THE RULE OF PARALLELOGRAM FOR ELEMENTARY PARTICLES AND FOR DIFFERENT TYPES OF FORCES

 

The world around us is woven from Forces, as Force - is Ether and Ether in the universe is everywhere. Force - this is what tends to move something from the place.

One of the differences between mechanics of bodies and mechanics of stable elementary particles is that the particles under the influence of forces may only move.

They can not to be deformed and disintegrate for one reason - they are inseparable. While a body (or even unstable particle - conglomerate), when a force acts on it (or forces), may move and be deformed and broken down.

In mechanics of bodies (in classical mechanics) there is a wonderful way to help find out in which direction the body will tend to move under an influence of all forces that act on it. Also, to calculate the resultant forces. This method is well known as the Rule of the Parallelogram of Forces.

It was opened by Galileo Galilei, and the precise definition of this rule was given by Pierre Varinon in 1687.

The Rule of Parallelogram of Forces says that the resultant force vector is the diagonal of the parallelogram formed by the vectors of two summands of forces as on the sides.

This rule surprisingly well helps to calculate precisely the direction in which a body will move (or will try to move) if it is acted upon more than one of the Force. And in our world every body is always at the same time experiencing an impact of the myriad of external forces (because any particle in any chemical element - is a source of Force).

Moreover this Rule is perfectly suited for elementary particles. With it, we can see the direction in which an elementary particle will shift at every moment of time if two or more Forces act on it at the same time. And also we can know the ratio of the values ​​of Forces - an original and a resultant. And the type of each of the forces can be any. The diagonal of Parallelogram - this is an indication of direction, as well as a measure of the resultant Force. However, please note an important factor - a new Parallelogram of Forces should be built to each next moment of being of the particle.

Let's take a little closer look at the essence of the Rule of Parallelogram. And in the course of this analysis we will give it a slightly different name – the Rule of Subordination to the Dominant Force. This will allow us to better understand the characteristics of behaviour of elementary particles (and any conglomerates of particles) because the Rule of Parallelogram in the form of which it exists now, not fully reveal the meaning of what is happening with the particle when more than one Force affects on it. For example, it says nothing about the fact that there are different types of Forces.

The Dominant Force – is the Force which is greater in magnitude. As we said earlier, a magnitude of a Force - is the rate of ethereal flow entraining the particle. Moreover, Ether just fills a particle can act as an ethereal flow (as in the case of the Force of Pressure of the particle surface).

The Rule of Subordination to the Dominant Force (the Rule of Parallelogram) represents that the particle, on which act more than one Force, to the greatest extent will be subject to the higher of them. What does this mean? This means that the vector of resultant forces at each moment will be more biased towards the vector of Force with the highest magnitude. That is, the biggest Force prevails, but other Forces also have an effect on the position of the resultant force vector. You can further specify the name of the rule - Subordination to the Dominant Force with an accounting of actions of the remaining forces.

The Dominant Force shifts the vector of resultant Force in its own direction more than others. And other, smaller forces do not give this vector to fully submit to this biggest Force. They pull the vector in their direction in proportion to their magnitude.

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In general, in the analysis of any situation in which an elementary particle is influenced by more than one force it is necessary to consider a number of factors. First, you need to know how many forces acting on the particle and the value of each of them. Secondly, you need to know at what angle the vectors of Forces are placed one against the other. And third, you must consider the type each of forces. Only evaluating all these factors, we can try to calculate the direction and velocity of a particle at every moment of time. Let's take a little closer look at these factors.








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