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Formulating High SPF Sun Care Products With A - External Factor ...

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SUN CARE<br />

LIQUID-MINERAL UV FILTER<br />

This purely mathematical model shows<br />

that the transmission properties of a homogenous<br />

film decreases significantly<br />

with increasing film irregularities represented<br />

by the step film parameters f and<br />

g and can be calculated as the sum of the<br />

transmissions through the two fractions<br />

of the film (Fig. 5).<br />

Herzog et al. (10,11) refined this simple<br />

model by correlation of calculated data<br />

with measured in vivo <strong>SPF</strong> data and<br />

hereby defining the parameters f and g<br />

to be g = 0.269 and f = 0.935. These values<br />

reflect a considerable roughness of a<br />

sunscreen film as visualized in Fig. 6.<br />

Using these parameters they have a<br />

calibrated tool at their hands, called ‘the<br />

sunscreen simulator’ (16). This tool allows<br />

a good prediction of in vivo <strong>SPF</strong>’s<br />

for a given roughness of the film and<br />

in dependency of the UV-filter concentration<br />

(Table 1, B1-B3). However, this<br />

method fails in the prediction of the in vivo<br />

performance for formulations containing<br />

Polysilicone-15 (Table 1, A1-A3).<br />

This result is not surprising as Polysilicone-15<br />

has a comparable low UV specific<br />

extinction. Nevertheless, there are<br />

other effects compensating the low UV<br />

specific extinction which can be explained<br />

using the same mathematical<br />

model based on the step film theory. Traditional<br />

organic UV-filters as well as inorganic<br />

or organic pigments are concentrated<br />

on the skin surface after application<br />

and evaporation of the water phase.<br />

During this concentration process, traditional<br />

organic UV-filters tend to aggregate<br />

(13) as well as pigments tend to agglomerate.<br />

Due to these reasons, it is difficult<br />

to distribute the UV-filters evenly<br />

over the inherently rough skin surface.<br />

The model proposed by Herzog (16) using<br />

formulation containing traditional<br />

UV filters takes these effects into account<br />

through the choice of the parameters<br />

f and g. However, this model does<br />

not consider effects which lead to a more<br />

even distribution of the UV-light absorbing<br />

units on the skin which would<br />

consecutively be reflected in higher values<br />

for g and lower values for f.<br />

Through the unique structure of Polysilicone-15<br />

the aggregation of the chromophoric<br />

systems is significantly reduced.<br />

This is the case as the chromophore units<br />

are hold apart by the dimethylsiloxy-<br />

Fig. 5 The step film model as introduced by O´Neill (12)<br />

Fig. 6 The calibrated step film model by Herzog et al (10,11,16) reflecting<br />

in vivo conditions<br />

INCI A1 B1 A2 B2 A3 B3<br />

Polysilicone-15<br />

Ethylhexyl<br />

PARSOL® SLX 5 3 3<br />

Methoxycinnamate<br />

Butyl Methoxy-<br />

PARSOL® MCX 5 3 3<br />

dibenzoymethane<br />

Phenylbenzimidazol<br />

PARSOL® 1789 2 2 2.5 2.5<br />

Sulfonic Acid<br />

4-Methylbenzylidene<br />

PARSOL® HS 2 2 2 2<br />

Campher PARSOL® 5000 3 3 4 4<br />

Titanium dioxide Uvinul® TiO2 4 4<br />

Calculated in vivo <strong>SPF</strong> according to (16) 4 7 14 20 33 44<br />

Measured in vivo <strong>SPF</strong>* 10 11 20 21 44 41<br />

*International <strong>Sun</strong> Protection <strong>Factor</strong> (<strong>SPF</strong>) Test Method, COLIPA, February 2003<br />

Table 1 The ‘sunscreen simulator’<br />

4 SÖFW-Journal | 131 | 7-2005

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