To find the spin-only magnetic moment of the \( \text{B}_2 \) molecule, we begin by understanding its molecular orbital (MO) electron configuration. Boron has an atomic number of 5, and therefore \( \text{B}_2 \) will have 10 electrons.
Molecular Orbital Theory tells us that the electrons will fill the molecular orbitals as follows:
The \( \pi_{2p} \) orbitals are of primary interest, possessing two electrons with parallel spins due to Hund's rule.
The spin-only magnetic moment \( \mu \) is given by:
\[ \mu = \sqrt{n(n+2)} \, \mu_B \]
Where \( n \) is the number of unpaired electrons.
Here, the number of unpaired electrons \( n = 2 \) (since the \( \pi_{2p} \) orbitals each contain one unpaired electron).
Substitute \( n = 2 \) into the formula:
\[ \mu = \sqrt{2(2+2)} \, \mu_B = \sqrt{8} \, \mu_B = 2.828 \, \mu_B \]
Upon rounding, \( \mu \approx 2.83 \, \mu_B \).
The calculated value of \( 2.83 \, \mu_B \) falls within the given range of \( 2.82 \, \mu_B \) to \( 2.83 \, \mu_B \), confirming the correctness of our solution.