The standard molar enthalpy of vaporization ($\Delta_{vap}H^\ominus$) is the enthalpy change required to vaporize one mole of a liquid at its standard state (usually 1 bar pressure, specified temperature - often the normal boiling point).
A higher enthalpy of vaporization indicates that more energy is required to overcome the intermolecular attractive forces in the liquid state and convert the liquid into a gas.
Therefore, a higher $\Delta_{vap}H^\ominus$ generally implies stronger intermolecular forces.
The question asks for the order of dipole-dipole attractive forces. While $\Delta_{vap}H^\ominus$ reflects the *total* strength of all types of intermolecular forces (London dispersion forces, dipole-dipole forces, hydrogen bonding), if we assume that dipole-dipole forces are a significant contributor and other factors are comparable or scale similarly, then a higher $\Delta_{vap}H^\ominus$ would suggest stronger dipole-dipole forces. This is a common simplifying assumption in such comparative questions unless other information (like molecular structure or polarity) is given.
Given $\Delta_{vap}H^\ominus$ values:
Liquid A: $23.3 \text{ kJ mol}^{-1}$
Liquid B: $41 \text{ kJ mol}^{-1}$
Liquid C: $29 \text{ kJ mol}^{-1}$
Arranging these values in decreasing order:
$41 \text{ kJ mol}^{-1}$ (B)>$29 \text{ kJ mol}^{-1}$ (C)>$23.3 \text{ kJ mol}^{-1}$ (A).
Since higher $\Delta_{vap}H^\ominus$ implies stronger intermolecular forces, the order of strength of these forces (and by inference, dipole-dipole forces if they are dominant or representative of the total) is:
B>C>A.
This matches option (a).
\[ \boxed{\text{B>C>A}} \]