Effect of Temperature on the Gel Strength of Some Gulf Coast Drilling Muds

1938 ◽  
Vol 1 (03) ◽  
pp. 1-7
Author(s):  
B.I. Routh ◽  
B.C. Craft
Keyword(s):  
Gulf Coast ◽  
Gel Strength ◽  
Effect Of Temperature ◽  
Drilling Muds

scholarly journals The effect of temperature and time of extraction on the quality of Semi Refined Carrageenan (SRC)

2018 ◽  
Vol 154 ◽  
pp. 01034 ◽  
Author(s):  
Heri Heriyanto ◽  
Indar Kustiningsih ◽  
Denni Kartika Sari
Keyword(s):  
Food Industry ◽  
Gel Strength ◽  
Effect Of Temperature ◽  
Pet Food ◽  
Sulfate Content ◽  
Cooking Process ◽  
Cooking Temperature ◽  
Kappa Carrageenan ◽  
Carrageenan Quality

Euchema cottonii is a good source of kappa-carrageenan and can be found cultivated in the Indonesia coastal areas in which one of them is in Banten Province. Carrageenans have many applications and are utilized in human food and pet-food industry. Carrageenans are also utilized in non-food industry such as pharmaceuticals, cosmetics, printing and textile formulations. Hence, the present study features on the cooking process cooking time and cooking temperature. The effects of these parameters on carrageenan quality such as gel viscosity and gel strength were studied. The process of extraction of carrageenan was conducted with variations temperature: 60, 70, and 80 °C and the variation of time: 1, 2, and 3 hours. Alkaline substance used was KOH with 8% concentration and the ratio of solvent to dry seaweed 8:1. From the present investigation, it was observed that SRC extraction reached the best condition at temperature 70 °C for 2 hours with the value of yield 30.20%, 5.90% moisture content, 18.34% ash content, sulfate content of 6.94%, viscosity of 190 cP, and the gel strength 714.45 g / cm2. The treatment of temperature and extraction time significantly affected the quality of the SRC yield parameter, viscosity and gel strength.

scholarly journals Rheology of Yanang solution: Effect of temperature, pH and divalent cation

2014 ◽  
Vol 17 (1) ◽  
pp. 87-93
Author(s):  
Vi Ngoc Ha Vu ◽  
Viet Bao Nguyen ◽  
Long Tien Vu
Keyword(s):  
Low Temperature ◽  
East Asia ◽  
Rheological Properties ◽  
Divalent Cation ◽  
Shear Thinning ◽  
Gel Strength ◽  
Effect Of Temperature ◽  
South East Asia ◽  
The Impact

The main objective of this work was to study rheological properties of Yanang (Tiliacora triandra) solution; a kind of food that derived from plants is being widely used in many countries in South East Asia and East Asia. Experiments were conducted to evaluate the impact of temperature on the viscosity and then build rheological curves of products. The results showed that viscosity of Yanang solutions changes with temperature in the shear - thinning models. These solutions formed gel at low temperature and gel strength can be improved by adjusting pH and adding Ca2+ due to the presence of uronic axit residues on the backbone of Yanang gums.

Effects of Temperature on the Viscosity of Some Gulf Coast Drilling Muds

1933 ◽  
Vol 103 (01) ◽  
pp. 112-115 ◽  
Author(s):  
B.C. Craft ◽  
J.D. Exner
Keyword(s):  
Gulf Coast ◽  
Effects Of Temperature ◽  
Drilling Muds

Nucleation of Disorder in Fe3Al Alloys

1967 ◽  
Vol 25 ◽  
pp. 312-313
Author(s):  
P. R. Swann ◽  
W. R. Duff ◽  
R. M. Fisher
Keyword(s):  
Electron Microscopy ◽  
Transmission Electron Microscopy ◽  
Annealing Temperature ◽  
Antiphase Domain ◽  
Effect Of Temperature ◽  
Domain Structures ◽  
Transmission Electron ◽  
Domain Boundaries ◽  
Higher Temperature ◽  
The One

Recently we have investigated the phase equilibria and antiphase domain structures of Fe-Al alloys containing from 18 to 50 at.% Al by transmission electron microscopy and Mössbauer techniques. This study has revealed that none of the published phase diagrams are correct, although the one proposed by Rimlinger agrees most closely with our results to be published separately. In this paper observations by transmission electron microscopy relating to the nucleation of disorder in Fe-24% Al will be described. Figure 1 shows the structure after heating this alloy to 776.6°C and quenching. The white areas are B2 micro-domains corresponding to regions of disorder which form at the annealing temperature and re-order during the quench. By examining specimens heated in a temperature gradient of 2°C/cm it is possible to determine the effect of temperature on the disordering reaction very precisely. It was found that disorder begins at existing antiphase domain boundaries but that at a slightly higher temperature (1°C) it also occurs by homogeneous nucleation within the domains. A small (∼ .01°C) further increase in temperature caused these micro-domains to completely fill the specimen.

The effect of temperature on high-resolution TEM image contrast

1995 ◽  
Vol 53 ◽  
pp. 640-641
Author(s):  
T. Geipel ◽  
W. Mader ◽  
P. Pirouz
Keyword(s):  
Form Factor ◽  
Inelastic Scattering ◽  
Accurate Method ◽  
Waller Factor ◽  
Effect Of Temperature ◽  
Specimen Thickness ◽  
Influence Of Temperature ◽  
Debye Waller Factor ◽  
Influence Of Temperature On ◽  
Atomic Form Factor

Temperature affects both elastic and inelastic scattering of electrons in a crystal. The Debye-Waller factor, B, describes the influence of temperature on the elastic scattering of electrons, whereas the imaginary part of the (complex) atomic form factor, fc = fr + ifi, describes the influence of temperature on the inelastic scattering of electrons (i.e. absorption). In HRTEM simulations, two possible ways to include absorption are: (i) an approximate method in which absorption is described by a phenomenological constant, μ, i.e. fi; - μfr, with the real part of the atomic form factor, fr, obtained from Hartree-Fock calculations, (ii) a more accurate method in which the absorptive components, fi of the atomic form factor are explicitly calculated. In this contribution, the inclusion of both the Debye-Waller factor and absorption on HRTEM images of a (Oll)-oriented GaAs crystal are presented (using the EMS software.Fig. 1 shows the the amplitudes and phases of the dominant 111 beams as a function of the specimen thickness, t, for the cases when μ = 0 (i.e. no absorption, solid line) and μ = 0.1 (with absorption, dashed line).

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