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加热圆柱体 heated cylinder英语短句 例句大全

时间:2020-07-12 16:27:40

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加热圆柱体 heated cylinder英语短句 例句大全

加热圆柱体,heated cylinder

1)heated cylinder加热圆柱体

2)hot cylinder热圆柱体

1.Processing the fringe images before and after heating thehot cylinder using the arithmetic o.介绍一种利用干涉原理测量热圆柱体表面温度的方法,首先,在对圆柱体周围空气的温度和折射率分布特点进行分析的基础上,建立Fizeau等厚干涉系统,调整光路使干涉条纹稳定且等间距。

3)vertical axis installed collector圆柱吸热体

1.In case of the center-to-center distance ofvertical axis installed collector .对建筑物南立面竖置和东西轴向横置的圆柱吸热体真空管集热器的日、年能量收益,以及上述两种集热器管中心距与能量收益的关系进行了分析研究。

4)cylinder heat conduction圆柱体导热

5)multi-beam-stiffened cylindrical shell多加筋圆柱壳体

1.Due to its structural characteristics of amulti-beam-stiffened cylindrical shell,it is widely used in engineering practices,so it is important to do vibration study on an elastic beam-stiffened cylindrical shell.弹性多加筋圆柱壳体由于其结构的特点,广泛应用于工程实际,因此对其进行振动研究具有重要的工程价值和应用意义。

6)unstiffened cylindrical shell加肋圆柱壳体

英文短句/例句

1.Sound radiation characteristics of finite double-layer annular-plate stiffened cylindrical shells有限长双层加肋圆柱壳体的声辐射特性

2.The Vibration and Acoustic Radiation from Axially Stiffened Finite Cylindrical Shells in Water水中有限长纵向加肋圆柱壳体振动与声辐射

3.Vibration and acoustic radiation of axially stiffened finite cylindrical shells in water水中有限长纵向加肋圆柱壳体振动与声辐射影响因素研究

4.Numerical Analysis of Vibration and Acoustic Radiation Characteristics of Stiffened Cylindrical Shells;加肋圆柱壳振动声辐射特性的数值计算研究

5.A Novel Method for Analyzing Circumferential Stiffened Non-Circular Cylindrical for Shell;环肋加强非圆柱壳强度计算的一种新方法

6.Optimal Design of Ring-stiffened Cylindrical Shell Based on ISIGHT基于遗传算法的加肋圆柱壳结构动力优化分析

7.Sound Radiation Analysis of Ribbed Cylindrical Shells with Viscoelastic Layer and Noise Characteristics Analysis;敷设阻尼层的加肋圆柱壳辐射性能及噪声特性分析

8.Study on Vibration and Acoustic Radiation from Tow Concentric Ring-reinforced Cylindrical Shells Covered with Sound-absorbing Layers;敷设消声瓦的双层加肋圆柱壳的振动和声辐射研究

9.The Reliability of Submarines Pressure Cylindrical Ring Hull潜艇耐压环肋圆柱壳结构可靠性分析

10.Vibration Characteristics Analysis of Submerged Ring-stiffened Cylindrical Shells;水下环肋圆柱壳的自由振动特性分析

11.Research on the residual strength of damaged ring-stiffened cylindrical shell环肋圆柱壳受损伤后的剩余强度探讨

12.The Strength Analysis and Transfer-Segment Design of Ring-stiffened Cylindrical Shells;带肋圆柱壳结构的强度分析和过渡段设计研究

13.The Strength Sensitivity Analysis of Ribbed Cylindrical Shell Construction Based on the Finite Element Method带肋圆柱壳结构强度灵敏性有限元法分析

14.Optimization of ring-stiffened circular cylindrical shells with natural frequency constraints计及频率约束的潜艇环肋圆柱壳优化设计研究

15.Researches on the Structural Response of Cylindrical Shell under MDF Impulse;柔爆索爆炸加载下圆柱壳体结构响应研究

16.Vibroacoustic Analysis of a Finite Stiffened-Cylindrical Shell Closed by Circular Plates;两端用圆板封口的环肋柱壳振动声辐射性能分析

17.Strength reliability analysis of ring-stiffened cylindrical shells based on response surface method基于响应面法的带肋圆柱壳结构强度可靠性分析

18.Analysis of acoustic radiation of a ring-stiffened cylindrical shell with finite length in underwater based on Riccati transfer matrix method基于Riccati传递矩阵法分析水下有限长环肋圆柱壳的声辐射性能

相关短句/例句

hot cylinder热圆柱体

1.Processing the fringe images before and after heating thehot cylinder using the arithmetic o.介绍一种利用干涉原理测量热圆柱体表面温度的方法,首先,在对圆柱体周围空气的温度和折射率分布特点进行分析的基础上,建立Fizeau等厚干涉系统,调整光路使干涉条纹稳定且等间距。

3)vertical axis installed collector圆柱吸热体

1.In case of the center-to-center distance ofvertical axis installed collector .对建筑物南立面竖置和东西轴向横置的圆柱吸热体真空管集热器的日、年能量收益,以及上述两种集热器管中心距与能量收益的关系进行了分析研究。

4)cylinder heat conduction圆柱体导热

5)multi-beam-stiffened cylindrical shell多加筋圆柱壳体

1.Due to its structural characteristics of amulti-beam-stiffened cylindrical shell,it is widely used in engineering practices,so it is important to do vibration study on an elastic beam-stiffened cylindrical shell.弹性多加筋圆柱壳体由于其结构的特点,广泛应用于工程实际,因此对其进行振动研究具有重要的工程价值和应用意义。

6)unstiffened cylindrical shell加肋圆柱壳体

延伸阅读

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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