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1)  cross-machine direction(CD)
机器横向
2)  transverse maneuver
横向机动
1.
Through simulations,the predictive performances of the lead point of the transverse maneuverable target from the predictors based on the two order ploynomial model and the current statistics model are compared.
分析了二阶多项式模型对机动目标进行跟踪和预测时存在的不足 ,研究了“当前”统计模型在火控预测器中的应用 ;通过仿真计算 ,比较了基于“当前”统计模型的火控预测器和基于二阶多项式模型的火控预测器对横向机动目标提前点的预测性能。
3)  transverse modulator
横向调制器
4)  lateral damper
横向减振器
1.
Influence of lateral damper on locomotive riding quality;
横向减振器对机车平稳性能的影响
2.
A semi-vehicle simple model and whole-vehicle model are established by software SIMPACK, for analysis of the impact on the critical velocity of locomotive hunting movement and locomotive s major lateral dynamic performance index by the length of suspension pendulum and the lateral damper damping of motor drive unit.
利用多体动力学软件SIMPACK建立“弹性架悬”机车的半车简化模型和整车模型,分析电机驱动装置悬挂摆杆长度和电机驱动装置横向减振器阻尼对机车蛇行运动临界速度和机车主要横向动力学性能指标的影响,得出电机驱动装置悬挂摆杆长度和电机驱动装置横向减振器阻尼对机车动力学性能的影响规律。
3.
In order to control the lateral vibration of car-bodies of high speed trains in tunnel sections due to atmospheric pressure fluctuation, the single-car equivalent model of installing lateral dampers between car-bodies is set up, with the consideration of actually marshalled train model, the effect of lateral dampers between car-bodies on control of car-body vibration is discussed.
为了抑制高速列车在隧道内因气压波动引起的车体横向振动,建立了安装车体间横向减振器的单车等效模型,结合实际编组列车模型,探讨了车体间横向减振器对抑制车体振动的效果。
5)  lateral resistant
横向阻力器
6)  transverse injectors
横向喷注器
1.
The configurations of transverse injectors with a rearward facing step, gas/liquid coaxial injectors, nozzles with different throat diameters were studied by a series of tests.
采用分段可拆卸的点火器,对带后向台阶的横向喷注器、气液同轴喷注器、不同喉部直径的喷管等结构进行了试验研究。
补充资料:横向磁场中的空心超导圆柱体(hollowsuperconductingcylinderinatransversalmagneticfield)
横向磁场中的空心超导圆柱体(hollowsuperconductingcylinderinatransversalmagneticfield)

垂直于柱轴(横向)磁场H0中的空心超导长圆柱体就其磁性质讲是单连通超导体。徐龙道和Zharkov由GL理论给出中空部分的磁场强度H1和样品单位长度磁矩M的完整解式,而在`\zeta_1\gt\gt1`和$\Delta\gt\gt1$条件下为:

$H_1=\frac{4H_0}{\zeta_1}sqrt{\frac{\zeta_2}{\zeta_1}}e^{-Delta}$

$M=-\frac{H_0}{2}r_2^2(1-\frac{2}{\zeta_2})$

这里r1和r2分别为空心柱体的内、外半径,d=r2-r1为柱壁厚度,ζ=r/δ(r1≤r≤r2),Δ=d/δ,δ=δ0/ψ,δ0为大样品弱磁场穿透深度,ψ是有序参量。显然此时H1→0,M→-H0r22/2,样品可用作磁屏蔽体。当$\zeta_1\gt\gt1$,$\Delta\lt\lt1$时,则

H1=H0/(1 ζ1Δ/2),
M=-H0r23[1-(1 ζ1Δ/2)-1]。

若$\zeta_1\Delta\gt\gt1$,则$H_1\lt\ltH_0$或H1≈0。所以,虽然$d\lt\lt\delta$,但磁场几乎为薄壁所屏蔽而难于透入空心,称ζ1Δ/2为横向磁场中空心长圆柱体的屏蔽因子。当$\zeta_1\Delta\lt\lt1$时,则H1≈H0,磁场穿透薄壁而均进入空腔,失去屏蔽作用,此时M≈0。类似于实心小样品,由GL理论可求出薄壁样品的临界磁场HK1,HK,HK2和临界尺寸等。

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