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Coherent Backscattering from Multiple Scattering Systems - KOPS ...

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4 Samples<br />

Figure 4.4: Titania and teflon samples. (Clockwise <strong>from</strong> left:) Teflon sample with 4 cm<br />

diameter and 5 cm height, titania sample with 15 mm diameter and < 1 mm height in<br />

sample container, titania powder. Even on the photo one can observe the significant<br />

difference in the albedos or ”whiteness” of Teflon and titania.<br />

With a diameter of 4 cm and a thickness of 5 cm our teflon sample is not exactly a slab,<br />

which however would be the condition for eqn. 2.12 to be valid. The value of D = 27500 m2 /s<br />

measured in time of flight experiments is therefore not correct. In time of flight experiments<br />

on shorter teflon blocks the diffusion coefficient drops to D = 20000 m2 /s for samples with<br />

thickness L ≈ 2 − 3 cm, and even to D = 16500 m2 /s for L ≈ 1 − 1.5 cm. With this last value<br />

eqns. 2.7 and 2.16 propose a transport mean free path of about 220 µm and a cone width<br />

of approximately 0.01 ◦ . This is very close to the results of the backscattering experiments<br />

reported in sec. 5.2.2, which yield l ∗ = 180 µm, and correspondingly a diffusion coefficient<br />

D = 13300 m2 /s, which however could not be measured in the time of flight experiments due<br />

to the still insufficient size of the teflon samples. a For the absorption time τ the time of flight<br />

data yield 3.3 ns, the refractive index of teflon is given in literature as n = 1.35 [4].<br />

4.2.3 Fluidized beds<br />

A fluidized bed is a mixture of a fluid and a granular medium that has fluid-like properties. As<br />

a dispersion of particles in an upward flux of low-viscosity fluid (gas or liquid) it represents an<br />

intermediate system between suspensions in viscous fluids and dry granular materials. It has<br />

excellent heat and mass transfer characteristics, and the fluid-solid mixture is easy to remove<br />

[a] For technical reasons – the samples have to fit into the time of flight setup – it is impossible to use teflon samples<br />

with larger radii that can reasonably be described as an infinite slab. The adaption of the setup to accommodate<br />

larger samples seems to be the only solution.<br />

40

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