The structure of liquid mercury

Rivlin, V. G.; Waghorne, R.M.; Williams, Geoffrey T.

doi:10.1080/14786436608213533

Cited by 59 publications

(13 citation statements)

References 17 publications

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“…3 that there are differences between the results of Rivlin et al [15] and those of the present work a t temperatures below room temperature. This may be related to the normalization procedure of Rivlin et al because they used only the long-wavelength radiation of CuK,.…”

Section: Resultscontrasting

confidence: 64%

The structure of liquid mercury over a wide range of temperature (−30 to 290 °C)

Waseda

Miller

1979

Physica Status Solidi (b)

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X-ray diffraction patterns are obtained from liquid mercury a t -30, 20, 120, 220 and 290 "C.The structure factors obtained are insensitive to temperature and applied to the calculation of the electrical resistivity and the thermoelectric power on the basis of the t-matrix formulation of the Ziman nearly free electron theory. The calculated values show reasonable agreement with the available experimental data.Rontgenbeugungsbilder werden von fliissigem Queclrsilber bei -30, 20, 120, 220 und 290 "C beobachtet. Die gefundenen Strukturfaktoren sind nahezu unabhangig von der Temperatur. Es wird der elektrische Widerstand und die Thermospannung mittels des t-Matrizen-Formalismus der Ziman-Theorie der fast-freien Elektronen berechnet. Der berechnete U'ert zeigt eine ziemlich gute Ubereinstimmung mit den verfugbaren experimentellen Daten.

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Section: Resultscontrasting

confidence: 64%

The structure of liquid mercury over a wide range of temperature (−30 to 290 °C)

Waseda

Miller

1979

Physica Status Solidi (b)

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“…The values of the resistivity should be good to about 2% and those of the thermopower to about 5 "/,. Rivlin et al (1966) have measured the structure factor of pure liquid mercury at -36"C, -10°C and 27 "C. (We are grateful to Dr Rivlin for supplying this data). From these measurements we can calculate the resistivity at the three temperatures.…”

Section: Calculation Of Electrical Transport Coefficients 41 Pure Mmentioning

confidence: 99%

Investigation on Sub-20 fs Fiber-soliton Compression Performance of Dispersion-Flattened Fibers

Igarashi

Saitô

Nagai

et al. 2004

Jpn. J. Appl. Phys.

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Model potentials for zinc, indium, thallium, lead, cadmium and mercury are constructed using an adaptation of Shaw's energy-dependent formalism which allows the effect of high d-core states to be included. In the case of mercury this leads to a striking change in the shape of the screened form factor. Numerical calculations of the thermopower in liquid zinc, indium, thallium and mercury are in better agreement with experiment than previous calculations which did not include the energy-dependent term. Calculations of the resistivity of alloys of mercury with indium, thallium, zinc and lead are presented. These show a sharp decrease of the resistivity on alloying which is in reasonable agreement with the experimental results.

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“…The strong correlation between the data obtained from the two methods is apparent. The energyscanning result has been compared also with recent existing data* (Black & Cundall, 1965;Wagner, Ocken & Joshi, 1965;Ocken & Wagner, 1966;Rivlin, Waghorne & Williams, 1966;Halder & Wagner, 1967Caputi, Rodriquez & Pings, 1968;Waseda & Suzuki, 1970;Ruppersberg & Reiter, 1972). Both the peak positions and the value of si(s) at each peak correlate well.…”

Section: Evaluation Of the Energy-scanning Techniquementioning

confidence: 99%

Liquid-structure analysis by energy-scanning X-ray diffraction: mercury

Prober¹,

Schultz²

1975

J Appl Cryst

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Quantitative liquid-structure analysis using energy-scanning diffraction rather than the traditional angle-scanning diffraction is introduced. In the experimental method, white radiation and a solid-state detector are employed. This new method is inherently faster and less beset with problems of experimental instability than are angular-scanning methods. However, many differences in analysis are introduced. In particular, measurement of the primary beam spectrum, the nature of the absorption and dispersion corrections, details of the polarization correction, the ranges of the atomic scattering factor and of the incoherent scattering term, and the mating of different scattering regimes all require special consideration. Application of the new instrumental method and the reconstructed analytical procedure to liquid mercury at room temperature has produced a result in agreement with other recent studies.

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The structure of liquid mercury

Cited by 59 publications

References 17 publications

The structure of liquid mercury over a wide range of temperature (−30 to 290 °C)

The structure of liquid mercury over a wide range of temperature (−30 to 290 °C)

Investigation on Sub-20 fs Fiber-soliton Compression Performance of Dispersion-Flattened Fibers

Liquid-structure analysis by energy-scanning X-ray diffraction: mercury

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