German Gliders in World War II by Heinz J. Nowarra

By Heinz J. Nowarra

This not often awarded subject is proven in its makes use of as team of workers, attack and gear shipping.

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The time-dependent solution for the lowest mode of diffusion can now be written n(r, z, t) = G U J 0 cos where Figure 1-11-6. Hyperbolic sine and cosine. (1-11-41) AMBIPOLAR DIFFUSION 25 The total solution which contains the radial higher modes as well as the fundamental is n(r,z,f) = f GfJJ0(a,r) [cos U=l \_ (2j ~H ^l g "' /t

W. McDaniel (1973). Mobility, diffusion, and clustering of K + ions in gases, J. Chem. Phys. 58, 2402-2411. Townsend, J. S. (1899). The diffusion of ions into gases, Philos. Trans. R. Soc. London A193, 129-158. Wannier, G. H. (1953). Motion of gaseous ions in strong electric fields, Bell Syst. Tech. J. 32, 170-254. 2 MEASUREMENT OF DRIFT VELOCITIES AND LONGITUDINAL DIFFUSION COEFFICIENTS Direct measurements of drift velocities and longitudinal diffusion coefficients are made with apparatus called drift tubes, descriptions of which are given in Section 2-5.

The solution for the /cth mode can then be written n0(x)k = Akcos^-. /v k (1-11-5) The function cos(x/Afc) assumes negative values in certain regions within the cavity for all modes of diffusion except the lowest, or fundamental, mode corresponding to k = 1. Therefore, if we consider each solution singly, we must discard all but the fundamental mode on physical grounds, since the ionic number density can never be negative. Since, however, the diffusion equation is linear, the total solution consists of an infinite number of modes, many of which may be excited simultaneously.

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