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  • 1
    ISSN: 1573-904X
    Keywords: skin resistance and impedance ; skin appendages ; human and snake skin ; iontophoresis ; peptide delivery ; azone
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Notes: Abstract Purpose. 1. The assessment of the role of hair follicles and sweat glands in skin resistance and percutaneous iontophoretic flux of 9-desglycinamide, 8-arginine vasopressin (DGAVP) by comparing two skin species: human stratum corneum which contained hair follicles, sweat and sebaceous glands, and shed snake skin which lacked all appendages. 2. The effect of l-dodecylazacycloheptan-2-one (dodecyl-Azone, a lipid perturbing agent) on the iontophoretic DGAVP flux. Methods. Iontophoresis in vitro was performed in a transport cell (0.79 cm2 area available for percutaneous transport) by 8-hours application of a pulsed constant current of 100 Hz, 50% duty cycle and 0.26 mA.cm−2 current density delivered by a pair of Ag/AgCl electrodes, of which the anode was facing the anatomical surface of the skin samples. Results. The initial resistances of human stratum corneum and shed snake skin samples were of the same order of magnitude (20–24 kΩ.cm2) and both skin species showed a comparable resistance-decrease profile during 8-hours iontophoresis, indicating that the resistances were mainly determined by the stratum corneum and not greatly influenced by the appendageal structures. The initial resistances of the skin samples pretreated with dodecyl-azone were less than 50% of the values of untreated samples. Because dodecyl-azone is known to perturb the ordering of the intercellular lipids, the effect of azone on the resistance confirms that the resistance mainly resides within the intercellular lipids of the stratum corneum. No correlation was found between the iontophoretic DGAVP-flux and the conductance of human skin. For shed snake skin, however, a good correlation was found, indicating that the iontophoretic permeability of human skin in vitro for a peptide such as DGAVP is, unlike shed snake skin, not related to its overall permeability to ions. While the initial resistances of both human and snake skin were in the same order of magnitude and showed the same declining profile during iontophoresis, the steady state iontophoretic DGAVP flux across human stratum corneum was approximately 140 times larger than through shed snake skin. These findings suggest that small ions follow pathways common to both skin types, presumably the intercellular route, while the peptide on the other hand is transported differently: across snake skin presumably along intercellular pathways only, but across human stratum corneum along additional pathways (most likely of appendageal origin) as well. This interpretation is supported by the observations made of the effects of dodecyl-azone on DGAVP-iontophoresis. Pretreatment with dodecyl-azone did not significantly change steady state fluxes and lag times of DGAVP-iontophoresis across human stratum corneum, but resulted in a significant 3-fold lag time decrease and a 3-fold flux increase of DGAVP-iontophoresis across snake skin. Conclusions. The results of these in vitro studies emphasize the importance of the appendageal pathway for iontophoretic peptide transport across human stratum corneum.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1573-904X
    Keywords: iontophoresis ; Nernst-Planck equation ; percutaneous penetration ; skin resistance ; skin capacitance ; peptide DGAVP ; human skin
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Notes: Abstract This study deals with effects of electrical (current density, frequency and duty cycle) and chemical (buffer pH and ionic strength) conditions on the flux of the octapeptide, 9-desglycinamide, 8-arginine-vasopressin (DGAVP), through dermatomed human skin. A pulsed constant current was applied during iontophoresis. The anode faced the anatomical surface of the skin samples inside the diffusion cells. The resistive and capacitative components of the equivalent electrical circuit of human skin could be calculated by fitting the voltage response to a bi-exponential equation. The skin resistance prior to iontophoresis varied between 20 and 60 k Ω.cm2. During iontophoresis a decrease of skin resistance and an increase of the series capacitances was observed, which were most pronounced during the first hour of iontophoresis; thereafter both quantities gradually levelled off to an apparent steady state value. The reduction of the resistance during iontophoresis increased non-linearly with increasing current density between 0.013–0.64 mA.cm−2. The steady state resistance and capacitances did not vary significantly with frequency and duty cycle of the current pulse. There was no pH dependence of skin resistance at steady state. Between pH 4 and 10, the steady state peptide flux had a bell-shaped pH-dependence with a maximum of 0.17 nmol.cm−2.h−1 at pH 7.4, which is close to the I.E.P. of the peptide. Lowering the ionic strength from 0.15 to 0.015 M NaCl increased the steady state flux at pH 5 and pH 8 by a factor 5 to 0.28 ± 0.21 and 0.48 ± 0.37 nmol.cm−2.h−1, respectively. Together these observations suggested that DGAVP is transported predominately by volume flow. At pH 6, at which 65% of the peptide carried a net single positive charge, the steady state flux increased with increasing current density (0.013–0.64 mA.cm−2) from 0.11 ± 0.03 to 0.19 ± 0.04 nmol.cm−2.h−1. Skin permeability during passive diffusion preceding iontophoresis at pH 6.0 was 2.9 ± 0.6 * 10−7 cm.h−7. In accordance with theoretical predictions based on the Nernst-Planck equation, to which a volume flow term was added, the flux was proportional to the mean voltage across the skin between 0.013 and 0.32 mA.cm−2.h−1. Variation of frequency or duty cycle did not result in significantly different peptide transport rates. From these studies it is concluded that DGAVP can be transported iontophoretically through human skin. The pH- and ionic strength-dependence of the iontophoretic peptide flux suggests that transport of DGAVP mainly occurs by volume flow. Furthermore, the flux of DGAVP appears to be controlled by the applied voltage rather than by the current density, as predicted by the Nernst-Planck equation.
    Type of Medium: Electronic Resource
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