Category Archives: Einstein

Einstein 1920 (XXVII) The Space-Time Continuum of General Theory

Reference: Einstein’s 1920 Book

Section XXVII (Part 2)
The Space-Time Continuum of the General Theory of Relativity Is not a Euclidean Continuum

Please see Section XXVII at the link above.

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Summary

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Final Comments

A body in uniform motion may not have acceleration, but it has a constant velocity. This constant velocity differs from body to body due to differences in their inherent structure. This inherent structure appears as the mass, inertia, rigidity or consistency of the body.

Light has near zero consistency and near infinite velocity; whereas, matter has near infinite consistency and extremely low range of velocities. By extrapolating between these data points, the special theory of relativity manages to come up with an approximate method to calculate the relative velocity in uniform motion for matter.

The general theory of relativity accounts for acceleration by relating instantaneous changes in consistency to changes in velocity throughout a continuum. Thus, it accounts for acceleration that manifests in the form of gravitational field.

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Einstein 1920 (XXVI) The Space-Time Continuum of Special Theory

Reference: Einstein’s 1920 Book

Section XXVI (Part 2)
The Space-Time Continuum of the Special Theory of Relativity Considered as a Euclidean Continuum

Please see Section XXVI at the link above.

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Summary

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Final Comments

The space coordinates (x, y, z) and the time coordinate (t) represent two very different dimensions in our experience; but they may be combined geometrically to form a “Euclidean” four-dimensional continuum. This continuum may be interpreted as follows.

The greater is the “duration” of substance at a location, the lesser is its flexibility at that location. Whereas, the coordinate t represents the “duration” of substance at a location in space (x, y, z); the Minkowki’s coordinate “√(-1) ct” represents the consistency of substance at that location.

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Einstein 1920 (XXV) Gaussian Co-ordinates

Reference: Einstein’s 1920 Book

Section XXV (Part 2)
Gaussian Co-ordinates

Please see Section XXV at the link above.

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Summary

Gauss invented a method for the mathematical treatment of continua in general, in which “size-relations” (“distances” between neighbouring points) are defined. To every point of a continuum are assigned as many numbers (Gaussian co-ordinates) as the continuum has dimensions. This is done in such a way, that only one meaning can be attached to the assignment, and that numbers (Gaussian co-ordinates) which differ by an indefinitely small amount are assigned to adjacent points.

The Gaussian co-ordinate system is a logical generalization of the Cartesian co-ordinate system. It is also applicable to non-Euclidean continua, but only when, with respect to the defined “size” or “distance,” small parts of the continuum under consideration behave more nearly like a Euclidean system, the smaller the part of the continuum under our notice.

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Final Comments

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Einstein 1920 (XXIV) Euclidean and Non-Euclidean Continuum

Reference: Einstein’s 1920 Book

Section XXIV (Part 2)
Euclidean and Non-Euclidean Continuum

Please see Section XXIV at the link above.

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Summary

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Final Comments

The Euclidean geometry is basically considering the surface of a sphere of infinite radius. Such a surface appears flat and it supports straight lines. These are boundary conditions that represent a substance of total flexibility. Within this boundary is substance that varies in the flexibility of its structure, such that the farthest point from the boundary is totally rigid.

The Euclidean geometry arbitrarily assumes a substance of totally rigid structure at the boundary and within that boundary throughout. The non-Euclidean geometry introduces the required flexibility, and the methods of Riemann accounts for the variations in that flexibility.

This flexibility represents the variations in the inertia of matter or, more generally, the variations in the consistency of substance filling the space-time.

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Einstein 1920 (XXIII) Rotating Body of Reference

Reference: Einstein’s 1920 Book

Section XXIII (Part 2)
Behaviour of Clocks and Measuring Rods on a Rotating Body of Reference

Please see Section XXIII at the link above.

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Summary

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Final Comments

The space-time continuum in the gravitational field of a rotating body of reference shall have a varying sense of  inertia/consistency associated with different locations.

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