• 实验验证预测误差小于5%。

    The prediction error is within 5% through experimental verification.

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  • 原子吸收比较相对误差小于5%。

    Compare this method with AAS, its relatively error were less than 5%.

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  • 声速检测采用比较法,相对误差小于0.5%。

    The relative error of the velocity is less than 0.5%.

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  • 分析实验结果表明系统传输误差小于1%。

    The analytical and experimental results show that transmission errors of the system is smaller than 1%.

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  • 试验结果对比,二者最大相对误差小于10 %。

    The maximum relatively error between the results of test and theory is less than 10%.

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  • 最后通过实验数据验证系统泛化结果误差小于6%。

    Finally experimental data show that the system generalization error is less than 6%.

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  • 实验结果表明系统工作可靠测量误差小于0.2%。

    The result shows the system works reliably and the measure error is less than 0.2%.

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  • 测试结果表明并行电源系统负载均流误差小于1%。

    Experimental results show that the current sharing error at full load is kept within 1%.

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  • 试验结果表明方法测试误差小于2%,很好的重现性。

    The results show that the error of this method less than 2%(parallel error)and the repeatability are well.

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  • 实验结果表明补偿系统测量的相对误差小于0 2 %。

    The experiment results show that the measurement accuracy is less than reach 0 2% after compensating.

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  • 对其进行了浓度测量实验验证实验,测量误差小于0.14%。

    Liquid concentration measuring experiments and verifying experiments show that the measurement error is less than 0.14%.

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  • 复合卤化物颗粒各组分比例一致性较好,相对误差小于5% ;

    The component proportion of complex halide sphere keeps stable basically with the relative error< 5%.

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  • 经过涅耳菱体型相位延迟器件测试测量误差小于0.3%。

    The retardation of the Fresnel rhomb phase retarder was measured with the measurement error less than 0.3%.

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  • 宽和点火提前网络输出最大误差小于1%,平均误差小于0。

    The maximum network output error of fuel injection pulse width and ignition advance Angle is less than 1%, with an average error of less than 0.

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  • 文中间断函数进行了相位最小二乘方逼近,逼近误差小于传统方法

    All Phase least square approximation to the discontinuous signal is also introduced with less error than the traditional method.

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  • 本文简介一种输出能量最大相对误差小于2%的红宝石激光器及其结构特点

    This paper simply introduces a ruby laser with max. relative error of output energy< 2% and it's features about construction.

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  • 实验结果表明,本文给出方法能获得误差小于4%且压缩小于10 %。

    The experimental results show that the compression rate is less than 10% under 4% error.

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  • 相同条件下,最萃取精确方程计算结果误差小于现有最优萃取比方程。

    The calculation error of the optimized extractor by the precise equation is lower than the error by the simple equation.

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  • 动物试验结果相对误差小于5%,证明了方法可靠性实用意义。

    The result measuring liver volume of living animal is satisfying (the relative error is less than 5%), and shows the correctness and reliability of the method.

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  • 结果表明,“平均受害丛率”在不同调查者之间误差小于“平均受害株率”。

    The results showed that the error of mean DPRC was lower than that of mean DPRP.

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  • 配电监测系统模拟实验结果参量测量误差小于1%,误差满足设计要求

    The simulation experimental result is that the measure error is less than 1% and meet designing requirement.

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  • 不同浓度酒精溶液进行了测量实验,浓度测量绝对误差小于0.02%。

    Different concentrations of a set of alcohol solution were measured experimentally; the system measurement error is no more than 0.02 %.

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  • 纯砂岩校正精度百分误差小于5%;砂岩校正误差绝大多数小于10%。

    Correction accuracy for clean sand and most of the shaly sand is less than 5% and 10% respectively.

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  • 最后给出了文中算法理论误差曲线,分析表明测距误差小于辐照度测量误差

    At last, it's illustrated by the theoretic ranging error curve that the relative ranging error is less than that of the irradiance measurement.

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  • 有限元共轭变形进行了计算机模拟,模拟计算结果误差小于1%。

    The deformation of rolled piece in conjugate deep cut pass is simulated by finite element method. The error of simulated result is less than 1%.

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  • 通过与现场试验数据相比较的预测误差小于5%,对扭矩预测误差小于7%。

    Compared the calculated data with the field data, the errors of the hook load was less than 5% and that of torque was less than 7%.

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  • 本法用于分析模拟样品混合弱酸反应,并用离子色谱法进行对照计算误差小于7%。

    Simulated sample and mixed reaction solution of polybasic acids are analyzed in comparison with the results of ion-chromatography. The calculation error is less than 7%.

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  • 计算关联式具有较高精度热力学参数计算误差小于1 %,迁移特性参数误差小于4%。

    The calculation shows a high accuracy: the error is less than 1% in thermodynamic properties and 4% in thermophysical properties.

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  • 数值结果表明本方法测轨,向、垂迹方向误差小于0.1,沿迹方向误差小于1米。

    The numerical results show that the errors in radius and across-track are less than 0.1 m, and that in along-track less than 1 m.

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  • 数值结果表明本方法测轨,向、垂迹方向误差小于0.1,沿迹方向误差小于1米。

    The numerical results show that the errors in radius and across-track are less than 0.1 m, and that in along-track less than 1 m.

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