General Characteristics of p-Block Elements
The p-block of the periodic table consists of elements belonging to Groups 13 to 18, characterized by the progressive filling of the outermost $np$ valence subshell. Their general valence electronic configuration is $ns^2 np^{1-6}$ (where $n = 2$ to $6$). Unlike the $s$-block elements, which are exclusively electropositive metals, $p$-block elements encompass metals, metalloids (semimetals), and non-metals.
A governing periodic phenomenon in the heavier $p$-block elements is the Inert Pair Effect. This refers to the reluctance of the outermost valence $s$-electrons ($ns^2$) to participate in chemical bond formation, resulting in the stabilization of an oxidation state that is two units lower than the group oxidation state.
- Origin: As we descend the group to Period 6 elements (such as Thallium $\text{Tl}$ in Group 13 and Lead $\text{Pb}$ in Group 14), electrons fill the inner $(n-1)d^{10}$ and $(n-2)f^{14}$ subshells. The $d$- and $f$-orbitals have highly diffused spatial distributions and exhibit very poor shielding efficiency against the increasing nuclear charge ($Z$).
- Relativistic Contraction: The effective nuclear charge ($Z_{\text{eff}}$) experienced by the outermost $6s^2$ electrons increases drastically. This contracts the $6s$ orbital and binds the electron pair tightly to the nucleus, requiring exceptionally high energy to unpair and promote them into bonding orbitals.
- Oxidation State Hierarchy: In Group 13, the group oxidation state is $+3$, but down the group, the stability of the $+1$ oxidation state increases: $$\text{B}^{3+} > \text{Al}^{3+} > \text{Ga}^{3+} > \text{In}^{3+} > \text{Tl}^{3+}$$ $$\text{Tl}^+ > \text{In}^+ > \text{Ga}^+ > \text{Al}^+ > \text{B}^+$$ Consequently, $\text{TlCl}$ is a thermally stable ionic solid, whereas $\text{TlCl}_3$ is unstable and acts as a powerful oxidizing agent: $\text{Tl}^{3+} + 2e^- \to \text{Tl}^+$. Conversely, for lighter elements, $\text{Al}^+$ is intensely reducing and rapidly disproportionates.
| Element | Symbol | Atomic No. | Outer Configuration | Atomic Radius (pm) | First $\text{IE}_1$ (kJ/mol) |
|---|---|---|---|---|---|
| Boron | $\text{B}$ | 5 | $[\text{He}]\, 2s^2 2p^1$ | 85 | 801 |
| Aluminum | $\text{Al}$ | 13 | $[\text{Ne}]\, 3s^2 3p^1$ | 143 | 577 |
| Gallium | $\text{Ga}$ | 31 | $[\text{Ar}]\, 3d^{10} 4s^2 4p^1$ | 135 | 579 |
| Indium | $\text{In}$ | 49 | $[\text{Kr}]\, 4d^{10} 5s^2 5p^1$ | 167 | 558 |
| Thallium | $\text{Tl}$ | 81 | $[\text{Xe}]\, 4f^{14} 5d^{10} 6s^2 6p^1$ | 170 | 589 |
Ordinarily, atomic radius increases down a periodic group due to the addition of a new principal electron shell. However, the atomic radius of Gallium ($135\text{ pm}$) is unexpectedly smaller than that of Aluminum ($143\text{ pm}$). This contraction occurs because Gallium is preceded by the ten $3d$-transition elements ($3d^{10}$). The intervening $d$-electrons exert poor screening on the valence $4s$ and $4p$ electrons, causing an elevated $Z_{\text{eff}}$ that pulls the valence electron cloud closer to the nucleus.