This means that the star should only depend on the distance from the star (Hawley and Holcomb 1998). As a result of this fact, it was not possible to disregard the angular terms (Hawley and Holcomb 1998). Lastly, the star along with its gravitational field do not change with time, this means that the metric terms are independent of time, but only when the time coordinate is chosen correctly (Hawley and Holcomb 1998). The time coordinate Schwarzschild used was a rational one because it can be correlated to the time calculated by an observer who was a significant distance away from the central mass, where gravity's effects ebb down to zero (Hawley and Holcomb 1998).
The authors point out that Schwarzschild radius is the identical to the radius used for the Newtonian dark star (Hawley and Holcomb 1998). However because Newtonian gravitation is suitable as it relates to a good approximation, it should be anticipated that the radius would not be too far from its prediction (Hawley and Holcomb 1998). However the black hole is a much more interesting and foreign theory than is the dark star, and as such reflecting upon the black hole as if it were a Newtonian dark star may cause a misunderstanding of the important aspects of the black hole (Hawley and Holcomb 1998).
With these things being understood, why is every round object not considered a black hole? The answer to this has to do with the fact that the Schwarzschild radius can be found in the outer surface of any "normal" object, including a neutron star. For instance, the Schwarzschild radius of the Sun is 3 kilometers; on the other hand the solar radius is more than 1 million kilometers. In addition the Schwarzschild radius of the Earth is below 1 centimeter. Again, the solution presented by Schwarzschild relates only to the empty space contained in the exterior of the sphere (Hawley and Holcomb 1998). This means that if the Schwarzschild radius is less than the radius of the body, it is immaterial inside the body (Hawley and Holcomb 1998). The author also asserts that the metric contained inside of a star is not consistent with a Schwarzschild metric, but is instead a different metric that incorporates the existence of the matter which produces the gravitational field (Hawley and Holcomb 1998). A black hole can only be formed if the object has totally collapsed and vanished beneath its Schwarzschild radius (Hawley and Holcomb 1998).
The authors further explain that at the Schwarzschild radius, the coefficient of the time interval in the Schwarzschild metric is zero (Hawley and Holcomb 1998). As a result, the time interval itself becomes infinite (Hawley and Holcomb 1998). Likewise, radial intervals decrease to zero, which is the definitive length contraction. These effects occur as a result of the choice of coordinates, and these coordinates are not ever absolute even as it relates to Newtonian physics. Nonetheless, the length contraction, time dilation, and other relativistic effects that are dependent upon the metric coefficients, are actual physical occurrences and can be calculated with the right type of instruments (Hawley and Holcomb 1998). In addition the gravitational field in the vicinity of the black hole is more significant at small radius than it is when it is at some distance away, and as a result light moving from near the object endures a gravitational redshift (Hawley and Holcomb 1998).
As it relates to the black hole, any light sent from the Schwarzschild radius is perpetually redshifted (Hawley and Holcomb 1998). As a result the sphere that is derivative of the Schwarzschild radius is reflective of a surface from which light is not able travel to an outside observer. In addition an observer from outside this horizon can not see within the horizon because the inside of the black hole is infinitely unable to communicate with the rest of the universe (Hawley and Holcomb 1998). Likewise the Events that take place inside the black hole can have no contributory contact with events outside the black hole (Hawley and Holcomb 1998). This limit that exists between the inside...
scientific notation, its uses and rules for calculations. One example from everyday life: a computer hard disk holds 4 gigabytes of information, that is 4,000,000,000 bytes of information. Written in scientific notation, that is 4 X 109 bytes. Scientific notation is used to write very large and very small numbers. While ordinary numbers are useful for everyday measurements, for large measurements like astronomical distances, scientific notations offers a way of
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