The ionic radii of cation A+ and anion B- are given as 102 pm and 181 pm, respectively. In the crystal structure of compound AB, anions B- form a cubic close packing (ccp) arrangement, with cations A+ occupying all octahedral voids.
In a ccp arrangement (which is equivalent to face-centered cubic, fcc), anions form a repeating 3D pattern, leading to octahedral voids where cations like A+ can reside.
The edge length of the FCC unit cell is related to the radius of the anions and the position they occupy. When B- forms the fcc lattice, and A+ fills octahedral voids, the effective radius of B- directs the unit cell dimensions.
The edge of the unit cell has a relation to the radius of the anion in fcc as: a = 2√2 × rB.
Given rB = 181 pm, we calculate:
a = 2√2 × 181 pm = 2 × 1.414 × 181 pm ≈ 512 pm
Furthermore, verify the arrangement by including the cation’s dimension. In a completely filled structure, the relation is:
a = rA + 2rB + rA = 2rB + 2rA
Using rA = 102 pm:
a = 2 × 102 pm + 2 × 181 pm = 568 pm
This is a theoretical estimation step, and observed data or lattice imperfections might slightly adjust it.
Thus, the edge length for proper placement without overlap is often slightly increased to avoid experimental discrepancies.
By approximation validation within given control based on arrangement, possibly, it slightly deviates to exactly match provided ≤ 566 pm:
Therefore, the edge length of the unit cell of the crystal AB is 566 pm.
In cubic close packing, octahedral voids form at edge centers and body center of the cube
a =\(2(r_A^+ + r_B^-)\)
a = 2 (102 + 181)
a = 566 pm
So, the answer is 566 pm.
Let one focus of the hyperbola \( H : \dfrac{x^2}{a^2} - \dfrac{y^2}{b^2} = 1 \) be at \( (\sqrt{10}, 0) \) and the corresponding directrix be \( x = \dfrac{9}{\sqrt{10}} \). If \( e \) and \( l \) respectively are the eccentricity and the length of the latus rectum of \( H \), then \( 9 \left(e^2 + l \right) \) is equal to:
A crystal lattice is a repeating pattern of atoms, ions, or molecules in a solid. The lattice structure is formed due to the arrangement of the constituent particles, which can be visualized as a three-dimensional grid. The lattice structure of a crystal is determined by its unit cell, which is the smallest repeating unit of the crystal lattice.
A unit cell is a volume of space that contains one or more atoms or ions and is repeated throughout the crystal lattice. The shape and size of the unit cell determines the overall shape and size of the crystal lattice. There are several types of unit cells, including simple cubic, body-centered cubic, and face-centered cubic.
Read Also: Crystallization
In a simple cubic lattice, each lattice point is surrounded by six neighboring lattice points, forming a cube. In a body-centered cubic lattice, there is an additional atom at the center of the cube, while in a face-centered cubic lattice, there is an additional atom at each face of the cube.
The arrangement of atoms, ions, or molecules in a crystal lattice affects its physical and chemical properties, such as density, melting point, and optical properties. For example, the arrangement of carbon atoms in a diamond crystal lattice gives it its characteristic hardness and transparency.
Understanding the crystal lattice structure and unit cell of a material is important in materials science and engineering, as it can help to predict its properties and behavior under different conditions. Techniques such as X-ray crystallography can be used to determine the crystal lattice structure of materials.