Given:
The magnetic moment (\( \mu \)) for a transition metal ion is given by the spin-only formula: \[ \mu = \sqrt{n(n+2)} \, \text{BM} \] where \( n \) is the number of unpaired electrons.
We need to determine the electronic configuration for each ion and find the number of unpaired electrons.
Nickel (Ni) has an atomic number of 28, and its electronic configuration is: \[ \text{Ni:} \, [Ar] \, 3d^8 4s^2 \] When Ni forms a \( 2+ \) ion, it loses two electrons, typically from the 4s orbital. So, the electronic configuration for Ni\(^{2+}\) is: \[ \text{Ni}^{2+}: \, [Ar] \, 3d^8 \] This leaves 2 unpaired electrons in the \( 3d \) orbitals. \[ n = 2 \] Therefore, the magnetic moment is: \[ \mu = \sqrt{2(2+2)} = \sqrt{8} = 2.83 \, \text{BM} \] Since this is less than 3 BM, Ni\(^{2+}\) satisfies the condition.
Iron (Fe) has an atomic number of 26, and its electronic configuration is: \[ \text{Fe:} \, [Ar] \, 3d^6 4s^2 \] When Fe forms a \( 2+ \) ion, it loses two electrons, typically from the 4s orbital. So, the electronic configuration for Fe\(^{2+}\) is: \[ \text{Fe}^{2+}: \, [Ar] \, 3d^6 \] This leaves 4 unpaired electrons in the \( 3d \) orbitals. \[ n = 4 \] Therefore, the magnetic moment is: \[ \mu = \sqrt{4(4+2)} = \sqrt{24} = 4.90 \, \text{BM} \] This is greater than 3 BM, so Fe\(^{2+}\) does not satisfy the condition.
Cobalt (Co) has an atomic number of 27, and its electronic configuration is: \[ \text{Co:} \, [Ar] \, 3d^7 4s^2 \] When Co forms a \( 2+ \) ion, it loses two electrons, typically from the 4s orbital. So, the electronic configuration for Co\(^{2+}\) is: \[ \text{Co}^{2+}: \, [Ar] \, 3d^7 \] This leaves 3 unpaired electrons in the \( 3d \) orbitals. \[ n = 3 \] Therefore, the magnetic moment is: \[ \mu = \sqrt{3(3+2)} = \sqrt{15} = 3.87 \, \text{BM} \] This is greater than 3 BM, so Co\(^{2+}\) does not satisfy the condition.
Vanadium (V) has an atomic number of 23, and its electronic configuration is: \[ \text{V:} \, [Ar] \, 3d^3 4s^2 \] When V forms a \( 3+ \) ion, it loses three electrons, typically from the 4s and \( 3d \) orbitals. So, the electronic configuration for V\(^{3+}\) is: \[ \text{V}^{3+}: \, [Ar] \, 3d^2 \] This leaves 2 unpaired electrons in the \( 3d \) orbitals. \[ n = 2 \] Therefore, the magnetic moment is: \[ \mu = \sqrt{2(2+2)} = \sqrt{8} = 2.83 \, \text{BM} \] Since this is less than 3 BM, V\(^{3+}\) satisfies the condition.
Titanium (Ti) has an atomic number of 22, and its electronic configuration is: \[ \text{Ti:} \, [Ar] \, 3d^2 4s^2 \] When Ti forms a \( 2+ \) ion, it loses two electrons, typically from the 4s orbital. So, the electronic configuration for Ti\(^{2+}\) is: \[ \text{Ti}^{2+}: \, [Ar] \, 3d^2 \] This leaves 2 unpaired electrons in the \( 3d \) orbitals. \[ n = 2 \] Therefore, the magnetic moment is: \[ \mu = \sqrt{2(2+2)} = \sqrt{8} = 2.83 \, \text{BM} \] Since this is less than 3 BM, Ti\(^{2+}\) satisfies the condition.
From the calculations above, the species with a magnetic moment less than 3 BM are: \[ \text{Ni}^{2+}, \text{V}^{3+}, \text{Ti}^{2+} \] Thus, there are 3 species with magnetic moments less than 3 BM.
The number of species with a magnetic moment (spin-only) less than 3 BM is \( \boxed{3} \).