Tags:
General,
science,
Performing Arts,
Mathematics,
Physics,
Astrophysics & Space Science,
Dance,
Astrophysics,
History & Criticism,
working,
Television Plays And Programs,
Physics (Specific Aspects),
Star trek (Television program),
Video games,
Television,
Space sciences,
Television - History & Criticism,
Television - General
shoots a phaser beam at Picard as he sits on the bridge
of his captain's yacht
Calypso,
having just engaged the impulse drive (we will assume the inertial dampers are turned off
for this example)? Picard would accelerate forward, narrowly missing the brunt of the
phaser blast. When viewed in Picard's frame of reference, things would look like the
figure at the top of the following page.
So, for Picard, the trajectory of the phaser ray would be curved. What else would Picard
notice? Well, recalling the argument in the first chapter, as long as the inertial dampers
are turned off, he would be thrust back in his seat. In fact, I also noted there that if
Picard was being accelerated forward at the same rate as gravity causes things to
accelerate downward at the Earth's surface, he would feel exactly the same force pushing
him back against his seat that he would feel pushing him down if he were standing on
Earth. In fact, Einstein argued that Picard (or his equivalent in a rising elevator) would
never be able to perform any experiment that could tell the difference between the
reaction force due to his acceleration and the pull of gravity from some nearby heavy
object outside the ship. Because of this, Einstein boldly went where no physicist had gone
before, and reasoned that whatever phenomena an accelerating observer experienced would be
identical to the phenomena an observer in a gravitational field experienced.
Our example implies the following: Since Picard observes the phaser ray bending when he is
accelerating away from it, the ray must also bend in a gravitational field. But if light
rays map out spacetime, then
spacetime
must bend in a gravitational field. Finally, since matter produces a gravitational field,
then
matter must bend spacetime!
Now, you may argue that since light has energy, and mass and energy are related by
Einstein's famous equation, then the fact that light bends in a gravitational field is no
big surpriseand certainly doesn't seem to imply that we have to believe that spacetime
itself need be curved. After all, the paths that matter follows bend too (try throwing a
ball in the air). Galileo could have shown, had he known about such objects, that the
trajectories of baseballs and Pathfinder missiles bend, but he never would have mentioned
curved space.
Well, it turns out that you can calculate how much a light ray should bend if light
behaved the same way a baseball does, and then you can go ahead and measure this bending,
as Sir Arthur Stanley Eddington did in 1919 when he led an expedition to observe the
apparent position of stars on the sky very near the Sun during a solar eclipse.
Remarkably, you would find, as Eddington did, that light bends exactly
twice
as much as Galileo might have predicted if it behaved like a baseball in flat space. As
you may have guessed, this factor of 2 is just what Einstein predicted if spacetime was
curved in the vicinity of the Sun and light (or the planet Mercury, for that matter) was
locally traveling in a straight line in this curved space! Suddenly, Einstein's was a
household name.
Curved space opens up a whole universe of possibilities, if you will excuse the pun.
Suddenly we, and the
Enterprise,
are freed from the shackles of the kind of linear thinking imposed on us in the context of
special relativity, which Q, for one, seemed to so abhor. One can do many things on a
curved manifold which are impossible on a flat one. For example, it is possible to keep
traveling in the same direction and yet return to where you beganpeople who travel around
the world do it all the time.
The central premise of Einstein's general relativity is simple to state in words: the
curvature of spacetime is
directly determined by the distribution of matter and energy contained within it.