Skip to main content

Page of 3
and
  1. No Access

    Chapter

    Estimation of error introduced by ignoring the background

    Whenever X-ray intensity measurements are made on a selected peak, occuring at a certain setting of the goniometer, some fraction of the measured counting rate is always due to background. The significance of ...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  2. No Access

    Chapter

    Variation of limit of detection with analysis time

    A series of measurements of fluorine in cement sample yielded a peak counting rate of 4 c/s/% for fluorine (F Kα) over a background of 6.5 c/s.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  3. No Access

    Chapter

    Continuous radiation — Scattered radiation

    The continuous radiation from an X-ray tube is scattered by the sample, diffracted by the analyzing crystal and measured by the detector.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  4. No Access

    Chapter

    Particle statistics in X-ray diffractometry

    Only those crystallites having the reflecting planes almost parallel to the specimen surface can contribute to a certain reflection. The intensity of the resulting diffraction is thus dependent on this number ...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  5. No Access

    Chapter

    Dispersion as a function of ‘d’ spacing

    LiF is commonly used as an analysing crystal. The (200) reflection planes are commonly used, having a “2 d” value of 4.028 Å. It is, however, possible to use reflecting planes with other Miller indi...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  6. No Access

    Chapter

    Determination of CaO in cement (ratio measurement)

    The following data were obtained using a series of cement samples. Counting ratios were determined on the Ca Kα line using sample 5 as the ratio standard.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  7. No Access

    Chapter

    Absorption correction involving primary and secondary absorption

    The slope of a calibration curve for a certain element is dependent upon the total absorption of the measured wavelength within the sample matrix. Although it is common practice to assume that only secondary a...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  8. No Access

    Chapter

    Pulse height selection — crystal fluorescence

    It is necessary to set up an X-ray spectrometer for the measurement of sodium in a series of rock specimens. An argon/methane flow counter is being employed and a KAP (potassium hydrogen phthalate) analysing c...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  9. No Access

    Chapter

    Calculation of matrix absorption and prediction of absorption effects

    The total secondary absorption of a matrix is given by (16) $$\mu_{matrix} = \sum\limits_i {\left({\mu_i w_i} \right)\left({16...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  10. No Access

    Chapter

    Use of α correction factor (intensity correction)

    A series of eight samples were analysed for a certain element A. An element B, also present in major concentration, was found to strongly absorb element A.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  11. No Access

    Chapter

    Excitation probability

    It is often thought that the wavelength in the primary spectrum most efficient in exciting the fluorescent radiation of an element A is that which is closest to the absorption edge of element A. The probabilit...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  12. No Access

    Chapter

    Quantitative X-ray diffractometry use of internal standard

    The weight fraction of α quartz (SiO2) has to be determined in a natural specimen. To correct for the unknown absorption in this specimen, 200mg KC1 are added to 1000 mg of the sample, both very finely, ground, a...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  13. No Access

    Chapter

    Estimation of gold plating thickness

    The following intensities were obtained from a series of gold plated steel samples measured on the Au Lα line.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  14. No Access

    Chapter

    Quantitative x-ray diffractometry

    Very often the quantity of a compound has to be determined in a complex mineral, the composition and absorption coefficients of which are unknown. To correct for these unknown facts, the attenuation of a diffr...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  15. No Access

    Chapter

    Background variation

    A scan is being made on a rock sample in the region of the barium K spectra.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  16. No Access

    Chapter

    Calculation of ß filter thickness and transmission

    A Ni filter has been constructed in such a way that only 2% of the incident Cu Kβ radiation may pass. Given that the density of Ni is 8.92 g/cm3 and that the mass absorption of Ni for Cu Kα and Cu Kβ is 49.2 cm2/...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  17. No Access

    Chapter

    Choice of detectors

    A A choice has to be made between the scintillation counter and the flow proportional counter for the measurement of a certain wavelength.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  18. No Access

    Chapter

    Determination of lattice constants for a cubic lattice

    The following 12 lines were obtained from a crystalline powder. Data were obtained using nickel filtered Cu Kβ radiation. The powder is known to belong to the cubic system.

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  19. No Access

    Chapter

    Dispersion of the diffractometer

    The dispersion of the diffractometer (dθ/dλ) can be expressed in the given form obtained by differentiating the Bragg law = 2dsinθ (5) ...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

  20. No Access

    Chapter

    Spurious peaks in X-ray diffractograms

    Adiffractogram of quartz exhibited an additional spurious peak at approximately 6° (2θ).The effect was observed both in specimens containing only low atomic number elements and specimens containing high atomic...

    R. Jenkins, J. L. de Vries in Worked Examples in X-Ray Analysis (1970)

Page of 3