Radiation Pressure of a Monochromatic Plane Wave on a Flat Mirror
... While today we might prefer using the Lorentz force law rather than the stress tensor to deduce eq. (22), the Lorentz force law is based on an understanding of electric charge not available in Maxwell’s time. Hence, it is all the more impressive that the concept of radiation pressure was understood ...
... While today we might prefer using the Lorentz force law rather than the stress tensor to deduce eq. (22), the Lorentz force law is based on an understanding of electric charge not available in Maxwell’s time. Hence, it is all the more impressive that the concept of radiation pressure was understood ...
[ G69 ]
... centre surrounded by a sphere of electrification coutaining a charge -T-Ne supposed unifarmly distributed throughout a sphere of radius R. e is the fundamental unit of charge, which in this paper is taken as 4"65x 10 -1~ E.s. unit. W e shall suppose that for distances less than 10 -12 cm. the centra ...
... centre surrounded by a sphere of electrification coutaining a charge -T-Ne supposed unifarmly distributed throughout a sphere of radius R. e is the fundamental unit of charge, which in this paper is taken as 4"65x 10 -1~ E.s. unit. W e shall suppose that for distances less than 10 -12 cm. the centra ...
Forces and movement of small water droplets in oil due to applied
... the measured drag forces. The result presented show good agreement between the measured force and the calculated dielectric force. In this case the droplet was small compared to the distance between electrodes, and the degree of inhomogenity is low. The results indicate that the measured force oscil ...
... the measured drag forces. The result presented show good agreement between the measured force and the calculated dielectric force. In this case the droplet was small compared to the distance between electrodes, and the degree of inhomogenity is low. The results indicate that the measured force oscil ...
Today`s Powerpoint
... Two identical metal spheres are firmly fastened to and electrically insulated from frictionless plastic air pucks that ride on an air table as shown below. The pucks are held in place as a charge of 2.0 x 10-8 C is placed on sphere A on the left and a charge of 6.0 x 10-6 C is placed on sphere B on ...
... Two identical metal spheres are firmly fastened to and electrically insulated from frictionless plastic air pucks that ride on an air table as shown below. The pucks are held in place as a charge of 2.0 x 10-8 C is placed on sphere A on the left and a charge of 6.0 x 10-6 C is placed on sphere B on ...
Slide 1
... We use the symbol B for magnetic field. Remember: magnetic field lines point away from north poles, and towards south poles. S ...
... We use the symbol B for magnetic field. Remember: magnetic field lines point away from north poles, and towards south poles. S ...
Electrostatics
Electrostatics is a branch of physics that deals with the phenomena and properties of stationary or slow-moving electric charges with no acceleration.Since classical physics, it has been known that some materials such as amber attract lightweight particles after rubbing. The Greek word for amber, ήλεκτρον electron, was the source of the word 'electricity'. Electrostatic phenomena arise from the forces that electric charges exert on each other. Such forces are described by Coulomb's law.Even though electrostatically induced forces seem to be rather weak, the electrostatic force between e.g. an electron and a proton, that together make up a hydrogen atom, is about 36 orders of magnitude stronger than the gravitational force acting between them.There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to your hand after you remove it from a package, and the attraction of paper to a charged scale, to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and the operation of photocopiers. Electrostatics involves the buildup of charge on the surface of objects due to contact with other surfaces. Although charge exchange happens whenever any two surfaces contact and separate, the effects of charge exchange are usually only noticed when at least one of the surfaces has a high resistance to electrical flow. This is because the charges that transfer to or from the highly resistive surface are more or less trapped there for a long enough time for their effects to be observed. These charges then remain on the object until they either bleed off to ground or are quickly neutralized by a discharge: e.g., the familiar phenomenon of a static 'shock' is caused by the neutralization of charge built up in the body from contact with insulated surfaces.