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Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

993
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
993
Torque On A Current Loop In A Magnetic Field01:13

Torque On A Current Loop In A Magnetic Field

4.1K
The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
4.1K
Magnetic Vector Potential01:15

Magnetic Vector Potential

680
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
680
Divergence and Curl of Magnetic Field01:26

Divergence and Curl of Magnetic Field

3.0K
The magnetic field due to a volume current distribution given by the Biot–Savart Law can be expressed as follows:
3.0K
Symmetry in Maxwell's Equations01:28

Symmetry in Maxwell's Equations

3.5K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
3.5K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

8.8K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
8.8K

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Scanning SQUID Study of Vortex Manipulation by Local Contact
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基于准塔尔博特效应的旋转阵列生成.

JiaoHui Li, FaJing Li, KeLi Chen

    Journal of the Optical Society of America. A, Optics, image science, and vision
    |September 14, 2023
    PubMed
    概括
    此摘要是机器生成的。

    一种新的没有镜头的技术使用准塔尔博特效应和第四阶交叉相生成可调节的光阵列. 这种方法为各种应用提供了对阵列生成位置和形状的灵活控制.

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    科学领域:

    • 光学和光子学 在光学和光子学.
    • 衍射物理 衍射物理
    • 光学计量学 在光学计量学

    背景情况:

    • 光学阵列对于光学子和微观操纵等应用至关重要.
    • 现有的生成光学阵列的方法通常需要复杂的光学设置,限制灵活性.

    研究的目的:

    • 提出和演示一种新的没有镜头的方法,用于生成具有可调节参数的光学阵列.
    • 为了探索控制阵列生成位置和结构的控制,使用量身定制的跨相调制.

    主要方法:

    • 用带有第四阶交叉相的旋转束照明2D周期性正弦格的照明.
    • 利用准塔尔博特效应在弗雷内尔衍射区域生成连续状阵列结构.
    • 调节第四阶交叉相的常数参数以控制阵列生成位置和形状.

    主要成果:

    • 成功生成了没有镜头的连续光阵列.
    • 通过调整第四阶交叉相参数,证明了阵列生成位置的调整性.
    • 通过使用更高阶交叉相实现了多边形光学阵列的生成.

    结论:

    • 拟议的无透镜方法提供了一种灵活和高效的方法来生成可调节的光阵列.
    • 这种技术扩大了无透镜光学阵列在各种科学和技术领域的适用性.
    • 潜在的应用包括先进的光学操纵,多颗粒选和高分辨率显微镜.