不均的磁场对自组装磁柱的集体行为
Juan J Huaroto1, Franco N Piñan Basualdo1, Dionne Lisa Roos Ariëns1
1Surgical Robotics Laboratory, Department of Biomechanical Engineering, University of Twente, 7522 NB Enschede, The Netherlands.
概括
本研究探讨使用非均磁场来控制自组装磁柱. 这种新的方法使磁性微粒子集体能够进行先进的操纵,运动和独立执行.
科学领域:
- 物理 物理学 物理
- 材料科学 材料科学 材料科学
- 微流体学 微流体学
背景情况:
- 自组装的磁柱对于控制微粒集体至关重要.
- 目前的方法依赖于均的,时间变化的磁场.
- 不均磁场对磁柱起动的潜力仍然未被探索.
研究的目的:
- 调查使用不均的磁场来驱动自组装的磁柱.
- 展示新的操纵,机动和执行能力.
- 探索磁柱在狭窄和动态环境中的适应性.
主要方法:
- 利用一个九线圈电磁系统来产生不均的磁场.
- 分析了减少铁微粒的静电磁自组合.
- 在不均和时间变化的场域下研究了动态反应.
- 展示了玻璃珠的二维操纵和在流体管中执行.
主要成果:
- 实现对象操纵,上游/下游运动,以及独立的驱动.
- 确定了磁柱的四种不同的动态响应模式.
- 在狭窄的流体环境中展示了支柱的适应性.
- 成功启动了两个独立的磁柱集群.
结论:
- 不均的磁场提供了一个多功能平台,用于驱动自组装的磁柱.
- 这种方法可以对形态重构,对象操纵和运动进行高级控制.
- 这些发现为微粒子集体应用开辟了新的途径.
相关概念视频
Magnetic Fields
7.1K
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
A magnetic field is defined by the force that a charged particle experiences...
7.1K
Potential Due to a Magnetized Object
757
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
757
Paramagnetism
3.0K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
3.0K
Magnetic Field due to Moving Charges
11.4K
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...
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...
11.4K
Diamagnetism
2.9K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.9K
Magnetic Field Of A Current Loop
6.2K
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
6.2K


