Taylor–von Neumann–Sedov blast wave
Self-similar solution describing the fluid dynamics of explosions / From Wikipedia, the free encyclopedia
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Taylor–von Neumann–Sedov blast wave (or sometimes referred to as Sedov–von Neumann–Taylor blast wave) refers to a blast wave induced by a strong explosion. The blast wave was described by a self-similar solution independently by G. I. Taylor, John von Neumann and Leonid Sedov during World War II.[1][2]