<abstract xmlns="http://www.w3.org/1999/xhtml">
The distribution of the air flow through the porous wrapping of a cigarette is
<disp-formula><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/Fig.1.png"></inline-graphic></disp-formula>
ν (λ, l) being the density of the air flow (cm3 sec-1 cm-1) on the paper wrapping at the position l if l is the length of the porous paper wrapping between the non-porous tip and the burning cone and l is the distance of the position in question from the non-porous tip. ν (λ, l) is given in air flow per cm rather than in air flow per cm2 because of the cylindrical shape of the cigarette. I denotes the total stream at the mouth piece, a is the specific conductivity to air flow of the paper wrapping, b is the specific resistance to air flow of the tobacco rod, RG is the resistance to air flow of the burning cone [compare (1)]. The formula is derived and discussed. The dependence of the distribution of the ventilation stream on the length l and on the resistance RG is demonstrated for the case of a formerly investigated cigarette rod (1). The gradient of ν (λ, l) is
<disp-formula><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/Fig.2.png"></inline-graphic></disp-formula>
so that the density of the ventilation stream through the paper wrapping decreases almost linearly from its maximum at the tip to its minimum at the burning cone if the degree of ventilation is low, i.e. if the air flow I (λ, l) in the cigarette is not much higher at λ = 0 than at λ = l
</abstract>

The distribution of the air flow through the porous wrapping of a cigarette is

ν (λ, l) being the density of the air flow (cm3 sec-1 cm-1) on the paper wrapping at the position l if l is the length of the porous paper wrapping between the non-porous tip and the burning cone and l is the distance of the position in question from the non-porous tip. ν (λ, l) is given in air flow per cm rather than in air flow per cm2 because of the cylindrical shape of the cigarette. I denotes the total stream at the mouth piece, a is the specific conductivity to air flow of the paper wrapping, b is the specific resistance to air flow of the tobacco rod, RG is the resistance to air flow of the burning cone [compare (1)]. The formula is derived and discussed. The dependence of the distribution of the ventilation stream on the length l and on the resistance RG is demonstrated for the case of a formerly investigated cigarette rod (1). The gradient of ν (λ, l) is

so that the density of the ventilation stream through the paper wrapping decreases almost linearly from its maximum at the tip to its minimum at the burning cone if the degree of ventilation is low, i.e. if the air flow I (λ, l) in the cigarette is not much higher at λ = 0 than at λ = l

The Distribution of the Air Flow through a Cigarette / Die Verteilung des Ventilationsstromes auf einer Cigarette

Contributions to Tobacco & Nicotine Research

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The distribution of the air flow through the porous wrapping of a cigarette is

ν (λ, l) being the density of the air flow (cm3 sec-1 cm-1) on the paper...

The Distribution of the Air Flow through a Cigarette / Die Verteilung des Ventilationsstromes auf einer Cigarette

Pubblicato online: 13 giu 2014

Pagine: 505 - 516

DOI: https://doi.org/10.2478/cttr-2013-0147

© Beiträge zur Tabakforschung International

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 3.0 License.