On the Intrinsically Ambiguous Nature of Space-Time Diagrams

IF 0.1 Q4 HISTORY & PHILOSOPHY OF SCIENCE
É. During
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引用次数: 1

Abstract

When the German mathematician Hermann Minkowski first introduced the space-time diagrams that came to be associated with his name, the idea of picturing motion by geometric means, holding time as a fourth dimension of space, was hardly new. But the pictorial device invented by Minkowski was tailor-made for a peculiar variety of space-time: the one imposed by the kinematics of Einstein’s special theory of relativity, with its unified, non-Euclidean underlying geometric structure. By plo tting two or more reference frames in relative motion on the same picture, Minkowski managed to exhibit the geometric basis of such relativistic phenomena as time dilation, length contraction or the dislocation of simultaneity. These disconcerting effects were shown to result from arbitrary projections within four-dimensional space-time. In that respect, Minkowski diagrams are fundamentally different from ordinary space-time graphs. The best way to understand their specificity is to realize how productively ambiguous they are.
论时空图的内在模糊性
当德国数学家赫尔曼·闵可夫斯基(Hermann Minkowski)首次提出与他的名字联系在一起的时空图时,用几何方法描绘运动,将时间视为空间的第四维的想法并不新鲜。但闵可夫斯基发明的图像装置是为一种特殊的时空而量身定做的:它是由爱因斯坦狭义相对论的运动学所强加的,具有统一的、非欧几里得的底层几何结构。闵可夫斯基通过在同一幅图上绘制相对运动的两个或多个参照系,成功地展示了时间膨胀、长度收缩或同时性错位等相对论性现象的几何基础。这些令人不安的影响被证明是由四维时空中的任意投影造成的。在这方面,闵可夫斯基图与普通的时空图有着根本的不同。要理解它们的特殊性,最好的方法是认识到它们是多么的模棱两可。
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