Victor,
The reason that highly hydrated ions are weakly retained in ion exchange is a direct consequence of the hydrated ionic radius. For monoatomic ions such as simple halogen anions, alkali metal cations or alkaline earth cations there is a simple relationship between position in the periodic table and hydrated ionic radius. Ionic radius increases as one proceeds to higher atomic weight ions in the same column. Hydrated ionic radius follows the inverse trend. Thus, in the case of halogen anions, fluoride has the smallest ionic radius and the largest hydrated ionic radius. Since, to a first approximation, the forces involved in ion exchange retention are directly related to the distance between a given ion exchange site and a given counterion (with the force being greatest when opposite charges are the smallest distance apart) one can predict elution order based on hydrated ionic radius. In the case of the simple halogen anions, the prediction is for fluoride, the anion with the largest hydrated ionic radius to elute first and astatide, the anion with the smallest hydrated ionic radius to elute last (not that I ever had access to this anion to determine its retention time). Likewise, in the case of alkali metal cations there is a similar relationship with the prediction being: lithium, the cation with the largest hydrated ionic radius eluting first and francium, the cation with the smallest hydrated ionic radius eluting last.
Extending this relationship beyond simple monoatomic anions and cations is more difficult, though. Unfortunately, there is no readily available resource with accurate tabulated data for the hydrated ionic radius of polyatomic ions. For this reason, hydrated ionic radius information cannot be used in general to predict selectivity. In addition, cross-linked ion exchange materials add a new dimension to the selectivity equation, further complicating matters. The selectivity of a given material can be varied significantly depending upon cross-link because cross-linked phases must expand to accommodate larger ions. The opposing forces of the stationary phase cross-link impair the ability of highly hydrated ions to enter the matrix. Hydrated ionic radius is more closely correlated to entropy of hydration whereas enthalpy of hydration is a better indicator of the ease with which in ion can shed its waters of hydration in order to enter a cross-linked matrix. By changing the cross-link one can shift the relative importance of entropy and enthalpy of hydration. For that reason, elution order can be varied by changing the cross-link of the stationary phase to favor specific ions. For example, it requires a relatively large amount of energy for fluoride with its extremely large hydrated radius to shed a significant fraction of its waters of hydration in order to enter a highly cross-linked matrix. For that reason, fluoride is nearly unretained in highly cross-linked materials but exhibits significantly more retention relative to chloride as the cross-link approaches zero.