ohadohad2 said:
Ok I got a question.
So we know that in space light travels at a constant speed of 3X10^8m/s.
We also know that light can't escape a black hole gravity field.
So let's assume I got a light source just near a black hole (lets assume the gravity field is radial) ,my light source is transmiting light outwards fron the black hole,in the exact oposite direction of the gravity vector.
Now since we know the light can't escape than we know it will change direction and move to the black hole.
The paradox is:Since the light changed its direction it had to slow down,stop and start accelerating in the diffrent direction.Thus not compling with what we all learnt,that light moves at a constant speed.
Yes I know I look at this mostly on Newtonic physics,I would love to hear your quantom physics awnser to this.
Note that the speed of light is always equal to c in
special relativity. It is also always equal to c in General relativity,
as long as one uses local clocks and rulers to measure that speed. This is important, because (to use the slightly over-simple popular explanation) clocks are known to tick at different rates depending on their location when one considers the effects of General relativity. It should be reasonably obvious that if clocks tick at different rates, one has to specify which clock to use to measure the time to compute the speed. There is, however, a choice of clock (and a corresponding choice of ruler) that makes the speed of light always constant and equal to c even in GR - this is a clock and ruler of some physical (jargon: timelike) observer at the same location as the light is.Here's a specific example relevant to your question.
Suppose you are in a spaceship falling into a black hole. We will assum in this simple example that the spaceship is free-falling into the black hole and that its engines are off.
The front of the spaceship emits a particle of light (a photon, if you will, though you should think of it clasically and not quauntum mechanically) just as it enters the event horizon. The light particle is emitted away from the black hole.
The light particle will follow a very simple path. It will maintain constant Schwarzschild coordinates. To speak slightly losely, it will neither approach nor recede from the black hole, it will just "hang in space" - (using Schwarzschild coordinates as a reference).
The spaceship, however, can and must fall into the black hole.
The person on the spaceship knows the length of the spaceship, and has clocks on the front and rear of the spaceship which he has synchronized. He computes the travel time from when the light particle was emitted at the front, and when the light particle is received at the back. Taking the length of the spaceship divided by the time to traverse it gives the speed of the light particle relative to the spaceship. This measured speed will be exactly equal to 'c'.
Here's a more formal reference on the topic from the sci.physics.faq
http://math.ucr.edu/home/baez/physics/Relativity/SpeedOfLight/speed_of_light.html
Einstein went on to discover a more general theory of relativity which explained gravity in terms of curved spacetime, and he talked about the speed of light changing in this new theory. In the 1920 book "Relativity: the special and general theory" he wrote: . . . according to the general theory of relativity, the law of the constancy of the velocity of light in vacuo, which constitutes one of the two fundamental assumptions in the special theory of relativity [. . .] cannot claim any unlimited validity. A curvature of rays of light can only take place when the velocity of propagation of light varies with position. Since Einstein talks of velocity (a vector quantity: speed with direction) rather than speed alone, it is not clear that he meant the speed will change, but the reference to special relativity suggests that he did mean so. This interpretation is perfectly valid and makes good physical sense, but a more modern interpretation is that the speed of light is constant in general relativity.
The problem here comes from the fact that speed is a coordinate-dependent quantity, and is therefore somewhat ambiguous. To determine speed (distance moved/time taken) you must first choose some standards of distance and time, and different choices can give different answers. This is already true in special relativity: if you measure the speed of light in an accelerating reference frame, the answer will, in general, differ from c.
In special relativity, the speed of light is constant when measured in any inertial frame. In general relativity, the appropriate generalisation is that the speed of light is constant in any freely falling reference frame (in a region small enough that tidal effects can be neglected). In this passage, Einstein is not talking about a freely falling frame, but rather about a frame at rest relative to a source of gravity. In such a frame, the speed of light can differ from c, basically because of the effect of gravity (spacetime curvature) on clocks and rulers.
Thus, talking about "speed" is ambiguous, there are multiple definitions of what it might mean. With the modern definition of speed, the speed of light is always constant in SR and in GR. With some other defintions of speed, definitions which are commonly used (though not "modern"), the speed of light is still always constant in SR, but with these alternate defintions, the speed is not necessarily constant in GR.