L I G H T  S A B R E  C O N S TR U C T I O N S 

O F   A  P A R T I C L E    Q U A N T    F L O W

By Henryk Szubinski

work on the motivator for large scale reference computations on the productions of minimal prticle flow systems with a resistant predefinitions for lim x = usage by input length..

 

formative construction ;

Kinetic energy alterations into (electron volts by a impulse construct pressuriser)—————————————-as the format for interior internals…

simple illustartions project type construct;

a Polymer shell construct of a sphere

the divisions of the spheres surface area as divied so that a compression on its surface area by nodes or points can deliver pressure while the internal volume is filled with a fluid…the concept is designed to deliver fluid formats of silid interactions basis of the same concept continued by the illustrations of similar speheres inside the main sphere that dieliver minimal or controlled values of fluid /solid interface distributions..

internally a distributions flow might be wire formatted to a controll section around the mid section on the sagital plane..by bending the emission cause in flow as related to data on full interaction of the sphere levels and the circuit dump core values…

the system needs only a gravity inetractions on the basis of time as a interval of the resistancy value of a collective dump in the core by interactions of a basic circuitry with X Current and Voltage…

 

Series circuits are sometimes called current-coupled or daisy chain-coupled. The current that flows in a series circuit will flow through every component in the circuit. Therefore, all of the components in a series connection carry the same current.

[edit] Resistors

[edit] Inductors

Inductors follow the same law, in that the total inductance of non-coupled inductors in series is equal to the sum of their individual inductances:

However, in some situations it is difficult to prevent adjacent inductors from influencing each other, as the magnetic field of one device couples with the windings of its neighbours. This influence is defined by the mutual inductance M. For example, if you have two inductors in series, there are two possible equivalent inductances depending on how the magnetic fields of both inductors influence each other.

 

————————————————————————————————————–the freedoom of knowledge law might indicate the fluid interactions of water environments by the different basic point interactions as being

1..curvature variant to a = resultant of dissorientations when the direction is to be 1 vector

2…the point dispersals of a process to connect the dots as the general parameter of involvement by dissorientation ( simply a vector alterance without designated vector displacement of 1 ..basis

3..the resultant vector displacement certainty as fro0m 1 to 3 in one displacements..

the interactions of a..the formats for relations with the subsedimentary level of sand and shale on the base level of the fluid énvironmnet as = the point involvances of 1,2,3 variants

b..the involvances with body ponts in associations by 1,2,3 and a)1,2,3 ——->b) 1,2,3

c…the usage of the direct displacement vectors as basic involvance with observations of turbulence flow of body fluid / solid basis of interactions..

a,b,c are based on (x,y,z) = to the designations of divisive 1,2,3 formats in a,b,c =

to the high velocity motivations of the process = x

the y value designations of the applied coreness of interactions of fluid / surface area environmnet = y

and the z = as the reverse functtionings of the linear or fabric artificiality of fluid / solid substances in their relations————>displaceing passed the circuit data ————————————>capacitators or the general field of electronics..

When there are more than two inductors, the mutual inductance between each of them and the way the coils influence each other complicates the calculation. For a larger number of coils the total combined inductance is given by the sum of all mutual inductances between the various coils including the mutual inductance of each given coil with itself, which we term self-inductance or simply inductance. For three coils, there are six mutual inductances M₁₂, M₁₃, M₂₃ and M₂₁, M₃₁ and M₃₂. There are also the three self-inductances of the three coils: M₁₁, M₂₂ and M₃₃.

Therefore

L_total = (M₁₁ + M₂₂ + M₃₃) + (M₁₂ + M₁₃ + M₂₃) + (M₂₁ + M₃₁ + M₃₂)

By reciprocity M_ij = M_ji so that the last two groups can be combined. The first three terms represent the sum of the self-inductances of the various coils. The formula is easily extended to any number of series coils with mutual coupling. The method can be used to find the self-inductance of large coils of wire of any cross-sectional shape by computing the sum of the mutual inductance of each turn of wire in the coil with every other turn since in such a coil all turns are in series.

[edit] Capacitors

Capacitors follow the same law using the reciprocals. The total capacitance of capacitors in series is equal to the reciprocal of the sum of the reciprocals of their individual capacitances:

.

The working voltage of a series combination of identical capacitors is equal to the sum of voltage ratings of individual capacitors provided that equalizing resistors are used to ensure equal voltage division. This is all because of Ohm’s law V = RI

[edit] Memristors

Memristors in series are given by the sum of their memristance:

[edit] Switches

Two or more switches in series form a logical AND; the circuit only carries current if all switches are ‘on’. See AND gate.

[edit] Parallel circuits

If two or more components are connected in parallel they have the same potential difference (voltage) across their ends. The potential differences across the components are the same in magnitude, and they also have identical polarities. Hence, the same voltage is applicable to all circuit components connected in parallel. The total current I is the sum of the currents through the individual components, in accordance with Kirchhoff’s circuit laws. The current in each individual resistor is found by Ohm’s law. Factoring out the voltage gives

.

To find the total resistance of all components, add the reciprocals of the resistances R_i of each component and take the reciprocal of the sum:

 

The sign of M depends on how the magnetic fields influence each other. For two equal tightly coupled coils the total inductance is close to that of each single coil. If the polarity of one coil is reversed so that M is negative, then the parallel inductance is nearly zero or the combination is almost non-inductive. We are assuming in the “tightly coupled” case M is very nearly equal to L. However, if the inductances are not equal and the coils are tightly coupled there can be near short circuit conditions and high circulating currents for both positive and negative values of M, which can cause problems.

More than 3 inductors becomes more complex and the mutual inductance of each inductor on each other inductor and their influence on each other must be considered. For three coils, there are three mutual inductances M₁₂, M₁₃ and M₂₃. This is best handled by matrix methods and summing the terms of the inverse of the L matrix (3 by 3 in this case).

The pertinent equations are of the form:

[edit] Capacitors

Capacitors follow the same law using the reciprocals. The total capacitance of capacitors in parallel is equal to the sum of their individual capacitances:

.