
NCERT Solutions for Class 12 Chemistry Chapter 1 – The Solid State are highly important for students preparing for the CBSE Class 12 Chemistry Board Exam scheduled on 28 February 2026. As the examination date approaches, it becomes essential for students to revise fundamental chapters that focus on crystal structures, unit cells, packing efficiency, defects in solids, and electrical as well as magnetic properties of solids.
Chapter 1 plays an important role in building conceptual clarity for both theory-based and numerical questions frequently asked in the board examination. Referring to NCERT-based solutions at this stage helps students understand key definitions, improve their approach to application-based questions, and strengthen accuracy in calculation-oriented problems related to unit cells and packing efficiency.
NCERT Solutions for Class 12 Chemistry Chapter 2
Answer the following Questions of NCERT Solutions for Class 12 Chemistry Chapter 1:
Question 1. Name the parameters that characterize a unit cell. Solution : The six parameters that characterise a unit cell are as follows. (i) Its dimensions along the three edges, a, b, and c These edges may or may not be equal. (ii) Angles between the edges These are the angle ∝ (between edges b and c), β (between edges a and c), and γ (between edges a and b).NCERT Solutions for Class 12 Chemistry Chapter 3
Question 2. Distinguish between (i)Hexagonal and monoclinic unit cells (ii) Face-centred and end-centred unit cells.
Monoclinic unit cell For a monoclinic cell,
NCERT Solutions for Class 12 Chemistry Chapter 4
Question 4. What is the two dimensional coordination number of a molecule in square close packed layer?
of the number of atoms of N. Therefore, ratio of the number of atoms of M to that of N is M: N
= 2 : 3 Thus, the formula of the compound is M 2 N 3 .
NCERT Solutions for Class 12 Chemistry Chapter 5
Question 7. Which of the following lattices has the highest packing efficiency (i) simple cubic (ii) body-centred cubic and (iii) hexagonal close-packed lattice?
p-type semiconductor: The semiconductor whose increased in conductivity is a result of electron hole is called a p-type semiconductor. When a crystal of group 14 elements such as Si or Ge is doped with a group 13 element such as B, Al, or Ga (which contains only three valence electrons), a p-type of semiconductor is generated. When a crystal of Si is doped with B, the three electrons of B are used in the formation of three covalent bonds and an electron hole is created. An electron from the neighbouring atom can come and fill this electron hole, but in doing so, it would leave an electron hole at its original position. The process appears as if the electron hole has moved in the direction opposite to that of the electron that filled it. Therefore, when an electric field is applied, electrons will move toward the positively-charged plate through electron holes. However, it will appear as if the electron holes are positively-charged and are moving toward the negatively- charged plate. 
On the other hand, in the case of an insulator, the valence band is fully- filled and there is a large gap between the valence band and the conduction band. (ii) In the case of a conductor, the valence band is partially-filled or it overlaps with a higher energy, unoccupied conduction band. So, the electrons can flow easily under an applied electric field.
On the other hand, the valence band of a semiconductor is filled and there is a small gap between the valence band and the next higher conduction band. Therefore, some electrons can jump from the valence band to the conduction band and conduct electricity.
(ii) Frenkel defect: Ionic solids containing large differences in the sizes of ions show this type of defect. When the smaller ion (usually cation) is dislocated from its normal site to an interstitial site, Frenkel defect is created. It creates a vacancy defect as well as an interstitial defect. Frenkel defect is also known as dislocation defect. Ionic solids such as AgCl, AgBr, AgI, and ZnS show this type of defect.
(iii) Interstitials: Interstitial defect is shown by non-ionic solids. This type of defect is created when some constituent particles (atoms or molecules) occupy an interstitial site of the crystal. The density of a substance increases because of this defect.
(iv) F-centres: When the anionic sites of a crystal are occupied by unpaired electrons, the ionic sites are called F-centres. These unpaired electrons impart colour to the crystals. For example, when crystals of NaCl are heated in an atmosphere of sodium vapour, the sodium atoms are deposited on the surface of the crystal. The Cl ions diffuse from the crystal to its surface and combine with Na atoms, forming NaCl. During this process, the Na atoms on the surface of the crystal lose electrons. These released electrons diffuse into the crystal and occupy the vacant anionic sites, creating F-centres. 
= 2.27 × 10 22
mol of SrCl 2 = 10 −5 mol of SrCl 2 Cation vacancies produced by one Sr 2+ ion = 1
Hence, the concentration of cation vacancies created by SrCl 2 is 6.022 × 10 8 per mol of NaCl.
Schematic alignment of magnetic moments in ferromagnetic substances (ii) Paramagnetism: The substances that are attracted by a magnetic field are called paramagnetic substances. Some examples of paramagnetic substances are O 2 , Cu 2t , Fe 3t , and Cr 3t . Paramagnetic substances get magnetised in a magnetic field in the same direction, but lose magnetism when the magnetic field is removed. To undergo paramagnetism, a substance must have one or more unpaired electrons. This is because the unpaired electrons are attracted by a magnetic field, thereby causing paramagnetism. (iii) Ferrimagnetism: The substances in which the magnetic moments of the domains are aligned in parallel and anti-parallel directions, in unequal numbers, are said to have ferrimagnetism. Examples include Fe 3 O 4 (magnetite), ferrites such as MgFe 2 O 4 and ZnFe 2 O 4 . Ferrimagnetic substances are weakly attracted by a magnetic field as compared to ferromagnetic substances. On heating, these substances become paramagnetic.
Schematic alignment of magnetic moments in ferrimagnetic substances (iv) Antiferromagnetism: Antiferromagnetic substanceshave domain structures similar to ferromagnetic substances, but are oppositely-oriented. The oppositely-oriented domains cancel out each other’s magnetic moments.
Schematic alignment of magnetic moments in antiferromagnetic substances (v) 12-16 and 13-15 group compounds: The 12-16 group compounds are prepared by combining group 12 and group 16 elements and the 13-15 group compounds are prepared by combining group 13 and group15 elements. These compounds are prepared to stimulate average valence of four as in Ge or Si. Indium (III) antimonide (IrSb), aluminium phosphide (AlP), and gallium arsenide (GaAS) are typical compounds of groups 13-15. GaAs semiconductors have a very fast response time and have revolutionised the designing of semiconductor devices. Examples of group 12-16 compounds include zinc sulphide (ZnS), cadmium sulphide (CdS), cadmium selenide (CdSe), and mercury (II) telluride (HgTe). The bonds in these compounds are not perfectly covalent. The ionic character of the bonds depends on the electronegativities of the two elements. Question 35. Define the term 'amorphous'. Give a few examples of amorphous solids. Solution : Amorphous solids are the solids whose constituent particles are of irregular shapes and have short range order. These solids are isotropic in nature and melt over a range of temperature. Therefore, amorphous solids are sometimes called pseudo solids or super cooled liquids. They do not have definite heat of fusion. When cut with a sharp-edged tool, they cut into two pieces with irregular surfaces. Examples of amorphous solids include glass, rubber, and plastic.
⇒ d =zm / a 3----------------------------(1) [Since mass of the unit cell = Number of atoms in the unit cell × mass of one atom] [Volume of the unit cell = (Edge length of the cubic unit cell) 3 ] From equation (i), we have: m = da 3 /z -----------------------------------------(ii) Now, mass of one atom of metal (m)
Therefore,
If the edge lengths are different (say a, b and c), then equation (ii) becomes: M = d(abc)NAz (iv) From equations (iii) and (iv), we can determine the atomic mass of the unknown metal.
Let ,the edge length = a Radius of each particle = r. Thus, a = 2r Volume of spheres = πr 3 (4/3) Volume of a cubic unit cell = a 3 = (2r) 3 = 8r 3 We know that the number of particles per unit cell is 1. Therefore, Packing efficiency = Volume of one particle/Volume of cubic unit cell = [ πr 3 (4/3) ] / 8r 3 = 0.524 or 52.4 % (b) Body-centred cubic:
From ∆FED, we have: b 2 = 2a 2 b = ( 2a ) 1/2 Again, from ∆AFD, we have : c 2 = a 2 + b 2 => c 2 = a 2 + 2a 2 c 2 = 3a 2 => c = (3a) 1/2 Let the radius of the atom = r. Length of the body diagonal, c = 4r => (3a) 1/2 = 4r => a = 4r/ (3) 1/2 or , r = [ a (3) 1/2 ]/ 4 Volume of the cube, a 3 = [4r/ (3) 1/2 ] 3 A BCC lattice has 2 atoms. So, volume of the occupied cubic lattice = 2πr 3 (4/3) = πr 3 ( 8/3) Therefore, packing efficiency = [ πr 3 ( 8/3) ]/ [ { 4r/(3) 1/2 } 3 ] = 0.68 or 68% (iii) Face-centred cubic:
Let the edge length of the unit cell = a let the radius of each sphere = r Thus, AC = 4r From the right angled triangle ABC, we have : AC = ( a 2 + a 2 ) 1/2 = a(2) 1/2
Therefore, 4r = a(2) 1/2 => a = 4r/( 2) 1/2 Thus, Volume of unit cell =a 3 = { 4r/( 2) 1/2 } 3 a 3 = 64r 3 /2(2) 1/2 = 32r 3 / (2) 1/2 No. of unit cell in FCC = 4 Volume of four spheres = 4 × πr 3 (4/3) Thus, packing efficiency = [πr 3 (16/3) ] / [32r 3 / (2) 1/2 ] = 0.74 or 74 %
Let the edge length of the cube be ‘a’ and the radius of each particle be r. So, we can write: a = 2r Now, volume of the cubic unit cell = a 3 = (2r) 3 = 8r 3 We know that the number of particles per unit cell is 1. Therefore, volume of the occupied unit cell
Hence, packing efficiency
(ii) Body-centred cubic
It can be observed from the above figure that the atom at the centre is in contact with the other two atoms diagonally arranged. From ΔFED, we have:
Again, from ΔAFD, we have:
Let the radius of the atom be r. Length of the body diagonal, c = 4π
or,
Volume of the cube,
A body-centred cubic lattice contains 2 atoms. So, volume of the occupied cubic lattice
(iii) Face-centred cubic Let the edge length of the unit cell be ‘a’ and the length of the face diagonal AC be b.
From ΔABC, we have:
Let r be the radius of the atom. Now, from the figure, it can be observed that:
Now, volume of the cube,
We know that the number of atoms per unit cell is 4. So, volume of the occupied unit cell
= 74%
= 107.13 gmol −1 Therefore, atomic mass of silver = 107.13 u
It is also given that the atoms of P are present at the body-centre. Therefore, number of atoms of P in one unit cell = 1 This means that the ratio of the number of P atoms to the number of Q atoms, P:Q = 1:1 Hence, the formula of the compound is PQ. The coordination number of both P and Q is 8.
= 3.612 × 10 −23 cm 3 So, a = 3.306 × 10 −8 cm For body-centred cubic unit cell:
= 1.432 × 10 −8 cm = 14.32 × 10 −9 cm = 14.32 nm
A sphere with centre O, is fitted into the octahedral void as shown in the above figure. It can be observed from the figure that ΔPOQ is right-angled ∠POQ = 90 0 Now, applying Pythagoras theorem, we can write: 
= 8.97 g cm −3 The measured value of density is given as 8.92 g cm −3 . Hence, the calculated density 8.97 g cm −3 is in agreement with its measured value.