Sensor for Distinguishing Liquid-Vapor Phases of Superfluid Helium

1960 ◽  
pp. 244-246
Author(s):  
D. Petrac ◽  
J. Gatewood ◽  
P. Mason
Keyword(s):  
Superfluid Helium ◽  
Liquid Vapor

High-Resolution Cryo-Electron Microscopy of Biological Macromolecules

1990 ◽  
Vol 48 (1) ◽  
pp. 126-127
Author(s):  
Yoshinori Fujiyoshi
Keyword(s):  
Electron Microscopy ◽  
High Resolution ◽  
Diffraction Pattern ◽  
Superfluid Helium ◽  
Copper Phthalocyanine ◽  
Optical Diffraction ◽  
Irradiation Damage ◽  
Biological Macromolecules ◽  
Cross Sectional ◽  
Instrumental Resolution

The resolution of direct images of biological macromolecules is normally restricted to far less than 0.3 nm. This is not due instrumental resolution, but irradiation damage. The damage to biological macromolecules may expect to be reduced when they are cooled to a very low temperature. We started to develop a new cryo-stage for a high resolution electron microscopy in 1983, and successfully constructed a superfluid helium stage for a 400 kV microscope by 1986, whereby chlorinated copper-phthalocyanine could be photographed to a resolution of 0.26 nm at a stage temperature of 1.5 K. We are continuing to develop the cryo-microscope and have developed a cryo-microscope equipped with a superfluid helium stage and new cryo-transfer device.The New cryo-microscope achieves not only improved resolution but also increased operational ease. The construction of the new super-fluid helium stage is shown in Fig. 1, where the cross sectional structure is shown parallel to an electron beam path. The capacities of LN2 tank, LHe tank and the pot are 1400 ml, 1200 ml and 3 ml, respectively. Their surfaces are placed with gold to minimize thermal radiation. Consumption rates of liquid nitrogen and liquid helium are 170 ml/hour and 140 ml/hour, respectively. The working time of this stage is more than 7 hours starting from full LN2 and LHe tanks. Instrumental resolution of our cryo-stage cooled to 4.2 K was confirmed to be 0.20 nm by an optical diffraction pattern from the image of a chlorinated copper-phthalocyanine crystal. The image and the optical diffraction pattern are shown in Fig. 2 a, b, respectively.

VISCOSITY OF NORMAL AND SUPERFLUID HELIUM THREE

1978 ◽  
Vol 39 (C6) ◽  
pp. C6-35-C6-36 ◽  
Author(s):  
J. M. Parpia ◽  
D. J. Sandiford ◽  
J. E. Berthold ◽  
J. D. Reppy
Keyword(s):  
Superfluid Helium ◽  
Helium Three

Mechanical experiments in superfluid helium

1994 ◽  
Vol 164 (12) ◽  
pp. 1278 ◽  
Author(s):  
H.E. Hall
Keyword(s):  
Superfluid Helium

Stability of an Interface in a Liquid-Vapor System

2002 ◽  
Vol 33 (3-4) ◽  
pp. 4
Author(s):  
S. N. Syromyatnikov ◽  
P. A. Pavlov
Keyword(s):  
Liquid Vapor

A Numerical Description of a Liquid-Vapor Interface Based on the Second Gradient Theory

1995 ◽  
Vol 22 (1) ◽  
pp. 1-14 ◽  
Author(s):  
Didier Jamet ◽  
Olivier Lebaigue ◽  
Jean-Marc Delhaye ◽  
N. Coutris
Keyword(s):  
Gradient Theory ◽  
Vapor Interface ◽  
Second Gradient ◽  
Liquid Vapor

Liquid-Vapor Phase-Change and Mixed Convection in a Porous Layer Discretely Heated

2006 ◽  
Vol 9 (7) ◽  
pp. 671-681 ◽  
Author(s):  
Mustapha Najjari ◽  
Sassi Ben Nasrallah
Keyword(s):  
Mixed Convection ◽  
Phase Change ◽  
Porous Layer ◽  
Vapor Phase ◽  
Liquid Vapor
Sign in / Sign up

Export Citation Format

Share Document