Abstract:(1) INTRODUCTION.THE refractive index of a protein solution is greater than that of pure water, and, according to the observations of Reiss [1904] and Robertson [1912], the difference between the refractions of the protein solution and the solvent is equal to the protein concentration in g. per 100 cc. of solution, multiplied by a constant. This constant is termed the specific refraction increment or the specific refraction of the protein.A critical account of the work of previous investigators on the refract… Show more
“…If sodium and potassium citrates are assumed to have the same molar tonicity, interpolation from the data of Heller and Paul (13) The specific refraction, k, is defined by equation 2. In addition to its dependence on the temperature, the wavelength, and the type of protein, k also varies with the nature of the buffer electrolytes due to the unequal distribution of the buffer ions between the two solutions when the latter are in a Donnan equilibrium (14). Moreover, owing to the presence of nitrogen-free constituents, such as lipids and carbohydrates, in many of the plasma proteins, a dry-weight determination of p, equation 2, yields a smaller value for k than a determination of protein nitrogen if the latter is multiplied by the conventional factor of 6.25.…”
“…If sodium and potassium citrates are assumed to have the same molar tonicity, interpolation from the data of Heller and Paul (13) The specific refraction, k, is defined by equation 2. In addition to its dependence on the temperature, the wavelength, and the type of protein, k also varies with the nature of the buffer electrolytes due to the unequal distribution of the buffer ions between the two solutions when the latter are in a Donnan equilibrium (14). Moreover, owing to the presence of nitrogen-free constituents, such as lipids and carbohydrates, in many of the plasma proteins, a dry-weight determination of p, equation 2, yields a smaller value for k than a determination of protein nitrogen if the latter is multiplied by the conventional factor of 6.25.…”
“…We develop a simple model that derives from the empirically well-established linear relationship between the change in refractive index of a protein or nucleic acid solution and their concentration or mass density. [25][26][27][28] This relationship was further validated by the work of Lee et al 29 and Popescu et al, 30 among others. Mathematically, it is described as…”
Section: Correction Model For Stain-induced Refractive Index Variationmentioning
Abstract. For any technique to be adopted into a clinical setting, it is imperative that it seamlessly integrates with well-established clinical diagnostic workflow. We recently developed an optical microscopy techniquespatial-domain low-coherence quantitative phase microscopy (SL-QPM) that can extract the refractive index of the cell nucleus from the standard histology specimens on glass slides prepared via standard clinical protocols. This technique has shown great potential in detecting cancer with a better sensitivity than conventional pathology. A major hurdle in the clinical translation of this technique is the intrinsic variation among staining agents used in histology specimens, which limits the accuracy of refractive index measurements of clinical samples. In this paper, we present a simple and easily generalizable method to remove the effect of variations in staining levels on nuclear refractive index obtained with SL-QPM. We illustrate the efficacy of our correction method by applying it to variously stained histology samples from animal model and clinical specimens. C 2011 Society of Photo-Optical Instrumentation Engineers (SPIE).
“…It has long been known that a molecule of ovalbumin, having a radius of 55.~ (Adair and Adair, 1940) unrolls into a surface fill of but 9.5A thickness (Astbury, Bell, Gorter, and van Ormondt, 1938). Some members of this group do it instantly (group B1) giving anomalous flow diagrams in the first instance, while others (group B~) require a considerable time to do so, and only give anomalous flow diagrams after the film has built itself up for half an hour or more.…”
Section: Discussionmentioning
confidence: 99%
“…Serum Globulin.--The globulin fraction of ox serum was prepared following the details in Adair and Robinson (1930), Elford and Ferry (1934), and the review of Cohn (1941). Repeated precipitation by half saturation with ammonium sulphate followed by dialysis through cellophane against weak phosphate buffer solution gave the euglobulin fraction, readily separable from the pseudoglobulins which remain unprecipitated in the supernatant liquid within the dialysis bag.…”
In the foregoing paper a description has been given of apparatus whereby the flow-birefringence and the relative viscosity of a protein solution may be measured and its anomalous viscosity assessed, careful distinction being made between effects due to the bulk phase and those due to the surface film at the air-water interface. We have now to turn to the more specific detailed results of the investigation of a number of proteins. 1
Beha~iour o/ProteinsTobacco Mosaic Disease Virus Nudeoprotein.--This plant virus protein, 2 (for full descriptions of which see Bawden, 1939;Bernal and Fankuchen, 1941) has already been subjected to measurements of viscosity and birefringence, in the work of Robinson (1939). The specimen used by us gave the flow-birefringenee curves seen in Fig. 1; allowing for differences in conditions (in our experiments 1.5 cm. column as against 21 cm.; 0.5 per cent as against 0.02 per cent concentration of virus; shear rate 13.1 as against 18.8; Robinson's rumple was more flow-birefringent than ours. In the viscosimeter it was interesting to find that under both low level (film) and flood level (bulk) conditions, the virus gives a strongly anomalous type of flow, see Figs. 2 and 3.) This probably means that the virus aggregates retain their anisometric shape when they enter into the formation of the surface film.The only difference is that the viscosity curve of 0.025 per cent virus for the bulk descends to its orientation plateau by about 20 R.p.,x. while that for the film does not do so until a speed of between 70 and 80 g.P.~, is attained. Orientation within the film must therefore be a good deal more difficult than oriental
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