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首页> 外文期刊>Advances in Materials Physics and Chemistry >The Loading Curve of Spherical Indentions Is Not a Parabola and Flat Punch Is Linear
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The Loading Curve of Spherical Indentions Is Not a Parabola and Flat Punch Is Linear

机译:球形压痕的装载曲线不是抛物线和平拳是线性的

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The purpose of this paper is the physical deduction of the loading curves for spherical and flat punch indentations, in particular as the parabola assumption for not self-similar spherical impressions appears impossible. These deductions avoid the still common first energy law violations of ISO 14577 by consideration of the work done by elastic and plastic pressure work. The hitherto generally accepted "parabolas" exponents on the depth h ("2 for cone, 3/2 for spheres, and 1 for flat punches") are still the unchanged basis of ISO 14577 standards that also enforce the up to 3 + 8 free iteration parameters for ISO hardness and ISO elastic indentation modulus. Almost all of these common practices are now challenged by physical mathematical proof of exponent 3/2 for cones by removing the misconceptions with indentation against a projected surface (contact) area with violation of the first energy law, because the elastic and inelastic pressure work cannot be obtained from nothing. Physically correct is the impression of a volume that is coupled with pressure formation that creates elastic deformation and numerous types of plastic deformations. It follows the exponent 3/2 only for the cones/pyramids/wedges loading parabola. It appears impossible that the geometrically not self-similar sphere loading curve is an h~(3/2) parabola. Hertz did only deduce the touching of the sphere and Sneddon did not get a parabola for the sphere. The radius over depth ratio is not constant with the sphere. The apparently good correlation of such parabola plots at large R/h ratios and low h-values does not withstand against the deduced physical equation for the spherical indentation loading curve. Such plots are unphysical for the sphere and so tried regression results indicate data-treatments. The closed physical deduction result consists of the exponential factor h3/2 and a dimensionless correction factor that is depth dependent. The non-parabola against force plot using published data is concavely bent even for large radius/depth-ratios at the shallow indents. The capabilities of conical/pyramidal/wedged indentations are thus lost. These facts are outlined for experimental nano- and micro-indentations. Spherical indentations reveal that linear data regression is suspicious and worthless if it does not correspond with physical reality. This stresses the necessity of the straightforward deductions of the correct relations on the basis of iteration-less and fitting-less undeniable calculation rules on an undeniable basic physical understanding. The straightforward physical deduction of the flat punch indentation is therefore also presented, together with formulas for the physical indentation hardness, indentation work, and applied work for these geometrically self-similar indentations. It is exemplified with a macroindentation.
机译:本文的目的是球形和平坦打孔凹口的装载曲线的物理扣除,特别是由于抛物线假设而不是自相似的球形印象似乎是不可能的。这些扣除通过考虑通过弹性和塑料压力工作完成的工作,避免仍然是ISO 14577的仍然常见的第一能源法。迄今为止通常接受“抛物线”指数在深度h(“2的锥形,3/2为球体,平拳1的1个”)仍然是ISO 14577标准的不变基础,该标准也强制执行高达3 + 8免费ISO硬度和ISO弹性压痕模量的迭代参数。现在几乎所有这些常见做法都是通过在违反第一能量法的投影表面(接触)区域的误解,通过侵犯缩进的误解来挑战指数3/2的物理数学证明,因为弹性和无弹性工作不能从无到有。物理校正是一种体积的印象,其与压力形成联接,产生弹性变形和许多类型的塑性变形。它遵循仅针对锥形/金字塔/楔形载荷抛物线的指数3/2。几何不是自我相似的球形加载曲线似乎不可能是H〜(3/2)抛物线。赫兹确实只推断了球体的触摸,斯奈登没有得到球体的抛物线。半径过度比与球体不恒定。这种抛物线图以大的R / H比率和低H值的显然良好的相关性不会抵抗球形压痕加载曲线的推导的物理方程。这种绘图对于球体是不经理的,因此尝试的回归结果表明了数据处理。闭合物理扣除结果包括指数因子H3 / 2以及深度依赖的无量纲校正因子。即使在浅腺中的大半径/深度比下,使用公开数据的非抛物线抵抗力曲线凹凸不平。因此丧失了锥形/金字塔/楔形凹口的能力。这些事实概述了实验纳米和微压痕。球形缩进揭示了线性数据回归是可疑的,如果它与物理现实不相对应。这强调了基于不可席位的基本身体理解的迭代和廉价的无可否认的计算规则,对正确关系的简单扣除的必要性。因此,平压凹口的直接物理扣除也与用于物理压痕硬度,压痕作品和应用于这些几何自相似缩进的适用性的公式一起呈现。它是用宏观的例子。

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