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Physical Chemistry - Solid State
Rating: 4.8 out of 5(7 ratings)
37 students

Physical Chemistry - Solid State

Complete Chemistry for Engg and Medical Entrance Exam Preparation. ( IIT JEE Main | Advanced | BITSAT | SAT | NEET etc.)
Created bystudi live
Last updated 3/2022
English

What you'll learn

  • Describe general characteristics of solid state
  • Distinguish between amorphous and crystalline solids
  • Classify crystalline solids on the basis of the nature of binding forces
  • Define crystal lattice and unit cell
  • Explain close packing of particles
  • Describe different types of voids and close packed structures
  • Calculate the packing efficiency of different types of cubic unit cells
  • Correlate the density of a substance with its unit cell properties
  • Describe the imperfections in solids and their effect on properties
  • Correlate the electrical and magnetic properties of solids and their structure

Course content

2 sections46 lectures7h 29m total length
  • Introduction2:40

    Explore solid state fundamentals, comparing solids with liquids and gases, and examine conductivity, magnetic and dielectric properties, impurities, and their relevance to batteries.

  • Classification of Solids12:49

    classify solids into crystalline or amorphous by particle arrangement; crystalline solids show regular order and anisotropy with a sharp melting point, while amorphous solids are isotropic with no sharp melting.

  • Classification of Crystalline Solids13:34

    Classify crystalline solids into ionic, metallic, covalent, and molecular solids; compare their constituent particles, bonding, melting points, and electrical conductivity.

  • Crystal Lattice and Unit Cell11:29

    Discover how solids form a repeating crystal lattice and identify the unit cell as the smallest 3D repeating unit with lattice parameters a, b, c and angles alpha, beta, gamma.

  • Effective Number of Atoms in a Unit Cell6:01

    Determine the effective number of atoms in a unit cell by accounting for sharing of corner, face-centered, and body-centered atoms. Illustrate corners shared among eight units and faces contributing half.

  • Types of Unit Cell10:12

    Identify the basic classifications of unit cells in solids: simple cubic, body-centered, and face-centered structures, and explain how corners and faces host particles to determine the atoms per cell.

  • Number of Atoms Per Unit Cell9:33

    Count atoms in simple cubic, fcc, and bcc unit cells by summing corner and center or face contributions, revealing 1, 4, and 2 atoms per unit cell.

  • Seven Crystal Systems and Fourteen Bravais Lattice15:07

    Explore the seven crystal systems and fourteen Bravais lattices using the a, b, c parameters and alpha, beta, gamma angles to classify crystal structures.

  • Unit Cell Parameters Part - 112:23

    Explore unit cell parameters in solid state chemistry, focusing on simple cubic and body-centered cubic structures, including corner and center atoms, body diagonals, and edge length and radius relations.

  • Unit Cell Parameters Part - 29:25

    Explore unit cell parameters for fcc and hexagonal close packing, derive edge length relations using Pythagoras in a simple diagram, and compute hexagonal area and volume formulas.

  • Density of Cubic Unit Cell9:09

    Compute the density of a cubic unit cell by using its mass, volume, and the number of particles, and apply this to simple, bcc, and fcc structures.

  • Packing of Particles in a Solid11:44

    Explore how particles pack in solids by analyzing one-dimensional coordination of two neighbors, and two-dimensional square and hexagonal close packing, with coordination numbers 2, 4, and 6 respectively.

  • Packing of Particles in a Solid Part - 213:48

    Explore three-dimensional packing of particles in solids, from simple cubic structures and coordination numbers to hexagonal close packing and cubic close packing with ABAB and ABC stacking.

  • Packing Fraction (PF)12:59

    Analyze packing fraction in simple cubic, body-centered, and face-centered cubic lattices by comparing sphere volume to unit cell volume, revealing about 52%, 68%, and 74%, with FCC most densely packed.

  • Voids13:48

    Explore voids in close-packed structures, detailing tetrahedral and octahedral voids in two- and three-dimensional arrangements. Identify their locations relative to FCC/ccp lattices and body diagonals.

  • Radius Ratio Rule7:18

    Explore the radius ratio rule for ionic solids, linking radius ratios to coordination numbers and crystal structure types, and predict the shape and Miller-type arrangements of ionic crystals.

  • Structure of AB Type Ionic Crystal (NaCl)12:27

    Explain the structure of ab type ionic crystals using NaCl as the example, where Cl− occupies fcc lattice sites and Na+ sits in octahedral voids, giving 6-fold coordination.

  • Structure of AB Type Ionic Crystal (CsCl)9:40

    Examine AB-type ionic crystals with CsCl as a model, featuring a body-centered cubic lattice where Cs+ and Cl− occupy alternating sites and each ion has coordination number 8.

  • Structure of AB Type Ionic Crystal (ZnS)8:33

    This lecture explains the zinc blende ab-type ZnS structure in a fcc lattice, detailing how S2- occupy corners and faces while Zn2+ occupy tetrahedral sites.

  • Structure of A2B Type Ionic Crystal (Sodium Oxide)15:04

    Explore the structure of a2b type ionic crystal using sodium oxide as an example, showing Na+ in tetrahedral holes of an O2- fcc lattice and coordination 4 and 8.

  • Structure of AB2 Type Ionic Crystal (Calcium Fluoride)18:15

    Explore the CaF2 structure as an AB2-type ionic crystal with Ca2+ in a face-centered cubic lattice and F− in tetrahedral voids, yielding Ca2+ eightfold and F− fourfold coordination.

  • Stoichiometric Defects9:17

    Define stoichiometric defects as fixed ion ratios and explain vacancy and interstitial defects, introduced via heating, and analyze how these defects affect mass, volume, and density.

  • Stoichiometric Defects Part - 216:19

    Examine stoichiometric defects in ionic crystals, focusing on Schottky and Frankel defects, their formation conditions, and how coordination number and ion size govern their mass, volume, and electrical neutrality.

  • Impurity Defects10:10

    Analyze impurity defects in solids: substitutional impurities replacing a host atom and interstitial defects where small atoms occupy lattice voids, illustrated by brass and carbon in iron.

  • Non-stoichiometric Defects17:19

    Explain non-stoichiometric defects in solids, detailing metal deficiency and metal excess, how vacancies and charge compensation alter composition, and how f-centers cause color changes.

  • Bragg's Law12:49

    Present Bragg's law for solid state, showing x-ray diffraction from crystal planes produces constructive interference when the path difference equals an integer multiple of the wavelength.

  • Applications of Bragg's Law7:40

    Apply Bragg's law to identify crystal structure and plane spacing from X-ray diffraction patterns, and use electron and neutron diffraction to characterize materials, distinguishing metals from organic by reflected intensity.

  • Electrical Properties of Solids8:30

    Classify solids by electrical properties into conductors, insulators, and semiconductors, and show how each type controls current flow with examples like metals, plastic, and Silicon.

  • Band Theory15:32

    Explore how band theory explains why some solids conduct, insulate, or act as semiconductors by examining valence and conduction bands, band gaps, and temperature-driven electron transfer.

  • Extrinsic Semiconductors15:17

    Extrinsic semiconductors form when silicon or germanium is doped with small impurities, creating p-type holes or n-type extra electrons to boost conductivity.

  • Dielectric Properties of Solid9:21

    Explore dielectric properties of solids by studying how insulators polarize under an electric field, forming dipoles with net, canceled, or absent moments, and note piezoelectric behavior.

  • Magnetic Properties of Solids6:53

    Explore how electrons give solids magnetic properties through orbital motion and spin, creating tiny magnets and influencing permanent angular momentum, measured by the standard magnetic unit.

  • Classification of Substances Based on Their Magnetic Properties15:02

    Classify solids by magnetic properties, distinguishing diamagnetic, paramagnetic, ferromagnetic, antiferromagnetic, and ferrite materials through unpaired electrons, dipole moments, and curie temperature.

  • Classification of Solids Based on Their Magnetic Properties12:47

    Explore how solids are classified by magnetic properties, including diamagnetic, paramagnetic, ferromagnetic, ferrimagnetic, and antiferromagnetic behaviors, with unpaired electrons, examples, and Curie temperature insights.

  • Spinal Structure12:15

    Learn about the spinel structure in solid-state chemistry, focusing on normal spinel AB2O4 with A2+ in tetrahedral sites and B3+ in octahedral sites, and the inverse spinel arrangement.

Requirements

  • Basic understanding of chemistry and math's

Description

SUMMARY

Solids have definite mass, volume and shape. This is due to the fixed position of their constituent particles, short distances and strong interactions between them. In amorphous solids, the arrangement of constituent particles has only short range order and consequently they behave like super cooled liquids, do not have sharp melting points and are isotropic in nature. In crystalline solids there is long range order in the arrangement of their constituent particles. They have sharp melting points, are anisotropic in nature and their particles have characteristic shapes. Properties of crystalline solids depend upon the nature of interactions between their constituent particles. On this basis, they can be divided into four categories, namely: molecular, ionic, metallic and covalent solids. They differ widely in their properties.

The constituent particles in crystalline solids are arranged in a regular pattern which extends throughout the crystal. This arrangement is often depicted in the form of a three dimensional array of points which is called crystal lattice. Each lattice point gives the location of one particle in space. In all, fourteen different types of lattices are possible which are called Bravais lattices. Each lattice can be generated by repeating its small characteristic portion called unit cell. A unit cell is characterised by its edge lengths and three angles between these edges. Unit cells can be either primitive which have particles only at their corner positions or centred. The centred unit cells have additional particles at their body centre (bodycentred), at the centre of each face (face-centred) or at the centre of two opposite faces (end-centred). There are seven types of primitive unit cells. Taking centred unit cells also into account, there are fourteen types of unit cells in all, which result in fourteen Bravais lattices.

Close-packing of particles result in two highly efficient lattices, hexagonal close-packed (hcp) and cubic close-packed (ccp). The latter is also called facecentred cubic (fcc) lattice. In both of these packings 74% space is filled. The remaining space is present in the form of two types of voids-octahedral voids and tetrahedral voids. Other types of packing are not close-packings and have less efficient packing of particles. While in body-centred cubic lattice (bcc) 68% space is filled, in simple cubic lattice only 52.4 % space is filled.

Solids are not perfect in structure. There are different types of imperfections or defects in them. Point defects and line defects are common types of defects. Point defects are of three types - stoichiometric defects, impurity defects and non-stoichiometric defects. Vacancy defects and interstitial defects are the two basic types of stoichiometric point defects. In ionic solids, these defects are present as Frenkel and Schottky defects. Impurity defects are caused by the presence of an impurity in the crystal. In ionic solids, when the ionic impurity has a different valence than the main compound, some vacancies are created. Nonstoichiometric defects are of metal excess type and metal deficient type. Sometimes calculated amounts of impurities are introduced by doping in semiconductors that change their electrical properties. Such materials are widely used in electronics industry. Solids show many types of magnetic properties like paramagnetism, diamagnetism, ferromagnetism, antiferromagnetism and ferrimagnetism. These properties are used in audio, video and other recording devices. All these properties can be correlated with their electronic configurations or structures.


Who this course is for:

  • Parents whose wards are students preparing for Indian Engineering and Medical Entrance Exams
  • IIT JEE | JEE Main | JEE Advanced | BITSAT | NEET | AIPMT | KVPY | SAT | GATE | M