Rapid analysis of oil shales for oil yield using X-ray spectrometry

Fuel ◽  
1988 ◽  
Vol 67 (5) ◽  
pp. 733-734 ◽  
Author(s):  
Leslie S. Dale ◽  
Christian E. Matulis
Keyword(s):  
X Ray ◽  
1999 ◽  
Vol 121 (1) ◽  
pp. 13-21 ◽  
Author(s):  
S. M. Ford ◽  
J. Davies ◽  
B. Kar ◽  
S. D. Qi ◽  
S. McWhorter ◽  
...  

Micromachining was performed in polymethylmethacrylate (PMMA) using X-ray lithography for the fabrication of miniaturized devices (microchips) for potential applications in chemical and genetic analyses. The devices were fabricated using two different techniques: transfer mask technology and a Kapton® mask. For both processes, the channel topography was transferred (1:1) to the appropriate substrate via the use of an optical mask. In the case of the transfer mask technique, the PMMA substrate was coated with a positive photoresist and a thin Au/Cr plating base. Following UV exposure, the resist was developed and a thick overlayer (∼3 μm) of Au electroplated onto the PMMA substrate only where the resist was removed, which acted as an absorber of the X-rays. In the other technique, a Kapton® film was used as the X-ray mask. In this case, the Kapton® film was UV exposed using the optical mask to define the channel topography and following development of the resist, a thick Au overlayer (8 μm) was electrodeposited onto the Kapton® sheet. The PMMA wafer during X-ray exposure was situated directly underneath the Kapton® mask. In both cases, the PMMA wafer was exposed to soft X-rays and developed to remove the exposed PMMA. The resulting channels were found to be 20 μm in width (determined by optical mask) with channel depths of ∼50 μm (determined by x-ray exposure time). In order to demonstrate the utility of this micromachining process, several components were fabricated in PMMA including capillary/chip connectors, injectors for fixed-volume sample introduction, separation channels for electrophoresis and integrated fiber optic fluorescence detectors. These components could be integrated into a single device to assemble a system appropriate for the rapid analysis of various targets.


1980 ◽  
Vol 17 (1) ◽  
pp. 13-21
Author(s):  
C. William Keighin

Inter- and intra-laboratory comparison of Fischer assay data and testing of these data by correlation analysis indicate good correlation but varied amounts of scatter in the data. The scatter seems to be due to both mechanical and analytical factors; it is possible that non-uniform sample preparation is a dominant factor in causing scatter, but variable analytical results are also apparent. The range in precision of the Fischer assay data is generally small and probably does not seriously affect the accuracy of the calculated shale-oil resources. It is highly desirable to have an accurate and uniform assay method to determine the oil yield of oil shales. If inter- or intra-laboratory precision is to be maintained, it is imperative that sample preparation and analytical conditions are uniform and closely supervised.


1980 ◽  
Vol 17 (9) ◽  
pp. 1315-1321 ◽  
Author(s):  
K. Rajeshwar ◽  
J. DuBow ◽  
R. Thapar

Laboratory measurements on the radio-frequency (10–103 MHz) electrical behavior of Green River oil shales were carried out using an automated frequency domain technique. Data are presented which show the variation of the relative dielectric constant (ε′), dielectric loss (ε″), and loss tangent (tan δ) with shale oil yield, frequency, temperature, and water content. The magnitude of these electrical parameters is shown to be sensitive to water content and possibly to varve geometry. The ε′ values tend to decrease and tan δ increases with increasing oil yield for shales subjected to prior thermal treatment at ~110 °C for 1–2 weeks. A systematic variation is observed in the degree of scatter and in the extent of correlation of tan δ and ε′ as a function of oil yield with each subsequent thermal treatment cycle. The manner in which variations in shale water content and (or) varve geometry influence the magnitude of the measured dielectric parameters is illustrated by duplicate measurements on samples with identical organic content. Such effects are shown to be important at low measurement frequencies (< 200 MHz). The temperature dependence of ε′ and ε″ is seen to be weak in the range 25–250 °C and appears to be largely dominated by temperature-induced changes in the water content of the shale.


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