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Classification of Crystalline Solids is considered one of the most asked concept.
41 Questions around this concept.
Total volume of atoms present in a face-centred cubic unit cell of a metal is (r is atomic radius )
The interaction energy of London force is inversely proportional to sixth power of the distance between two interacting particles but their magnitude depends upon
Frenkel defect is also known as ________.
(i) stoichiometric defect
(ii) dislocation defect
(iii) impurity defect
(iv) non-stoichiometric defect
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The sharp melting point of crystalline solids is due to ___________.
Which of the following is an amorphous solid?
Which of the following is true about the value of the refractive index of quartz glass?
Which of the following is not a characteristic of a crystalline solid?
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Which of the following statement is not true about amorphous solids?
In solid state, $\mathrm{BeCl}_2$ exists as
Which of the following is not a property of ionic solid
General Characteristics of Solid State
Solid is the state of any matter in which constituents are firmly attached due to strong forces.
Solids have a definite shape, mass and volume.
Solids are almost incompressible, rigid and have mechanical strength.
Solids have close packed arrangement of atoms.
Solids have high density but very slow diffusion rate.
Solids can have only vibrational motion as the constituents have fixed positions.
In solids, constituents have strong force of attraction as intermolecular distances are short.
Type of Solids
Solids are mainly of the following two types:
Crystalline Solids
In such solids, the constituents are arranged in a definite or orderly manner which repeats itself over long distances.
They have a definite geometry with flat faces and sharp edges.
Such solids have sharp melting points and undergo clean cleavage.
They are considered as true solids.
These show anisotropy that is, different physical properties in different directions.
They show clean cleavage.
They are normally incompressible. For example, Diamond, Quartz.
Amorphous Solids
In such solids, the constituents are arranged in an irregular or disorderly manner over the long-range.
Such solids do not have sharp melting points and clean cleavage that is, have an irregular cut.
These are considered as pseudo solids.
These show isotropy that is, the same physical properties in all directions.
They do not show clean cleavage.
Note: Due to short-range order. amorphous solids may even have small parts in crystalline and the rest in non-crystalline form, crystalline parts of an otherwise amorphous substance are called crystallites.
Property |
Crystalline solids |
Amorphous solids |
Shape |
Definite characteristic geometrical shape |
Irregular shape
|
Melting point |
Melt at a sharp and characteristic temperature |
Gradually soften over a range of temperature |
Cleavage property |
When cutting with a sharp-edged tool, they split into two pieces and the newly generated surfaces are plain and smooth |
When cutting with a sharp-edged tool, they cut into two pieces with irregular surfaces |
Heat of fusion |
They have a definite and characteristic enthalpy of fusion |
They do not have a definite enthalpy of fusion |
Anisotropy |
Anisotropic in nature |
Isotropic in nature |
Nature |
True solids |
Pseudo solids or super cooled liquids |
Order in the arrangement of constituent particles |
Long-range order |
Only short-range order |
Isotropy and Anisotropy
Isotropic :
Amorphous solids are isotropic in nature. Their properties such as mechanical strength, refractive index, and electrical conductivity, etc. are the same in all directions. It is because there is no long-range order in them and the arrangement of particles is not definite along with all the directions. Hence, the overall arrangement becomes equivalent in all directions. Therefore, the value of any physical property would be the same in any direction.
Anisotropic :
Crystalline solids are anisotropic in nature, that is, some of their physical properties like electrical resistance or refractive index show different values when measured along with different directions in the same crystals. This arises from the different arrangements of particles in different directions. This is illustrated in Fig. 1.2. This figure shows a simple two - dimensional pattern of arrangement of two kinds of atoms. Mechanical properties such as resistance to shearing stress might be quite different in the two directions indicated in the figure. Deformation in CD direction displaces row which has two different types of atoms while in AB direction rows made of one type of atoms are displaced.
Molecular Solids
Their molecules are held together by dispersion forces, London forces, dipole-dipole forces or hydrogen bonds. On the basis of the type of interactive forces these solids are studied under the following sub-headings.
Ionic Solids
There is a regular arrangement of positively and negatively charged ions throughout the solid Where ions are held together by strong coulombic or electrostatic forces. These solids are very hard and brittle and have very high melting points. In solid state, as ions are not free to move, hence they are insulators but in molten state or in aqueous state, it's ions become free to move and it becomes a conductor. Ionic solids have high enthalpies of vaporisation. They are soluble in polar solvents like H2O but insoluble in non-polar solvents such as C6H6, CS2, CCl4 etc.
Examples : LiF, NaCl, KNO3, Na2SO4 etc.
Metallic Solids
Metal cores (ie., kernels) and a sea of mobile electrons are the constituents of metallic solids. Each metal atom contributes one or more electrons towards the sea of electrons. These electrons are evenly spread out throughout the crystals and weak forces of attraction or metallic bond binds together kernels and sea of electrons.
Metallic crystals may be hard as well as soft having moderate enthalpies Of fusion. Mobile sea Of electrons is responsible for many properties of metals such as malleability (can be beaten into thin sheets), ductility (can be drawn into wires), metallic lustre, thermal conductivity and electrical conductivity etc.
Example: Copper, Iron. Nickel. Metal alloys etc.
Covalent or Network Solids
In these, atoms are bonded together by covalent bond formation throughout the crystal It means there is a continuous network of covalent bonds a giant three-dimensional structure, or giant molecule. Covalent bonds are strong and directional in nature. These solids are very hard, brittle, and very high melting. Due to the absence of any free electrons or ions, they are insulators. Their enthalpies of fusion are very high.
Example: Diamond, Graphite, Boron Nitride (BN), Silicon Carbide (SiC), etc. are common examples of these solids.
Diamond: It has a three-dimensional network of a large number of sp3 hybridised carbon atoms each bonded tetrahedrally to four more carbon atoms by single covalent bonds. It makes diamond extremely hard crystal with very high mp ≃ 3843 K. Diamond does not conduct electricity at all.
Graphite: Each carbon atom is sp2 hybridised and covalently bonded to three other carbon atoms of the same layer by single bonds. forming a layer of hexagonal rings. At each carbon atom, the fourth valence electron is available free, which moves among different layers and provides good electrical and thermal conducting nature to graphite. Different layers connect by van der Waals forces. As the forces are quite weak, the layers can slide over each other and make graphite a soft, lubricating solid.
Different Types of Solid
Type of Solid |
Constituent Particles |
Bonding/ Attractive Forces |
Examples |
Physical Nature |
Electrical Conductivity |
Melting Point (in K) |
Bond Energy in KJ/mol |
(1)Molecular solids (i) Non polar
|
Molecules |
Dispersion or London forces |
Ar, CCl4, H2, I2, CO2 |
Soft |
Insulator |
Very low < 273 |
Low<40 |
(ii) Polar |
Dipole-dipole interactions |
HCl, SO2 |
Soft |
Insulators |
Low < 273 |
Low < 40 |
|
(iii) Hydrogen Bonded |
Hydrogen Bonding |
H2O(ice) |
Hard |
Insulators |
Low < 273 |
Low < 40 |
|
(2) Ionic solids |
Ions |
Coulombic or electrostatic |
NaCl, MgO, ZnS, CaF2 |
Hard But Brittle |
Insulators in solid state but conductors in molten state and aqueous solutions |
High > 1300K |
400 - 4000 |
(3) Metallic solids |
Positive ions in a sea of delocalised electrons |
Metallic Bonding |
Fe, Cu, Ag, Mg |
Hard but malleable and ductile |
Conductors in solid state as well as in molten state |
Fairly High 800 - 1000 |
80 - 1000 |
(4) Covalent or network solids |
Atoms |
Covalent Bonding |
SiO2(quartz), SiC, C(diamond), C(graphite) |
Hard Soft |
Insulators Conductor (exception) |
Very High > 3900 |
150 - 500 |
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