Interests in solutions and suspension of macroions has been renewed in the past few years, as evidenced by the mini symposium upon which this present volume is based. Presented in this introductory chapter is a brief presentation of a selection of six topics that I believe deserves further consideration regarding these complex systems: 1) the definition of the screening parameter; 2) the mathematical form of the pairwise electrostatic energy between macroions; 3) the phenomenon of counterion condensation and its application to specific molecular geometry; 4) the use of the Gibbs versus the Helmholtz free energy in describing the thermodynamics of these charged systems; 5) the calculation of the electrostatic component to the persistence length of flexible polyions; and 6) the splitting of relaxation modes as detected by dynamic light scattering measurements.Studying polyelectrolytes is like taking a roller coaster ride. In the beginning one knows nothing about the field and therefore faces a steep upward learning curve. At some point one reaches a degree of understanding of the field and begins to publish the new results. Further investigations into the field have their ups and downs, sometimes even being thrown for a loop when unexpected results are obtained. Eventually, however, the excursion through the field of polyelectrolytes returns one to the starting point. To illustrate the above metaphor one only has to follow the history of a simple basic question: "Is the interaction between the charged macroions attractive or repulsive?"In 1938 Langmuir treated a solution of micelles in a manner similar to that of a simple salt crystal. He thus considered the counterions between the micelles as part of the interaction energy, which led to a major result (7):The interaction of these charges, just as in the sodium chloride crystal, gives an excess of attractive force and in order to have equilibrium it will be necessary not to have an additional attractive force, such as the van der Waals force postulated by Hamaker, but some new kind of repulsive force.In contrast to the conclusion of Langmuir, the currently accepted paradigm for the majority of the practitioners in the colloid field is the DLVO (Derjaguin-Landau-0097-6156/94/0548-0001$06.50/0