💡

Board Exam Tips

  • →Learn the three radius–edge relations (sc: a = 2r, bcc: √3a = 4r, fcc: √2a = 4r) from the geometry of the cube — every packing-efficiency derivation and most numericals depend on them.
  • →A common long-answer question is the derivation of packing efficiency for sc, bcc or fcc. Write z, the r–a relation, the volume of spheres and the volume of the cell as separate steps.
  • →In density numericals convert the edge length to cm first (1 pm = 10⁻¹⁰ cm) so that ρ comes out in g cm⁻³.
  • →To identify the type of cubic lattice, compute z = ρa³N_A/M and round to 1 (sc), 2 (bcc) or 4 (fcc).
  • →For the formula of a compound from voids, remember N close-packed spheres give N octahedral and 2N tetrahedral voids.
  • →When comparing Schottky and Frenkel defects, state which ions are missing or displaced, give an example of each, and give the effect on density.

📐 Formulas(13)

✏️ Solved Examples

1Solved Exampleeasy3 steps

Atoms of element Q form a ccp lattice and atoms of element P occupy one-third of the tetrahedral voids. Find the formula of the compound.

1

Let the number of Q atoms be N. A ccp lattice of N atoms has 2N tetrahedral voids.

2Solved Exampleboard3 steps

Copper crystallises in an fcc lattice with edge length 361 pm. Calculate the density of copper. (Cu = 63.5 g mol⁻¹, N_A = 6.022 × 10²³ mol⁻¹)

1

For fcc, z = 4. Convert the edge length to cm and find the cell volume.

3Solved Exampleboard3 steps

Iron has a bcc unit cell and density 7.87 g cm⁻³. Calculate the edge length of the unit cell and the atomic radius of iron. (Fe = 55.85 g mol⁻¹, N_A = 6.022 × 10²³ mol⁻¹)

1

For bcc, z = 2. Rearrange the density formula for a³.

4Solved ExampleHOTS3 steps

A metal (molar mass 27 g mol⁻¹) crystallises in a cubic lattice with edge length 405 pm. Its density is 2.70 g cm⁻³. Identify the type of unit cell and find the atomic radius. (N_A = 6.022 × 10²³ mol⁻¹)

1

Find the cell volume in cm³.

⚠️ Traps & Common Mistakes

⚠️Common Mistakes5
  • 1

    Counting every corner atom of a cube as a whole atom (z = 8 for simple cubic).

    ✓Each corner atom is shared by 8 cells and contributes 1/8. Simple cubic z = 1, bcc z = 2, fcc z = 4.

  • 2

    Using a = 2r for bcc and fcc lattices.

    ✓a = 2r only for simple cubic. In bcc atoms touch along the body diagonal (√3a = 4r); in fcc along the face diagonal (√2a = 4r).

  • 3

    Putting the edge length in pm into ρ = zM/(a³N_A) and expecting g cm⁻³.

    ✓Convert first: 1 pm = 10⁻¹⁰ cm, so a³ in pm³ must be multiplied by 10⁻³⁰ to get cm³.

  • 4

    Taking the number of tetrahedral voids equal to the number of spheres.

    ✓N close-packed spheres give 2N tetrahedral voids and N octahedral voids.

  • 5

    Saying that a Frenkel defect lowers the density.

    ✓In a Frenkel defect ions only shift to interstitial sites, so mass and volume are unchanged. Only the Schottky defect (ions missing) lowers density.

🎯 Practice Yourself

🎯Practice Yourself6 questions
  1. Q1

    Silver crystallises in an fcc lattice with edge length 408 pm. Calculate the atomic radius of silver.

  2. Q2

    What percentage of the volume of a bcc unit cell is empty space?

  3. Q3

    Polonium crystallises in a simple cubic lattice with edge length 335 pm. Calculate its density. (Po = 209 g mol⁻¹, N_A = 6.022 × 10²³ mol⁻¹)

  4. Q4

    Nickel has an fcc lattice with edge length 352 pm and density 8.9 g cm⁻³. How many unit cells and how many atoms are present in 10 g of nickel?

  5. Q5

    Anions B form a ccp lattice and cations A occupy half of the octahedral voids. What is the formula of the compound?

  6. Q6

    NaCl is doped with 10⁻³ mol % SrCl₂. Each Sr²⁺ ion replaces two Na⁺ ions and creates one cation vacancy. Find the number of cation vacancies per mole of NaCl.

📝 Notes

Solid State — Maharashtra HSC Overview

Chapter 1 of the Maharashtra State Board Std XII Chemistry textbook moves from the types of solids to cubic unit cells, packing, density and defects. Almost every numerical in the chapter uses just three ideas: the number of atoms per unit cell zz, the radius–edge relation, and the density equation.

One cube, three lattices

Start every problem by writing zz and the r–a relation for the lattice:

  • Simple cubic: z=1z = 1, a=2ra = 2r, coordination number 6, packing 52.36%.
  • Body-centred cubic: z=2z = 2, 3a=4r\sqrt{3}a = 4r, coordination number 8, packing 68%.
  • Face-centred cubic (ccp): z=4z = 4, 2a=4r\sqrt{2}a = 4r, coordination number 12, packing 74%.

The packing-efficiency derivation is the same in all three cases: volume of zz spheres divided by a3a^3, after replacing aa with its value in terms of rr.

Density numericals

ρ=zM/(a3NA)\rho = zM/(a^3N_A) links five quantities. A question gives four and asks for the fifth. If it asks for the type of lattice, solve for zz and round to 1, 2 or 4. Keep the edge length in cm: a slip in the power of ten is a common source of a wrong answer.

Voids and formulas

In ccp or hcp, NN spheres create NN octahedral and 2N2N tetrahedral voids. Multiply the number of voids by the fraction occupied, compare with NN, and reduce to the simplest whole-number ratio.

Defects

Stoichiometric defects keep the formula unchanged: vacancy, interstitial, Schottky and Frenkel. Non-stoichiometric defects (metal deficiency, metal excess with F-centres) change the cation–anion ratio. Impurity defects such as SrCl₂ in NaCl create cation vacancies, one for each Sr²⁺ ion.

🔗 Related chapters

📖 Related study tips

Deep-dive articles to complement this chapter