连续带电物质的离散状态

C. Simáne
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引用次数: 2

摘要

通过在欧拉方程中引入非机械力密度等于相应势与物质密度梯度的乘积,并假设动力学过程具有扩散特性,得到了具有正负内源的连续性方程。这些源与静电、动能和固有能量密度的代数和成正比,比例常数为扩散常数D = h/2m的反值,取负号。如果连续性方程的解在物体的任何一点上成立,则得到稳态,只有能量维的常数E的离散值进入连续性方程才有可能。连续性方程可转化为具有量子势的玻姆方程,并可化简为相应的薛定谔方程求解。因此,物理学的空间概念,Vol. V, No. 3 (2008) DOI: 10.2478/v10005-007-0043- 3 499物质密度的分布是由薛定谔波函数的平方给出的。一旦密度分布函数已知,就可以计算扩散过程中的速度~u,扩散过程是确定的。与扩散过程相叠加的是速度为~v的经典运动,对于该运动,无内部物质源的连续性方程成立。物理概念500 Vol. V . No. 3(2008)连续带电物质的离散态
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Discrete States of Continuous Electrically Charged Matter
By introducing in the Euler equation non mechanical (mesic) force densities equal to the products of corresponding potentials and gradient of the matter density, and supposing that the dynamical process has a diffusion character, the equation of continuity with internal sources (both positive and negative) is obtained. These sources are proportional to the algebraical sum of electrostatic, kinetic and proper energy densities, the constant of proportionality being the inverse value of the diffusion constant D = h/2m, taken with negative sign. The stationary state is obtained if the solution of the continuity equation holds in any point of the object, which is possible only for discrete values of the constant E with dimension of energy, entering in the equation of continuity. The equation of continuity can be transformed to the Bohm equation with the quantum potential, which may be solved by reducing it to the corresponding Schrodinger equation. Thus the spatial Concepts of Physics, Vol. V, No. 3 (2008) DOI: 10.2478/v10005-007-0043-6 499 distribution of the density of matter is given by the square of the Schrodinger wave function. Once the density distribution function is known, the velocity ~u in the diffusion process can be calculated and the process is deterministic. Superimposed to the diffusion process is the classical motion with velocity ~v, for which the equation of continuity without internal sources of matter holds. 500 Concepts of Physics, Vol. V, No. 3 (2008) Discrete states of continuous electrically charged matter
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