Measurement of Dispersion of the Refractive Index of Microscopic Volumes of the BSA Aqueous Solution Using an Interference Microscope

Author(s):  
G. V. Maksimov ◽  
A. D. Ivanov ◽  
A. A. Samoilenko ◽  
A. A. Golopolosov ◽  
G. G. Levin
1957 ◽  
Vol s3-98 (44) ◽  
pp. 435-454
Author(s):  
K.F. A. ROSS

The difficulties involved in the direct measurement, by eyepiece-micrometer or from photomicrographs, of small microscopic objects such as living bacteria are discussed. The accuracy with which this can be done is limited by the numerical aperture of the optical system and the wavelength of light used. With visible light it is scarcely possible to determine the dimensions of an object more accurately than to the nearest 0.4µ. It also seems probable, from the nature of the diffraction pattern at the edges of images of objects of circular cross-section such as bacteria, that direct measurement of the width of the image will tend to give an underestimate of the true width of the object. An interference microscope enables thickness measurements to be made that are not subject to these particular limitations, because with it, the phase-change in the light passing through the middle of a bacterium can be measured very accurately. This phase-change is proportional to the product of the refractive index of the bacterium minus that of the mounting medium, and its true thickness. Two methods were used to determine the mean thickness of the living bacilli in a number of different cultures of Lactobacillus bulgaricus. With the first, the mean refractive index of the bacilli was measured directly by the method of immersion refractometry first used by Barer and Ross (1952), and phase-change measurements were made on the bacilli mounted in dilute saline. Their mean thickness was calculated from these measurements. With the second method, phase-change measurements were made on the bacilli mounted in saline and also mounted in protein solutions with refractive indices ranging from 1.365 to 1.376; and, from these, both their mean thickness and their mean refractive index were calculated. The phase-change measurements were made with a Smith interference microscope and half-shade eyepiece (manufactured by Messrs. Charles Baker). The values for the mean thickness of the living L. bulgaricus from 14 different cultures obtained by the first method ranged from 1·13 µ to 1·23 µ; and those from 9 different cultures obtained by the second method ranged from 1·02 µ to 1·14 µ. The mean refractive indices of the latter calculated by the second method agreed very closely with that obtained by immersion refractometry, and differed by a maximum of 0.009 in all the cultures measured. It therefore seems unlikely that the mean thickness measurements obtained by either method are wrong by more than about ±0.1 µ.


2007 ◽  
Vol 16 (03) ◽  
pp. 359-366 ◽  
Author(s):  
AHMAD Y. NOORALDEEN ◽  
A. N. DHINAA ◽  
P. K. PALANISAMY

Nonlinear optical (NLO) properties of the aqueous solution of Acid Orange 10 dye have been studied using the closed aperture and open aperture Z-scan technique at different concentrations and various powers of Ar+laser at 488 nm wavelength. The nonlinear refractive index (n2) shows negative nonlinearity for all concentrations studied, and it is measured to be -13.5 × 10-9cm2/ W at 0.05 mM concentration. Moreover, the nonlinear refractive index is found to vary with intensity and concentration. The nonlinear absorption coefficient (β) is measured to be -3.8 × 10-4cm/W . Optical limiting behavior has been demonstrated for this dye. These results show that Acid Orange 10 dye has potential applications in nonlinear optics.


1960 ◽  
Vol s3-101 (54) ◽  
pp. 223-239
Author(s):  
K.F. A. ROSS ◽  
W.G. B. CASSELMAN

Living muscle-fibres from freshly killed mice were mounted in isotonic saline / protein media and examined with a Smith interference microscope, usually with a white light-source. When the A or I bands near the edge of a fibre were observed to match the colour of the background field, their refractive indices were close to that of the mounting medium; although it is extremely probable that diffraction at the edges of the adjacent unmatched bands affected their apparent match, so that they were not exactly of this refractive index. Matched A bands were distinguished from matched I bands by examining them in plane-polarized light, by rotating the preparation through a right angle under the interference microscope to display their birefringence, and from the colour of the unmatched bands when the fringe system of the microscope was left unaltered. In any one fibre, the refractive indices of the A-band regions were always higher than that of the I-band regions. The H bands had lower refractive indices than the A bands, and the Z bands higher than the I bands, but these were both too narrow to be matched satisfactorily by this method. The refractive indices of the solutions in which matched I bands were found ranged from 1.358 to 1.363, and those in which matched A bands were found from 1.360 to 1.366. The mean refractive index of the A and I bands was very close to 1.363, which is equivalent to a total solid content of 16% w/v. These findings are in good general agreement with those of H. Huxley and Hanson (1957) and Bennett (1955), who measured the distribution of solid material in isolated glycerinated mammalian myofibrils; but the difference between the refractive indices of the A- and I-band regions of the living fibres appeared to be very much less. Only part of this discrepancy can be accounted for by the presence of non-fibrillar solid material, because the total amount of this is extremely unlikely to exceed 50% of the total myofibrillar fibrous protein. It therefore seems probable that, because of the diffraction from the unmatched bands, the true refractive indices of the A bands were higher than those of the solutions in which they appeared matched, and those of the I bands were correspondingly lower than those of the solutions in which they appeared matched. The maximum error involved here (when the sarcomere interval was approximately 2.5 µ) can be quantified from independent estimations of the non-fibrillar material in whole muscle (Szent-Györgyi and others, 1955; Hanson and H. Huxley, 1957); and from this it seems highly probable that the refractive indices of the I bands were not lower than 1.350 (equivalent to a solid content of 9% w/v), and those of the A bands were not higher than 1.375 (equivalent to a solid content of 33% w/v).


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