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  • 65 N 05  (1)
  • INSTRUMENTATION AND PHOTOGRAPHY  (1)
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  • 1
    Publication Date: 2019-07-12
    Description: A high-speed video instrumentation system was used to observe solidification of undercooled Ti-51 at. pct Al. The camera system developed by Battelle is capable of operation at rates up to 12,000 frames per second. The system digitizes and stores video images acquired by a 64 x 64 pixel silicon photodiode array. In a joint effort with Vanderbilt University the camera was used to observe three transformations of the undercooled alloys, using containerless processing by electromagnetic levitation. The first was solidification where nucleation was induced at an undercooling of 9 percent Tl, where Tl is the liquidus temperature of the alloy, and the second was solidification where nucleation was spontaneous at an undercooling of 15 percent Tl. The third event was a solid-state nucleation and growth transformation following the solidification at an undercooling of 15 percent Tl.
    Keywords: INSTRUMENTATION AND PHOTOGRAPHY
    Type: Review of Scientific Instruments (ISSN 0034-6748); 63; 6 Ju
    Format: text
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Computing 25 (1980), S. 299-316 
    ISSN: 1436-5057
    Keywords: 65 N 05 ; 65 N 10 ; 65 M 05 ; 65 M 10
    Source: Springer Online Journal Archives 1860-2000
    Topics: Computer Science
    Description / Table of Contents: Zusammenfassung Für 0≤x≤1, 0≤t≤T betrachten wir die Diffusionsgleichung $$\gamma (x)u_t (x, t) - (B u)_x (x, t) = f(x, t)$$ mitB u:=(a(x)u) x +b(x)u oder (alternativ)a(x)u x +β(x)u. Vorgegeben sind Anfangswerteu(x,0), Zuflußraten −(B u) (0,t) und (B u) (1,t) und eine Zuflußrate (B u) (ζ−0,t)−(B u) (ζ+0,t) and einer Zwischenstelle ζ∈(0, 1), an der die sonst glatten Funktionen γ,a, b, β Sprungstellen haben dürfen.a und γ sind als positiv vorausgesetzt. Faßt manu(x, t) als Temperatur und γ(x) u (x, t) als Energiedichte auf, so kann man die Gesamtenergie $$E(t) = \int\limits_0^1 {\gamma (x) u (x, t)} $$ als Integral über die Daten schreiben. Wir analysieren explizite und implizite Einschritt-Differenzenschemata, die an den Zeitgitterpunkten über ein Quadratur-Analogon exaktE (t) reproduzieren. Diese Schemata imitieren auch die isotone Abhängigkeit der Lösung von den Daten, und somit kann ihre Stabilität mit Hilfe von Gerschgorins Methode bewiesen werden, unter entsprechenden Glattheitsannahmen ergibt sich die Konvergenz als 0 ((Δx)2+Δt).
    Notes: Abstract For 0≤x≤1, 0≤t≤T we consider the diffusion equation $$\gamma (x)u_t (x, t) - (B u)_x (x, t) = f(x, t)$$ with (alternatively)B u:=(a(x)u) x +b(x)u ora(x)u x +β(x)u. There are given initial valuesu(x,0), influx rates−(B u) (0,t) and (B u) (1,t) across the lateral boundaries and an influx rate (B u) (ζ−0,t)−(B u) (ζ+0,t) at an interface ζ∈(0, 1) where the elsewhere smooth functions γ,a, b, β are allowed to have jump discontinuities.a and γ are assumed to be positive. Interpretingu(x, t) as temperature and γ(x) u (x, t) as energy density we can easily express the total energy $$E(t) = \int\limits_0^1 {\gamma (x) u (x, t)} $$ in terms of integrals of the given data. We describe and analyse explicit and implicit one-step difference schemes which possess a discrete quadrature analogue exactly matchingE(t) at the time grid points. These schemes also imitate the isotonic dependence of the solution on the data. Hence stability can be proved by Gerschgorin's method and, under appropriate smoothness assumptions, convergence is 0 ((Δx)2+Δt).
    Type of Medium: Electronic Resource
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