scholarly journals Evaluation of the analytical performances of Cobas 6500 and Sysmex UN series automated urinalysis systems with manual microscopic particle counting

2018 ◽  
Vol 28 (2) ◽  
Author(s):  
Ebubekir Bakan ◽  
Zafer Bayraktutan ◽  
Nurcan Kilic Baygutalp ◽  
Mehmet Ali Gul ◽  
Fatma Zuhal Umudum ◽  
...  
2006 ◽  
Vol 6 (1) ◽  
pp. 1-9
Author(s):  
V. Miska ◽  
J.H.J.M. van der Graaf ◽  
J. de Koning

Nowadays filtration processes are still monitored with conventional analyses like turbidity measurements and, in case of flocculation–filtration, with phosphorus analyses. Turbidity measurements have the disadvantage that breakthrough of small flocs cannot be displayed, because of the blindness regarding changes in the mass distributions. Additional particle volume distributions calculated from particle size distributions (PSDs) would provide a better assessment of filtration performance. Lab-scale experiments have been executed on a flocculation–filtration column fed with effluent from WWTP Beverwijk in The Netherlands. Besides particle counting at various sampling points, the effect of sample dilution on the accuracy of PSD measurements has been reflected. It was found that the dilution has a minor effect on PSD of low turbidity samples such as process filtrate. The correlation between total particle counts, total particle volume (TPV) and total particle surface is not high but is at least better for diluted measurements of particles in the range 2–10 μm. Furthermore, possible relations between floc-bound phosphorus and TPV removal had been investigated. A good correlation coefficient is found for TPV removal versus floc-bound phosphorus removal for the experiments with polyaluminiumchloride and the experiments with single denitrifying and blank filtration.


The Analyst ◽  
2021 ◽  
Author(s):  
Xiaojun Liu ◽  
Zhangjian Wu ◽  
Xinyi Lin ◽  
Wei Bu ◽  
Lei Qin ◽  
...  

Monitoring ctDNA in blood is important to cancer management. Here, we develop a one-step single particle counting approach for directly quantifying ctDNA in plasma. Hairpin DNA containing a triple helix...


AIHAJ ◽  
1976 ◽  
Vol 37 (2) ◽  
pp. 103-108 ◽  
Author(s):  
DAVID LEITH ◽  
MELVIN W. FIRST
Keyword(s):  

Allergy ◽  
1983 ◽  
Vol 38 (3) ◽  
pp. 173-182 ◽  
Author(s):  
R. Djurup ◽  
C. G. M. Magnusson ◽  
U. Minuva ◽  
I. Søndergaard ◽  
O. østerballe ◽  
...  

2008 ◽  
Author(s):  
Dayong Jin ◽  
Belinda Ferrari ◽  
Robert C. Leif ◽  
Sean Yang ◽  
Lidia M. Vallarino ◽  
...  

2003 ◽  
Vol 125 (5) ◽  
pp. 895-901 ◽  
Author(s):  
Michael G. Olsen ◽  
Chris J. Bourdon

In microscopic particle image velocimetry (microPIV) experiments, the entire volume of a flowfield is illuminated, resulting in all of the particles in the field of view contributing to the image. Unlike in light-sheet PIV, where the depth of the measurement volume is simply the thickness of the laser sheet, in microPIV, the measurement volume depth is a function of the image forming optics of the microscope. In a flowfield with out-of-plane motion, the measurement volume (called the depth of correlation) is also a function of the magnitude of the out-of-plane motion within the measurement volume. Equations are presented describing the depth of correlation and its dependence on out-of-plane motion. The consequences of this dependence and suggestions for limiting its significance are also presented. Another result of the out-of-plane motion is that the height of the PIV signal peak in the correlation plane will decrease. Because the height of the noise peaks will not be affected by the out-of-plane motion, this could lead to erroneous velocity measurements. An equation is introduced that describes the effect of the out-of-plane motion on the signal peak height, and its implications are discussed. Finally, the derived analytical equations are compared to results calculated using synthetic PIV images, and the agreement between the two is seen to be excellent.


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