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Ludong University Journal

A Tentative Explanatory Theory on Quantum Phenomenon

Luo Ling-xiao

Published Jan 1, 2007• 0 citations
OpenAlex

Abstract

The view of that the move of an uniform motion particle is not even is considered in this paper.In fact,the particle is in pulsation,and its pulsation velocity is in cyclical change.The relation between the particle's kinetic energy and its pulsation period is given.Furthermore,by using methods of elementary mathematics,the harmonic oscillator's and a series of other bound state's energy levels can be deduced.

Related papers

Speculation on Describing All Uniform Motion by the Same Constant

Francesco R. Ruggeri

It is well known that uniform classical motion may be described by a constant velocity ie. one which does not change in time. A different constant number, however, is needed for each velocity so uniform motion in general is not being represented by a single number in this scenario. In (1) we noted how a single number such as energy E could represent systems linked to different physical theories. For example, a classical particle may move according to .5mvv + V(x) = E where v is velocity. On the one hand a single number E describes each point (x,t), but at each point there is different detailed motion such as potential energy, velocity etc. Similarly in a Maxwell-Boltzmann gas exp(- ( .5mvv + V(x))/T) is proportional to probability. For a given E1 = .5mvv + V(x) there are many v,x points which have the same E1 and thus probability. Finally for a quantum bound state there is a single En (energy) even though there is a potential energy V(x) and average kinetic energy -1/2m d/dx dW/dx / W (W=wavefunction) at each x. In this note we ask whether a single number may apply to all uniform motion with this constant being equal then to different details in each system. The reason we ask this question is that we think a given constant velocity, say 25 m/s, does not characterize uniform motion. The problem we argue is one of resolution of x and t. For example, 25 m/s may characterize very erratic motion from x=0 to x=25 m in a period of 1 sec. This simply means the average speed is 25 m/s, not that the motion is uniform. To bypass this argument one may suggest perfect x, t resolution for all speeds. In such a case erratic motion may only exist in an extremely tiny dx or dt which approaches 0. This suggests there exists a spacetime (x,t) which may analyze all uniform motion with infinitesimal precision i.e is all-seeing. It is not clear that there exists any physical mechanism for this. We argue instead that velocity is a property of a moving object, not of spacetime. An object undergoes force over distance and receives a velocity which is one of its properties. In such a case infinitesimal resolution of t and x may not apply to all velocities. In fact if v velocity is a property of the object, x,t resolution may also be associated properties. Thus details of a particular uniform motion are not simply v (which yields p and E=pp/2m nonrelativistically), but also x and t resolution. Is it possible that these details may combine to create a single constant representing all uniform motion? We argue that this is possible and that this constant is in fact the free particle action -Et+px which holds both relativistically and nonrelativistically. For t proportional to 1/E and p proportional to 1/p (same proportionality constant) one has a single constant, Action=0, describing all uniform motion. We however, arrive at the form -Et+px without using notions of action or Lagrangian.

•Oct 17, 2022•0 citations

The Correlation Chart with Elementary Particle Pulsation

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1) An elementary particle is the quantum which assumed darkness energy to meet outer space a place and repeats a particle trip, a wave trip, the pulsation of the minus number particle trip. 2)The pulsation is expressed in the wave function of the Schrodinger equation, and the real number axis of the equation is equivalent to horizon (mc²=0) of the pulsation model. 3)The wave packet representing the particle which an equation shows is elementary particle pulsation, and the natural collapse of the wave packet does not occur. It is not a pilot wave leading a particle. 4)The elementary particle has minus number mass by original mass, a minus number particle trip by a particle trip, and it is a particle having size intermittently, and it is by the wave trip with the point that there is not of the size. 5)All mass of the elementary particle converts it into energy by a pulsatile wave trip and are released in the horizon (three-dimensional space) and it is absorbed again and becomes the particle. 6)Negative energy is offset plus every pulsation 1 cycle, and the energy grand total of the place of the dark energy to pulsate becomes zero. (supersymmetry).

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American Journal of Physics•May 1, 1964•33 citations

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Dali Xueyuan xuebao•Jan 1, 2008•0 citations

K

P. W. Atkins

Abstract The kinetic energy, T, of a particle is the energy it possesses on account of its motion. In classical mechanics, the kinetic energy is related to the linear momentum p by T= p2 /2m (and by T=½mv2, where v is the velocity). In quantum mechanics the kinetic energy is proportional to the second derivative of the wavefunction (Box K.1). As the wavefunction becomes more sharply curved, so the kinetic energy of the particle increases. Conversely, a particle with a wavefunction that is almost flat everywhere has almost zero kinetic energy.

•Apr 11, 1991•0 citations
The view of that the move of an uniform motion particle is not even is considered in this paper.In fact,the particle is in pulsation,and its pulsation velocity is in cyclical change.The relation between the particle's kinetic energy and its pulsation period is given.Furthermore,by using methods of elementary mathematics,the harmonic oscillator's and a series of other bound state's energy levels can be deduced.
It is well known that uniform classical motion may be described by a constant velocity ie. one which does not change in time. A different constant number, however, is needed for each velocity so uniform motion in general is not being represented by a single number in this scenario. In (1) we noted how a single number such as energy E could represent systems linked to different physical theories. For example, a classical particle may move according to .5mvv + V(x) = E where v is velocity. On the one hand a single number E describes each point (x,t), but at each point there is different detailed motion such as potential energy, velocity etc. Similarly in a Maxwell-Boltzmann gas exp(- ( .5mvv + V(x))/T) is proportional to probability. For a given E1 = .5mvv + V(x) there are many v,x points which have the same E1 and thus probability. Finally for a quantum bound state there is a single En (energy) even though there is a potential energy V(x) and average kinetic energy -1/2m d/dx dW/dx / W (W=wavefunction) at each x. In this note we ask whether a single number may apply to all uniform motion with this constant being equal then to different details in each system. The reason we ask this question is that we think a given constant velocity, say 25 m/s, does not characterize uniform motion. The problem we argue is one of resolution of x and t. For example, 25 m/s may characterize very erratic motion from x=0 to x=25 m in a period of 1 sec. This simply means the average speed is 25 m/s, not that the motion is uniform. To bypass this argument one may suggest perfect x, t resolution for all speeds. In such a case erratic motion may only exist in an extremely tiny dx or dt which approaches 0. This suggests there exists a spacetime (x,t) which may analyze all uniform motion with infinitesimal precision i.e is all-seeing. It is not clear that there exists any physical mechanism for this. We argue instead that velocity is a property of a moving object, not of spacetime. An object undergoes force over distance and receives a velocity which is one of its properties. In such a case infinitesimal resolution of t and x may not apply to all velocities. In fact if v velocity is a property of the object, x,t resolution may also be associated properties. Thus details of a particular uniform motion are not simply v (which yields p and E=pp/2m nonrelativistically), but also x and t resolution. Is it possible that these details may combine to create a single constant representing all uniform motion? We argue that this is possible and that this constant is in fact the free particle action -Et+px which holds both relativistically and nonrelativistically. For t proportional to 1/E and p proportional to 1/p (same proportionality constant) one has a single constant, Action=0, describing all uniform motion. We however, arrive at the form -Et+px without using notions of action or Lagrangian.
1) An elementary particle is the quantum which assumed darkness energy to meet outer space a place and repeats a particle trip, a wave trip, the pulsation of the minus number particle trip. 2)The pulsation is expressed in the wave function of the Schrodinger equation, and the real number axis of the equation is equivalent to horizon (mc²=0) of the pulsation model. 3)The wave packet representing the particle which an equation shows is elementary particle pulsation, and the natural collapse of the wave packet does not occur. It is not a pilot wave leading a particle. 4)The elementary particle has minus number mass by original mass, a minus number particle trip by a particle trip, and it is a particle having size intermittently, and it is by the wave trip with the point that there is not of the size. 5)All mass of the elementary particle converts it into energy by a pulsatile wave trip and are released in the horizon (three-dimensional space) and it is absorbed again and becomes the particle. 6)Negative energy is offset plus every pulsation 1 cycle, and the energy grand total of the place of the dark energy to pulsate becomes zero. (supersymmetry).
Abstract The kinetic energy, T, of a particle is the energy it possesses on account of its motion. In classical mechanics, the kinetic energy is related to the linear momentum p by T= p2 /2m (and by T=½mv2, where v is the velocity). In quantum mechanics the kinetic energy is proportional to the second derivative of the wavefunction (Box K.1). As the wavefunction becomes more sharply curved, so the kinetic energy of the particle increases. Conversely, a particle with a wavefunction that is almost flat everywhere has almost zero kinetic energy.