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相关概念视频

Unsymmetric Bending - Angle of Neutral Axis01:15

Unsymmetric Bending - Angle of Neutral Axis

438
Unsymmetrical bending occurs when a structural member is subjected to bending moments in a plane that does not align with the member's principal axes. This scenario typically arises in beams and other structural components when loads are applied at non-ideal angles, introducing complexities in stress analysis.
When a bending moment is applied at an angle θ concerning the vertical axis of a symmetrical member, it can be resolved into components along the member's principal...
438
Unsymmetric Bending01:18

Unsymmetric Bending

435
Unsymmetrical bending occurs when the bending moment applied to a structural member does not align with its principal axis. This misalignment leads to complex stress distributions and deflection patterns that differ from those in symmetrical bending, and are essential for designing structures to withstand different loading conditions. In unsymmetrical bending, the neutral axis—where stress is zero—does not necessarily align with the geometric axes of the cross-section. The...
435
Design of Prismatic Beams for Bending01:23

Design of Prismatic Beams for Bending

370
The design of prismatic beams, structural elements with a uniform cross-section, focuses on ensuring safety and structural integrity under load. The design process begins by determining the allowable stress, either from material properties tables, or by dividing the material's ultimate strength by a safety factor. This safety factor is essential for accommodating uncertainties, and varies depending on the material—timber, steel, or concrete—with each having unique strength and...
370
Bending01:10

Bending

430
Pure bending is a fundamental concept in structural mechanics, essential for understanding how materials deform under symmetrical loads without direct forces. Pure bending occurs when prismatic members, such as beams, are subjected to equal and opposite moments that induce bending. The phenomenon is crucial as it allows for predicting stress distributions without the influence of axial or shear forces.
In pure bending, the bending stress in a beam is calculated based on the bending moment and...
430
Angle of Twist - Elastic Range01:13

Angle of Twist - Elastic Range

392
Consider a cylindrical shaft with a length denoted by L and a consistent cross-sectional radius referred to as r. This shaft undergoes a torque at the free end. The highest shearing strain within the shaft is directly proportional to the twist angle and the radial distance from the shaft axis. When the shaft behaves elastically, this shearing strain can be articulated using variables such as the applied torque, radial distance, the polar moment of inertia, and the modulus of rigidity. By...
392
Singularity Functions for Bending Moment01:18

Singularity Functions for Bending Moment

274
Singularity functions simplify the representation of bending moments in beams subjected to discontinuous loading, allowing the use of a single mathematical expression. For a supported beam AB, with uniform loading from its midpoint M to the right side end B, the approach involves conceptual 'cuts' at specific points to determine the bending moment in each segment. By cutting the beam at a point between A and M, the bending moment for the segment before reaching midpoint M is represented...
274

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超紧的多模式波导曲时具有任意的曲角度.

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    科学领域:

    • 光子学是指光子学的使用方法.
    • 集成光学 集成光学 集成光学
    • 纳米技术纳米技术

    背景情况:

    • 在芯片上的模式分割复杂化 (MDM) 需要紧的波导路由,以实现更高的集成和灵活的布局.
    • 现有的多模波导曲线 (MWB) 仅限于90°,阻碍了复杂的芯片内设计.

    研究的目的:

    • 提出和演示具有任意曲角度的超紧的多模波导曲线 (MWB).
    • 提高芯片上MDM系统的设计灵活性和集成密度.

    主要方法:

    • 在在绝缘体 (SOI) 平台上设计和实验证明了15°,30°,45°和60°的曲角度的MWB.
    • 采用双贝齐尔轮来优化MWB的轨迹.
    • 支持前三种横向电 (TE) 模式.

    主要成果:

    • 实现了超紧的MWB,其足迹只有7.5 × 5.1 μm2.2.
    • 已证明插入损失低于0.417dB,模式间交叉声低于-16.6dB.
    • 在1500-1600纳米的宽波长范围内运行,适用于所有三个TE模式.

    结论:

    • 拟议的任意角MWB显著提升了芯片上的MDM功能.
    • 这些MWB作为复杂的波导布局和S曲的多功能构建块.
    • 为超紧和高度集成的芯片上MDM系统铺平了道路.