By Hans-Peter Dabrowski
This strange late-war tandem bomb was once really utilized by the Luftwaffe in the course of global conflict II. coated listed below are technical info of plane used, in addition to operational info.
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Extra resources for Mistel, The Piggyback Aircraft of the Luftwaffe
B*. The qualitative behaviours of ~ ( b * for ) three different values of g** = E / E are reported in Fig. 4. Fig. 4 The figure shows the behaviour of the function X(b*) for three different values of g **=HE. For b* b& the function X(b*) diverges 4 -) (point 0. ,f, are reported in Fig. 5. The quoted Tables show that: i) For b* = 0 and any value of g *2 we always have = n. This is typical of a “head on collision” in which the incoming particle is back reflected along the rn axis (see Fig. 5a); ii) The value b*,for which is = 0 increases when g* is decreased (see Fig.
10) ii) Z l , = Number of collisions/sec suffered by “one” molecule of species 1 encountering n molecules /cm3 of the species 2. 1 1) iii) Z2, = Number of collisions/sec undergone by a molecule of species 2 in the encounter with n molecules /cm3 of the species 1. 12) iv) Z;l, = Total number of collisions/(cm3sec) among the molecules of species 1. 13) v) 2;; = Total number of collisions/(cm3sec) among the molecules of both species 1 and 2. , T allow us to approximately estimate such quantities. Eqs.
In Fig. 3 for the point I is ( d 3 V l d r 3 ) p< O and the force F ( p + S r ) is for 6r(> Oor < 0) always direct in the positive direction of the r axis. So, if we exclude a very small region around point I where F ( p ) = 0 , the forces are always repulsive. The orbit radius r, appears as the limit approached by the orbits of radius r M A x when L and E both increase. Indeed, orbits with a radius r < rl are impossible since V(r) is monotonically decreasing while the repulsive force F ( r ) is always dominating.