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Measurement of the refractive index of air in a low-pressure regime and the applicability of traditional empirical formulae

机译:低压制度中空气折射率的测量及传统经验公式的适用性

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The refractive index of air is a major limiting factor in length measurements by interferometry, which are mostly performed under atmospheric conditions. Therefore, especially in the last century, measurement and description of the air refractive index was a key point in order to achieve accuracy in the realisation of the length by interferometry. Nevertheless, interferometric length measurements performed in vacuum are much more accurate since the wavelength of the light is not affected by the air refractive index. However, compared with thermal conditions in air, in high vacuum heat conduction is missing. In such a situation, dependent on the radiative thermal equilibrium, a temperature distribution can be very inhomogeneous. Using a so-called contact gas instead of high vacuum is a very effective way to enable heat conduction on nearly the same level as under atmospheric pressure conditions whereby keeping the effect of the air refractive index on a small level. As physics predicts, and as we have demonstrated previously, helium seems like the optimal contact gas because of its large heat conduction and its refractive index that can be calculated from precisely known parameters. On the other hand, helium gas situated in a vacuum chamber could easily be contaminated, e.g. by air leakage from outside. Above the boiling point of oxygen (-183 degrees C) it is therefore beneficial to use dry air as a contact gas. In such an approach, the air refractive index could be calculated based on measured quantities for pressure and temperature. However, existing formulas for the air refractive index are not valid in the low-pressure regime. Although it seems reasonable that the refractivity (n-1) of dry air simply downscales with the pressure, to our knowledge there is no experimental evidence for the applicability of any empirical formula. This evidence is given in the present paper which reports on highly accurate measurements of the air refractive index n for the wavelengths 532 nm, 633 nm and 780 nm in the low-pressure regime from 0 Pa to 1300 Pa. In our approach, using a vacuum cell, n-1 is obtained from the comparison of optical path lengths in vacuum and air along the same path by imaging interferometry. These measured values are compared with the ones obtained from Bonsch's formula. An agreement of +/- 10(-9) is found in the low-pressure regime. Accordingly, this formula could be applied for the accurate determination of the refractive index of dry air even at low pressures, provided that the pressure is measured with high accuracy.
机译:空气的折射率是干涉测量中长度测量的主要限制因子,主要在大气条件下进行。因此,特别是在上世纪,空气折射率的测量和描述是通过干涉测量来实现长度的精度的关键点。然而,由于光的波长不受空气折射率的影响,真空执行的干涉测量长度测量更准确。然而,与空气中的热条件相比,缺少高真空导热。在这种情况下,取决于辐射热平衡,温度分布可以非常不均匀。使用所谓的接触气而不是高真空是一种非常有效的方法,可以在大气压条件下实现几乎与近似相同的水平的热传导,从而保持空气折射率对较小水平的影响。随着物理学预测,并且随着我们之前展示的,氦气似乎是最佳的接触气体,因为它的热导热和其折射率可以从精确已知的参数计算。另一方面,位于真空室中的氦气很容易被污染,例如污染。通过外部空气泄漏。高于氧气的沸点(-183℃),因此有利于使用干燥空气作为接触气体。在这种方法中,可以基于测量的压力和温度的量来计算空气折射率。然而,空气折射率的现有公式在低压方案中无效。虽然干燥空气的折射率(N-1)似乎是合理的,但是,在较压力下,较小的折射率,对于我们的知识,没有任何经验公式的适用性的实验证据。本文给出了本文给出了本文,其中报告了从0Pa至1300 pa的低压制度中的波长532nm,633nm和780nm的空气折射率n的高精度测量。在我们的方法中,使用a真空电池,通过成像干涉测量法从真空和空气中的真空和空气的比较获得N-1。将这些测量值与由盆景的公式获得的值进行比较。在低压制度中发现了+/- 10(-9)的协议。因此,即使在低压下,可以应用该公式用于精确测定干燥空气的折射率,只要通过高精度测量压力。

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