Preferred Dialysis Fluid for the High-Performance Membrane

2011 ◽  
pp. 44-52 ◽  
Author(s):  
Tadashi Tomo
Keyword(s):  
High Performance ◽  
Dialysis Fluid

Liquid-chromatographic assay of cefamandole in serum, urine, and dialysis fluid.

1986 ◽  
Vol 32 (1) ◽  
pp. 197-200 ◽  
Author(s):  
M Bliss ◽  
M Mayersohn
Keyword(s):  
Mobile Phase ◽  
High Performance ◽  
Biological Fluids ◽  
High Performance Liquid Chromatographic ◽  
Reversed Phase ◽  
Pharmacokinetic Studies ◽  
Dialysis Fluid ◽  
Serum Samples ◽  
Liquid Chromatographic ◽  
Phase Column

Abstract We describe a "high-performance" liquid-chromatographic assay for quantifying cefamandole in biological fluids from patients with renal impairment. Serum samples are deproteinized with acetonitrile, then extracted with dichloromethane; dialysis-fluid samples are injected directly; urine samples are diluted appropriately before injection onto the reversed-phase column. The mobile phase is a methanol/aqueous solution (31/69 by vol) containing 500 microL of phosphoric acid, 20 mmol of sodium sulfate, and 200 microL of triethylamine per liter, the mixture being adjusted to pH 6.0 with NaOH. Retention time for cefamandole is 12 min. Its peak is well resolved in highly contaminated samples from renally impaired subjects. The assay's selectivity, reproducibility (within-day and between-day CVs less than 8% in all three sample fluids), and sensitivity--0.5 mg/L in serum, 1.0 mg/L in dialysis fluid, and 5.0 mg/L in urine--make it applicable to pharmacokinetic studies.

Identification and characterisation of fluorescent substances in spent dialysis fluid

2020 ◽  
Vol 43 (9) ◽  
pp. 579-586
Author(s):  
Jörn Meibaum ◽  
Silvie Krause ◽  
Hartmut Hillmer ◽  
Daniele Marcelli ◽  
Christof Strohhöfer
Keyword(s):  
High Performance Liquid Chromatography ◽  
Liquid Chromatography ◽  
End Stage Renal Disease ◽  
High Performance ◽  
Physiological Solution ◽  
Dialysis Fluid ◽  
Chromatography Analysis ◽  
Stage Renal Disease ◽  
End Stage ◽  
Indole 3 Acetic Acid

Patients who suffer from end-stage renal disease require renal replacement therapy, including haemodialysis. While applying extracorporeal blood treatment, uraemic toxins accumulated in the patients’ blood pass into a physiological solution, the dialysis fluid. Thus, important information about the patient’s health status can be obtained by analysing the spent dialysis fluid. To make use of this information, corresponding analysis concepts must be developed. In this context, this article reports the analysis of fluorescence in spent dialysis fluid. Excitation and emission maxima of fluorescence in spent dialysis fluid were recorded, and the main fluorescent substances were identified and quantified using high-performance liquid chromatography analysis. Fluorescence in spent dialysis fluid has two prominent excitation maxima at λex1 = 228 nm and λex2 = 278 nm. However, both excitation maxima cause emission with maxima at λem = 350 nm. Identification of fluorescent substances using high-performance liquid chromatography showed that the main contributors to the overall fluorescence in spent dialysis fluid are tyrosine, tryptophan, indoxyl sulphate and indole-3-acetic acid. However, these substances are responsible for only one-third of the overall fluorescence of spent dialysis fluid. A large number of substances, each of which contributes only to a small part to the overall fluorescence, emit the remaining fluorescence.

A High Performance Energy Analyzer for Use in Electron Scanning Microscopy

1969 ◽  
Vol 27 ◽  
pp. 14-15
Author(s):  
A. V. Crewe ◽  
M. Isaacson ◽  
D. Johnson
Keyword(s):  
High Performance ◽  
Vertical Plane ◽  
Median Plane ◽  
Electron Gun ◽  
Uniform Field ◽  
Loss Mechanism ◽  
Electron Scanning Microscopy ◽  
Sector Type ◽  
Double Focusing ◽  
Electron Energy Loss

A double focusing magnetic spectrometer has been constructed for use with a field emission electron gun scanning microscope in order to study the electron energy loss mechanism in thin specimens. It is of the uniform field sector type with curved pole pieces. The shape of the pole pieces is determined by requiring that all particles be focused to a point at the image slit (point 1). The resultant shape gives perfect focusing in the median plane (Fig. 1) and first order focusing in the vertical plane (Fig. 2).

Vacuum System to Minimize the Specimen Contamination of High-Performance EM

1977 ◽  
Vol 35 ◽  
pp. 68-69
Author(s):  
N. Yoshimura ◽  
K. Shirota ◽  
T. Etoh
Keyword(s):  
Electron Microscope ◽  
High Speed ◽  
High Performance ◽  
High Vacuum ◽  
Vacuum System ◽  
Pump System ◽  
Pumping System ◽  
Diffusion Pump ◽  
Almost All ◽  
Cascade Type

One of the most important requirements for a high-performance EM, especially an analytical EM using a fine beam probe, is to prevent specimen contamination by providing a clean high vacuum in the vicinity of the specimen. However, in almost all commercial EMs, the pressure in the vicinity of the specimen under observation is usually more than ten times higher than the pressure measured at the punping line. The EM column inevitably requires the use of greased Viton O-rings for fine movement, and specimens and films need to be exchanged frequently and several attachments may also be exchanged. For these reasons, a high speed pumping system, as well as a clean vacuum system, is now required. A newly developed electron microscope, the JEM-100CX features clean high vacuum in the vicinity of the specimen, realized by the use of a CASCADE type diffusion pump system which has been essentially improved over its predeces- sorD employed on the JEM-100C.

Use of the Magnetostatic Analogue In Electromagnetic Lens Engineering

1970 ◽  
Vol 28 ◽  
pp. 360-361
Author(s):  
John W. Coleman
Keyword(s):  
Boundary Conditions ◽  
High Performance ◽  
Force Fields ◽  
Optical Design ◽  
Direct Conversion ◽  
Design Engineering ◽  
Design Data ◽  
Scalar Potentials ◽  
Geometric Elements ◽  
At Will

In the design engineering of high performance electromagnetic lenses, the direct conversion of electron optical design data into drawings for reliable hardware is oftentimes difficult, especially in terms of how to mount parts to each other, how to tolerance dimensions, and how to specify finishes. An answer to this is in the use of magnetostatic analytics, corresponding to boundary conditions for the optical design. With such models, the magnetostatic force on a test pole along the axis may be examined, and in this way one may obtain priority listings for holding dimensions, relieving stresses, etc..The development of magnetostatic models most easily proceeds from the derivation of scalar potentials of separate geometric elements. These potentials can then be conbined at will because of the superposition characteristic of conservative force fields.

Prospects for convergent beam electron diffraction with a 200kV cold field-emission transmission electron microscope

1991 ◽  
Vol 49 ◽  
pp. 466-467
Author(s):  
J W Steeds ◽  
R Vincent
Keyword(s):  
Field Emission ◽  
High Performance ◽  
Small Diameter ◽  
Convergent Beam Electron Diffraction ◽  
Zone Axis ◽  
Medium Voltage ◽  
Transmission Electron ◽  
Good Crystallinity ◽  
Special Modification ◽  
Convergent Beam

We review the analytical powers which will become more widely available as medium voltage (200-300kV) TEMs with facilities for CBED on a nanometre scale come onto the market. Of course, high performance cold field emission STEMs have now been in operation for about twenty years, but it is only in relatively few laboratories that special modification has permitted the performance of CBED experiments. Most notable amongst these pioneering projects is the work in Arizona by Cowley and Spence and, more recently, that in Cambridge by Rodenburg and McMullan.There are a large number of potential advantages of a high intensity, small diameter, focussed probe. We discuss first the advantages for probes larger than the projected unit cell of the crystal under investigation. In this situation we are able to perform CBED on local regions of good crystallinity. Zone axis patterns often contain information which is very sensitive to thickness changes as small as 5nm. In conventional CBED, with a lOnm source, it is very likely that the information will be degraded by thickness averaging within the illuminated area.

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