The Enigma of Transition Metals
When we dive into the world of transition metals, we are greeted by a fascinating array of colors, catalytic properties, and most intriguingly, magnetism. The root of this magnetism lies deep within the atomic structure, specifically in the behavior of electrons residing in the d-orbitals. In this problem, we are tasked with finding the spin-only magnetic moment of a divalent ion with an atomic number of 29. Let's embark on this quantum journey.
Copper
The Rule Breaker
The first step is to identify our protagonist. An atomic number of Z=29 unmistakably points to Copper (Cu). If you recall your Aufbau principle, you might be tempted to write its electronic configuration as [Ar]4s23d9. However, Copper is a classic rebel.
Nature favors stability, and stability in the quantum realm is often achieved through symmetry and exchange energy. A fully filled d-subshell (3d10) is highly symmetrical and allows for maximum exchange energy between electrons of the same spin. To achieve this zen state, Copper borrows an electron from the 4s orbital, resulting in the anomalous ground state configuration:
The Art of Ionization
Who Leaves First?
The question specifically asks for a divalent ion, which means our Copper atom has lost two electrons to become Cu2+. This brings us to a critical trap where many students stumble: Which electrons are removed first?
Even though the 3d orbitals are filled after the 4s orbital, the 4s orbital is physically further from the nucleus (it belongs to the 4th principal quantum shell). When ionization occurs, the outermost electrons are always the first to be stripped away. Therefore, we remove the single 4s electron first, and then one electron from the 3d subshell.
Hund's Rule and the Lone Electron
Now that we have our 3d9 configuration, we need to visualize how these nine electrons occupy the five available d-orbitals. Enter Hund's Rule of Maximum Multiplicity.
We first place one electron in each of the five orbitals with parallel spins. That accounts for five electrons. We then begin pairing them up with the remaining four electrons. After filling four orbitals with pairs, we are left with exactly one unpaired electron in the final orbital.
Thus, the number of unpaired electrons, denoted by n, is exactly 1.
The Spin-Only Magnetic Moment
In transition metal complexes, especially those of the 3d series in aqueous solutions, the orbital contribution to the magnetic moment is largely "quenched" by the surrounding electric fields of the water ligands. This allows us to rely entirely on the spin-only magnetic moment formula:
Here, μ is the magnetic moment and BM stands for Bohr Magneton, the fundamental unit of atomic magnetism.
The Final Calculation
Substituting our value of n=1 into the master equation:
We know that the square root of 3 is approximately 1.732. The question, however, demands the answer rounded off to the nearest integer.
Since 1.732 is closer to 2 than it is to 1, we round it up.
Final Answer: 2
This problem is a beautiful symphony of exceptions in electronic configuration, the rules of ionization, and the quantum mechanics of magnetism. Always remember to watch out for those anomalous configurations!