Chapter 1: Solid State
Exhaustive Revision Guide - 50 Subjective Questions with Detailed Solutions
Click on any question to reveal its answer.
1. Define crystalline solids. State any two characteristics.
Definition: A crystalline solid is a homogeneous solid in which the constituent particles (atoms, ions, or molecules) are arranged in a definite, repeating three-dimensional pattern over a long range.
Characteristics:
- They have a sharp and well-defined melting point.
- They exhibit anisotropy (physical properties like refractive index vary in different directions).
2. What are amorphous solids? Give two examples.
Definition: Amorphous solids are those in which the constituent particles are not arranged in any regular, repeating pattern over a long range. They possess short-range order.
Examples: Glass, rubber, plastics.
3. Distinguish between crystalline and amorphous solids. (Any 4 points)
| Property | Crystalline Solids | Amorphous Solids |
|---|---|---|
| Arrangement | Regular, long-range order | Irregular, short-range order |
| Melting Point | Sharp melting point | Melt over a range of temperatures |
| Isotropy | Anisotropic | Isotropic |
| Nature | True solids | Pseudo solids or supercooled liquids |
4. Explain the term 'Isomorphism' with an example.
Isomorphism: When two or more different chemical substances crystallize in the same crystalline structural form, the phenomenon is called isomorphism. Such substances have the same atomic ratio.
Example: Sodium fluoride ($NaF$) and Magnesium oxide ($MgO$) are isomorphous (atomic ratio 1:1).
5. What is 'Polymorphism'? Give an example.
Polymorphism: The phenomenon where a single substance can exist in two or more different crystalline forms under different conditions of temperature and pressure is called polymorphism. In elements, it is called allotropy.
Example: Carbon exists as diamond, graphite, and fullerenes. Calcium carbonate ($CaCO_3$) exists as calcite and aragonite.
6. Define Anisotropy and Isotropy.
Anisotropy: The ability of a crystalline solid to exhibit different values of physical properties (like electrical resistance, refractive index, thermal expansion) when measured in different directions is called anisotropy.
Isotropy: The property of amorphous solids where physical properties have the same value regardless of the direction of measurement is called isotropy.
7. Why is glass considered a supercooled liquid?
Glass is an amorphous solid. Like liquids, it has a tendency to flow, though very slowly. This is observed in old buildings where glass panes are slightly thicker at the bottom due to gravity. Because of this sluggish flow property, glass is termed a pseudo solid or a supercooled liquid.
8. Classify crystalline solids based on intermolecular forces.
Based on intermolecular forces, crystalline solids are classified into four types:
- Molecular Solids: Constituent particles are molecules held by Van der Waals forces. (e.g., Ice, solid $CO_2$)
- Ionic Solids: Constituent particles are ions held by strong electrostatic forces. (e.g., $NaCl$)
- Metallic Solids: Positive metal ions in a sea of delocalized electrons held by metallic bonds. (e.g., Copper, Iron)
- Covalent (Network) Solids: Atoms held together by continuous covalent bonds forming a network. (e.g., Diamond, Quartz)
9. Write a short note on Ionic Solids.
Ionic Solids consist of positively (cations) and negatively (anions) charged ions. They are held together by strong coulombic or electrostatic forces of attraction.
Properties:
- They are hard and brittle.
- They have very high melting and boiling points due to strong ionic bonds.
- They are electrical insulators in the solid state but become good conductors when melted (molten state) or dissolved in water because the ions become free to move.
10. Why are covalent network solids exceptionally hard and have very high melting points?
In covalent network solids (like diamond), atoms are linked to adjacent atoms by strong and highly directional covalent bonds throughout the entire crystal, forming a giant three-dimensional network structure. Breaking this massive network requires immense thermal energy, resulting in exceptional hardness and extremely high melting points.
11. Define: (a) Crystal lattice (Space lattice) (b) Unit cell.
(a) Crystal Lattice: A regular, three-dimensional arrangement of points in space representing constituent particles (atoms, ions, or molecules) of a crystal is called a crystal lattice.
(b) Unit Cell: The smallest repeating structural unit of a crystal lattice, which when repeated in different directions generates the entire crystal, is called a unit cell.
12. What are the parameters that characterize a unit cell?
A unit cell is characterized by 6 parameters:
- Edge lengths: Three edge lengths $a, b, c$ along the three crystallographic axes. They may or may not be mutually perpendicular.
- Interaxial angles: Three angles $\alpha, \beta, \gamma$ between the edges. ($\alpha$ between $b$ and $c$, $\beta$ between $a$ and $c$, $\gamma$ between $a$ and $b$).
13. What are Bravais lattices? How many are possible?
Bravais Lattices are the distinct three-dimensional arrangements of lattice points that describe the repeating structure of a crystal. The French mathematician Auguste Bravais proved that there are exactly 14 possible three-dimensional lattices, grouped into 7 crystal systems.
14. Differentiate between Simple, Body-Centered, and Face-Centered cubic unit cells.
- Simple Cubic (SC): Particles are present only at the 8 corners of the cube.
- Body-Centered Cubic (BCC): Particles are present at the 8 corners plus one particle exactly at the body center of the cube.
- Face-Centered Cubic (FCC): Particles are present at the 8 corners plus one particle at the center of each of the 6 faces of the cube.
15. Calculate the total number of atoms per unit cell in a Simple Cubic (SC) lattice.
In a simple cubic unit cell, atoms are present only at the 8 corners.
Each corner atom is shared by 8 adjacent unit cells. Thus, its contribution to one unit cell is $\frac{1}{8}$.
Total number of atoms ($Z$) = $8 \text{ corners} \times \frac{1}{8} \text{ atom per corner} = 1 \text{ atom}$.
16. Calculate the total number of atoms per unit cell in a Body-Centered Cubic (BCC) lattice.
A BCC unit cell has atoms at the 8 corners and 1 atom at the body center.
- Contribution of 8 corner atoms = $8 \times \frac{1}{8} = 1$ atom.
- Contribution of the atom at the body center (unshared) = $1 \times 1 = 1$ atom.
Total number of atoms ($Z$) = $1 + 1 = 2 \text{ atoms}$.
17. Calculate the total number of atoms per unit cell in a Face-Centered Cubic (FCC) lattice.
An FCC unit cell has atoms at 8 corners and 6 face centers.
- Contribution of 8 corner atoms = $8 \times \frac{1}{8} = 1$ atom.
- Each face center atom is shared by 2 unit cells. Contribution of 6 face atoms = $6 \times \frac{1}{2} = 3$ atoms.
Total number of atoms ($Z$) = $1 + 3 = 4 \text{ atoms}$.
18. What is Coordination Number in a crystal lattice?
Coordination Number: It is defined as the number of nearest neighboring particles (atoms, ions, or molecules) that are in direct contact with a given central particle in a crystal lattice.
Examples: In Simple Cubic, it is 6. In BCC, it is 8. In FCC/HCP/CCP, it is 12.
19. Differentiate between Hexagonal Close Packing (hcp) and Cubic Close Packing (ccp).
- HCP (AB AB AB... type): The spheres of the third layer are aligned exactly above the spheres of the first layer. It generates a hexagonal unit cell. Tetrahedral voids of the second layer are covered by the third layer.
- CCP (ABC ABC... type): The spheres of the third layer are not aligned with either the first or the second layer. It aligns with the first layer only at the fourth layer. It generates an FCC unit cell. Octahedral voids are covered by the third layer.
Both have a coordination number of 12 and a packing efficiency of 74%.
20. Define Packing Efficiency. State the packing efficiency of SC, BCC, and FCC.
Packing Efficiency: It is the percentage of total space in the unit cell that is occupied by the constituent particles (spheres).
$\text{Packing Efficiency} = \frac{\text{Volume occupied by particles}}{\text{Total volume of unit cell}} \times 100$
- Simple Cubic (SC): $52.4\%$
- Body-Centered Cubic (BCC): $68\%$
- Face-Centered Cubic (FCC / ccp / hcp): $74\%$
21. Derive the packing efficiency of a Simple Cubic unit cell.
In a simple cubic cell, particles touch each other along the edges.
Let edge length = $a$, radius of particle = $r$. Therefore, $a = 2r \Rightarrow r = a/2$.
Volume of the cubic unit cell = $a^3 = (2r)^3 = 8r^3$.
Number of atoms in SC cell ($Z$) = $1$.
Volume of 1 atom (sphere) = $\frac{4}{3}\pi r^3$.
$\text{Packing Efficiency} = \frac{\text{Volume of 1 atom}}{\text{Volume of unit cell}} \times 100$
$= \frac{\frac{4}{3}\pi r^3}{8r^3} \times 100 = \frac{\pi}{6} \times 100 \approx 52.36\%$.
22. Derive the relationship between atomic radius (r) and edge length (a) for a BCC lattice.
In a BCC unit cell, atoms touch each other along the body diagonal.
Length of the body diagonal in a cube of edge '$a$' is $\sqrt{3}a$.
Along the body diagonal, there are two corner radii and the full diameter of the center atom, so the length equals $4r$.
Therefore, $4r = \sqrt{3}a$
$r = \frac{\sqrt{3}}{4} a$
23. Derive the relationship between atomic radius (r) and edge length (a) for an FCC lattice.
In an FCC unit cell, atoms touch each other along the face diagonal.
Length of the face diagonal in a cube of edge '$a$' is $\sqrt{2}a$.
Along the face diagonal, there is one full atom and two half atoms from the corners touching, which equals $4r$.
Therefore, $4r = \sqrt{2}a$
$r = \frac{\sqrt{2}}{4} a = \frac{1}{2\sqrt{2}} a$ or $a = 2\sqrt{2}r$.
24. Define Tetrahedral Void and Octahedral Void.
Tetrahedral Void: The empty space left between four mutually touching spheres, where their centers form a regular tetrahedron, is called a tetrahedral void.
Octahedral Void: The empty space surrounded by six touching spheres, formed when a triangular void of one layer overlaps with a reversed triangular void of another layer, is called an octahedral void.
25. What is the relation between the number of constituent particles and the number of tetrahedral and octahedral voids in a close-packed structure?
Let the number of close-packed spheres (constituent particles) in a lattice be $N$.
- The number of Octahedral voids generated = $N$.
- The number of Tetrahedral voids generated = $2N$.
Therefore, total voids = $3N$.
26. State the formula to calculate the density of a unit cell. Explain the terms involved.
The density ($\rho$) of a unit cell is given by:
$$ \rho = \frac{Z \cdot M}{a^3 \cdot N_A} $$
Where:
- $Z$ = Number of atoms per unit cell (1 for SC, 2 for BCC, 4 for FCC)
- $M$ = Molar mass of the substance (g/mol)
- $a$ = Edge length of the unit cell (in cm)
- $N_A$ = Avogadro's number ($6.022 \times 10^{23} \text{ mol}^{-1}$)
- $\rho$ = Density (g/cm³)
27. What are crystal defects (imperfections)? Mention the main types of point defects.
Crystal Defects: Any deviation from the perfectly ordered arrangement of constituent particles in a crystal is called a crystal defect or imperfection. These occur naturally during crystallization, especially when the process is fast.
Main types of Point Defects:
- Stoichiometric Defects (Vacancy, Interstitial, Schottky, Frenkel)
- Non-Stoichiometric Defects (Metal excess, Metal deficiency)
- Impurity Defects
28. Explain Schottky Defect with an example.
Schottky Defect: It is a type of point defect in ionic solids that occurs when equal numbers of cations and anions are missing from their regular lattice sites, creating vacancies. This maintains the electrical neutrality of the crystal.
Conditions: Observed in highly ionic compounds with high coordination numbers and where cation and anion are of similar size.
Consequence: Decreases the density of the crystal.
Example: $NaCl, KCl, CsCl, AgBr$.
29. Explain Frenkel Defect with an example.
Frenkel Defect: It occurs when an ion (usually the smaller cation) is displaced from its normal lattice site and occupies an interstitial site between the lattice points.
Conditions: Observed in ionic compounds with low coordination numbers and a large difference in the size of cations and anions.
Consequence: Does not change the density of the crystal (mass and volume remain same).
Example: $ZnS, AgCl, AgBr, AgI$.
30. Distinguish between Schottky and Frenkel defects.
| Schottky Defect | Frenkel Defect |
|---|---|
| Equal number of cations and anions are missing from lattice sites. | An ion leaves its site and occupies an interstitial site. |
| Decreases the density of the crystal. | Density of the crystal remains unchanged. |
| Occurs when sizes of cation and anion are almost similar. | Occurs when there is a large difference in size between ions. |
| Found in high coordination number crystals. | Found in low coordination number crystals. |
31. Name a compound that exhibits both Schottky and Frenkel defects.
Silver Bromide ($AgBr$) exhibits both Schottky and Frenkel defects.
32. What are F-centers? How do they affect the properties of a crystal?
F-centers (Farbenzemtrum or Color Centers): In a metal excess defect caused by anion vacancies, an electron is trapped in the vacant anion lattice site to maintain electrical neutrality. This electron-occupied site is called an F-center.
Effect: They impart color to the crystal by absorbing visible light to excite the unpaired electron. For example, excess Sodium makes $NaCl$ yellow, excess Potassium makes $KCl$ violet/lilac. They also make the crystal paramagnetic and slightly electrically conductive.
33. Explain why ZnO turns yellow on heating.
Zinc oxide ($ZnO$) is white at room temperature. On heating, it loses oxygen gas and leaves behind $Zn^{2+}$ ions and electrons:
$$ ZnO \xrightarrow{\text{heat}} Zn^{2+} + \frac{1}{2}O_2 + 2e^- $$
The $Zn^{2+}$ ions move to interstitial sites, and the electrons move to neighboring interstitial sites. This creates a metal excess defect. The trapped electrons absorb radiation in the visible region, making the crystal appear yellow.
34. What is a metal deficiency defect? Give an example.
This defect occurs when the metal shows variable valency. A metal cation is missing from its lattice site, and to maintain electrical neutrality, an adjacent metal ion acquires a higher positive charge.
Example: In Ferrous oxide ($FeO$), some $Fe^{2+}$ ions are missing. To balance the charge, two other $Fe^{2+}$ ions become $Fe^{3+}$ ions. As a result, its actual formula ranges from $Fe_{0.93}O$ to $Fe_{0.96}O$.
35. Explain impurity defect with the example of $NaCl$ doped with $SrCl_2$.
When molten $NaCl$ containing a little amount of $SrCl_2$ is crystallized, some of the sites of $Na^+$ ions are occupied by $Sr^{2+}$ ions. Each $Sr^{2+}$ ion replaces two $Na^+$ ions (to maintain electrical neutrality). It occupies the site of one $Na^+$ ion, leaving the other site vacant. Hence, the number of cation vacancies produced is equal to the number of $Sr^{2+}$ ions added.
36. Explain Band Theory for classifying solids as conductors, insulators, and semiconductors.
Band theory describes the energy levels in a solid as continuous bands: the Valence Band (VB, highest occupied band) and the Conduction Band (CB, lowest unoccupied band). The energy gap between them is the Forbidden Energy Gap ($E_g$).
- Conductors: The VB and CB overlap, or the VB is partially filled. Electrons move freely, hence excellent conductivity ($E_g = 0$).
- Insulators: Large energy gap ($E_g > 3$ eV) between full VB and empty CB. Electrons cannot cross, so they do not conduct.
- Semiconductors: Small energy gap ($E_g < 3$ eV). At absolute zero, they are insulators. At room temperature, some electrons gain enough thermal energy to jump from VB to CB, causing slight conductivity.
37. What is doping? Why is it done?
Doping: The process of intentionally adding an appropriate amount of a suitable impurity to a pure intrinsic semiconductor to increase its electrical conductivity is called doping.
Reason: Intrinsic semiconductors (like pure Si or Ge) have very low conductivity at room temperature, making them useless for practical electronic devices. Doping creates extrinsic semiconductors with highly tunable and increased conductivity.
38. Explain n-type semiconductors.
When a Group 14 element (like Si or Ge, which has 4 valence electrons) is doped with a Group 15 element (like P, As, Sb, which has 5 valence electrons), four out of five electrons form covalent bonds with the host lattice. The fifth extra electron becomes delocalized and serves to conduct electricity. Because conductivity is due to negative charge carriers (electrons), it is called an n-type (negative type) semiconductor.
39. Explain p-type semiconductors.
When a Group 14 element (like Si or Ge) is doped with a Group 13 element (like B, Al, Ga, which has 3 valence electrons), the dopant can only form three covalent bonds. This creates a missing electron in the fourth bond, leaving a 'hole' (electron vacancy). These holes act as positive charge carriers that move through the lattice. Hence, it is called a p-type (positive type) semiconductor.
40. What is Paramagnetism? Give examples.
Paramagnetism: Substances that are weakly attracted by a magnetic field are called paramagnetic substances. This occurs when atoms/ions/molecules contain one or more unpaired electrons. They are magnetized in a magnetic field in the same direction, but lose their magnetism in the absence of the magnetic field.
Examples: $O_2, Cu^{2+}, Fe^{3+}, Cr^{3+}$.
41. What is Diamagnetism? Give examples.
Diamagnetism: Substances that are weakly repelled by a magnetic field are called diamagnetic substances. This occurs when all electrons in the substance are paired. The pairing cancels out their magnetic moments.
Examples: $H_2O, NaCl$, Benzene ($C_6H_6$), $N_2$.
42. What is Ferromagnetism? Give examples.
Ferromagnetism: Substances that are very strongly attracted by a magnetic field and can be permanently magnetized are called ferromagnetic substances. In solid state, the metal ions of these substances are grouped together into small regions called "domains". Each domain acts as a tiny magnet. In an unmagnetized piece, domains are randomly oriented. When placed in a magnetic field, all domains align in the direction of the field permanently.
Examples: Iron ($Fe$), Cobalt ($Co$), Nickel ($Ni$), Gadolinium ($Gd$), $CrO_2$.
43. Define Anti-ferromagnetism. Give an example.
Anti-ferromagnetism: Substances like $MnO$ have domain structures similar to ferromagnetic substances, but their domains are oppositely oriented in exactly equal numbers. The opposite magnetic moments perfectly cancel each other out, resulting in a zero net magnetic moment.
Example: Manganese oxide ($MnO$).
44. Define Ferrimagnetism. Give an example.
Ferrimagnetism: This is observed when the magnetic moments of the domains in the substance are aligned in parallel and anti-parallel directions in unequal numbers. They have a small net magnetic moment and are weakly attracted to a magnetic field compared to ferromagnetic substances. They lose ferrimagnetism on heating and become paramagnetic.
Example: Magnetite ($Fe_3O_4$), Ferrites like $MgFe_2O_4$.
45. What is Curie Temperature?
Curie Temperature ($T_c$): It is the specific temperature above which a ferromagnetic substance loses its ferromagnetism and becomes paramagnetic due to the randomization of its domains by thermal agitation.
46. Copper crystallizes in fcc with a unit cell length of 361 pm. What is the radius of the copper atom?
For an FCC lattice, the relationship between edge length ($a$) and radius ($r$) is:
$a = 2\sqrt{2}r \Rightarrow r = \frac{a}{2\sqrt{2}}$
Given $a = 361$ pm.
$r = \frac{361}{2 \times 1.414} = \frac{361}{2.828} \approx 127.6 \text{ pm}$.
The radius of the copper atom is approximately 127.6 pm.
47. Why are ionic solids hard and brittle?
Ionic solids are hard because they consist of positive and negative ions held together by strong electrostatic (coulombic) forces of attraction arranged in a fixed 3D lattice. High energy is needed to break these bonds.
They are brittle because when a shearing force is applied, layers of ions slide over one another. This brings ions of the same charge close together, causing strong repulsion which shatters the crystal.
48. What makes diamond a good thermal conductor but an electrical insulator?
In diamond, each carbon atom is covalently bonded to four other carbon atoms in a rigid tetrahedral network.
It is an electrical insulator because there are no free or delocalized electrons available to carry a charge; all valence electrons are tied up in strong $C-C$ bonds.
It is a good thermal conductor because its rigid, continuous covalent network rapidly transfers thermal vibrations (phonons) throughout the crystal without scattering.
49. How do we determine the number of atoms in an unknown cubic unit cell from its density?
Using the density formula: $\rho = \frac{Z \cdot M}{a^3 \cdot N_A}$
We can rearrange it to find $Z$ (number of atoms per unit cell):
$$ Z = \frac{\rho \cdot a^3 \cdot N_A}{M} $$
By measuring the density ($\rho$), molar mass ($M$), and finding edge length ($a$) using X-ray diffraction, we compute $Z$. If $Z \approx 1$, it's Simple Cubic; if $Z \approx 2$, it's BCC; if $Z \approx 4$, it's FCC.
50. Explain the effect of temperature on the conductivity of a semiconductor.
At absolute zero, semiconductors behave as perfect insulators because the valence band is completely full and the conduction band is completely empty. The thermal energy is too low to cross the energy gap.
As the temperature increases, electrons in the valence band gain enough thermal energy to jump across the small energy gap ($E_g$) into the conduction band. This creates free electrons in the conduction band and holes in the valence band, increasing the electrical conductivity exponentially with temperature.
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