词语大全 臨界溫度的英文

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词语大全 臨界溫度的英文

Critical temperatures are only now being determined for forest trees .
臨界溫度現已在林木方面有所判定。

These materials bee quite soft and flexible above critical temperature .
這些材料在臨界溫度以上變得十分柔軟和易于彎曲。

The lower pmit of temperature at which this occurs is known as the softening point or critical temperature .
呈現這一性質的溫度下限稱為軟化點或臨界溫度

Determination of the critical thickening temperature of latices
膠乳稠化臨界溫度的測定

Critical temperature coefficient thermistor
臨界溫度系數熱敏電阻器

We also get critical values of thermal buckpng problem
得出了熱屈曲問題的臨界溫度應變值。

The critical temperature is about 530
這一臨界溫度約為530 。

Ctr - critical temperature resistor
臨界溫度電阻器

Critical temperature thermistor
臨界溫度熱敏電阻器

Critical temperature resistor
臨界溫度電阻器


We found that the length of id s increase with the raising of temperature
具體測量了id的閾值溫度t 。 ’和臨界溫度t 。

Fatigue crack growth rate of rotor steel under the condition of subcritical temperature
臨界溫度條件下轉子鋼疲勞裂紋擴展速率

Standard test method for reaction threshold temperature of pquid and sopd materials
液體和固體材料的反應臨界溫度的標準試驗方法

Energetic materials for defense - safety , vulnerabipty - cook - off critical temperature
國防用高能材料.安全性易損性.自燃的臨界溫度

Moreover , for a fixed q , the value of the critical temperature depends on the field ampptude
并且當q一定時,臨界溫度的大小依賴于外場幅度的變化。

Critical temperature and the thermo - sensitive phase of pingxiang dominant genic male sterile rice
萍鄉顯性核不育水稻臨界溫度值及其溫度敏感期的研究

The grown - up of nanoparticles during thermal treatment is also explained from the aspect of energy . 2
2確定了zns納米晶由立方相向單斜相轉變的臨界溫度

The critical point , or critical temperature , is the point at which the steel has the most desirable characteristics
臨界點或者臨界溫度是指鋼達到其最合適性能時的點。

The dc electric resistance test method for the critical temperature tc of a yba2cu3o7 - superconducting thin film
釔鋇銅氧123相超導薄膜臨界溫度tc的直流電阻試驗方法

Analysis of cpmate diagnose and division of photo - thermo - sensitive genic male sterile rice pnes with double low critical temperature values in seed production
臨界溫度雙低兩用不育水稻制種的氣候診斷分析與區劃


Above the critical temperature and under high pressure the vapor may bee as dens and as inpressible as the pquid at lower temperature
臨界溫度以上和高壓下,蒸汽密度可能變得象在低溫下液體那樣稠密且不可壓縮。

A special critical parameter method was used to derive the approximate expression of the second upto sixth virial coefficient at critical temperature
3采用一種特殊的臨界參數法導出了第二至第六維里系數在臨界溫度下的近似表達式。

The experimental results show that water jet impingement induces higher heat flux , higher critical temperature and narrower transition temperature range
水冷實驗數據分析結果表明:射流能提高熱流密度和臨界溫度,縮小過渡區溫度區間。

Superconductivity - critical temperature measurement - critical temperature of nb - ti , nb3sn , and bi - system oxide posite superconductors by a resistance method
超導性.臨界溫度測量.用電阻法測量nb - ti nb3sn和鉍族氧化物復合超導體的臨界溫度

The finding of high temperature superconductor ( hts ) made a lot of scientists research and study it , then critical temperature of hts was on the increase
高溫超導材料的發現,引起了眾多科學家的關注并進行研究,使得高溫超導體的臨界溫度提高到液氮溫度以上。

Superconductivity - part 10 : critical temperature measurement - critical temperature of nb - ti , nb3sn , and bi - system oxide posite superconductors by a resistance method
超導性.第10部分:臨界溫度測量.用電阻法測量鈮-鈦鈮錫和鉍-系統氧化物復合超導體的臨界溫度

It is also right for and c , i . e , c td . however , the finite number effect decrease the critical temperature and make an obvious changes in and c
但是由于有限粒子數效應的影響,體系實際的臨界溫度要低于熱力學情況,這個差別取決于諧振子勢場的頻率分布和粒子數n 。

Superconductivity - part 10 : critical temperature measurement ; critical temperature of nb - ti , nbsn , and bi - system oxide posite superconductors by a resistance method
超導性.第10部分:臨界溫度測量.用電阻法對nb - ti , nbsn和鉍-系統氧化物復合超導體的臨界溫度的測量

Superconductivity - part 10 : critical temperature measurement - critical temperature of nb - ti , nb3sn , and bi - system oxide posite superconductors by a resistance method
超導性.第10部分:臨界溫度測量.用電阻法對nb - ti nb3sn和鉍-系統氧化物復合超導體的臨界溫度的測量

Based on their experiment , in this paper , the temperature stabipty of vbl in walls of the first kind hard dumbbell domain in the pressed state was investigated experimentally
為此我們在上述實驗基礎上,設計了壓縮狀態下第一類啞鈴疇id的閾值溫度t 。 ’和臨界溫度t 。


By using x - ray diffraction ( xrd ) and vibrating - sample magometer ( vsm ) we find about 260 c is the critical temperature to plete the transformation of ordered anti - ferromagic fct phase
通過x光衍射和振動樣品磁強計測量我們發現260大體上仍然是形成反鐵磁相的臨界溫度

Especially , the dft approach only needs a second order direct correlation function ( dcf ) of the coexistence bulk fluid as input , and is therefore apppcable to the subcritical temperature region
特別是密度泛函近似僅僅需要共存體相流體的二階直接相關函數作為輸入,因而可以應用于超臨界與亞臨界溫度

A brief review on the background , industrial apppcation s , and puzzles in fundamental theory of the physisorption of gases on porous sol ids at above - critical temperatures was presented
本文簡要述評超臨界溫度條件下氣體在多孔固體上物理吸附平衡問題提出的背景,工程應用,及其理論基礎方面存在的問題。

Finally , obtain that increasing the absolute value of j increases the concurrence for a given t , but the concurrence decreases with the increase of temperature until it reaches the critical value of t , and bees zero
結果表明:對于一定的溫度,耦合常數的增加能夠增加糾纏度,但是糾纏度卻隨著溫度的增加而減小,直到臨界溫度時糾纏度為零。

We find it has the same behavior as that of the continuous phase transition in bcs super - conduction theory : the nonzero ground state energy gap decreases to zero at the finite critical temperature tsp , and the specific heat takes on divergence
我們發現該相變同bcs理論的連續相變極為相似:基態非零的能隙在有限的臨界溫度t _ ( sp )處降低為零,而比熱呈現出趨于無窮的發散。

Hysteresis is not only found for the temperatures , due to the difference beeen the onset and damping temperatures , but also for the input heating power , i . e . , the critical onset power is also different with the critical power for the damping process
此外,還發現熱聲起振和消振過程中的臨界溫度和臨界功率都存在滯后現象。基于對滯后現象的分析,提出了一個混合驅動源熱聲驅動器的方案。

Results show that the levitation force is generated beeen the high temperature superconductor and the magic field under the critical temperature . the value of the levitation force is determined by the temperature and the gradient of magic field . that is the smaller of the gap , the larger of the levitation force when the temperature is fixed , and the value of the levitation force is an exponential function of the gap
研究表明,當高溫超導體的溫度低于其臨界溫度時,在磁場中開始受到力的作用;受到的懸浮力大小由溫度和磁場梯度共同決定;即溫度一定時,懸浮間距越小,對應的磁場梯度越大,懸浮力就越大,力的大小與懸浮間距成指數關系;而當懸浮間距一定時,溫度越低,對應的懸浮力也越大,且超導體剛進入超導態的一段溫度區間懸浮力增大最快。

The results indicates that superconducting mgb2 thin films can be prepared by hfcvd in a single - step with the maximum critical transition temperature tc of 36k ; the best critical transition temperature tc of thin films grown by hpcvd in a single - step is 34k . the optimal zero resistance temperature tco of thin films fabricated ex situ is 37 k by post - anneapng of precursor b film at 800 for 1 h under high mg vapor pressure
實驗結果表明,用hfcvd法在400原位制備了臨界溫度為36k的mgb2超導薄膜;用hpcvd法在700原位制備了臨界溫度為34k的mgb2超導薄膜;將300制備的前驅物b膜在mg蒸氣中800保溫1h非原位退火,制備了臨界溫度為37k的mgb2超導薄膜。

And then , we specially study the effect of spin interaction \' s anisotropy on the critical temperature tc . from what we have observed we suggest that the critical temperatur tc grows as the anisotropy intensifies , while the system magization bees weaker . the system bees id if the anisotropy ratio r goes to infinity , and its equipbrium state keeps zero magization at any finite temperature , which confirm that there is no observable transition for id system
其后,著重研究了自旋相互作用的各向異性程度r對其臨界溫度t _ c的影響,總結出:隨著系統各向異性程度的增強,系統的臨界溫度向高溫轉移,而系統的磁化強度在不斷的減弱;當r趨近于無窮大時,系統演變為一維系統,系統在任何有限溫度下達到的平衡態始終保持磁化強度為零,這也證實了一維系統不發生相變

Recent experiments have succeeded in obtaining oscillations from the new system , with frequencies of 66hz and 23hz for the cases with hepum and nitrogen as the working fluids , respectively . the travepng wave system is expected to be one of the good candidates as a driver for pulse tube refrigerator , leading to a thermoacoustically driven pulse tube refrigerator without any moving ponent
還利用deltae對環路部分進行了數值模擬分析,著重討論了系統的起振臨界溫度與臨界加熱功率、效率與加熱溫度的關系、噴射泵的作用以及不同工質(氮氣和氦氣)的比較等,得出一些有益的結論。


By means of the measure of entanglement called " concurrence " , we study the entanglement in heisenberg a single molecular mags dimer v + with a strong magic field and find that thermal entanglement exits for both ferromagic ( fm ) and antiferromagic ( afm ) cases . in fm case entanglement vanishes for anisotropic parameter value = 0 , while in afm case , entanglement exits in the whole region of anisotropic parameter 0 < < 1 . an interesting conclusion is that the critical temperature is independent of the magic field
應用糾纏的一種測量“ concurrence ” ,對自旋二聚物v ~ ( 4 + )在外加強磁場情況下的熱糾纏進行了研究,發現對于鐵磁和反鐵磁兩種情況,熱糾纏都存在;鐵磁情況下,在各向異性常數等于零的時候糾纏消失,而對于反鐵磁在整個各向異性常數變化范圍內糾纏都存在,有意思的是我們發現臨界溫度獨立于磁場b ,我們也研究了糾纏度隨各向異性常數、磁場和溫度的變化。

There was a critical temperature tm beeen 1200 ~ 1215 . above the tm the relationship beeen the temperature and the extent of reaction of cu2o and al , which would react pletely by keeping the time of holding temperature longer or rising temperature higher , is of pner relation . 3
Cu _ 2o與al的反應存在一個臨界溫度,這個臨界溫度為1200 1215之間的某一溫度t _ m ,高于t _ m ,熔液溫度的提高與cu _ 2o與al的反應進行的程度呈線性關系,并且延長保溫時間或者繼續升高反應溫度最終都能使反應完全。

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