Atoms touch along the edges.
\[ 2r = a \]
Therefore, radius for SC:
\[ r = \frac{a}{2} \]
Atoms touch along the body diagonal of the cube.
\[ 4r = \sqrt{3}a \]
Therefore, radius for BCC:
\[ r = \frac{\sqrt{3}a}{4} \]
Atoms touch along the face diagonal.
\[ 4r = \sqrt{2}a \]
Therefore, radius for FCC:
\[ r = \frac{\sqrt{2}a}{4} = \frac{a}{2\sqrt{2}} \]
Simple cubic : Body-centered cubic : Face-centered cubic
\[ \frac{a}{2} : \frac{\sqrt{3}a}{4} : \frac{a}{2\sqrt{2}} \]
The correct ratio is:
\( \frac{1}{2}a : \frac{\sqrt{3}}{4}a : \frac{1}{2\sqrt{2}}a \)
Correct Answer: Option (B)
The edge length 'a' refers to the edge length of the unit cell. The relationship between the radii in different cubic structures can be derived as follows:
1. Simple cubic (SC): In a simple cubic unit cell, the atoms are located at the corners. The radius of the atom \( r \) is half the edge length of the unit cell. Therefore, \( r_{\text{SC}} = \frac{a}{2} \).
2. Body-centered cubic (BCC): In a body-centered cubic unit cell, the atoms are at the corners and at the center of the cell. The diagonal of the cube passes through the center, and it is equal to \( 4r \). From geometry, the diagonal is \( \sqrt{3}a \), so: \[ \sqrt{3}a = 4r_{\text{BCC}} \quad \Rightarrow \quad r_{\text{BCC}} = \frac{\sqrt{3}}{4}a \]
3. Face-centered cubic (FCC): In a face-centered cubic unit cell, the atoms are at the corners and the centers of the faces. The diagonal across the face is equal to \( 4r \). The face diagonal is \( \sqrt{2}a \), so: \[ \sqrt{2}a = 4r_{\text{FCC}} \quad \Rightarrow \quad r_{\text{FCC}} = \frac{\sqrt{2}}{4}a \]
Thus, the ratio of the radii in simple cubic, body-centered cubic, and face-centered cubic unit cells is: \[ r_{\text{SC}} : r_{\text{BCC}} : r_{\text{FCC}} = \frac{a}{2} : \frac{\sqrt{3}}{4}a : \frac{\sqrt{2}}{4}a \]
The correct answer is option (B).
The graph between variation of resistance of a wire as a function of its diameter keeping other parameters like length and temperature constant is
While determining the coefficient of viscosity of the given liquid, a spherical steel ball sinks by a distance \( x = 0.8 \, \text{m} \). The radius of the ball is \( 2.5 \times 10^{-3} \, \text{m} \). The time taken by the ball to sink in three trials are tabulated as shown: