scholarly journals The absolute viscosity of protoplasm

PROTOPLASMA ◽  
1927 ◽  
Vol 2 (1) ◽  
pp. 381-381 ◽  
Keyword(s):  
Absolute Viscosity ◽  
The Absolute

scholarly journals Note on the Standard of Relative Viscosity, and on “Negative Viscosity.”

1906 ◽  
Vol 25 (1) ◽  
pp. 227-230 ◽  
Author(s):  
W. W. Taylor
Keyword(s):  
Capillary Tube ◽  
Relative Viscosity ◽  
Absolute Viscosity ◽  
Flow Through ◽  
The Absolute ◽  
Negative Viscosity ◽  
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The absolute viscosity calculated from the formula(where p = the pressure, t the time, r the radius, l the length of capillary, and v the volume of liquid), which connects the viscosity of a liquid with the rate of flow through a long capillary tube, is not often made use of, mainly on account of the difficulty of accurately determining some of the constants (r in particular).

The absolute viscosity of protoplasm

1926 ◽  
Vol 44 (1) ◽  
pp. 255-278 ◽  
Author(s):  
L. V. Heilbrunn
Keyword(s):  
Absolute Viscosity ◽  
The Absolute

The absolute viscosity of some lead-thallium alloys

1979 ◽  
Vol 64 (1) ◽  
pp. 135-143 ◽  
Author(s):  
Frank A Kanda ◽  
John A Domingue
Keyword(s):  
Absolute Viscosity ◽  
The Absolute ◽  
Thallium Alloys

Absolute Viscosity of CCl2F2 and CHCl2F

1970 ◽  
Vol 12 (2) ◽  
pp. 135-142 ◽  
Author(s):  
B. Latto ◽  
A. J. Al-Saloum
Keyword(s):  
Maximum Error ◽  
Vapour Phase ◽  
Maximum Energy ◽  
Absolute Temperature ◽  
Maximum Deviation ◽  
Theory Approach ◽  
Fourth Degree ◽  
Temperature Range ◽  
Absolute Viscosity ◽  
The Absolute

The absolute viscosity at atmospheric pressure was determined experimentally for the vapour phase of two halogenated hydrocarbon compounds, refrigerants R12 (CCl2F2) and R22 (CHCl2F) in the general temperature range −39·7° to 91·8°C. The maximum error of the data is believed to be ±3 per cent. Comparison with previous secondary measurements on the same compounds reveals that the maximum deviation of previous measurements are +5 per cent and −6 per cent for R12 and R22, respectively, over the common temperature range. The data obtained in this work and by others were correlated using third and fourth degree polynomials, a power function of the absolute temperature, and a collision theory approach, which yielded values for the reduced dipole energy, the velocity collision diameter, and the maximum energy of attraction for the molecules. Comparison of the data with that predicted by simple kinetic theory has been made.

Errata

1983 ◽  
Vol 38 (1) ◽  
pp. 146-146
Keyword(s):  
Fluid Mechanics ◽  
Absolute Viscosity ◽  
The Absolute

A. A. Mills, Newton’s Water Clocks and the Fluid Mechanics of Clepsydrae Notes & Records R. Soc. Lond. , 37 (1982), 35—61 (i) p. 50, penultimate line. Replace Napier by Navier. (ii) p. 51, Fig. 7. The line denoting variation of the absolute viscosity of mercury with temperature is incorrect. It should be replaced by a line (straight within the limits of the diagram) joining the points: o°, 16-8 millipoise 40°, 14*5 millipoise (iii) p. 52, second paragraph. The first phrase should be ignored, although it is true for the kinematic viscosity of mercury.

New Method for Measuring the Absolute Viscosity of Liquid Helium II

1956 ◽  
Vol 102 (3) ◽  
pp. 607-613 ◽  
Author(s):  
Henry H. Kolm ◽  
Melvin A. Herlin
Keyword(s):  
Liquid Helium ◽  
New Method ◽  
Helium Ii ◽  
Absolute Viscosity ◽  
The Absolute
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