0 Members and 1 Guest are viewing this topic.
Quote from: lean beanPerhaps I'm being pernickety. Some time ago on a NASA site there was a question... '' is spacetime a thing'' the answer given was... ''Yes, it's another name for the gravitational field of the universe''Then that NASA site is wrong. Another name for the gravitationall field is not the universe. That's just plain silly.
Perhaps I'm being pernickety. Some time ago on a NASA site there was a question... '' is spacetime a thing'' the answer given was... ''Yes, it's another name for the gravitational field of the universe''
Why is the gravitational field of the universe another name for space-time?The development of any mathematical theory of natural phenomena such as gravity requires that the mathematical symbols defining the theory must be related to qualities of the phenomena such as the symbol T representing temperature, V representing velocity or M representing mass. In general relativity, a similar association had to be made by Einstein. We have seen how Einstein defined the gravitational field to be identical to the so-called metric tensor, g mu,nu used by Riemann to describe the geometry of a space. This means that where Newtonian gravity dealt with one quantity to measure the gravitational field, Einstein's theory in the guise of "g-mu-nu" required a total of 10 unique quantities to more completely define how the gravitational field behaved. The force of gravity defined as changes in the gravitational field from place to place in Newtonian mechanics, was replaced by changes in the geometry of space from place to place in spacetime measured by the degree of curvature symbolized by "C-mu-nu" at each point. Einstein's minimalist adoption of "g-mu-nu" as the embodiment of the gravitational field was significant and has far-reaching ramifications. Before Einstein, the metric tensor "g-mu-nu" was a purely geometric quantity that expresses how to determine the distances between points in space. Geometers from the time of Gauss knew nothing about forces, mass and momentum, they did however use the metric tensor to uncover new and bizarre spaces resembling nothing that humans have ever experienced.Einstein's appropriation of the metric tensor so that it also represented the gravitational field led to an inevitable, logical conclusion: If you took away the gravitational field, this meant that "g-mu-nu" would be everywhere and for all time equal to zero, but so too would the metric for spacetime. Spacetime would lose its metric, the distance between points in the manifold would vanish, and the manifold itself would disappear into nothingness. In Relativity: The Special and General Theory page 155, Einstein expressed this quality of spacetime as follows,"Spacetime does not claim existence on its own but only as a structural quality of the [gravitational] field"
I have found another site where a Dr Sten Odenwald goes into more detail as to why he thinks...
Why is the gravitational field of the universe another name for space-time?The development of any mathematical theory of natural phenomena such as gravity requires that the mathematical symbols defining the theory must be related to qualities of the phenomena such as the symbol T representing temperature, V representing velocity or M representing mass. In general relativity, a similar association had to be made by Einstein. We have seen how Einstein defined the gravitational field to be identical to the so-called metric tensor, g mu,nu …Einstein's appropriation of the metric tensor so that it also represented the gravitational field led to an inevitable, logical conclusion: If you took away the gravitational field, this meant that "g-mu-nu" would be everywhere and for all time equal to zero, but so too would the metric for spacetime.
The case of the ordinary theory of relativity arises out of the here case considered if it is possible, by reason of the particular relations of the g-mu-nu in a finite region, to choose the system of reference in the finite region in such a way that the g-mu-nu assume the constant values diag(1, -1, -1, -1)
The force of gravity defined as changes in the gravitational field from place to place in Newtonian mechanics, was replaced by changes in the geometry of space
I do not agree with the idea that the general theory of relativity is geometerzing physics or the gravitational field. The concepts of physics have always been geometrical concepts and I cannot see why the g_ik field should be called more geometrical than f.i. the electromagnetic field or the distance of bodies in Newtonian mechanics. The notion probably comes from the fact that the origin of the g_ik field is the Gauss-Riemann theory of the metrical continuum which we are wont to look at as a part of geometry. I am convinced, however, that the distinction between geometrical and other kinds of fields is not logically founded.
Space-time does not claim existence on its own, but only as a structural quality of the field.
On the basis of the general theory of relativity, on the other hand, space as opposed to "what fills space", which is dependent on the co-ordinates, has no separate existence. Thus a pure gravitational field might have been described in terms of the gik (as functions of the co-ordinates), by solution of the gravitational equations. If we imagine the gravitational field, i.e. the functions gik, to be removed, there does not remain a space of the type (1), but absolutely nothing, and also no "topological space". For the functions gik describe not only the field, but at the same time also the topological and metrical structural properties of the manifold.
A space of the type (1), judged from the standpoint of the general theory of relativity, is not a space without field, but a special case of the gik field, for which – for the co-ordinate system used, which in itself has no objective significance – the functions gik have values that do not depend on the co-ordinates. There is no such thing as an empty space, i.e. a space without field.
There is no such thing as an empty space, i.e. a space without field.
In any case he did not mean that such a field was a gravitational field.
If we imagine the gravitational field, i.e. the functions gik, to be removed, there does not remain a space of the type (1), but absolutely nothing, and also no "topological space". For the functions gik describe not only the field, but at the same time also the topological and metrical structural properties of the manifold.
And as he says, if you remove the gravitational field, your not even left with a type one space, your left with but absolutely nothing…
It will be seen from these reflexions that in pursuing the general theory of relativity we shall be led to a theory of gravitation, since we are able to "produce" a gravitational field merely by changing the system of coordinates.
In his text Einstein identifies the presence of a gravitational field with the spacetime variability of the copmponents of the metric tensor. Thusds2 = (1 + gz/c2)2 (cdt)2 - dx2 - dy2 - dz2denotes the presence of a uniform gravitational field whileds2 = (cdt)2 - dx2 - dy2 - dz2denotes the absence of a gravitational field.
In accordance with classical mechanics and according to the special theory of relativity, space (space-time) has an existence independent of matter or field.
On the basis of the general theory of relativity, on the other hand, space as opposed to "what fills space", which is dependent on the co-ordinates, has no separate existence.
A question about observer dependencies?If I assumed that 'gravity' always need to be observed in some coordinate system to 'exist' as a global phenomena, including all observers description. Can we then assume a 'space' that no observers would be able to define a 'gravity' too?If we can then 'space' clearly exist on its own, gravity not needed. If we can't?
Can you link to anywhere where that's shown. google's not helping me.
Gravity is observer dependent to me. It has to do with what coordinate system you use.
Gravity is observer dependent to me. It has to do with what coordinate system you use. But that's also because I think of it as local definitions.
Before proceeding farther, however, I must warn the reader against a misconception suggested by these considerations. A gravitational field exists for the man in the chest, despite the fact that there was no such field for the co-ordinate system first chosen. Now we might easily suppose that the existence of a gravitational field is always only an apparent one. We might also think that, regardless of the kind of gravitational field which may be present, we could always choose another reference-body such that no gravitational field exists with reference to it. This is by no means true for all gravitational fields, but only for those of quite special form. It is, for instance, impossible to choose a body of reference such that, as judged from it, the gravitational field of the earth (in its entirety) vanishes.
I'm wondering here, does Einstein mean a uniform gravitational field when he refers to special form? ''but only for those of quite special form''
No. He means those gravitational fields in flat spacetime. Consider a rotating frame of reference. In that frame there will be two inertial forces, The Coriolis force and the centrifugal force. Since there is an inertial force in the rotating frame there are gravitational forces/gravitational field in such a frame. But you can transform the field away by the proper coordinate transformation. The "special kind" that Einstein refers to are gravitational fields in which the spacetime is flat.
It is, for instance, impossible to choose a body of reference such that, as judged from it, the gravitational field of the earth (in its entirety) vanishes.