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Q.(a) An element crystallises in bcc lattice with a cell edge of 3×10−83 \times 10^{-8} cm. The density of the element is 6.89 g cm−36.89\ g\ cm^{-3}. Calculate the molar mass of the element. (NA=6.022×1023 mol−1N_A = 6.022 \times 10^{23}\ mol^{-1})

(b) What type of semiconductor is obtained when
(i) Ge is doped with In ?
(ii) Si is doped with P ?
CBSECBSE Class XII Board 2019Subjective· 3mImportance★★★★★est
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For a bcc lattice, the number of atoms per unit cell is 2. Using the density formula d=Z⋅Ma3⋅NAd = \frac{Z \cdot M}{a^3 \cdot N_A}, we solve for molar mass MM to get M≈56.0 g mol−1M \approx 56.0\ \text{g mol}^{-1}. For doping, Ge with In gives a p-type semiconductor, and Si with P gives an n-type semiconductor.

The key to solving part (a) is connecting the macroscopic property of density to the microscopic arrangement of atoms in the crystal lattice. Density is mass per volume. For a crystal, the mass of one unit cell is the mass of the atoms inside it, and the volume is the cube of the edge length. The number of atoms per unit cell (ZZ) depends on the lattice type — for body-centered cubic (bcc), it's 2 atoms per cell.

Let's work through it step by step.

  1. Identify the known quantities.

    Edge length, a=3×10−8 cma = 3 \times 10^{-8}\ \text{cm}

    Density, d=6.89 g cm−3d = 6.89\ \text{g cm}^{-3}

    Avogadro's number, NA=6.022×1023 mol−1N_A = 6.022 \times 10^{23}\ \text{mol}^{-1}

    For bcc lattice, number of atoms per unit cell, Z=2Z = 2

  2. Write the density formula for a crystal.

    The density dd is given by:

d=Z⋅Ma3⋅NAd = \frac{Z \cdot M}{a^3 \cdot N_A}

where MM is the molar mass in g mol−1\text{g mol}^{-1}. This formula works because Z⋅MZ \cdot M gives the mass of atoms in one unit cell (since MM is mass per mole, and NAN_A atoms make a mole), and a3a^3 is the volume of the cell.

  1. Rearrange to solve for molar mass MM. Multiply both sides by a3⋅NAa^3 \cdot N_A and divide by ZZ:

M=d⋅a3⋅NAZM = \frac{d \cdot a^3 \cdot N_A}{Z}

  1. Substitute the values. First, compute a3a^3:

a3=(3×10−8 cm)3=27×10−24 cm3=2.7×10−23 cm3a^3 = (3 \times 10^{-8}\ \text{cm})^3 = 27 \times 10^{-24}\ \text{cm}^3 = 2.7 \times 10^{-23}\ \text{cm}^3

Now plug everything in:

M=6.89×(2.7×10−23)×(6.022×1023)2M = \frac{6.89 \times (2.7 \times 10^{-23}) \times (6.022 \times 10^{23})}{2}

  1. Simplify step by step. Notice 10−23×1023=110^{-23} \times 10^{23} = 1, so the powers of ten cancel:

M=6.89×2.7×6.0222M = \frac{6.89 \times 2.7 \times 6.022}{2}

Compute the numerator: 6.89×2.7=18.6036.89 \times 2.7 = 18.603, then 18.603×6.022≈112.018.603 \times 6.022 \approx 112.0 (let's do it carefully: 18.603×6=111.61818.603 \times 6 = 111.618, 18.603×0.022=0.40926618.603 \times 0.022 = 0.409266, sum = 112.027266112.027266). So numerator ≈ 112.03112.03.

Divide by 2:

M≈56.01 g mol−1M \approx 56.01\ \text{g mol}^{-1}

As a check, a bcc metal of molar mass ≈ 56 g mol⁻¹ at this density is consistent with iron (Fe, bcc, a≈2.87×10−8a \approx 2.87 \times 10^{-8} cm, density 7.877.87 g cm⁻³, molar mass 55.8555.85 g mol⁻¹), so the result is reasonable.

Watch out

A common mistake is forgetting that bcc has Z=2Z=2, not 1. Using Z=1Z=1 would give half the molar mass, which is wrong. Also, ensure units are consistent — edge length in cm gives volume in cm³, density in g/cm³, so molar mass comes out in g/mol.

So the molar mass is approximately 56.0 g mol−156.0\ \text{g mol}^{-1}.

Now for part (b), we need to understand doping in semiconductors.

  1. Recall the principle of doping. …

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