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Minimum Required Distance of Strain Gauge from Specimen for Measuring Transmitted Signal in Split Hopkinson Pressure Bar Test

机译:分体霍普金森压力棒测试中测量传输信号的应变仪距试样的最小距离

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The minimum required distance of the strain gauge on the transmitted bar of the split Hopkinson bar has been determined from the position of a metallic specimen via an explicit finite element analysis. The minimum required distance was determined when the strain-time profiles at r = 0, 0.5 R _(o)and 1.0 R _(o), were coincident (r is the radial position and R _(o)is the radius of the bar.). The determined minimum required distance, f(x), is presented as a function of the relative specimen diameter to that of the bar ( x = D/D_(0)): j(x) = - 0.9385. x ~(3)+ 0.6624. x ~(2)- 0.7459. x + 1.4478 (0.1 ≤ x ≤ 0.9). This result demonstrates the Saint-Venant's principle of rapid dissipation of localized stress in transient loading. The result will be useful for the design/modification of the pseudo-one-dimensional impact instruments that utilise a stress pulse transmitted through the specimen. The result will also allow one to avoid unnecessarily remote strain gage position from the specimen.
机译:通过明确的有限元分析,根据金属试样的位置确定了应变计在分开的霍普金森杆的透射杆上的最小所需距离。当r = 0、0.5 R _(o)和1.0 R _(o)的应变时间曲线重合时(r是径向位置,R _(o)是半径的半径),确定了最小所需距离。酒吧。)。确定的最小所需距离f(x)是与试件相对于钢筋的相对直径的函数(x = D / D_(0)):j(x)=-0.9385。 x〜(3)+ 0.6624。 x〜(2)-0.7459。 x + 1.4478(0.1≤x≤0.9)。该结果证明了圣文南特原理在瞬态载荷中快速消散局部应力的原理。该结果对于利用通过样品传递的应力脉冲的伪一维冲击仪器的设计/修改将是有用的。结果也将使人们避免样品不必要地远离应变仪位置。

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