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[PdFClBrI]^(2-) Number of Geometrical Is...

`[PdFClBrI]^(2-)` Number of Geometrical Isomers = n. For `[Fe(CN)_6]^(n-6)`, Determine the spin only magnetic moment and CFSE (Ignore the pairing energy)

A

`1.73 B.M., -2delta_0`

B

`2.84 B.M., -1.6delta_0`

C

`0, -1.6delta_0`

D

`5.92 B.M., -2.4 delta_0`

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To solve the problem step by step, we will break it down into two parts: determining the number of geometrical isomers for the complex \([PdFClBrI]^{2-}\) and then calculating the spin-only magnetic moment and CFSE for the complex \([Fe(CN)_6]^{n-6}\). ### Step 1: Determine the number of geometrical isomers for \([PdFClBrI]^{2-}\) 1. **Identify the coordination number and geometry**: - Palladium (Pd) typically forms square planar complexes when it is in the +2 oxidation state. - The complex has four different ligands: F, Cl, Br, and I. 2. **Apply the formula for geometrical isomers**: - For a square planar complex with four different ligands, the number of geometrical isomers can be determined using the formula: \[ \text{Number of geometrical isomers} = \frac{n!}{(n-2)! \cdot 2!} \] - Here, \(n\) is the number of different ligands (4 in this case). - Thus, the number of geometrical isomers is: \[ \frac{4!}{(4-2)! \cdot 2!} = \frac{24}{2 \cdot 2} = 6 \] - However, we need to consider the symmetry of the ligands. After analyzing the possible arrangements, we find that there are actually 3 unique geometrical isomers. 3. **Conclusion**: - The number of geometrical isomers \(n\) for \([PdFClBrI]^{2-}\) is 3. ### Step 2: Calculate the spin-only magnetic moment and CFSE for \([Fe(CN)_6]^{n-6}\) 1. **Determine the oxidation state of iron**: - Given that \(n = 3\), we can substitute this into the complex: \[ [Fe(CN)_6]^{3-6} = [Fe(CN)_6]^{-3} \] - The charge of the complex is -3. Since CN is a strong field ligand with a charge of -1, the total contribution from the ligands is -6. Therefore, the oxidation state of iron is: \[ x + (-6) = -3 \implies x = +3 \] - Thus, iron is in the +3 oxidation state. 2. **Determine the electronic configuration of \(Fe^{3+}\)**: - The electronic configuration of neutral iron (Fe) is \([Ar] 3d^6 4s^2\). - For \(Fe^{3+}\), we remove three electrons (two from 4s and one from 3d): \[ Fe^{3+} = [Ar] 3d^5 \] 3. **Determine the number of unpaired electrons**: - In an octahedral field created by the six CN ligands, the \(3d\) orbitals split into \(t_{2g}\) and \(e_g\) levels. - Since CN is a strong field ligand, it causes pairing of electrons in the \(t_{2g}\) orbitals. - The \(3d^5\) configuration will fill the \(t_{2g}\) orbitals first: - All five electrons will occupy the \(t_{2g}\) orbitals, resulting in 5 unpaired electrons. 4. **Calculate the spin-only magnetic moment**: - The formula for the spin-only magnetic moment (\(\mu\)) is: \[ \mu = \sqrt{n(n+2)} \text{ Bohr magneton} \] - Where \(n\) is the number of unpaired electrons (5 in this case): \[ \mu = \sqrt{5(5+2)} = \sqrt{35} \approx 5.92 \text{ Bohr magneton} \] 5. **Calculate the CFSE (Crystal Field Stabilization Energy)**: - The CFSE can be calculated using the formula: \[ \text{CFSE} = (n_{t_{2g}} \times -0.4 \Delta_o) + (n_{e_g} \times 0.6 \Delta_o) \] - For \(Fe^{3+}\) in \([Fe(CN)_6]^{-3}\): - \(n_{t_{2g}} = 5\) and \(n_{e_g} = 0\): \[ \text{CFSE} = (5 \times -0.4 \Delta_o) + (0 \times 0.6 \Delta_o) = -2.0 \Delta_o \] ### Final Results: - The spin-only magnetic moment is approximately \(5.92 \text{ Bohr magneton}\). - The CFSE is \(-2.0 \Delta_o\).

To solve the problem step by step, we will break it down into two parts: determining the number of geometrical isomers for the complex \([PdFClBrI]^{2-}\) and then calculating the spin-only magnetic moment and CFSE for the complex \([Fe(CN)_6]^{n-6}\). ### Step 1: Determine the number of geometrical isomers for \([PdFClBrI]^{2-}\) 1. **Identify the coordination number and geometry**: - Palladium (Pd) typically forms square planar complexes when it is in the +2 oxidation state. - The complex has four different ligands: F, Cl, Br, and I. ...
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