Animated Solution for Chemistry - Chemical Bonding and Molecular Structure: The spin-only magnetic moment value of B2+ species is ......... ×10−2 BM. (Nearest integer) [Given, 3=1.73]
Imagine you are shrinking down to the subatomic level, staring at a B2+ ion. Our mission today is to uncover its spin-only magnetic moment.
This isn't just a random calculation; it is a beautiful demonstration of how the invisible quantum world dictates the physical properties we can measure in a lab.
The Master Equation
To unlock this puzzle, we need our trusty mathematical tool. The spin-only magnetic moment, denoted by μ, is given by the formula:
μ=n(n+2) BM
Here, n represents the number of unpaired electrons, and BM stands for Bohr Magnetons, the standard unit for magnetic moment.
Our entire goal now boils down to finding the exact value of n. To do that, we must build the molecular orbital structure of the ion.
Decoding the Electron Count
Before we can place electrons into orbitals, we need to know how many we have.
A neutral boron atom (atomic number 5) has 5 electrons. Since we have a diatomic molecule, B2, that gives us 5+5=10 electrons.
But wait! We are dealing with the B2+ cation. The positive charge means it has lost one electron.
Total electrons=10−1=9
Building the Molecular Orbitals
Now comes the fun part: Molecular Orbital (MO) Theory.
For lighter elements like boron, carbon, and nitrogen, a phenomenon called s-p mixing occurs. This alters the standard energy order of the molecular orbitals, pushing the σ2pz orbital higher in energy than the degenerate π2px and π2py orbitals.
Let's distribute our 9 electrons. The first 4 electrons fill the inner core orbitals:
\sigma_{1s}^2, \sigma^*_{1s}^2
This leaves us with 9−4=5 valence electrons to play with.
Moving up the energy ladder, we fill the 2s bonding and anti-bonding orbitals:
\sigma_{2s}^2, \sigma^*_{2s}^2
That accounts for 4 of our valence electrons. We have exactly 1 electron left.
Following Hund's rule and the Aufbau principle, this final, lone electron enters the next available energy level, which is the π2px orbital:
π2px1
The Final Calculation
Looking at our completed electron configuration, it is clear that there is exactly 1 unpaired electron.
n=1
Let's substitute this back into our master equation:
μ=1(1+2)
μ=3 BM
The problem kindly provides the value of 3 as 1.73.
μ=1.73 BM
However, the question asks for the answer in a specific format: x×10−2.
By shifting the decimal point two places to the right, we can rewrite our answer:
1.73=173×10−2
Therefore, our final integer value is 173.
This problem is a fantastic reminder of how a single, lonely electron in a quantum orbital can give rise to measurable magnetic properties in the macroscopic world!