On the Analysis of Concentration versus Reciprocal Temperature Curves in Semiconductors

1992 ◽  
Vol 133 (2) ◽  
pp. K65-K67
Author(s):  
B. Pödör
Keyword(s):  
Reciprocal Temperature

scholarly journals Effects of a temperature-sensitiveMinutemutation on gene expression inDrosophila melanogaster

1984 ◽  
Vol 43 (3) ◽  
pp. 257-275 ◽  
Author(s):  
Donald A. R. Sinclair ◽  
Thomas A. Grigliatti ◽  
Thomas C. Kaufman
Keyword(s):  
Gene Expression ◽  
Temperature Shift ◽  
Temperature Sensitive ◽  
Restrictive Temperature ◽  
Gene Products ◽  
The Past ◽  
Reciprocal Temperature ◽  
Sex Comb ◽  
Mutant Phenotypes

SUMMARYMinute(M) lesions exhibit a striking propensity for interacting with many different mutations. In the past, few attempts have been made to explain these diverse phenomena. This study describes a variety of temperature-sensitive (ts) interactions exhibited by the ts third chromosomeMinutemutationM(3)LS4Q-III(Q-III). Most of these interactions (i.e. those involvingvg, cp, Dl, DfdorLy) reflectQ-III-induced enhancement of the respective mutant phenotypes at the restrictive temperature. However,Q-IIIalso suppresses the extra-sex-comb phenotypes ofPcandMscat 29 °C and evokes lethal and bristle traits when combined withJ34eat the restrictive temperature. All of these interactions are characteristic of non-tsMinutelesions and thus they appear to be correlated with general physiological perturbations associated with theMsyndrome. In addition, our findings show that mutations that affect ribosome production and/or function, namelysu(f)ts67gandbbts−1, exhibit interactions comparable to those elicited byQ-III. Hence, in accordance with previous findings, we argue that most of theQ-IIIinteractions can be attributed to reduced translational capacity at the restrictive temperature. Finally, reciprocal temperature shift studies were used to delineate TSPs for interactions betweenQ-IIIandvg(mid to late second instar),cp(about mid-third instar),Dfd(early third instar) andDl(late second to mid third instar). We believe that these TSPs represent developmental intervals during which the respective gene products are utilized.

scholarly journals GENETIC AND DEVELOPMENTAL ANALYSIS OF A TEMPERATURE-SENSITIVE MINUTE MUTATION OF DROSOPHILA MELANOGASTER

Genetics ◽  
1981 ◽  
Vol 97 (3-4) ◽  
pp. 581-606 ◽  
Author(s):  
Donald A R Sinclair ◽  
David T Suzuki ◽  
Thomas A Grigliatti
Keyword(s):  
Larval Instar ◽  
Temperature Shift ◽  
Heat Pulse ◽  
Sensitive Period ◽  
Temperature Sensitive ◽  
Direct Effects ◽  
First Instar ◽  
Reciprocal Temperature ◽  
Morphological Defects ◽  
Developmental Analysis

ABSTRACT A temperature-sensitive (ts) third chromosome Minute (M) mutation, designated Q-III, has been recovered and characterized. Q-III heterozygotes raised at 29" exhibit all of the dominant traits of M mutants including small bristles, rough eyes, prolonged development, reduced viability 2nd interactions with several unrelated mutations. Q-III homozygotes raised at 29° are lethal; death occurs primarily during the first larval instar. When raised at 22°, Q-Ill heterozygotes are phenotypically normal and Q-III homozygotes display moderate Mtraits. In addition, Q-IIIelicits ts sterility and maternal-effect lethality. As it true of Mlesions, the dominant traits of Q-111 are not expressed in triploid females raised at 29°. Complementation tests suggest that Q-III is a ts allele of M(3)LS4, which is located in 3L near the centromere.——Reciprocal temperature-shift experiments revealed that the temperature-sensitive period (TSP) of Q-111 lethality is polyphasic, extending from the first instar to the latter half of pupation. Heat-pulse experiments further resolved this into two post-embryonic TSPs: one occurring during the latter half of the second larval instar, and the other extending from the larval/pupal boundary to the second half of pupation. In addition, heat pulses elicited a large number of striking adult phenotypes in Q-III individuals. These included pattern alterations such as deficiencies and duplications and cther morphological defects in structures produced by the eye-antennal, leg, wing and genital imaginal discs and the abdominal histoblasts. Each defect or pattern alteration is associated with a specific TSP during development.——We favor the interpretation that most of the major Q-III defects, particularly the structural duplications and deficiencies, result from temperature-induced cell death in mitotically active imaginal anlagen, while the small macrochaete phene probably results from the direct effects of Q-III on bristle synthesis. The hypothesis that the Q-III locus specifices a component required for protein synthesis is discussed, and it is concluded that this hypothesis can account for the pleiotropy of Q-III, and that perhaps it can be extended to M loci in general.

scholarly journals DETERMINATION OF THE ORDER OF GENE FUNCTION IN THE YEAST NUCLEAR DIVISION PATHWAY USING cs AND ts MUTANTS

Genetics ◽  
1982 ◽  
Vol 100 (4) ◽  
pp. 565-577
Author(s):  
Don Moir ◽  
David Botstein
Keyword(s):  
Gene Function ◽  
Nuclear Division ◽  
Temperature Shift ◽  
Yeast Saccharomyces Cerevisiae ◽  
Lethal Mutations ◽  
Reciprocal Temperature ◽  
Cold Sensitive ◽  
Cell Cycle Pathway ◽  
Mutant Phenotypes

ABSTRACT Cold-sensitive (cs) and heat-sensitive (ts) conditional-lethal mutations that affect specifically the cell division cycle of budding yeast (Saccharomyces cerevisiae) were used to determine the order of gene function. Reciprocal temperature-shift experiments using cs-ts double mutants revealed a detailed order of function among genes whose execution points and mutant phenotypes are very similar. The data suggest that the nuclear branch of the overall cell-cycle pathway itself contains at least one branch.

Estimation of Glass Transition Temperatures from Gas Chromatographic Studies on Polymers

1973 ◽  
Vol 46 (1) ◽  
pp. 1-6 ◽  
Author(s):  
A. Lavoie ◽  
J. E. Guillet
Keyword(s):  
Glass Transition ◽  
Retention Volume ◽  
Polymeric Materials ◽  
Similar Data ◽  
Transition Temperatures ◽  
Gas Chromatograph ◽  
Specific Retention Volume ◽  
Glass Transition Temperatures ◽  
Reciprocal Temperature ◽  
Specific Retention

Abstract In a recent communication, Smidsrød and Guillet showed that thermodynamic data on the interactions between poly (isopropylacrylamide) and various gaseous solutes could be obtained by making the polymer the stationary phase in a gas Chromatograph. It was also shown that if a solute was used which was a nonsolvent for the polymer, a plot of the logarithm of the specific retention volume as a function of reciprocal temperature showed a marked inflection at a temperature close to the glass transition temperature for the polymer. We wish to report similar data on several additional polymers which lead us to believe that the phenomenon is a general one and may be used to obtain an estimate of transition temperatures for a variety of polymeric materials.

Kernresonanzuntersuchung der Molekülrotation in festem Benzol: T1-Spektroskopie / Nuclear Magnetic Resonance Investigation of Molecular Rotation in Solid Benzene: T1-spectroscopy

1974 ◽  
Vol 29 (11) ◽  
pp. 1660-1670 ◽  
Author(s):  
J. Wendt ◽  
F. Noack
Keyword(s):  
Activation Energy ◽  
Gear Wheel ◽  
Larmor Frequency ◽  
Molecular Rotation ◽  
Frequency Range ◽  
Temperature Dependent ◽  
Resonance Investigation ◽  
Reciprocal Temperature ◽  
Nuclear Magnetic Resonance Investigation ◽  
Magnetic Resonance Investigation

We have extended Haeberlen’s and Maier’s NMR investigation of the molecular rotation in solid polycrystalline benzene (C6H6), performed in 1967 in the Larmor frequency range from 88 MHz to 22 MHz, to lower frequencies down to 4.4 MHz. In some cases monocrystalline samples were also studied. The extensive data show that the presently accepted model of purely uncorrected rotations of the benzene molecules around their sixfold axis has to be rejected. Instead, two results found, namely- a slight increase of the rotational activation energy when approaching the melting point of benzene and- the width of the T1 relaxation minima as a function of the reciprocal temperature suggest an additional relevance of correlated molecular motions, like e.g. the ‘gear-wheel mechanism’ first proposed by Cox. By appropriate modifications of Haeberlen’s theory, i.e. by assuming a rate equation with temperature dependent activation energy and by emphasizing the effect of simultaneous rotations of neighbouring rings compared with the purely statistical, uncorrelated case, we succeeded to describe the considered T1 measurements quantitatively.

Reactions with half-lives of several years

1964 ◽  
Vol 17 (4) ◽  
pp. 406 ◽  
Author(s):  
GA Bottomley ◽  
GL Nyberg
Keyword(s):  
Activation Energy ◽  
Thermal Decomposition ◽  
Gas Phase ◽  
Virial Coefficient ◽  
Energy Equation ◽  
Second Virial Coefficient ◽  
First Order ◽  
First Order Kinetics ◽  
Reciprocal Temperature ◽  
Temperature Activation

The gas-phase thermal decomposition of dimethyldiazirine, (CH3)2CN2, at very slow rates has been investigated using precision gas-volumetric techniques previously applied to second virial coefficient studies. At 50-70� the first-order kinetics correspond to half-lives about 0.3-3.0 years. The present results, together with data obtained by other workers using conventional apparatus at 124-174�, fit a single log rate-reciprocal temperature activation energy equation.

Comparison of Two Methods of Calculation of Activation Energy for some Chosen Industrial Steels after its Oxidation at High-Temperatures in Air

2005 ◽  
Vol 237-240 ◽  
pp. 979-984
Author(s):  
Krzysztof Adamaszek ◽  
Zbigniew Jurasz
Keyword(s):  
Activation Energy ◽  
Parabolic Rate Constant ◽  
Bearing Steel ◽  
Chamber Furnace ◽  
Parabolic Law ◽  
Methods Of Calculation ◽  
Reciprocal Temperature ◽  
Kinetics Of ◽  
Energy Activation ◽  
Good Agreement

In this work it will be presented the results of calculation of energy activation Q of selected industrial steels (e.g. grade 55 - carbon steel, LH15 – bearing steel, H10S2M, 4H14N14W2M and 50H21G9N4 valve steels) according to Polish Norm by two methods. In the first method the calculations of Q are based on the dependence of value of parabolic growth rate constants kp in function of reciprocal temperature. The second method is based on the calculated parameters, which allow to determine the value of Q for examined steels by using value of Q for pure iron, taken from literature data, and the particular values of mass concentrations of elements in oxidised steels. The growth kinetics of layers were almost according to parabolic law. The values of parabolic rate constant kp were calculated on the basis of measurements of thickness of oxide layers. To the experiment the cylindrical specimens were used. The isothermal process of oxidation was conducted in chamber furnace at 1100, 1060, 1020, 980 and 940°C in the air. Time of oxidation various from 3 till 1303.5 hrs. The comparison of obtained results of activation energy Q for mentioned methods of each individual examined steels gives a good agreement.

Influence of Data Scattering on Estimation of 100,000 hrs Creep Rupture Strength of Alloy 617 at 700 °C by Larson–Miller Method

2016 ◽  
Vol 139 (1) ◽  
Author(s):  
Fujio Abe ◽  
M. Tabuchi ◽  
M. Hayakawa
Keyword(s):  
Regression Analysis ◽  
Rupture Strength ◽  
Large Data ◽  
Creep Rupture ◽  
Creep Rupture Strength ◽  
Alloy 617 ◽  
Time To Rupture ◽  
Reciprocal Temperature ◽  
Rupture Data ◽  
C Value

The 100,000 hrs creep rupture strength of Alloy 617 at 700 °C is estimated by Larson–Miller method using the rupture data of longer duration than 500 hrs in the temperature range between 593 and 816 °C, corresponding to 700 ± 100 °C. The maximum time to rupture was 40,126.7 hrs. The rupture data exhibit large scattering, especially at 760 °C. After eliminating the shorter time to rupture data at 760 °C, the regression analysis gives us the Larson–Miller constant C = 12.70 and the 100,000 hrs creep rupture strength of 100 MPa at 700 °C, by Swindeman program. The present regression analysis underestimates the constant C and 100,000 hrs creep rupture strength. The linear extrapolation of log tr versus reciprocal temperature 1/T plots to 1/T = 0 gives us an average C value of Cav = 18.5, which is much larger than the constant C of 12.70 obtained by the Swindeman program. It is concluded that the origin of underestimation of the constant C and corresponding 100,000 hrs creep rupture strength is large data scattering. Using an appropriate constant C of 18.45, the 100,000 hrs creep rupture strength at 700 °C is estimated to be 123 MPa. Using the rupture data including the shorter time to rupture data at 760 °C and using C = 18.45, the 100,000 hrs creep rupture strength at 700 °C is estimated to be 116 MPa.

Sign in / Sign up

Export Citation Format

Share Document