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Expressing n dimensions as n-1 John R. Laubenstein IWPD Research Center Naperville, Illinois 630-428-9842 www.iwpd.org 2009 APS March Meeting Pittsburgh, Pennsylvania March 20, 2009

Expressing n dimensions as n-1

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Expressing n dimensions as n-1. John R. Laubenstein IWPD Research Center Naperville, Illinois 630-428-9842 www.iwpd.org. 2009 APS March Meeting Pittsburgh, Pennsylvania March 20, 2009. Presentation Goal. IWPD Scale Metrics (ISM) DOES NOT : - PowerPoint PPT Presentation

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Page 1: Expressing n dimensions as n-1

Expressing n dimensions as n-1

John R. LaubensteinIWPD Research Center

Naperville, Illinois630-428-9842

www.iwpd.org

2009 APS March MeetingPittsburgh, Pennsylvania

March 20, 2009

Page 2: Expressing n dimensions as n-1

IWPD Scale Metrics (ISM) DOES NOT:

Claim to identify some past error or oversight that sets the world right

Suggest that past achievements should be discarded for some new vision of reality

Page 3: Expressing n dimensions as n-1

IWPD Scale Metrics DOES:

Suggest an alternative description of space-time

Show that ISM is equivalent to 4-Vector space-time (at least in terms of velocity)

Modify gravitation so that it can be described using ISM

Show that ISM makes predictions consistent with observation

Page 4: Expressing n dimensions as n-1

ISM quantitatively links Scale Metrics and 4-Vector space-time through a mathematical relationship

Scale Metrics and 4-Vectors are shown to be equivalent (at least for specific conditions)

Scale Metrics adds to the body of knowledge

Page 5: Expressing n dimensions as n-1

Approach. We will conceptually develop ISM using a two-dimensional flat manifold

Why? Because in our world we understand both 3D and 2D Euclidean geometry

Verification. You can serve as the judge and jury over the decisions made by the “Flatlanders”

Result. If successful, a model of n dimensions as n-1 will result in describing 4-Vector space-time using only three dimensions

Page 6: Expressing n dimensions as n-1

When pondering a description for space-time this individual decides to plot time as an abstract orthogonal dimension to the two dimensions of space known in the Flatlander world

This requires three pieces of information to identify an event

(x,y) coordinates for position and a (z) coordinate for time

Page 7: Expressing n dimensions as n-1

A series of events are depicted as a Worldline

Page 8: Expressing n dimensions as n-1

A point tangent to the Worldline defines the 3-Velocity, which is normalized to a value of 1

Page 9: Expressing n dimensions as n-1

The observed (2D) velocity is depicted by the blue vector that lies in the plane of the observable dimensions

Page 10: Expressing n dimensions as n-1

The orientation of the 3-Velocity vector can be determined from its angle ( ) relative to the 2D observable plane of the Flatlander world

Page 11: Expressing n dimensions as n-1

To describe the observed velocity of an object during a specific event will require 4 pieces of information:

x,y: position coordinates z: time coordinate for the orientation of the 3-Velocity vector

Page 12: Expressing n dimensions as n-1

If a Worldline is due to gravitation, the challenge becomes to accurately describe the curvature of space and spacetime to accurately depict the curve of the Worldline The simplest case (a uniform spherical non rotating mass

with no charge) requires the Schwarzschild solution

22

2222221

22 2

1sin2

1 dtrc

Gmcddrdr

rc

Gmds

Page 13: Expressing n dimensions as n-1

When pondering a description for space-time

this individual decided to plot time as an abstract orthogonal dimension to the two known dimensions of space in the Flatlander world

This individual decides to account for time within the 2 observed dimensions by plotting time – not as a point – but as a segment representing the passage of time

Page 14: Expressing n dimensions as n-1

This approach also requires three pieces of information to identify an event

(x,y) coordinates for position

A line segment plotted on the x-y plane to designate time

Three pieces of information are required to identify an event

(x,y) coordinates for position and a (z) coordinate for time

Page 15: Expressing n dimensions as n-1

For an object at rest, its Worldline is

orthogonal to the x-y plane

For an object at rest, the (x,y) ordered pair defines a “point” at the center of the time segment

Page 16: Expressing n dimensions as n-1

A series of events are depicted as a

Worldline

As viewed from above, the three points may be seen “plotted” on the 2D plane

Page 17: Expressing n dimensions as n-1

A series of events are depicted as a

Worldline

A series of events are depicted by ever-increasing time lines

Page 18: Expressing n dimensions as n-1

A series of events are depicted as a Worldline

Page 19: Expressing n dimensions as n-1
Page 20: Expressing n dimensions as n-1
Page 21: Expressing n dimensions as n-1

A series of events are depicted as points embedded in time segments

Page 22: Expressing n dimensions as n-1

The orientation of the point relative to the timeline is denoted as (X) and is equivalent to the value

The orientation of the 3-Velocity vector can be determined from its angle ( ) relative to the 2D observable plane of the Flatlander world

Page 23: Expressing n dimensions as n-1

The position of the timeline segment can change relative to the (x,y) position coordinates

(X) = 0.5

Page 24: Expressing n dimensions as n-1

The position of the timeline segment can change relative to the (x,y) position coordinates

(X) = 0.75

Page 25: Expressing n dimensions as n-1

The position of the timeline segment can change relative to the (x,y) position coordinates

(X) = 1.0

Page 26: Expressing n dimensions as n-1

The position of the timeline segment can change relative to the (x,y) position coordinates

(X) = 0.75

Page 27: Expressing n dimensions as n-1

The position the timeline segment can change relative to the (x,y) coordinate

(X) = 0.5

Page 28: Expressing n dimensions as n-1

(x,y) position coordinates

segment coordinate for time

X: orientation

(x,y) position coordinates

z coordinate for time

coordinate for the orientation of the worldline

Page 29: Expressing n dimensions as n-1

Both ( ) and (X) represent orientations

They are related by the following expression:

11sin X

Page 30: Expressing n dimensions as n-1

ANSWER:

X has allowable values ranging from 0.5 to 1

2vm

EX

t

(X) = 0.5 (X) = 1.0

Page 31: Expressing n dimensions as n-1

2 + 1 dimensions in the Flatlander world can be expressed in 2 dimensions with no information lost

4-Vector Space-Time may be expressed within the 3 spatial dimensions we experience

So What? Who Cares? Where is the advantage of this?

Page 32: Expressing n dimensions as n-1

When using ISM, time is not defined as orthogonal to the spatial dimensions

A time segment with a defined point is equivalent to the 4-Vector Worldline

The orientation of the point (X) is related to the velocity of an object just as the slope of the Worldline is related to velocity

Just as gravity influences the 4-Vector Worldline, gravity must also be shown to influence the value of X in ISM

Who c

Page 33: Expressing n dimensions as n-1

How do you determine the directionality of the time segment?

Page 34: Expressing n dimensions as n-1

Apply a factor of pi.

The resulting “ring” defines a fundamental entity dubbed as the “energime”

Page 35: Expressing n dimensions as n-1

Time emerges from everywhere within the Initial Singularity

Page 36: Expressing n dimensions as n-1

Time progresses as a quantized entity defining quantized space

Page 37: Expressing n dimensions as n-1
Page 38: Expressing n dimensions as n-1
Page 39: Expressing n dimensions as n-1
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The collective effort results in the creation of an overall flat Background Energime Field (BEF)

Page 41: Expressing n dimensions as n-1

Flat Background Energime Field (BEF)

Page 42: Expressing n dimensions as n-1

Flat Background Energime Field (BEF)

Perturbation due to local effects of a gravitating mass resulting in a Local Energime Field (LEF)

Page 43: Expressing n dimensions as n-1

Gravitation is an interaction between a local gravitating mass and the total mass-energy of the universe

Page 44: Expressing n dimensions as n-1

The more massive the gravitating entity, the stronger the gravitation effect

Page 45: Expressing n dimensions as n-1

The less massive the gravitating entity, the weaker the gravitational effect

Page 46: Expressing n dimensions as n-1

As time progresses, the initial singularity increases in size as the scaling metric changes.

Page 47: Expressing n dimensions as n-1
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Page 49: Expressing n dimensions as n-1
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Fundamental Unit Time

Fundamental Unit Length

Page 51: Expressing n dimensions as n-1

Velocity is typically determined by the orthogonal relationship between 4-Velocity and the observed 3-Velocity

Page 52: Expressing n dimensions as n-1

If you attempt to subtract the 3-Velocity from the 4-Velocity linearly, you will not get the correct answer

Page 53: Expressing n dimensions as n-1

If you attempt to subtract the 3-Velocity from the 4-Velocity linearly, you will not get the correct answer

a

b ba

Page 54: Expressing n dimensions as n-1

However, if you apply a scaling factor, you can achieve a linear relationship between 4- Velocity and 3-Velocity

Page 55: Expressing n dimensions as n-1

However, if you apply a scaling factor, you can achieve a linear relationship between 4- Velocity and 3-Velocity

a

b

ba

Page 56: Expressing n dimensions as n-1

ANSWER: The ISM Scaling Metric (M), relative to the Fundamental Unit Length (L), defines the magnitude of the Scaling Factor required to make a = b.

Fundamental Unit Time (T)

Fundamental Unit Length (L)

Scaling Factor = M/L

ISM Scaling Metric (M)

Page 57: Expressing n dimensions as n-1

Fundamental Unit Time (T)

Fundamental Unit Length (L)

Scaling Factor = M/L

ISM Scaling Metric (M)

L

MLEFBEFv

Page 58: Expressing n dimensions as n-1

If a Worldline is due to gravitation, the challenge becomes to accurately describe the curvature of space and space-time to accurately depict the curve of the Worldline

The simplest case (a uniform spherical non rotating mass with no charge) requires the Schwarzschild solution

In the case of ISM, an object under the influence of gravitation must have a specific value of X

The value of X and therefore the geometry of ISM space-time is defined by:

11sin X 22

2222221

22 2

1sin2

1 dtrc

Gmcddrdr

rc

Gmds

Page 59: Expressing n dimensions as n-1

All of the information in 4-Vector space-time can be captured in 3 spatial dimensions by incorporating:

a quantized time segment (ring) with an orientation value (X)

The relationship between time and (X) defines velocity ISM coordinates are consistent with a new formalism for gravitation ISM is supported by observational data

Page 60: Expressing n dimensions as n-1

A quantum theory of gravity Physical explanation of the fine structure constant

A university that is 14.2 billion years old A new interpretation of objectivity and local causality

An accelerating rate of expansion Absolute definition of mass, distance and time

Inflationary epoch falling naturally out of expansion A link between gravitation and electrostatic force

A clear definition of the initial singularity A link between gravitation and strong nuclear force

A physical definition of space Defined relationship between energy and momentum

A physical definition of Cold Dark Matter Explanation of the effects of Special Relativity

A physical explanation of Dark Energy 4-Vectors expressed in a 3D ISM coordinate system