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温度
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  temperature
     TEMPERATURE (4.2—300K) DEPENDENCE OF ELECTRICAL RESISTIVITY OF FeMB (M=Mn, Mo) AMORPHOUS ALLOYS
     FeMB(M=Mn,Mo)非晶态合金的电阻率与温度(4.2—300K)的关系
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     EPR INVESTIGATION OF LaOBr:Ce~(3+) ,Tb~(3+) POWDER AT LIQUID HELIUM TEMPERATURE(4.2K)
     液氦温度(4.2K)下LaOBr:Ce~(3+),Tb~(3+)粉末的电子顺磁共振研究
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     THE HIGH Tc (Tl -Ba-Ca-Cu-O) SUPERCONDUCTOR SYNTHESIZED AT LOWER TEMPERATURE (580 ~ 700 ℃ )
     较低温度(580~700℃)合成的高Tc(Tl-Ba-Ca-Cu-O)系超导体
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     The Study of Phase Inversion Temperature (PIT) of Sweet Orange Oil-Water Emulsiom
     甜橙油水乳系相转型温度(PIT)的研究
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     ON GENERALIZED SYNTHETICAL TEMPERATURE(GST)
     论广义综合温度(GST)
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  “温度(”译为未确定词的双语例句
     The rooting rate in the medium of 1/2 MS supplemented with ABT0.5mg/L, IBA0.5mg/L, and 2.5% sucrose could reach over 95%.
     生根培养以1/2MS+ABT0.5mg/L+IBA0.5mg/L+2.5%蔗糖在光强1500 ̄2000Lx,温度(25±1)℃条件下,生根率达95%以上。
短句来源
     The influences of Gd doping on macromagnetic properties and micromagnetic structure of La_(0.67) Sr_(0.33)CoO_3 and La_(0.7)Sr_(0.3)MnO_3 were studied by magnetization-temperature (M-T) curves and magnetization -magnetic field (M-H) curves.
     通过磁化强度-温度(M-T)曲线,磁化强度随磁场变化(M-H)曲线,研究了Gd掺杂对La_(0.67)Sr_(0.33)CoO_3和La_(0.7)Sr_(0.3)MnO_3宏观磁性质和微观磁结构影响。
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     At 25 ℃ the equation logCMC=-2.13-0.07n was defined.
     在所测定的温度(25℃)下,logCMC=-2.13-0.07n;
短句来源
     The densities and viscosities for solutions of FeSO_4-Fe_2(SO_4)_3-H_2SO_4 were determined with density bottle and capillary viscosimeter at 294.75-341.15 K,0.1-0.8 mol/L of hydrogen ion and 0.1-0.8 mol/L of ferric and ferrous ion.
     利用密度瓶和毛细管粘度计测量了在不同温度(294.75—341.15 K)、不同氢离子浓度(0.1—8 mol/L)和不同总铁离子浓度(0.1—0.8 mol/L)的FeSO4-Fe2(SO4)3-H2SO4溶液的密度和粘度。
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     Methods: Using HPLC method,we investigated the influence of different temperatures(-20 ℃, 6-8℃,60℃),sonification time(10-60 s) and pH values (pH 4.0,7.0 and 10.0) on thymosin α_1 stability.
     方法采用高效液相色谱法(HPLC),研究胸腺肽α1在不同温度(-20℃、6~8℃、60℃)、不同超声时间(10~60s)及不同pH值(4.0、7.0、10.0)条件下的稳定性。
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  相似匹配句对
     T is temperature, ℃.
     T为温度,℃。
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     TEMPERATURE OF HORIZONS
     视界的温度
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  temperature
The assumption that the temperature anisotropies of the CMB are a realisation of a statistically isotropic Gaussian random field on the sphere is questioned.
      
The reported method1 of their synthesis involves hydrogenation at high temperature and pressure.
      
The formed intermediate showed a lower thermal transition temperature (Tm) by a magnitude of 10°C in relation to the native DNA.
      
The nonlinear PDEs consist of a heat equation with the Joule heating as a source and a current conservation equation with temperature-dependent electrical conductivity.
      
In the theoretical analyses, the second-order error estimates are obtained for electrical potential in discrete L2 and H1 norms, and for the temperature in L2 norm.
      
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The dielectrie constants of toluene, carbon bisulphide, normal pentane, normal hexane, ethyl ether and iso-amyl alcohol were measured by a capacity bridge using a specially constructed liquid condenser at both 30° and 75℃ (22.4℃ only for the last liquid), for frequencies of 600,1000 and 2000 cycles per sec. and under pressures from 1 up to 12,000 kg/cm2. For the first four liquids, the dielectric constant is practically independent of the frequencies

作者用一电容桥及一特制之液体蓄电器以量甲苯,二硫化碳,正戊烷,正己烷,乙醚,及异戊醇之比电容。所用温度为摄氏三十及七十五度(异戊醇之温度仅为二十二度四),频率为每秒六百,一千及二千周,压力自一气压高至一万二千气压。前四液之比电容几与所用频率无关。(ε-1)/(ε+2)·1/d,(ε-1)/d及(ε~(1/2))-1/d三式中以第一式最近一常数,然压力渐增第一式之值恒随之而渐减,至一万二千气压时(在甲苯为九千五百气压),其减少约数在甲苯及二硫化碳为百分之三,在乙醚为百分之八,在异戊醇为百分之十九,显随电矩之增加而增加,至其原因篇中亦略加说明。 篇中图表惠蒙同事朱福炘先生代为抄绘,附誌谢忱。

The circumferential vibration of a hollow quartz cylinder has been thoroughly studied. The empirical relation connecting the dimensions of the cylinder and the frequency of vibration has been formulated, and the temperature coefficients of the frequency determined. The temperature coefficient is practically zero for a wide range of temperature, when the ratio of the internal radius to the external radius of the cylinder approaches a value which is very close to 0.5.

以纯粹水晶割成空心圆柱,令圆柱之轴平行於晶体之光轴。于其里外二面,敷以铜质管状电极、置诸最简单之Pierce式振荡线路中,即能自生振动其振动之方式繁多,俱经吾人详细阐求,已在另文发表,茲不复赘。 各种振动方式中,以绕周振动发生最易。设圆柱内径与外径之比小于一去0.5极近之数,则绕周分三段而振动;设大于此数,则分六段而振动, 绕周振动之温度系数,亦经测定其法置圆柱於一特制之电炉中,连其二电极於振荡电路,令生振动。以所生高周率电流与一周率甚近之水晶片所生之高周率电流相干涉,由 是而生之低周率音差,复与一低周率振荡器相比较,若是则加热后圆柱振动周率之变化,可在该低周率振荡器上直接读之。 若是所得之结果绕周振动之温度系数,随其内外径之比而异。圆柱之绕周分三段而振动者,其温度系数常为正;内外径之比率增加,则温度系数减少。圆柱之线周分六段而振动者,其温度系数常为负;内外径之比率愈高,则温度系数愈大。惟适当三段振动告终六段振动肇端之时,则亘十馀度其周率几不以温度而变合二十馀度而平均计之其温度系数约为0.5×10~(-6)/C,小...

以纯粹水晶割成空心圆柱,令圆柱之轴平行於晶体之光轴。于其里外二面,敷以铜质管状电极、置诸最简单之Pierce式振荡线路中,即能自生振动其振动之方式繁多,俱经吾人详细阐求,已在另文发表,茲不复赘。 各种振动方式中,以绕周振动发生最易。设圆柱内径与外径之比小于一去0.5极近之数,则绕周分三段而振动;设大于此数,则分六段而振动, 绕周振动之温度系数,亦经测定其法置圆柱於一特制之电炉中,连其二电极於振荡电路,令生振动。以所生高周率电流与一周率甚近之水晶片所生之高周率电流相干涉,由 是而生之低周率音差,复与一低周率振荡器相比较,若是则加热后圆柱振动周率之变化,可在该低周率振荡器上直接读之。 若是所得之结果绕周振动之温度系数,随其内外径之比而异。圆柱之绕周分三段而振动者,其温度系数常为正;内外径之比率增加,则温度系数减少。圆柱之线周分六段而振动者,其温度系数常为负;内外径之比率愈高,则温度系数愈大。惟适当三段振动告终六段振动肇端之时,则亘十馀度其周率几不以温度而变合二十馀度而平均计之其温度系数约为0.5×10~(-6)/C,小於寻常水晶片者五十馀倍。割制此种圆柱,并无繁难,且电极简单,装置便利以之控制振荡,校准周率,对无线电通讯,裨益实多也。

The absorption band at 2240 A discovered by Stucklen in an underwater spark does not agree with the band observed by Hulthen and Zumstein in a high temperature oven and later studied by Grundstrom. The important difference lies in the complete lacking of the R-branch lines in Stucklen's band. New experimental investigation led to the discovery of the unfound R-branch lines. This is a strong evidence that the bands are actually the same.

Stcklen氏发现用铜极在水中生火花有一吸收光带位於2240A区域此光带与Hulthen氏及Zumstein氏及Grund-strom氏在高温度炉中用铜之蒸气加以氢气所得之吸收光带(亦在2240A附近)不能一致最大之分别在Stucklen之光带全无R支谱线新实验工作发现R支谱线之存在得R(0)至R(13)之十四根线确实证明Stucklen之光带并非另一新带。

 
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