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Riemann's Contribution to Flight and Laser Fusion

Riemann's Contribution to Flight and Laser Fusion

Riemann's Contribution to Flight and Laser Fusion

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started <strong>to</strong> fly again, there was a new center in Braunschweig.There I built my own wind tunnels. I came <strong>to</strong> ) von Braun. We Germans talked <strong>to</strong> each other so that wetunnels, but rocketry, <strong>to</strong>o. It was then that I got <strong>to</strong> knowBraunschweig in 1936. Then I had a really different, transsonickind of a tunnel, with a very large diameter, <strong>and</strong> a ment. When they had experience, they <strong>to</strong>ld me about it,didn't spend a million reichsmarks on the same experi-supersonic tunnel with a small cross section. And I also ) <strong>and</strong> when we wanted a new experiment, we <strong>to</strong>ld eachhad a rocket test facility in the country. It was in the ! other. Of course, it is sometimes very good for twocountry, because a lot of people who invented rockets 5 different people <strong>to</strong> test the same thing. But we were notdied from the explosions; therefore, we couldn't build in i supposed <strong>to</strong> do that.the neighborhood of the <strong>to</strong>wn. But I had <strong>to</strong> go there a Icouple of times every month <strong>to</strong> see what they were doing. Question: What was the motivation for the research youTherefore, my problem was at that time not only wind i did on self-similar solutions in spherical geometry?Busemann's design of a conical focus for shock waveswas published in 1942 in Luftfarhrtforschung (vol. 79, p.737), the same journal that published K. Guderley'sfamous paper on self-similar solutions <strong>to</strong> the focusingof shock waves in a spherical geometry. Two of theview-graphs used in Busemann's secret 1940 talk onshaped charges are reproduced in a <strong>and</strong> b. Busemannreports that the initial motivation for these focusingFigure 2CONICAL FOCUSING OF SHOCK WAVESideas came from the conception of a dimensionalconstraint on the propagation of shock waves. Thus, ahighly symmetrical geometry is chosen, such as asphere, cylinder, or cone. The cone <strong>and</strong> sphere sharethe property of having a zero-dimensional focus (apoint), as opposed <strong>to</strong> the cylinder with a line focus.The result in practical terms is a technique for thegeneration of almost unlimited pressures at the focus.Some of the geometrical considerations in the reflection,interference, <strong>and</strong> concentration of shock wavesare shown in a <strong>and</strong> b. These flows are all steady, but itis possible <strong>to</strong> generalize these techniques if the numberof space dimensions is reduced by one, <strong>and</strong> then <strong>to</strong>treat nonsteady flows. Busemann notes that his firstnonsteady solutions, which are important in aerodynamics,were just adaptations of the conical supersonicsolutions.<strong>Laser</strong> fusion research <strong>to</strong>day uses this idea <strong>to</strong> generatethe pressures <strong>and</strong> temperatures necessary for ignitionin a spherical target. The figure on page 29 shows aspherical compression scheme used at Lawrence LivermoreNational Labora<strong>to</strong>ry for laser-compressed fusionfuel, using the geometry of Guderley.The conical geometry proposed by Busemann hasbeen extensively investigated in the Soviet Union, <strong>and</strong>has resulted in the first fusion reactions produced byan electron beam (by Leonid Rudakov in 1976) <strong>and</strong> bychemical explosives (by a Polish group under the directionof General Kaliski). The theoretical work on theSoviet conical pellet design appeared in a paper by V.A. Belokogne in 1965 (see c). The Polish configurationis shown in d.38 FUSION Oc<strong>to</strong>ber-November 1981

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