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Thermal shock resistance of infrared transmitting windows and domes

机译:Thermal shock resistance of infrared transmitting windows and domes

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摘要

Sudden exposure to a supersonic flight environment subjects a missile window, or missile dome, to intense convective heat loads stemming from the rise in temperature of the boundary layer. The thermal response of the window then results in temperature gradients through the thickness, which generate transient stresses that may exceed the tensile strength of the material, thus causing thermal-shock-induced fracture. Since most of the materials that possess favorable optical properties in the infrared (IR) are relatively weak brittle solids, the problem of selecting window or dome materials and assessing their performance on a fly-out trajectory requires a careful evaluation of the window's ability to withstand thermally induced shocks. In this context, it is essential to keep in mind that the transient stress intensity depends on the nature of the heat flow as characterized by the Blot number (Bi). The allowable heat flux depends not only on intrinsic material properties but also on the heat transfer coefficient, if the condition Bi>l holds, or the thickness of the window, if the condition Bi<l applies. In a first approximation, the thermal shock performance of a "thick" window is controlled by the figure of merit (FOM)↓(Bi>1)= R↓(H), i.e., the Hasselman parameter for strong shocks; in a thermally thin regime, however, if σ↓(f) designates the flexural strength the appropriate figure of merit is (FOM)↓(Bi<l) = σ↑(n)↓(f)R′↓(H) with n= 1/2 for flat plates and n=2/3 for hemispherical shells, and not the Hasselman parameter R# for mild shocks. Judging from the results of thermal shock testing performed elsewhere, we conclude that in a laminar flow environment the allowable heat flux on a thermally thin IR dome can be expressed as follows: Q↓(lim) = 2R′↓(H)/L, where L is the dome thickness. This expression provides a direct means of obtaining the Mach-altitude failure line for a dome of given thickness and given radius, if the initial wall temperature is known. Furthermore, it then becomes straightforward to assess the thermal shock resistance capability of a thickness-optimized IR dome in terms of either the allowable heat load or, more simply, the allowable stagnation temperature. # 1998 society of Photo-Optical Instrumentation Engineers. S0091-3286(98)02010-8 Subject terms: bending stress; figure of merit; heat flux; infrared material; infrared window; missile dome; stagnation temperature; thermal shock; thermal stress. Paper 980080 received Mar. 5, 1998; revised manuscript received May 26,1998; accepted for publication May 27, 1998.

著录项

  • 来源
    《Optical Engineering》 |1998年第12期|2826-2836|共11页
  • 作者

    Claude A. Klein;

  • 作者单位

    c.a.k, analytics, inc./ 9 Churchill Lane Lexington, Massachusetts 02173 E-mail: 105325.1146 @ compuserve. corn;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 英语
  • 中图分类 光学仪器;
  • 关键词

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