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correcting     
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  修正
     ④ correcting land price;
     ④修正土地价格;
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     ② EM provided essential diagnosis in 21.9%,and EM provided correcting or supplementary information in 23.7%,then EM supported or confirmed the LM plus IF findings in 54.4%.
     ②电镜检查对肾活检病理诊断起决定诊断作用的病例占21.9%,起修正补充作用的病例占23.7%,而起验证作用占54.4%;
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     Discusses the Methods of Correcting Electrode and PH - Meter Error
     电极与PH计误差修正方法的探讨
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     In order to get a better result, a better experiment method for low energy region, measuring the γray (59.5keV) of ~(241)Am then correcting the measurement result with different correction and comparing with reference value , was used in this article.
     通过实验的方法测量241Am的59.5keVγ射线,然后对结果采用不同的修正并与参考值进行比较分析,得到一种测量低能γ射线的实验方法。
短句来源
     Experimental sample with special surface was designed through error compensation by correcting NC data, and experimental proof for error compensation was conducted on MAKING machining center FNC86-A.
     文章采用修正NC数据实现误差补偿,设计了具有特殊表面的实验样件,在MAKINO FNC86-A加工中心上进行了误差补偿实验验证。
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  校正
     The highest correcting IOP was 24.3mmHgand lowest was 17.6mmHg, the average was 20.1mmHg.
     校正后眼压最大值为24.3mmHg,最小为17.6mmHg,均值为20.1mmHg。
短句来源
     Result The aerocysts pressure of patients was 2.85±0.23 kPa,2.00±0.35 kPa,1.81±1.98 kPa,1.77±0.00 kPa at 2h、4h、6h and 8h respectively after correcting for the first time,The number of patients who participating measured declined to inchoate 50% at 6h.
     结果首次气囊压力校正后2 h、4 h、6 h8、h,患者气囊压力分别为(2.85±0.23)kPa,(2.00±0.35)kPa,(1.81±1.98)kPa以及(1.77±0.00)kPa。
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     Experiment and Study on the Correcting Effect of Surge Pressure Signal on n_L,n_H and T_(t5) Channels of an Engine Electronic Controller
     喘振压力信号对某综合调节器n_L、n_H、T_(t5)通道的校正试验及研究
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     Nonlinear Correcting Method Platinum Resistance A/D Convert
     铂电阻的A/D非线性校正
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     A design for ΔS correcting lens of using CPT for HDTV
     HDTV用CPT的ΔS校正透镜的设计
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  纠正
     Conclusion Decoction of Huoxuetongmai could alleviate CIRI by correcting TXB_(2)/6-keto-PGF_(1α) imbalance after cerebral ischemia reperfusion injury and reduce the extension of cerebral ischemia at 24 hours and 48 hours after reperfusion.
     结论活血通脉汤可纠正脑缺血再灌注后循环血中TXB2/6-keto-PGF1α的平衡失调及降低脑组织缺血程度,减轻脑缺血再灌注损伤。
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     Result The blood gas turbulence correcting rate was 89.5% and the mortality rate was 9.7%.
     结果复查血气分析纠正率89.5%,死亡率9.7%。
短句来源
     Methods 85 patients with Kaliopenia used micro-injection pump to infuse 10% Potassium chloride via central vein at 5-15ml/h(6.65~20mmol/h) speed for correcting kaliopenia. Strict monitoring and nursing during 10% Potassium chloride infusion were done.
     方法85例低钾血症患者使用微量注射泵,以5~15 ml/h(6.65~20 mmol/h)的速度经中心静脉输注浓度为10%氯化钾原液,以纠正低钾血症,对补钾过程严密监测和护理。
短句来源
     Gene therapy refers to the introduction of proper genes into cells for treating diseases by correcting the defects of genes.
     基因治疗是指将人的正常基因或有治疗作用的基因通过一定方式导入人体靶细胞,以纠正基因的缺陷或发挥治疗作用,从而达到治疗疾病的目的。
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     In ten patients with ARDS, failing in correcting hypoxemia by instituting IPPV with F1O2 higher than 0.4-0.5, PEEP of 5-15 cmH2O was promptly used.
     10例成人呼吸窘迫综合征(ARDS)病人,应用间断正压通气(IPPV)治疗,在吸氧浓度(FiO_2)≥0.4~0.5仍不能纠正低氧血症时,及时采用了5~15cmH_2O的呼气末期正压通气(PEEP)治疗。
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  矫正
     The effect of correcting astigmatism of -0.59±0.38D occured(48.8%<-0.50?D and 51.2%≥-0.50?D). Axis direction of real corrected myopic astigmatism was 180°-44°~180°+44°.
     术后6 个月时产生(0 .59 ±0 .38)D 的矫正近视散光的效应,其中≥0 .50 D 者占51 .2 % (22/43) ,实矫近视散光轴位均在180°- 44°~180°+ 44°之间。
短句来源
     The horizontal distance between the C7 and S1 was 13.7mm and 3.8mm respectively before and after operation. Correcting rate was 72.3%.
     C7-S1水平距离术前平均为13.7mm,术后平均为3.8mm,矫正率72.3%;
短句来源
     All patients regain effective visual acuity. The best correcting visual acuity is 0.5 or better in 17 eyes(51.5%),0.3~0.4 in 12 eyes(36.4%),0.1~0.2 in 4 eyes (12.1%).
     其中末次随访最佳矫正视力≥ 0 .5者 17眼 ( 5 1 5 % ) ,0 3~ 0 .4者12眼 ( 3 6 4% ) ,0 1~ 0 .2者 4眼 ( 12 1% )。
短句来源
     After correcting defocus and astigmatism,the average visual acuity of subjects is 1.0,the CSF value is about 52 for lower frequency 20 c/mm and about 1 for higher frequency 80 c/mm.
     矫正了离焦与像散后,被测者的平均视锐度值达到了1.0,对比敏感度在低频(20 c/mm)处约为52,高频(80 c/mm)处约为1;
短句来源
     One-way ANOVA showed that mRNA expression of LVDCC α1c in AF>6 M was still low after correcting the effect of atrial diameter ( P <0.01).
     单因素协方差分析 (ANOVA)矫正心房内径的影响 ,AF >6M患者α1cmRNA表达仍明显下降 (P <0 0 1)。
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  correcting
The theory of linear error-correcting codes from algebraic geometric curves (algebraic geometric (AG) codes or geometric Goppa codes) has been well-developed since the work of Goppa and Tsfasman, Vladut, and Zink in 1981-1982.
      
In this paper we introduce to readers some recent progress in algebraic geometric codes and their applications in quantum error-correcting codes, secure multi-party computation and the construction of good binary codes.
      
It is based on predicting the trajectories of each of the nonlinear systems and correcting them by the deviation of the prediction from the desired value.
      
The ability of a discrete dynamic system for correcting functional errors is investigated.
      
The latter is preferentially exhibited towards mispaired (non-canonical) nucleotides, this being the reason why APE1 is considered as a proofreading enzyme correcting the misincorporations introduced by DNA polymerase β.
      
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An experimental verification of the theoretical peak current equation forreversible electrode reactions of the Randles-Sevcik oscillopolarography, i_p=Kn~(3/2)D~(1/2)m~(2/3)θ~(2/3)α~(1/2)cμΑ, is carried out with both single- and multisweep methods. Themultisweep method is essentially that of Delahay, while a simplified circuit isdevised for the single-sweep procedure. The constant K in the above equation has been worked out by Randlesand Sevcikc, but their values differ by some twenty-one percent. Experimentalresults...

An experimental verification of the theoretical peak current equation forreversible electrode reactions of the Randles-Sevcik oscillopolarography, i_p=Kn~(3/2)D~(1/2)m~(2/3)θ~(2/3)α~(1/2)cμΑ, is carried out with both single- and multisweep methods. Themultisweep method is essentially that of Delahay, while a simplified circuit isdevised for the single-sweep procedure. The constant K in the above equation has been worked out by Randlesand Sevcikc, but their values differ by some twenty-one percent. Experimentalresults as to which K value is correct have been contradictory. The authorspoint out that Sevcik's value of K is too low, due to the error in choosing too largea unit in his numerical integration. By taking smaller units and reperformingthe integration, the K value increases and approaches that of Randles. Thus thecorrectness of Randles' K value is ascertained and this value is used in calculatingthe theoretical slope. Their single-sweep results, with concentrations from 2×10~(-4) to 1×10~(-3) m/l andα~(1/2) from 1 to 4 volts/sec, agreement between experimental and theoretical slopesis obtained in the case of Tl~+ in m NaCl. In the case of Cd~(++) in m NaCl, experi-mental results deviate from the theoretical value, and the deviation increases withincreasing c and α~(1/2). Contrary to an unproven idea of Delahay, i_p obtained bymultisweep method is higher than that by the single-sweep procedure. However,in calculation of the theoretical values, a value of 15.0×16~(-6) obtained by polarLographic method is used for D of Tl~(+) in m NaCl. The use of the value of Dat infinite dilution is thought to be unjustified. If a D value of 15.0×10~(-6) is used,Delahay's results of Tl~+ in KNO_3 would be higher than the theoretical equationinstead of agreeing with it. This fact seems to support the findings of this paper. Various methods of correcting for capacity currents are compared and discus-sed. The authors point out that at α~(1/2) less than 2 volts/sec, the method of drawingan hbrizontal line introduces no appreciable error while at, high α, various methodsyield different results. This fact lowers the accurraey of data obtained at high α. The iR drop in the electrolytic cell and on the series resistance causes themeasured α to be different from the a actually applied on the drop electrode. Anelementary approximate correction of this effect is mentioned. Results after thiscorrection show that the deviation of Cd~(++) from theoretical at high c and α maybe due partly to this effect.

(1)以单波法及多波法验证Randles-Sevcik示波极谱理论公式之i_p~c及i_p~α~(1/2)关系,多波法用Delahay线路,单波法则用简化线路。单波法之结果,对亚铊离子在m氯化钠中,在2×10~(-4)~1×10~(-5)m浓度,α~(1/2)为1及4伏特/秒,实测结果和理论符合。镉离子在m氯化钠中,实测结果与理论有偏差,偏差随浓度及α~(1/2)加大而加大。多波法之i_p实测值高于单波法。 (2)在计算理论曲线时,作者肯定Sevcik之系数过低而采用Randles数值。亚铊离子于m氯化钠中之扩散系数D,采用极谱法测得之数值15.0×10~(-6)而不用无限稀时之D值(20.0×10~(-6))。 (3)在α~(1/2)低于2伏特/秒时,可用画水平线法扣除电容电流。在高α时各种扣除电容电流方法所得结果不同,影响结果之可靠性。 (4)电解池线路上之iR降使加在滴汞电极上之α改变。这种改变使实测i_p值偏低。作者曾作初步近似修正,结果说明α及浓度大时,镉离子实测数据对理论的偏差的一部分可能是由于iR降的作用。

We describe in this paper an experiment using a cloud chamber in a magnetic field of 6200 gauss to determine the average total cross-section of the direct production of electron pairs in aluminium by high energy electrons generated in cascade showers and having energies larger than 30 Mev. We have found after correcting for the spurious events 8.1 electron tridents, which were produced actually by electrons. This figure corresponds to a mean free path of 672±585 cm. or an average total cross-section of...

We describe in this paper an experiment using a cloud chamber in a magnetic field of 6200 gauss to determine the average total cross-section of the direct production of electron pairs in aluminium by high energy electrons generated in cascade showers and having energies larger than 30 Mev. We have found after correcting for the spurious events 8.1 electron tridents, which were produced actually by electrons. This figure corresponds to a mean free path of 672±585 cm. or an average total cross-section of (0.25± 0.22) X 10-25 cm2, for trident production. In the treatment of data, the elimination of spurious tridents has been appropriately considered. The formulas of the total cross-section derived by Bhabha[8] and by Murota et al[11] have been applied in accordance with our experimental conditions to compute the total cross-section. Finally, comparison between the theoretical and experimental values has been made. Our experiment is in fair agreement with the theory of Murota et al. While not in contradiction with that of Bhabha.

本文叙述利用场强为6200高斯的磁云室,对级联簇射中的能量大于30兆电子伏的电子在铝中直接产生电子对的平均总截面进行了测量。实验上总共找到真正由电子产生的电子三岔8.1个,相应于三岔产生的平均自由路程为672±585厘米或平均总截面为(0.25±0.22)×10~(-25)厘米~2。在数据处理中,对假三岔数目的除去作了应有的适当考虑。此外对Bhabha及Murota等的总截面公式也作了适合于于我们实验具体情况的修正,并算出总截面值,最后将它同实验值作了比较。结果我们认为实验上测得的值和Murota等的总截面值较为接近,但也不与Bhabha的截面值矛盾。

In this paper various factors influencing the image quality of plane grating spectrometer are discussed in detail. By means of vector elgebra a general formula is given for the form of the spectral lines in relation to the form of the entrance slit. A formula describing the angular dispersion of the spectral line resulting from a circular slit is also given. Investigation on the optical performance of the Ebert-Fastie grating spectrometer shows that among various residual optical aberrations, due to unsymmetrical...

In this paper various factors influencing the image quality of plane grating spectrometer are discussed in detail. By means of vector elgebra a general formula is given for the form of the spectral lines in relation to the form of the entrance slit. A formula describing the angular dispersion of the spectral line resulting from a circular slit is also given. Investigation on the optical performance of the Ebert-Fastie grating spectrometer shows that among various residual optical aberrations, due to unsymmetrical disposition of the incident and diffracting beams with respect to the grating surface, coma is the most serious image defect. This can however be corrected by changing the focal length of one of its reflecting mirrors and placing it at a definite distance from the other mirror. It is also shown that residual aberrations can be well eliminated by placing an aspherical correcting plate near the grating surface. By the latter means there is the potentiality of greatly improving the performance of the instrument; either the volume of the instrument may be greatly reduced where shorter focal length optical systems can be used, or much better light gathering capacity can be achieved without sacrificing its monochrometicity when the spectrometer is used as a monochrometor.

本文包括下列结果: 1.以矢量代数方法一般地讨论了狭缝形状和谱线形状的关系;导出了一般的角色散公式。 2.讨论了由于光栅角倍率特点所残留的不对称象差及其校正方法和其他象差之值,并举出一个校正象差的例。 3.探讨了完全校正象差的可能有的结构及其特性。

 
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