﻿ An Extension of the Correspondence Between Statically and Dynamically Determined Force Fields
San José State University

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Thayer Watkins
Silicon Valley
U.S.A.

An Extension of the Correspondence
Between Statically and Dynamically
Determined Force Fields

## Background

Consider the following two situations in mathematical physics.

## Corrsponding Static and Dynamic Situations

• A generic charge is distributed over some geometric region R and its density is known. The generic charge could be gravitational mass, electrical charge, magnetic charge or nucleonic charge (the charge associated with the nuclear strong force). The generic charge density is given by a function ρ(ζ), where ζ is a position vector. The force vector at any location Z is determined. This is the static situation.
• The center of a distributed generic charge of magnitude q traverses the same geometric region R. A probability density function for the center of the distributed charge is determined based on the proportion of the time the center spends at various locations. The expected value of the force at any location can be computed based upon that probability density function. This is the dynamic situation.

Suppose the function giving the force dF on a unit charge at position Z due to a charge of dq located at position ζ is given by

#### dF = F(s)dq

where s is the distance between point ζ and point Z and F(s) is a vector function. F(s) is general but the most important cases are the ones in which F(s) dependent on the inverse separation distance squared. This distance between Z and ζ is given by |Z−ζ|. The increment of charge is given by ρ(ζ)dR, where dR is a volume element.

The intensity vector G of the field at Z is then given by

#### G(Z) = ∫R F(|Z−ζ|)ρ(ζ)dR

The intensity at Z is constant so the expected value of G, E{ }, is just G; i.e.,

## The Dynamic Situation

On the other hand in the dynamic situation the field intensity at Z fluctuates. When the center of the distributed charge Q is at point ζ the force dH on a unit charge at point Z due to the charge of dq at ξ is given by

#### dH = F(|Z−ξ|)dq

The charge density dq at ξ is a function of the distance between ξ and ζ, say σ(|ξ-ζ|). The total force H is then given by the integration over the volume V of the distributed charge. Thus the force at point Z is

#### H(Z) = ∫V F(|Z−ξ|)σ(|ξ-ζ|)dV

H(Z) is a function of time because ζ is a function of time.

Let P(ζ) be the probability density function representing the proportion of the time the distributed charge center spends at point ζ. For a point traveling along a path at a velocity of v the probability density function is given by

#### P(ζ) = 1/(T|v(ζ|)

where T is the total time required to traverse the path.

The expected value of the vector of field intensity H is then given by

## The Correspondence

Note that if the charge density ρ(ζ) is given by [∫Vσ(|ξ-ζ|)dV]P(ζ) then the dynamic case problem is mathematically identical to the static case problem. This correspondence points up the significance of the time-spent probability density function to mechanics. It is as significant as the spatial distribution of any charge.

## Periodicity of Atomic and Subatomic Motion

The rate of rotation of an electron in a hydrogen atom, according to the Bohr model, is easily determined. The electrostatic force between an electron and a proton has to be balanced by the centrifugal force on the electron; i.e.,

#### Ge²/r² = mrω²

where G is a constant, e is the electrical charge of the electron and the proton, m is the mass of the electron and r is the orbit radius for the electron. Therefore

#### ω² = Ge²(m/r³)

The frequency ν is equal to ω/(2π). This works out to be 6.6×1015 times per second; i.e., 6.6 quadrillion times per second. Any observation will involve a time-average and at the above frequency the observation will be equal to the expected value. Thus the observed world is the world of the dynamic appearances of physical systems. In the case of electrons this would be elliptical rings.

## Conclusions

Consider a generic charge distribution with a density function σ(s) where s is the distance from the center ζ of the distribution and ζ traverses a periodic path with a spent-time probability density function of P(ζ). This dynamic system has the same expected value for force at a point Z as a static charge distribution density equal to P(ζ)Q where Q is equal to ∫Vσ(|ξ-ζ|)dV.

With subatomic particles executing cycles at rates on the order of quadrillions of times per second the observed quantities are equal to their expected values.