Distinct temperature changes between north and south sides of central–eastern Himalayas since 1970s

2019 ◽  
Vol 40 (9) ◽  
pp. 4300-4308
Author(s):  
Siyu Yue ◽  
Kun Yang ◽  
Hui Lu ◽  
Yingying Chen ◽  
Shankar Sharma ◽  
...  
Keyword(s):  
Eastern Himalayas ◽  
Temperature Changes ◽  
Central Eastern ◽  
North And South ◽  
Distinct Temperature

scholarly journals PSIII-10 Body temperature changes in piglets anesthetized for castration during the recovery phase

2019 ◽  
Vol 97 (Supplement_3) ◽  
pp. 191-192
Author(s):  
Simone M Schmid ◽  
Jason J Hayer ◽  
Celine Heinemann ◽  
Julia Steinhoff-Wagner
Keyword(s):  
Body Temperature ◽  
Linear Models ◽  
Recovery Phase ◽  
Temperature Changes ◽  
Prolonged Recovery ◽  
Life Threatening ◽  
Animal Number ◽  
Infrared Lamps ◽  
Distinct Temperature ◽  
Skin Temperatures

Abstract In several countries, an application of general anesthesia for pain prevention during castration is discussed. A disadvantage is the prolonged recovery phase, accompanied by severe body temperature drops in piglets. Aim of this study was to investigate effects on body temperature during recovery after anesthesia. Piglets were anesthetized, castrated and placed in boxes (0.24m2) for 4h. Before, 2 and 4h after the application (0.3ml ketamine+azaperone/kg BW), rectal temperatures (RT) and skin temperatures behind the ear (ST) were measured. In a first trial, impacts of infrared lamp (250W, 50-55cm height) and number of animals per box (3 vs 6) were analyzed (n = 30). In a complementary trial, infrared lamps’ height (60 vs 70cm) and piglet age were varied (n = 27) and temperatures measured half-hourly. Differences were estimated in linear models (SAS® 9.4). Mean RT before anesthesia was 39.1±0.4°C with ranges of less than 1.9°C. After 2h, mean RT in lamp-warmed piglets increased to 40.8°C (P < 0.01), whereas in absence of lamps RT dropped to 37.3 (P < 0.001), with significant differences between groups (P < 0.001). To prevent life-threatening cooling, piglets with RT as minimal as 33.5°C were warmed immediately, so that their mean RT after 4h was not different from initial temperatures. Animal number per box caused no differences. Variation between individual RT was up to 8.2°C at 2h (first trial). Means in the second trial did not differ, but variation pattern of individual temperatures was highest after 1h (6.1°C), indicating that individual differences regarding anesthetics or external factors might occur. When lamps hung lower ST were higher after 3h (P < 0.05) and 4h (P < 0.01). RT and ST were dependent on age after 0.5h (P < 0,05, respectively) and tendentious at 1h and 2h, indicating that older piglets can rely on more distinct temperature regulation abilities and use endogenous energy resources to regain homeostasis.

scholarly journals TEMPERATURE CHANGES IN NORTH AND SOUTH CAROLINA

1938 ◽  
Vol 66 (3) ◽  
pp. 70-73
Author(s):  
EARL C. THOM
Keyword(s):  
South Carolina ◽  
Temperature Changes ◽  
North And South

Cryo-TEM of amphiphilic polymer and amphiphile/polymer solutions

1993 ◽  
Vol 51 ◽  
pp. 876-877
Author(s):  
Yeshayahu Talmon
Keyword(s):  
Microstructural Characterization ◽  
Building Blocks ◽  
Quantitative Information ◽  
Physical Models ◽  
Specimen Preparation ◽  
Time Resolved ◽  
Temperature Changes ◽  
Temperature And Humidity ◽  
Microstructured Fluids ◽  
Air Streams

To achieve complete microstructural characterization of self-aggregating systems, one needs direct images in addition to quantitative information from non-imaging, e.g., scattering or Theological measurements, techniques. Cryo-TEM enables us to image fluid microstructures at better than one nanometer resolution, with minimal specimen preparation artifacts. Direct images are used to determine the “building blocks” of the fluid microstructure; these are used to build reliable physical models with which quantitative information from techniques such as small-angle x-ray or neutron scattering can be analyzed.To prepare vitrified specimens of microstructured fluids, we have developed the Controlled Environment Vitrification System (CEVS), that enables us to prepare samples under controlled temperature and humidity conditions, thus minimizing microstructural rearrangement due to volatile evaporation or temperature changes. The CEVS may be used to trigger on-the-grid processes to induce formation of new phases, or to study intermediate, transient structures during change of phase (“time-resolved cryo-TEM”). Recently we have developed a new CEVS, where temperature and humidity are controlled by continuous flow of a mixture of humidified and dry air streams.

Author response for "Geological and geophysical differences between the north and south sections of the Yap trench‐arc system and their relationship with Caroline Ridge subduction"

2020 ◽  
Author(s):  
Cheng‐Long Xia ◽  
Yan‐Peng Zheng ◽  
Bao‐Hua Liu ◽  
Qing‐Feng Hua ◽  
Kai Liu ◽  
...  
Keyword(s):  
Author Response ◽  
Ridge Subduction ◽  
The North ◽  
North And South

North and South Korea team up to tackle TB and malaria

Nature ◽  
2018 ◽  
Author(s):  
Mark Zastrow
Keyword(s):  
South Korea ◽  
North And South

Application of pyrometer and standard sample to determine surface temperature of studied materials

2019 ◽  
pp. 9-13
Author(s):  
V.Ya. Mendeleyev ◽  
V.A. Petrov ◽  
A.V. Yashin ◽  
A.I. Vangonen ◽  
O.K. Taganov
Keyword(s):  
Composite Material ◽  
Surface Temperature ◽  
Relative Error ◽  
Wavelength Range ◽  
Standard Sample ◽  
A Priori ◽  
Temperature Changes ◽  
Surface Temperatures ◽  
Relative Errors ◽  
Normal Emissivity

Determining the surface temperature of materials with unknown emissivity is studied. A method for determining the surface temperature using a standard sample of average spectral normal emissivity in the wavelength range of 1,65–1,80 μm and an industrially produced Metis M322 pyrometer operating in the same wavelength range. The surface temperature of studied samples of the composite material and platinum was determined experimentally from the temperature of a standard sample located on the studied surfaces. The relative error in determining the surface temperature of the studied materials, introduced by the proposed method, was calculated taking into account the temperatures of the platinum and the composite material, determined from the temperature of the standard sample located on the studied surfaces, and from the temperature of the studied surfaces in the absence of the standard sample. The relative errors thus obtained did not exceed 1,7 % for the composite material and 0,5% for the platinum at surface temperatures of about 973 K. It was also found that: the inaccuracy of a priori data on the emissivity of the standard sample in the range (–0,01; 0,01) relative to the average emissivity increases the relative error in determining the temperature of the composite material by 0,68 %, and the installation of a standard sample on the studied materials leads to temperature changes on the periphery of the surface not exceeding 0,47 % for composite material and 0,05 % for platinum.

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