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First Ionization Energy Values:
$$\mathrm{Be = 899\ kJ\ mol^{-1}}$$
$$\mathrm{B = 801\ kJ\ mol^{-1}}$$
$$\mathrm{N = 1402\ kJ\ mol^{-1}}$$
$$\mathrm{O = 1314\ kJ\ mol^{-1}}$$
Generally, ionization energy increases across a period due to increasing effective nuclear charge.
However, exceptions occur because completely filled and half-filled subshells possess extra stability.
1. Beryllium vs Boron
Electronic configurations:
$$\mathrm{Be : 1s^2\ 2s^2}$$
$$\mathrm{B : 1s^2\ 2s^2\ 2p^1}$$
Beryllium has a completely filled $$\mathrm{2s}$$ subshell, which is highly stable.
In boron, the outermost electron enters the higher-energy $$\mathrm{2p}$$ orbital.
It is easier to remove the single $$\mathrm{2p}$$ electron from boron than to disturb the stable filled $$\mathrm{2s}$$ subshell of beryllium.
Therefore:
$$\mathrm{IE(Be) > IE(B)}$$
2. Nitrogen vs Oxygen
Electronic configurations:
$$\mathrm{N : 1s^2\ 2s^2\ 2p^3}$$
$$\mathrm{O : 1s^2\ 2s^2\ 2p^4}$$
Nitrogen has an exactly half-filled $$\mathrm{2p}$$ subshell, giving extra stability due to symmetry and exchange energy.
In oxygen, one $$\mathrm{2p}$$ orbital contains paired electrons, producing inter-electronic repulsion.
Hence, it is easier to remove one electron from oxygen than to break the stable half-filled configuration of nitrogen.
Therefore:
$$\mathrm{IE(N) > IE(O)}$$
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