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In an atomic bcc lattie what fraction of...

In an atomic bcc lattie what fraction of edge is not covered by atoms?

A

0.32

B

0.16

C

0.134

D

0.268

Text Solution

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The correct Answer is:
To find the fraction of the edge that is not covered by atoms in a body-centered cubic (BCC) lattice, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the BCC Structure**: - In a BCC lattice, atoms are located at the eight corners of the cube and one atom is located at the center of the cube. 2. **Identifying the Edge Length**: - Let the edge length of the unit cell be denoted as \( a \). 3. **Identifying the Radius of the Atoms**: - Let the radius of the atoms be denoted as \( r \). 4. **Calculating the Covered Length on the Edge**: - On an edge of the BCC unit cell, two corner atoms are present. Each corner atom contributes a radius \( r \) to the edge length. - Therefore, the total length covered by the two corner atoms on one edge is \( 2r \). 5. **Calculating the Uncovered Length**: - The length of the edge that is not covered by atoms can be calculated as: \[ \text{Uncovered Length} = a - 2r \] 6. **Finding the Relationship Between \( r \) and \( a \)**: - To find the relationship between the radius \( r \) and the edge length \( a \), we can use the body diagonal of the cube. - The body diagonal of the cube can be expressed as: \[ \text{Body Diagonal} = \sqrt{3}a \] - This body diagonal consists of one atom at each corner and one atom at the center, which gives: \[ \text{Body Diagonal} = 4r \] - Therefore, we can set up the equation: \[ 4r = \sqrt{3}a \] - From this, we can express \( r \) in terms of \( a \): \[ r = \frac{\sqrt{3}}{4}a \] 7. **Substituting \( r \) Back into the Uncovered Length**: - Substitute \( r \) into the uncovered length equation: \[ \text{Uncovered Length} = a - 2\left(\frac{\sqrt{3}}{4}a\right) = a - \frac{\sqrt{3}}{2}a = a\left(1 - \frac{\sqrt{3}}{2}\right) \] 8. **Calculating the Fraction of the Edge Not Covered**: - The fraction of the edge that is not covered by atoms is given by: \[ \text{Fraction Not Covered} = \frac{\text{Uncovered Length}}{a} = 1 - \frac{\sqrt{3}}{2} \] - Evaluating this gives: \[ \text{Fraction Not Covered} \approx 1 - 0.866 \approx 0.134 \] 9. **Final Result**: - Therefore, the fraction of the edge that is not covered by atoms in a BCC lattice is approximately \( 0.134 \).
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