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感生
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  induced
     INDUCED ANISOTROPY IN METALLIC GLASSES (Fe_(1-x)Co_x)_(78) Si_(10)B_(12)
     金属玻璃(Fe_(1-x)Co_x)_(78)Si_(10)B_(12)的感生各向异性
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     Laser induced thermoelectric voltage effect in La_(0.67)Pb_ (0.33) MnO_3 thin films doped with Ag
     Ag掺杂的La_(0.67)Pb_(0.33)MnO_3薄膜中激光感生热电电压效应
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     ON THE INDUCED MAGNETIC ANISOTROPY OF METALLIC GLASS Fe__(78)Si_(10)B_(12)
     金属玻璃Fe_(78)Si_(10)B_(12)的感生磁各向异性
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     Laser induced thermoelectric voltage (LITV) signals from thin films of La1-xSrxMnO3 (LSMO), La1-xPbxMnO3 (LPMO) and La1-xSrxCoO3 (LSCO) were measured at different wavelengths.
     测量了La1-xSrxMnO3(LSMO),La1-xPbxMnO3(LPMO)和La1-xSrxCoO3(LSCO)三种薄膜在不同激光波长下的激光感生热电电压(LITV).
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     INDUCED MAGNETIC ANISOTROPIES IN METALLIC GLASS Fe40Ni40P12B8
     金属玻璃Fe_(40)Ni_(40)B_(12)B_8的感生磁各向异性
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  “感生”译为未确定词的双语例句
     PREPARATION AND LITV EFFECT IN YBa_2Cu_3O_(7-δ)/La_(0.6)Pb_(0.4)MnO_3 MULTILAYER
     YBa_2Cu_3O_(7-δ)/La_(0.6)Pb_(0.4)MnO_3多层膜的制备及激光感生热电电压效应的研究
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     Martesitic transformation and magnetic-field-induced strain in Ni_(52.5)Mn_(23.5)Ga_(23.6)Tb_(0.4) alloy
     Ni_(52.5)Mn_(23.5)Ga_(23.6)Tb_(0.4)合金马氏体相变和磁感生应变的研究
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     Elec-tron traps with level of E_1'(E_0-0.38eV), E_2'(E_0-0.57eV) aind E_3' (E_c-0.74eV) have beenfound in VPE n-GaAs active layer after irradiation.
     在n型VPE GaAs有源层中电子辐照感生了E_1~'(E_c-0.38eV)、E_2~'(E_c-0.57eV)、E_s~'(E_c-0.74eV)缺陷.
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     Laser-induced fluorescence of long chain molecular (C_6H_(10)O_5)_n
     (C_6H_(10)O_5)_n长链分子的激光感生荧光
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     Temperature dependence of the magnetic-field-induced strain in Ni_(50.5)Mn_(26.5)Ga_(23) single crystal
     Ni_(50.5)Mn_(26.5)Ga_(23)单晶磁感生应变的温度依赖性
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  相似匹配句对
     Study on Induced Electric Field Experiment
     感生电场实验研究
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     THE RADIOACTIVITY INDUCED IN LOW ENERGY ELECTRONIC ACCELERATOR
     低能电子加速器的感生放射性
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  induced
We show that they are induced by automorphisms ofG and that a surjective holomorphic self-map can be nonbijective only in the directions of the nilradical ofG.
      
LetRo andR1 be two Kempf-Ness sets arising from moment maps induced by strictly plurisubharmonic,K-invariant, proper functions.
      
In particular, the induced differentiable structures on the categorical quotientX G are diffeomorphic.
      
Then,SL(2, ?)-harmonic analysis, in the noncompact picture of induced representations, is used to decompose patterns into the components invariant under irreducible representations of the principal series ofSL(2, ?).
      
We study the properties of the continuous measures μk, induced by
      
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It is well-known that the stress-induced rotation of the magnetic domains in nickel gives rise to an internal friction peak (when internal friction is plotted as a function of temperature of measurement). An internal friction peak associated with the presence of carbon in nickel was recently observed in our laboratory. In this paper are described further experiments which demonstrate conclusively that this new internal friction peak is not connected with ferromagnetism of nickel but depends upon the amount of...

It is well-known that the stress-induced rotation of the magnetic domains in nickel gives rise to an internal friction peak (when internal friction is plotted as a function of temperature of measurement). An internal friction peak associated with the presence of carbon in nickel was recently observed in our laboratory. In this paper are described further experiments which demonstrate conclusively that this new internal friction peak is not connected with ferromagnetism of nickel but depends upon the amount of carbon in solid solution in nickel. More accurate determinations of the activation energy associated with this internal friction peak show that this activation energy is indeed very close to the activation energy for the diffusion of carbon in nickel. These experiments thus show that the new internal friction peak is associated with the stress-induced micro-diffusion of carbon in nickel.

镍中磁畴在应力作用下的转动可以引起一个内耗峰(当内耗表示为温度的函数时),是众所周知的现象。最近在我们的实验室中发现镍中含碳可以引起内耗峰。本文叙述进一步的实验,确切证明这个新内耗峰与镍的磁性无关,而与镍中固溶体所含的溶解碳量有关。关于激活能的较精确测量指出:与这个内耗峰相联系的激活能确与碳在镍中扩散的激活能很相近。这些实验说明这个新内耗峰是由于碳在镍中的应力感生微扩散而起的。 简单地讨论了这个内耗峰的机构,认为可能与镍的晶体点阵中的空穴有关。

Internal friction in hardened carbon steels was measured with a torsion pendulum and an internal friction peak was observed around 130℃when measurements were taken from room temperature upwards. This peak disappeared completely after the temperature of the specimen reached 170℃. This phenomenon was observed in carbon steels containing carbon ranging from 0.29% to 1.4%, and also in an alloy steel. The appearance of this internal friction peak seems to indicate that the transformation product ( ∈ -carbide) formed...

Internal friction in hardened carbon steels was measured with a torsion pendulum and an internal friction peak was observed around 130℃when measurements were taken from room temperature upwards. This peak disappeared completely after the temperature of the specimen reached 170℃. This phenomenon was observed in carbon steels containing carbon ranging from 0.29% to 1.4%, and also in an alloy steel. The appearance of this internal friction peak seems to indicate that the transformation product ( ∈ -carbide) formed in the first-stage tempering of martensite is in coherence with its parent phase, and the origin of internal friction is the stress-induced movement of the plane of coherence.

用扭摆测量淬硬碳钢的内耗,当测量温度由室温渐渐升高时,在130℃附近有一个内耗峰出现。当温度达到170℃后再降温测量,这个内耗峰完全消逝不见。上述的现象在含碳0.29%到1.4%的几种淬硬碳钢和淬硬滚珠钢中都曾经看到。由内耗峰的出现可以认为马氏体在第一个回火阶段中的转变产物(ε-碳化铁)与母体具有共格性,由于共格界面的应力感生运动而引起内耗。 曾用具有马氏体组织的0.25%碳钢试样作实验,没有观测到上述的内耗峰。但是当回火温度达到280-300℃以后,在降温或升温测量中都观测到一个内耗峰(在150℃附近)。这表示低碳马氏体在第三个回火阶段中的转变产物与母体具有共格性。但是由于这个内耗峰的表现与上述高碳试样的内耗峰不同,所以我们认为这转变产物并不是ε-碳化铁。

Internal friction in hardened low-carbon nickel steel was measured with a torsion pendulum and an internal friction peak was observed around 155℃ with a frequency of vibration of about 2 cycles per second. The condition for the appearance of this internal friction peak is that the steel specimens contain martensite, alloying element and carbon. This internal friction peak has also been observed in chromium steel and chromium-nickel steel under suitable conditions. Systematic observations were made with steel...

Internal friction in hardened low-carbon nickel steel was measured with a torsion pendulum and an internal friction peak was observed around 155℃ with a frequency of vibration of about 2 cycles per second. The condition for the appearance of this internal friction peak is that the steel specimens contain martensite, alloying element and carbon. This internal friction peak has also been observed in chromium steel and chromium-nickel steel under suitable conditions. Systematic observations were made with steel specimens containing 29.7% Ni, and the height of internal friction peak was found to be proportional to the carbon content in the specimen. The experimental results mentioned above show that the new internal friction peak is associated with the stress-induced micro-diffusion of carbon in low-carbon alloy martensite.

用扭摆测量淬硬低碳镍合金钢中的内耗,当振动频率约为每秒2周时,在155℃附近有一个内耗峰出现。这个内耗峰的出现条件是:钢中必须含有马氏体、合金元素和碳。在适当的条件下,铬钢和铬镍钢中也曾观察到这个内耗峰。用含镍29.7%的钢作了系统试验,观察到内耗峰高度与试样中的含碳量成正比。内耗峰的高度由于在较高温度(165℃以上)的回火处理而不断降低。由内耗测量所测得的激活能是25,000卡/克分子。以上的实验结果指出,所观测到的155℃新内耗峰是由于碳在合金马氏体中的应力感生微扩散所引起来的。 提出了一个产生内耗峰的初步模型。假定碳在四角马氏体中是处于00(1/2)型的间隙位置。合金元素原子的存在引起晶体点阵中不均匀的畸变,因而应力的作用便改变了碳原子在热平衡状态下在Fe-C-Fe和B-C-Fe(B是合金元素原子)两种00(1/2)型间隙位置之间的跳动几率。这种应力感生的碳原子运动便引起内耗。用这个模型可以定性地解释所观测到的事实。关于这方面的定量研究正在进行中。

 
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