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A metal crystallises as body centred cub...

A metal crystallises as body centred cubic lattice with the edge length of unit cell equal to 0.304 nm. If the molar mass of the metal is 50.3 g` mol^(−1)` , its density (in g `cm^(−3)` ) is :

A

5.945

B

2.9725

C

8.915

D

4.458

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The correct Answer is:
To calculate the density of the metal that crystallizes in a body-centered cubic (BCC) lattice, we can use the formula for density: \[ \text{Density} (d) = \frac{Z \cdot M}{a^3 \cdot N_A} \] Where: - \( Z \) = number of atoms per unit cell (for BCC, \( Z = 2 \)) - \( M \) = molar mass of the metal (given as 50.3 g/mol) - \( a \) = edge length of the unit cell (given as 0.304 nm) - \( N_A \) = Avogadro's number (\( 6.02 \times 10^{23} \) mol\(^{-1}\)) ### Step-by-Step Solution: **Step 1: Convert the edge length from nanometers to centimeters.** - Given edge length \( a = 0.304 \) nm. - To convert to centimeters: \[ a = 0.304 \, \text{nm} = 0.304 \times 10^{-7} \, \text{cm} \] **Step 2: Calculate \( a^3 \).** - Now calculate \( a^3 \): \[ a^3 = (0.304 \times 10^{-7})^3 = 0.304^3 \times 10^{-21} \, \text{cm}^3 \] Calculating \( 0.304^3 \): \[ 0.304^3 \approx 0.0283 \] Thus, \[ a^3 \approx 0.0283 \times 10^{-21} \, \text{cm}^3 \] **Step 3: Substitute values into the density formula.** - Now substitute \( Z = 2 \), \( M = 50.3 \, \text{g/mol} \), \( a^3 \approx 0.0283 \times 10^{-21} \, \text{cm}^3 \), and \( N_A = 6.02 \times 10^{23} \): \[ d = \frac{2 \cdot 50.3}{0.0283 \times 10^{-21} \cdot 6.02 \times 10^{23}} \] **Step 4: Calculate the denominator.** - Calculate \( a^3 \cdot N_A \): \[ 0.0283 \times 10^{-21} \cdot 6.02 \times 10^{23} \approx 0.1704 \, \text{cm}^3 \] **Step 5: Calculate the density.** - Now calculate the density: \[ d = \frac{2 \cdot 50.3}{0.1704} \approx \frac{100.6}{0.1704} \approx 5.91 \, \text{g/cm}^3 \] ### Final Result: The density of the metal is approximately \( 5.91 \, \text{g/cm}^3 \).
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