F52. A new method to calculate logarithmic damping factor in damped oscillation type rheometer

Biorheology ◽  
1995 ◽  
Vol 32 (2-3) ◽  
pp. 246-246
Author(s):  
Z WANG ◽  
X ZHENG ◽  
Y WU ◽  
E ZHENG ◽  
C PENG
1968 ◽  
Vol 3 (1) ◽  
pp. 23-32 ◽  
Author(s):  
K R Rushton

The analysis of the static deformation of elastic plates is achieved by studying the dynamic problem of the damped oscillation of the plate and arranging that the oscillations are rapidly reduced to zero by a suitable choice of the damping factor. This damped-wave equation, when written in an explicit finite-difference form, can readily be solved on a digital computer. The computer programme has been designed to determine automatically the critical damping factor for a rectangular plate carrying any load distribution and with any combination of edge conditions. The extension of the method to include elastic foundations is also described.


1986 ◽  
Vol 14 (3) ◽  
pp. 143-146
Author(s):  
Tadayoshi MURATA ◽  
Munehiro DATE ◽  
Makoto KAIBARA

2014 ◽  
Vol 136 (9) ◽  
Author(s):  
Sourav Roy ◽  
L. K. Mandal ◽  
Manoranjan Khan ◽  
M. R. Gupta

The combined effect of viscosity, surface tension, and the compressibility on the nonlinear growth rate of Rayleigh-Taylor (RT) instability has been investigated. For the incompressible case, it is seen that both viscosity and surface tension have a retarding effect on RT bubble growth for the interface perturbation wave number having a value less than three times of a critical value (kc=(ρh-ρl)g/T, T is the surface tension). For the value of wave number greater than three times of the critical value, the RT induced unstable interface is stabilized through damped nonlinear oscillation. In the absence of surface tension and viscosity, the compressibility has both a stabilizing and destabilizing effect on RTI bubble growth. The presence of surface tension and viscosity reduces the growth rate. Above a certain wave number, the perturbed interface exhibits damped oscillation. The damping factor increases with increasing kinematic viscosity of the heavier fluid and the saturation value of the damped oscillation depends on the surface tension of the perturbed fluid interface and interface perturbation wave number. An approximate expression for asymptotic bubble velocity considering only the lighter fluid as a compressible one is presented here. The numerical results describing the dynamics of the bubble are represented in diagrams.


1986 ◽  
Vol 14 (3) ◽  
pp. 140-142
Author(s):  
Makoto KAIBARA ◽  
Munehiro DATE

Author(s):  
C. C. Clawson ◽  
L. W. Anderson ◽  
R. A. Good

Investigations which require electron microscope examination of a few specific areas of non-homogeneous tissues make random sampling of small blocks an inefficient and unrewarding procedure. Therefore, several investigators have devised methods which allow obtaining sample blocks for electron microscopy from region of tissue previously identified by light microscopy of present here techniques which make possible: 1) sampling tissue for electron microscopy from selected areas previously identified by light microscopy of relatively large pieces of tissue; 2) dehydration and embedding large numbers of individually identified blocks while keeping each one separate; 3) a new method of maintaining specific orientation of blocks during embedding; 4) special light microscopic staining or fluorescent procedures and electron microscopy on immediately adjacent small areas of tissue.


1960 ◽  
Vol 23 ◽  
pp. 227-232 ◽  
Author(s):  
P WEST ◽  
G LYLES
Keyword(s):  

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