Analyzing the Setup
Imagine you are diving into the microscopic world of a crystal lattice. The problem presents us with a compound where anions (let's call them B) form a cubic close-packed (ccp) arrangement.
It is crucial to remember that a ccp lattice is geometrically identical to a face-centered cubic (fcc) unit cell. In this structure, the B atoms are positioned at all eight corners of the cube and at the centers of all six faces.
The Master Equation for Anions
To find the empirical formula, we first need to determine the effective number of B atoms per unit cell. We can't just count the atoms we see; we must account for how they are shared with neighboring unit cells.
Each corner atom is shared by eight adjacent cubes, so its contribution is 81. Each face-centered atom is shared by two cubes, contributing 21.
Let's set up the math:
So, there are exactly 4 effective B atoms in our unit cell.
Locating the Cations
Now, let's shift our focus to the cations, A. The problem states they occupy all the octahedral voids. But where exactly are these voids hiding in an fcc lattice?
Octahedral voids are located at the center of every single edge of the cube, plus one perfectly hidden right in the body center.
Final Calculation for Cations
Just like the atoms, these voids are shared. A void on an edge is shared by four unit cells, so it contributes 41. The void in the body center is entirely within our unit cell, contributing a full 1.
Let's calculate the effective number of A atoms:
We have exactly 4 effective A atoms.
The Empirical Formula
We now have the effective numbers for both ions: 4 A atoms and 4 B atoms. The ratio of A to B is 4:4.
An empirical formula must represent the simplest whole-number ratio. Simplifying 4:4 gives us 1:1.
Therefore, the empirical formula is AB.
The question tells us the formula is AxB. By comparing our result, it is beautifully clear that x=1.