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d a t a e x i t r a d i u s f o r c e
By Henryk Szubinski
where horizons are ultimately a value of motion to locate a system galaxy for example as the data on a non alterance by simple rotations but as a type retraction outof the whole parameter that is the universe>< the data on the linearity that sequencially measures a rate of multiples = x as the velocity of trakking increases..
the same values of 1/S
= S ( x +S)
in what is termed as
S(x+S)x
the reversal of a orbital view of a rotation of 1 degree as similar to the full rotation of a 10x value angle .x = to the same 1 value of a response to use conservations of force by the data on using STORE in the usage of minimal force:
the basics of the data on a volume exit not by velocity or gravity but by the retractions of a point of view as basic as the perspective spacetime function as the data on the processed retractions of spacetime surface area 3 x
where the data on the process of a rotation in counter angles to the radius of the extra exit state values where the raduis remains the same as r 2
defned on the basis of the basic fluidity offlow of a angle and the higher velocity stabilisations of counter radus values = 1/ x
where x = radius
data on the fromats of basic increase of the data as a extensionality of r .x = 1
as the frmats of the data on slidity of the basic values of similar radial rotations = r (x + 1/r)
= to rotation = Cir 2pi r
as the formats of a general inclusion of data on the positionality of the sections in a compounded background value of inclusive orbitality of nearlying systems with a r = stability of non exit fased values of
B/ g = r / x
as the background positional mini 1/B
as a universal r combinance compressed into a height value of earth gravity release = 1/r(h)
S(x+S)x
this data is responsive to any dimensionality and its positional hyperspace
S10 (x+S)x.D=hyperspace.B
this occurs wherever there is a higher flux than is the positionality of the universe
f r a c t i c u n i v e r s e s
By Henryk Szubinski
becaue a galaxy is the localised positionality as a strenght value of force, the very presence of black holes that are infinitely large in gravity value must define the very large universal value possibilities at work in the universe, as such the usage of :motion to such a parameter by a galaxy:
infinite ( g) (objective stepping x +1)3 .z. =F( S motion of galaxies as 3 x triangulation )
the combined values of such implicatively large localisations can then be accessed as super triangulations of every event in the universe
using fractal 1 as the background dial to construct a dial at the foreground and to make it a fractal altered by a specific angle =1 degree as to make dialing of fractals a specific activity of localised increases in accuracy by increasing the dial angle value:
the dial motion to define a accuracy of detailed fractal values as the dial controll part that mooves the measurement section as a black hole and its triangulational fractal value = 3 x
where 2 x = the general dial structure with its specific detail increase by using a 3 x type = fractal angle 1
A fractal is “a rough or fragmented geometric shape that can be split into parts, each of which is (at least approximately) a reduced-size copy of the whole,”[1] a property called self-similarity. Roots of mathematical interest in fractals can be traced back to the late 19th Century; however, the term “fractal” was coined by Benoît Mandelbrot in 1975 and was derived from the Latin fractus meaning “broken” or “fractured.” A mathematical fractal is based on an equation that undergoes iteration, a form of feedback based on recursion.[2]
A fractal often has the following features:[3]
- It has a fine structure at arbitrarily small scales.
- It is too irregular to be easily described in traditional Euclidean geometric language.
- It is self-similar (at least approximately or stochastically).
- It has a Hausdorff dimension which is greater than its topological dimension (although this requirement is not met by space-filling curves such as the Hilbert curve).[4]
- It has a simple and recursive definition.
using the size difference between a galaxy at the horizon prior to its motion and the value of it in a altered positional displacement by a value velocity in a dimensional increase of proximity which would be a type construct mould to put on the dialing specific instruments of the fractal dialing ( remeber the fractal is the same for every dial made)
USING ONLY TRIANGULATION BY 2 VALUES OF A GALACTIC POSITIONAL ALTERANCE FROM POSITION 1 TO POSITION 2 A TYPE FLAME FRACTAL GENERATION
showing some data that is incoherent with the specifics of triangulation made with the same values shown in a type horizon that can be bent to isolate a galctic event:
this process can utilise flame fractals as the begining fase of horizon fractality by encapsulement of a galaxy core at its vector displaced value to a NOW position:
using intervals of space time fractality by the positionality of galaxy motion in the universe as a type disruption spacetime function that generates a landscape usability for 3 to 10 dimensionality of the universes spacetime as a actual responsive environemnt generation of any parameter of detailed values in the imagery and detailing facilitations of spacetime by the relations of galactic motion velocity in the primary inversionality as usablity of the galactic processings of type computer articial intelligence fract generator motorics of a a.i computer ystem that will use 2 generator galactic values and their interactive 3 rd value computer fractics..
by actually using the positionality of black holes to mage a generation of a previous position of a galaxy in spacetime , the resultant angle alterance of a type interaction of DIALING A FRACTAL AS A MEASURE SYSTEM OF THE POWER OF FORCE USED TO DEFINE THE decimal value detailing on a scale of 1 % to 100& in the dial quantal limit value:
BY isolations of referencability by black hole triangulations
A black hole is often defined as an object whose escape velocity exceeds the speed of light. This picture is qualitatively wrong, but provides a way of understanding the order of magnitude for the black hole radius.
The escape velocity is the minimum speed at which an object needs to travel so as to escape a source of gravity without falling back into orbit before stopping. On the Earth, the escape velocity is equal to 11.2 km/s, so no matter what the object is, whether a bullet or a baseball, it must go at least 11.2 km/s to avoid falling back to the Earth’s surface. To calculate the escape velocity in Newtonian mechanics, consider a heavy object of mass M centered at the origin. A second object with mass m starting at distance r from the origin with speed v, trying to escape to infinity, needs to have just enough kinetic energy to make up for the negative gravitational potential energy, with nothing left over:
(where G is the gravitational constant). That way, as it gets closer to 
it has less and less kinetic energy, finally ending up at infinity with zero speed.
This relation gives the critical escape velocity v in terms of M and r. But it also says that for each value of v and M, there is a critical value of r so that a particle with speed v is just able to escape:
When the velocity is equal to the speed of light, this gives the radius of a hypothetical Newtonian dark star, a Newtonian body from which a particle moving at the speed of light cannot escape. In the most commonly used convention for the value of the radius of a black hole, the radius of the event horizon is equal to this Newtonian value.
In general relativity, the coordinate r is not completely straightforward to define due to the curved nature of space-time and the choice of different coordinates. For this result to be true, the value of r should be defined so that the surface area A of a sphere of radius r in the curved space time is still given by the formula A = 4πr2. This definition of r only makes sense when the gravitational field is spherically symmetric, so that there are concentric spheres on which the gravitational field is constant.
The velocity necessary to escape from an object’s gravitational field (called the object’s escape velocity) depends on how dense the object is; that is, the ratio of its mass to its volume. A black hole forms when an object is so dense that, within a certain distance of it, even light is not fast enough to escape, since the speed of light is slower than the black hole’s escape velocity. Unlike in Newtonian gravity, in general relativity, light going away from a black hole doesn’t slow down and turn around. The Schwarzschild radius is still the last distance from which light can escape to infinity, but outgoing light which starts at the Schwarzschild radius doesn’t go out and come back, it just stays there. Inside the Schwarzschild radius, everything must move inward, getting crushed somehow at the center.
In general relativity, the black hole’s mass can be thought of as concentrated at a singularity, which can be a point, a ring, a light-ray, or a sphere; the exact details are not currently well understood in all circumstances. Surrounding the singularity is a spherical boundary called the event horizon. The event horizon marks the ‘point of no return,’ a boundary beyond which matter and radiation inevitably fall inwards, towards the singularity. The distance from the singularity at the center to the event horizon is the size of the black hole, and is equal to twice the mass in units where G and c equal 1.
s u b s e q u e n t d e v e l o p m e n t s
flying car
By Henryk Szubinski
The drag coefficient Cd is defined as:
where
- Fd is the drag force, which is by definition the force component in the direction of the flow velocity,[6]
- ρ is the mass density of the fluid, [7]
- v is the speed of the object relative to the fluid, and
- A is the reference area.
The reference area depends on what type of drag coefficient is being measured. For automobiles and many other objects, the reference area is the frontal area of the vehicle (i.e., the cross-sectional area when viewed from ahead). For example, for a sphere A = π r2 (note this is not the surface area = 4 π r2).
For airfoils, the reference area is the chord of the airfoil multiplied with the length of span, which can be easily related to wing area. Since this tends to be a rather large area compared to the projected frontal area, the resulting drag coefficients tend to be low: much lower than for a car with the same drag, frontal area and at the same speed.
Airships and some bodies of revolution use the volumetric drag coefficient, in which the reference area is the square of the cube root of the airship volume. Submerged streamlined bodies use the wetted surface area.
Two objects having the same reference area moving at the same speed through a fluid will experience a drag force proportional to their respective drag coefficients. Coefficients for unstreamlined objects can be 1 or more, for streamlined objects much less.
F————————-p—————————-v—————————-A
the side booster turbines are used in their vertical orientations when used at the nose section.
a f l y i n g c a r
By Henryk Szubinski
functionality by relations to V=I.R
as a circuit break
DEFINITION OF BASIC of the proces vo9lume in a displacement made by the process of data as sectionaly stable while the extra volumetricality of the data on the similarity of stemmic processess of a resistance type value in the fluidity and solidity of the interactions
as the spacial restrictions of the data on a processed value of force used in the internal volumetrics of the basis in vector motion as the values of a process level 2 = non vectorised values of displacement by the process solidity / as the processing to a fluid surround interaction between the two levels as a type value in lower velocity as a warp speed and anti gravity type non restriction to the data on the non formative internal value relations with a positional warp format for the general minimal damage orientations of the same value to avoid priority by 3 x levels of the data to a parameter; implied as the same function of a human body to alter parameter faster if not equally in force function as the vechicle would:
the balance then is 3x = 1/ B ( S)
of the vechicle formats in sections 1 and 2 as layers of vechiclularity by a response 2 x prior to the vechicularity = 3 x
K———————–R———————d—————–p————————q
because a drag coefficiency is dimensionless the usage of Jungs theorem of gemetry to define a spherical interactions between many or mainfold spheres has a similarity to using any geometrical position divisions of a sphere with drag coefficiency as a hyperspace
10 ( Jung ) / sphere .x =Drag coefficiency / x (B universe +1/2) hyperpsace
The drag equation
is essentially a statement that the drag force on any object is proportional to the density of the fluid, and proportional to the square of the relative speed between the object and the fluid.
Cd is not a constant but varies as a function of speed, flow direction, object shape, object size, fluid density and fluid viscosity. Speed, kinematic viscosity and a characteristic length scale of the object are incorporated into a dimensionless quantity called the Reynolds number or Re. Cd is thus a function of Re. In compressible flow, the speed of sound is relevant and Cd is also a function of Mach number Ma.
For a certain body shape the drag coefficient Cd only depends on the Reynolds number Re, Mach number Ma and the direction of the flow. For low Mach number Ma, the drag coefficient is independent of Mach number. Also the variation with Reynolds number Re within a practical range of interest is usually small, while for cars at highway speed and aircraft at cruising speed the incoming flow direction is as well more-or-less the same. So the drag coefficient Cd can often be treated as a constant. [8]
For a streamlined body to achieve a low drag coefficient the boundary layer around the body must remain attached to the surface of the body for as long as possible, causing the wake to be narrow. A high form drag results in a broad wake. The boundary layer will remain attached longer if it is laminar than if it is turbulent. The boundary layer will transition from laminar to turbulent providing the Reynolds number of the flow around the body is high enough. Larger velocities, larger objects, and lower viscosities contribute to larger Reynolds numbers.[9]
1/2 hemispherical resistance multiple as a wire 1/2 resistance circuit in breakage:
V—————————————–I—————————————————R
From Wikipedia, the free encyclopedia
In geometry, Jung’s theorem is an inequality between the diameter of a set of points in any Euclidean space and the radius of the minimum enclosing ball of that set. It is named after Heinrich Jung, who first studied this inequality in 1901.
F——————-p——————v————————c———————–A
RADIAL VALUE 1/ 4 X = DIAMTER VALUE 4Z. 8Y
Consider a compact set
and let
be the diameter of K, that is, the largest Euclidean distance between any two of its points. Jung’s theorem states that there exists a closed ball with radius
that contains K. The boundary case of equality is attained by the regular n-simplex.
[edit] Jung’s theorem in the plane
Most common is the case of Jung’s theorem in the plane, that is n = 2. In this case the theorem states that there exists a circle enclosing all points whose radius satisfies
No tighter bound on r can be shown: when S is an equilateral triangle (or its three vertices), then
pioneer space programme
image courtesy of wikipedia
The Pioneer program is a series of United States unmanned space missions that was designed for planetary exploration. There were a number of such missions in the program, but the most notable were Pioneer 10 and Pioneer 11, which explored the outer planets and left the solar system. Both carry a golden plaque, depicting a man and a woman and information about the origin and the creators of the probes, should any extraterrestrials find them someday.
Credit for naming the first probe has been attributed to Stephen A. Saliga, who had been assigned to the Air Force Orientation Group, Wright-Patterson AFB, as chief designer of Air Force exhibits. While he was at a briefing, the spacecraft was described to him as a “lunar-orbiting vehicle with an infrared scanning device.” Saliga thought the title too long and lacked theme for an exhibit design. He suggested “Pioneer” as the name of the probe since “the Army had already launched and orbited the Explorer satellite and their Public Information Office was identifying the Army as ‘Pioneers in Space,’” and by adopting the name the Air Force would “make a ‘quantum jump’ as to who really [were] the ‘Pioneers in space.’”[1]
a f e y m a n d e c i m a l
By Henryk Szubinski
on the responses to parallellogramic interactions
GENERAL BACKGROUND:
The form of the propagator can be more easily found by using the equation of motion for the field. From the Lagrangian, the equation of motion is:
and in an expectation value, this says:
Where the derivatives act on x, and the identity is true everywhere except when x and y coincide, and the operator order matters. The form of the singularity can be understood from the canonical commutation relations to be a delta-function. Defining the (euclidean) Feynman propagator Δ as the Fourier transform of the time-ordered two-point function (the one that comes from the path-integral):
So that:
If the equations of motion are linear, the propagator will always be the reciprocal of the quadratic-form matrix which defines the free Lagrangian, since this gives the equations of motion. This is also easy to see directly from the Path integral. The factor of i disappears in the Euclidean theory.
fermion scattering
force field strength depends on the spherical size as a greater seperation for small volume spheres :
as a 3 value interactions the
360 /3x=1+x/2-x
as a type space time of a mean value x in the alterance of 2 x = force field registrations as actual space time intersections as the diemnsional value of smaller spheres with greater force field seperations so that a vergance to the process by soize discrepancies must occur in a time period of spacetime dimensionality:
t h e f o r c e o f s e p e r a t i o n
By Henryk Szubinski
ELASTIC LIMITS OF MAGNETIC POLARITY LINES OF FORCE
By Henryk Szubinski
a line of force ,by Newtons laws of motion 1
F=m.a
Density as a function of weight and surface area indentations by stretching of a materials value
the usage of a value BIT number B as the representation of the polarity of linear sections in the rotational fields of force generated when a force is used to remoove the linear section while maintaining the core reference of a limited value of vector pull out as the stage where the geneal magnetic field begins to draw back over the spherical format generating the captive magnetic field envelopment..
AS the magnetic flux begins to be fully drawn back to the opposite pole, the usage of a magnetic tube = a vacuume cha´mber inside a magnetic bar with its surround value magnetism as a = to polar force field in its responsive volume by a relational alteration
of :
volume / vacuume = 2 (( 2pi r squ ( S))+ magnetic force
the interactions of x format exchanges of vacuume and volume of magnetic bar as a type occilator of a type oxygenic exchange with the O2OH type reference with the surface area on the O2 type interactions of Oxygen atmospherical inclusions of a H2O elasticity of the pull effect on the elastic limit as a break off elastic H2O = O2 OH as the break value of the sectionality of the seperations of a minimal yet strong section of the break offs..
a objective mass object fallen at a track rate measured as a velocity in action to a spacetime continuiim surface area . Fallen as it is the objective gravity interactions of a type ripple occurs where the whole spacetime is disrupted by the responsive values of the surrounding spacetime unified by objects of mass type 1 gravity : meaning they are stablisators for the responsive sense of force as it acts with a action = reaction type response:
DATA ON HOW values of gravity rippling occurs is based on the basic law of the process of a stable objective with its gravity signature as the basics of involvement of
velocity = a incline increase by continuiim alterance of the fluid status = spacetime
and the solid fased gravity = objective forms in spacetime
of force as to verticality by the involvance of the subsequent disturbancy of a alteration = to a system in disorder where the general ripples = to a state of levels in ripple force
= 3 x .9x.81 x
as a type interactions by the whole state of gravity and anti gravity as a force of combined values
=729.3 =1487 as a Newton force
= gravity , where anti gravity would be the root value 1487 approximated to =33
as a state of force that combines the values the process 33%x=a.m
where a.m = anti matter
as shared between the 3 states =99 %= matter
the 1 % remaining is the general problem of the rule of 1/3 x =g
a.msqu.g=1%.1/3.x
In algebra, the absorption law is an identity linking a pair of binary operations.
Two binary operations, say ¤ and *, are said to be connected by the absorption law if:
- a ¤ (a * b) = a * (a ¤ b) = a.
A set equipped with two commutative and associative binary operations ∨ (“join”) and ∧ (“meet”) which are connected by the absorption law
- a ∨ (a ∧ b) = a ∧ (a ∨ b) = a
is called a lattice. Examples of lattices include Boolean algebras and Heyting algebras.
In classical logic, and in particular in Boolean algebra, the operations OR and AND, which are also denoted by ∨ and ∧, also satisfy the lattice axioms, including the absorption law. The same is true for intuitionistic logic.
The commutative and associative laws also hold for addition and multiplication in commutative rings, e.g. in the field of real numbers. The absorption law is the critical property that is missing in this case, since in general a · (a + b) ≠ a and a + (a · b) ≠ a.
The absorption law also fails to hold for relevance logics, linear logics, and substructural logics. In the last case, there is no one-to-one correspondence between the free variables of the defining pair of identities.
WOULD A BAR OF MAGNETIC METAL BAR , when subject to elastic pull as absorbing a photon value particle stream which causes a type spherical spectrality when breaking and after seperation by the similarity of a expansive magnetic effect of a polarity in envelopment as it expands without a limitation of a sphere..
the objective of spacetime absorbtions
the type referenced response resultance of the ripple effect
while one side is vectorised the remaining right side goes into absorbance= seperation
where the seperation is a simulative interaction of polar force of magnetic lines in a multiple state :
In spectroscopy, the absorbance A (also called optical density) is defined as
,
where I is the intensity of light at a specified wavelength λ that has passed through a sample (transmitted light intensity) and I0 is the intensity of the light before it enters the sample or incident light intensity. Absorbance measurements are often carried out in analytical chemistry, since the absorbance of a sample is proportional to the thickness of the sample and the concentration of the absorbing species in the sample, in contrast to the transmittance I / I0 of a sample, which varies logarithmically with thickness and concentration
the general smooth type alterance of the process of breaking by absorbtions in spherical gravity can only imply the seperations by absorbtions of a type spectrality in magnetic lines of force and their relations with the ripple effect of a object in magnetic flux = 99% of the sphericality =m
The remaining 1% = the magnetic flux of the sphere
Some filters, notably welding glass, are rated by shade number, which is 7/3 times the absorbance plus one:[3]
reversing the format of elasticity and the break zone as a type similar quantality = magnetic bars in alterance not by fysical strain but by the relations of simulating the break by
oxygenic values / water atomic mass = O2OH as the type mass number
as = to a volumetrical dispersion can be made into small devices with minimal nao detections of usage of molecular starains of string similar data on what is breaking and the simulations of a break off siulation going into anti matter formats by the connections to a surface volume sphere as a type reverse giudance system for space travel..
- shade number =
h u m a n c o m p a g n i o n s u n i t¨
By Henryk Szubinski
In anatomy, flexion is a position that is made possible by the joint angle decreasing. The skeletal (bones, cartilage, and ligaments) and muscular (muscles and tendons) systems work together to move the joint into a “flexed” position. For example the elbow is flexed when the hand is brought closer to the shoulder. The trunk may be flexed toward the legs or the neck to the chest.
The opposite term is extension, or straightening. Flexion decreases the angle between the bones of the limb at a joint, and extension increases it.
Note that specific flexion activities may occur only along the sagittal plane, i.e. from the forward to backward direction, and not side-to-side direction, which is further discussed in abduction.
as a type registration of the planar lunar surface areas where there is water is similar to a triangulation of values that can be inverted in convexity to concavity by a dgegree of flexation onto the general projective areas of EARTHS OWN continental shelves in what resembles a type generation by turbine interactions of a R2D2 artificiail compagnion for humans due to the general simplicity of communications made easy by Carbon motorics where a ATP 162 is involved has similarities with the basic human 3 levels of both the priority to include the units data expansions as reading the data on the possibilities of a ground level basic concave point into which the general data has basic levels of flex by concavity / convexity..
aftermath computations:
as a simple relation of the data on which format is prioritiesed for fluid / solid based seperations by a simple protractions value = h
which can read the general characteersitics of the process ACTIVATE / DISACTIVATIONS
by the general lw of the formations of altered rotations of the unit computations by minimal waveform interactions based on cir / x = as a x format value waveform by a multi orientative system of the generalisations made by compacting the two levels in concave / convex flexations which are in minimal data bits =on the formats of the compactions of the data on which the data on a frequency flow where both levels are similarily combined to a
convex 1= concave2
concave1= convex2
as the general formulations of multiple data systems on any gravity relations such a unit can monitor the multiple relation s that are active in the lunar EARTH UNIVERSE exchange values
as
a very flexible materials format
multiplex = 1/x
flex inversions can go through many sequenced interaction ALTERANCES BY MINIMAL WOBBLE
multiplex =2x
If d is small compared to R1 and R2, then the thin lens approximation can be made. For a lens in air, f is then given by
![\frac{1}{f} \approx \left(n-1\right)\left[ \frac{1}{R_1} - \frac{1}{R_2} \right].](http://upload.wikimedia.org/math/a/f/a/afad8f375f5846cea8f9e8091f145d60.png)
AS WITH A THIN LAYER OF GRAVITY OXIDE = O2OH AS a reversed format of OHO2
multiplex =3x
or hyperdioxidic gravity in a FLOAT STATE OF NEGATIVE GRAVITY = anti matter type applications by making the float value INVERT THE VOLUME of H2O
The focal length f is positive for converging lenses, and negative for diverging lenses. The reciprocal of the focal length, 1/f, is the optical power of the lens. If the focal length is in metres, this gives the optical power in dioptres (inverse metres).
Lenses have the same focal length when light travels from the back to the front as when light goes from the front to the back, although other properties of the lens, such as the aberrations are not necessarily the same in both directions.
multiplex =4x
An inverse multiplexer (often abbreviated to “inverse mux” or “imux“) allows a data stream to be broken into multiple lower data rate communication links. An inverse multiplexer differs from a demultiplexer in that each of the low rate links coming from it is related to the others and they all work together to carry their respective parts of the same higher rate data stream. By contrast, the output streams from a demultiplexer may be completely independent from each other and the demultiplexer does not have to understand them in any way.
Note that this is the opposite of a multiplexer which creates one high speed link from multiple low speed ones.
example:
|--low rate link #1--|
DTE ---high rate data---inverse mux |--low rate link #2--|(de)inverse mux--DTE
|--low rate link #3--|
DTE = Data terminal equipment DCE = Data circuit terminating equipment
This provides an end to end connection of 3 x the data rate available on each of the low rate data links. Note that, as with multiplexers, links are almost always bi-directional and an inverse mux will practically always be combined with its reverse and still be called an inverse mux. This means that the “de-inverse mux” will actually be an inverse mux.
the EARTH CAN ALSO HAVE THIS TYPE OF INTERACTIONS AS IN THIS CASE THE INTERACTIONS CAN ALSO BE MULTIPLE BY VECTOR SIMILARITY:of 2 forces along the same vector as a multiplex value =volumes 6 x
multiplexing = 5 x
MULTIPLEXING as the type transportations of anti matter transporters
Inverse muxes are used, for example, to combine a number of ISDN channels together into one high rate circuit, where the DTE needs a higher rate connection than is available from a single ISDN connection. This is typically useful in areas where higher rate circuits are not available.
An alternative to an inverse mux is to use three separate links and load sharing of data between them. In the case of IP, network packets could be sent in round robin mode between each separate link. Advantages of using an inverse mux over separate links include
- lower link latency (one single packet can be spread across all links)
- fairer load balancing (computing)
- network simplicity (no router needed between boxes with high speed interfaces)
multiplex states of combined pressure = OHO2 as hyperoxidic matter transportations as a type 1 anti matter drive
A simple analogy to transport can help explain the distinction between multiplexing and inverse multiplexing. When small cargoes such as pencils are shipped overseas, they are generally not carried one at a time. Rather, they are assembled into small boxes, which are grouped into larger cartons, which go into intermodal containers, which join multiple containers aboard a container ship. Each step is a multiplexing. Conversely a large cargo, for example in structure relocation, may be disassembled for carriage on multiple vehicles and then reassembled in the correct order at the destination. This is inverse multiplexing.
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