T H E  M E T H O D  O F  F L I G H T

By Henryk Szubinski

the format for underwater displacement

where the arms follow along in lability by sinusodial reflex

as a comparative of fluid based similarity in molecular structures ;

 the concept presented here regards a swimming style that incoorporates both the surface displacability and the fluid system of immersion

the format of elasticity is as important as the formats of both planes divided by a saggital divisive on the reference of the motion specifics in molecular acid similarities of displacement and the crucial need for flatness as the minimal planarity of a surface area that connects the formats of displacement into one plane.

 

Acid-base imbalance has several possible causes. An excess of acid is called acidosis and an excess in bases is called alkalosis. Acidosis is much more common than alkalosis. The imbalance is compensated by negative feedback to restore normal values. There are various renal responses to acidosis and alkalosis.

 

the similarity here of a forwards sweep to a similar pull in of the feet and the same response on the way out by the shoulders sweeping back.

 

flatness :

The Stefan–Boltzmann law, also known as Stefan’s law, states that the total energy radiated per unit surface area of a black body in unit time (known variously as the black-body irradiance, energy flux density, radiant flux, or the emissive power), j*, is directly proportional to the fourth power of the black body’s thermodynamic temperature T (also called absolute temperature):

 j^{\star} = \sigma T^{4}.

A more general case is of a grey body, the one that doesn’t absorb or emit the full amount of radiative flux. Instead, it radiates a portion of it, characterized by its emissivity, ε:

 j^{\star} = \epsilon\sigma T^{4}.

The irradiance j* has dimensions of energy flux (energy per time per area), and the SI units of measure are joules per second per square metre, or equivalently, watts per square metre. The SI unit for absolute temperature T is the kelvin. ε is the emissivity of the grey body; if it is a perfect blackbody, ε = 1. Still in more general (and realistic) case, the emissivity depends on the wavelength, ε = ε(λ).

To find the total absolute power of energy radiated for an object we have to take into account the surface area, A(in m2):

 P= A j^{\star} = A \epsilon\sigma T^{4}.

The constant of proportionality σ, called the Stefan–Boltzmann constant or Stefan’s constant, is non-fundamental in the sense that it derives from other known constants of nature. The value of the constant is

 \sigma=\frac{2\pi^5 k^4}{15c^2h^3}= 5.670 400 \times 10^{-8} \textrm{J\,s}^{-1}\textrm{m}^{-2}\textrm{K}^{-4}

where k is the Boltzmann constant, h is Planck’s constant, and c is the speed of light in a vacuum. Thus at 100 K the energy flux density is 5.67 W/m2, at 1000 K 56,700 W/m2, etc.

The law was deduced by Jožef Stefan (1835-1893) in 1879 on the basis of experimental measurements made by John Tyndall and was derived from theoretical considerations, using thermodynamics, by Ludwig Boltzmann (1844-1906) in 1884. Boltzmann treated a certain ideal heat engine with the light as a working matter instead of the gas. The law is valid only for ideal black objects, the perfect radiators, called black bodies. Stefan published this law in the article Über die Beziehung zwischen der Wärmestrahlung und der Temperatur (On the relationship between thermal radiation and temperature) in the Bulletins from the sessions of the Vienna Academy of Sciences.

 

Flatness refers to the shape of a liquid’s free surface. On planet Earth, the flatness of a liquid is a function of the curvature of the Earth, and from trigonometry, can be found to deviate from true flatness by approximately 19.6 nanometers over an area of 1 square meter, a deviation which is dominated by the effects of surface tension. This calculation using the Earth’s mean radius at sea level, however a liquid will be slightly flatter at the poles. this would indicate a type 1 civilisation while the surface area work on scillicates  would not.

Newton’s laws of motion are three physical laws that form the basis for classical mechanics. They are:

  1. A body at rest remains at rest and a body in linear motion remains in motion with constant velocity until and unless an external force is applied on it.

 

  1. Force applied on a body is directly proportional to the rate of change of momentum of the body or mass times acceleration (when proper units are chosen, F = ma).
  2. Every action has an equal and opposite reaction. That is whenever a first body exerts a force F on a second body, the second body exerts a force −F on the first body. F and −F are equal in size and opposite in direction.

In manufacturing and mechanical engineering, flatness is an important geometric condition for workpieces and tools.

In the manufacture of precision parts and assemblies, especially where parts will be required to be connected across a surface area in an air-tight or liquid-tight manner, flatness is a critical quality of the manufactured surfaces. Such surfaces are usually machined or ground to achieve the required degree of flatness. High-definition metrology, such as digital holographic interferometry, of such a surface to confirm and ensure that the required degree of flatness has been achieved is a key step in such manufacturing processes. Flatness may be defined in terms of least squares fit to a plane (“statistical flatness”), worst-case or overall flatness (the distance between the two closest parallel planes within.

 

These laws describe the relationship between the forces acting on a body to the motion of the body. They were first compiled by Sir Isaac Newton in his work Philosophiæ Naturalis Principia Mathematica, first published on July 5, 1687.[1] Newton used them to explain and investigate the motion of many physical objects and systems.[2] For example, in the third volume of the text, Newton showed that these laws of motion, combined with his law of universal gravitation, explained Kepler’s laws of planetary motion.

 

 

 

 underwater  was a format of developing high velocity underwater swimming methods that were based on ;

 

The formats were defined as the shoulders mooving forwards with a pull in of the angle of sweep of the feet as the motion back with the shoulders implied the motion of the feet outwards with a swing similar to a sinusodial format that could be maintained by the high velocity surface area relations of the planarity of most methods of jabbing at

LAW II: The alteration of motion is ever proportional to the motive force impressed; and is made in the direction of the right line in which that force is impressed. — If a force generates a motion, a double force will generate double the motion, a triple force triple the motion, whether that force be impressed altogether and at once, or gradually and successively. And this motion (being always directed the same way with the generating force), if the body moved before, is added to or subtracted from the former motion, according as they directly conspire with or are directly contrary to each other; or obliquely joined, when they are oblique, so as to produce a new motion compounded from the determination of both.

Using modern symbolic notation[12], Newton’s second law can be written as a vector differential equation:

\mathbf F = {\mathrm{d}(m \mathbf v) \over \mathrm{d}t}

where F is the force vector, m is the mass of the body, v is the velocity vector and t is time.

The product of the mass and velocity is momentum (which Newton himself called “quantity of motion”). Therefore, this equation expresses the physical relationship between force and momentum. Consistent with the law of inertia, the time derivative of the momentum is non-zero when the momentum changes direction, even if there is no change in its magnitude (see time derivative). The equation implies that, under zero net force, the momentum of a body is constant.

However, any mass that is gained or lost by the body will cause a change in momentum that is not the result of an external force. This equation does not hold in such cases (see open systems). Because the law describes the motion of bodies of constant mass only,[13][14][15] the mass can be moved outside the differential operator:

\mathbf F = m \ \frac{\mathrm{d} \mathbf v}{\mathrm{d}t}

By substitution using the definition of acceleration, this differential equation can be rewritten in a more familiar form:

\mathbf F = m \mathbf a

A verbal equivalent of this is “the acceleration of an object is proportional to the force applied, and inversely proportional to the mass of the object”. In general, at slow speeds (slow relative to the speed of light), the relationship between momentum and velocity is approximately linear. Nearly all speeds within the human experience fall within this category. At higher speeds, however, this approximation becomes increasingly inaccurate and the theory of special relativity

 

 the water pumping and motions to indicate the lower surface by jabbing to define the basic stabilisations that went into the surface area usage of the

 

 

 reversals of the training to learn the formats for a higher velocity finns with shoiulder motion as the work goes = F.S into the ability to use the  high irregularity of the the attract values in basic as the ability to learn to swim without similarity to any human functión.The motion simulations indicate that both finns and shoulder are in a similar motion meaning that there is no alterations of left to right .subsequent translations of the balck dragons that take both sides in their grasp as the tails go into simulative motion style. the basis of denial in most formats to worrk while you swim is the general method for a science of water H2O

 

 

and they survive

 

urvival

 

beyond type 1 civilisations by the freedoom of knowledge..The riffts that seperate the methods of swimming and the vechicularity of the derived methods for high displacements…simply shrugging the shoulders to antthing complicativelly unknown.

 

freedoom of knowledge implies no complications of using biological formats of similar duplications of bio from duplicative similarity..

1) the involvements of the characteristics by the similarity of stageings in the compsite full variance of the system.

 

from sea wale to dolphin to pinguin to seagull

as a basic descriptive by using formats of two dynamical tails from two frontal sphericals and the implications of a rail type similarity of the main body of a spaceship mooving ahead at the frontal nose by two residual forwards mooving bodies with the body undergoing the actions of the two side sections displaceing back while the tail end is assisted in the displacement into a larger value and the reaction of the whole system in a cyclic motion