Physics, asked by einstien6729, 1 year ago

what is spacetime or space and time? what is a worm hole? pls tell in detail​

Answers

Answered by pqramandhoni7
3

Wormhole

A wormhole is a theoretical passage through space-time that could create shortcuts for long journeys across the universe. Wormholes are predicted by the theory of general relativity. But be wary: wormholes bring with them the dangers of sudden collapse, high radiation and dangerous contact with exotic matter.

Common intuition previously supposed no connection between space and time. Physical space was held to be a flat, three-dimensional continuum—i.e., an arrangement of all possible point locations—to which Euclidean postulates would apply. To such a spatial manifold, Cartesian coordinates seemed most naturally adapted, and straight lines could be conveniently accommodated. Time was viewed independent of space—as a separate, one-dimensional continuum, completely homogeneous along its infinite extent. Any “now” in time could be regarded as an origin from which to take duration past or future to any other time instant. Uniformly moving spatial coordinate systems attached to uniform time continua represented all unaccelerated motions, the special class of so-called inertial reference frames. The universe according to this convention was called Newtonian. In a Newtonian universe, the laws of physics would be the same in all inertial frames, so that one could not single out one as representing an absolute state of rest.

In the Minkowski universe, the time coordinate of one coordinate system depends on both the time and space coordinates of another relatively moving system according to a rule that forms the essential alteration required for Einstein’s special theory of relativity; according to Einstein’s theory there is no such thing as “simultaneity” at two different points of space, hence no absolute time as in the Newtonian universe. The Minkowski universe, like its predecessor, contains a distinct class of inertial reference frames, but now spatial dimensions, mass, and velocities are all relative to the inertial frame of the observer, following specific laws first formulated by H.A. Lorentz, and later forming the central rules of Einstein’s theory and its Minkowski interpretation. Only the speed of light is the same in all inertial frames. Every set of coordinates, or particular space-time event, in such a universe is described as a “here-now” or a world point. In every inertial reference frame, all physical laws remain unchanged.

Einstein’s general theory of relativity (1916) again makes use of a four-dimensional space-time, but incorporates gravitational effects. Gravity is no longer thought of as a force, as in the Newtonian system, but as a cause of a “warping” of space-time, an effect described explicitly by a set of equations formulated by Einstein. The result is a “curved” space-time, as opposed to the “flat” Minkowski space-time, where trajectories of particles are straight lines in an inertial coordinate system. In Einstein’s curved space-time, a direct extension of Riemann’s notion of curved space (1854), a particle follows a world line, or geodesic, somewhat analogous to the way a billiard ball on a warped surface would follow a path determined by the warping or curving of the surface. One of the basic tenets of general relativity is that inside a container following a geodesic of space-time, such as an elevator in free-fall, or a satellite orbiting the Earth, the effect would be the same as a total absence of gravity. The paths of light rays are also geodesics of space-time, of a special sort, called “null geodesics.” The speed of light again has the same constant velocity c.

In both Newton’s and Einstein’s theories, the route from gravitational masses to the paths of particles is rather roundabout. In the Newtonian formulation, the masses determine the total gravitational force at any point, which by Newton’s third law determines the acceleration of the particle. The actual path, as in the orbit of a planet, is found by solving a differential equation. In general relativity, one must solve Einstein’s equations for a given situation to determine the corresponding structure of space-time, and then solve a second set of equations to find the path of a particle. However, by invoking the general principle of equivalence between the effects of gravity and of uniform acceleration, Einstein was able to deduce certain effects, such as the deflection of light when passing a massive object, such as a star.


pqramandhoni7: Bhai itna bada learn ka lega
einstien6729: bhai physics bas samajhne ki hoti hai
pqramandhoni7: but phir bhi
pqramandhoni7: Ye warmhole or spacetime samajh mein toh aata he but use long range mein batana mein toh learn karna hi padega
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