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The Evans Equations of Unified Field Theory - Alpha Institute for ...

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<strong>The</strong> Metric<br />

<strong>The</strong> metric <strong>of</strong> special relativity is the Minkowski metric. A metric is a map<br />

in a spacetime that defines the distance and also some mathematical functions <strong>of</strong><br />

the spacetime, like simple addition and multiplication. If one looks around the<br />

region in which they find themselves, a metric exists. It is the reality within which<br />

they find themselves and is a simple mapping. It establishes a distance from<br />

every point to every other. In relativity the metric is typically designated as ηµν =<br />

( -1, 1, 1, 1) and is multiplied against distances. At times it appears as (+1, -1, -1,<br />

-1). For example, (dt 2 , dx 2 , dy 2 , and dz 2 ) give the distances between two four<br />

dimensional points. <strong>The</strong>n ηαβ (dt 2 , dx 2 , dy 2 , and dz 2 ) = -dt 2 + dx 2 + dy 2 + dz 2<br />

<strong>The</strong> invariant distance is ds where<br />

ds 2 = -dt 2 + dx 2 + dy 2 + dz 2 (2)<br />

Alternatively, letting dx stand <strong>for</strong> dx, dy, and dz combined, ds 2 = dx 2 -dt 2 .<br />

This distance is sometimes called the “line element.” In relativity – both<br />

special and general – the spacetime metric is defined as above. When<br />

calculating various quantities, distance or momentum or energy, etc., the metric<br />

must be considered. Movement in time does change quantities just as<br />

movement in space does.<br />

We will see the equation g(a, b) or simply g used. It is the metric<br />

tensor and is a function <strong>of</strong> two vectors. All it means is the dot, more precisely the<br />

inner) product <strong>of</strong> the two vectors combined with the spacetime metric. <strong>The</strong> result<br />

is a 4-dimensional distance as shown in Figure 1-9 using curved Riemann<br />

geometry<br />

instead <strong>of</strong> the Euclidean in the figure. (See the Glossary under Metric<br />

Tensor.)<br />

<strong>The</strong> nature <strong>of</strong> the metric becomes very important as one moves on to<br />

general relativity and unified field theory. <strong>The</strong> metric <strong>of</strong> quantum theory is the<br />

same as that <strong>of</strong> special relativity. It is a good mathematical model <strong>for</strong><br />

approximations, but it is not the metric <strong>of</strong> our real universe. Gravitation cannot<br />

be described. In the same manner, Riemann geometry describes gravitational<br />

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