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Next in Fig. 5 μm of the same density. We find that increasing eccentricity increases the deposition probability for the particles of the above diameters. Larger diameters reach a constant higher probability plateau at 2 Respiratory Particle Deposition Probability Due to Sedimentation. . 33 Fig. 5 μm and density ρ ¼ 1,300 kg/m3 Fig. 3μm smaller eccentricities. In Fig. 5 s, respectively, from the bottom up. We find that the orbital inclination does not affect the deposition probability which appears to be constant for the various residence times indicated.

On the other hand if the eccentricity increases then the deposition probability increases as well. 7): 2 Respiratory Particle Deposition Probability Due to Sedimentation. . # À Á q2 R2 x2 1 þ 2f sin 2 ϕ þ f 2 sin 4 ϕ cos ξ À mε0 ðx À RÞ2 Q0 25 ð2:77Þ where in the case of the Earth is equal to Q0 ¼ 50:2655 GME À 37:699 GM 0E J 2 0 11 À50:2655 þ113:097GME J 2 cos 2ϕ þ R2E ω2E @ cos 2 ϕ@ þf 2 sin 4 ϕðÀ150:796 þ 50:2655f sin 2 f Þ AA: þ37:6991f sin 2 2ϕ ð2:78Þ This angle is independent of the residence time t, the particle densityρ, and the particle diameter d and depends only on the planetary parameters indicated.

The net effect of these parameters can be modeled in the theory of information. According to Shannon [28] information is transferred with an allowable degree of noise. Shannon allows the introduction of noise in the interaction of a biological organism and environment, where noise accounts for biological environment variation [3, 22, 32]. In this paper we do not quantify the effect of noise according to Shannon’s rate distortion theory, but we study how information or the self-information of the system can be reflected and codified via gravity in the natural phenomenon of sedimentation, taking into account that the respiratory system is itself a decoder of the information transmitted and contained in the system of the human body.

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