Continuous viscometric, detection is based on the measurement of ressure drop in an on-line small capillary tube in which cErornatogra hic eluents flow at constant flow rate. This detector is ayways coupled with a concentration detector (usually refractometer) and located before it t o avoid back presrura in the refractometer. In order to obtain reliable information f o r polymer samples, it is general1 necessary to connect these two detectors to a computer whicx performs data acquisition and treatment.First we discuss the rroblem of shape, g?ometry and dimensions of the viscometer. Tge typical charactsristlcs are the result of a comproaise between contradictory hrgets, mainly small internal vblume !ow shear rate,and low prassure drop. It is shown that $oiseullle's lammar flow is only obtained when coiling radius of the measurement tube ? s greater than 6 cm which is not the cass inside tne refractometer. Accbrdingly, tiro pressura transducers are necessary t o eliminate pressure drop data comlng from refractorneter.
LESEC, LECACHEUX, AND MAROTIn a second ,part, we show how to extract information from pressure variation data. By using conc?ntration data, pure solvent pressure and sample pressure it 1s possibl? to calculate intrinsic viscosity extrapolated to zsro concentration at,each,point of the chromato ram. By comparison rith intrinsic viscosity cf the pol mar use! for calibration, a correction of hydro& narcic v01une according : ? Benoit's universal calibration leads t o absolute aolecuiar welghts.In addition, for a linear polymor the knowled3~ of log [ q J versus log H leads to the determination of .'arkHouwin$ relationship coafficients. For branched polyaers. viscosity laws are curved aild the comparison betweer. the linear lar,corresponding to the linear equiyalent pol iiisr an$ the experimental law allows the daterminat:on ofl'the $ branching pirameter distribution.