% |
|
FCC = (π/3√2) =
74% |
|
|
|
3. NUMBER OF VOIDS (in CCP/HCP, n = number of atoms): |
|
Tetrahedral voids
= 2n |
|
Octahedral
voids = n |
|
|
|
4. RADIUS RATIOS for Voids: |
|
Tetrahedral void:
r/R = 0.225 |
|
Octahedral
void: r/R = 0.414 |
|
Cubic void: r/R = 0.732 |
|
|
|
5. ATOMS PER UNIT CELL: |
|
Corner atom → shared by 8 cells → contributes 1/8 |
|
Edge atom → shared by 4 cells → contributes 1/4 |
|
Face atom → shared by 2 cells → contributes 1/2 |
|
Body centre → 1 cell only → contributes 1 |
Quick Revision Table
|
Structure |
Z (Atoms) |
CN |
Pack. Eff. |
|
SC (Primitive) |
1 |
6 |
52.4% |
|
BCC |
2 |
8 |
68% |
|
FCC/CCP |
4 |
12 |
74% |
|
HCP |
6 (full cell) |
12 |
74% |
|
⭐ EXAM IMPORTANT POINTS |
|
1. Schottky Defect → DECREASES density (NaCl, KCl, KBr) |
|
2. Frenkel Defect →
NO change in density (ZnS, AgCl, AgBr) |
|
3. AgBr shows BOTH Schottky and Frenkel defects |
|
4. F-Centre → responsible for colour in crystals (NaCl →
yellow when heated in Na vapour) |
|
5. CrO₂ is ferromagnetic → used in magnetic audio/video
tapes |
|
6. Fe₃O₄ is ferrimagnetic (also called magnetite/lodestone) |
|
7. Graphite is covalent solid but good conductor (due to
delocalized π electrons in layers) |
|
8. Diamond is hardest natural substance (each C bonded to 4
C in tetrahedral arrangement) |
|
9. In n-type semiconductor: electrons are majority carriers
(doped with Group 15) |
|
10. In p-type semiconductor: holes are majority carriers
(doped with Group 13) |
🎯 END OF CHAPTER 1 — SOLID STATE
🎯
Best of luck for your exams! Keep learning and keep
growing. ✨