nelsyeung said:
I kinda understand what you are saying but, I don't quite get then how can gravity be calculated using gm/r^2
and also during the relativistic effect a particle will increases mass dramatically which causes the acceleration to slow down, so i thought there must be a clear link between mass and gravity.. :( hmm..
That is a common misconception that I am always fighting. Let's split our thoughts about gravity into the dynamics (i.e. the forces) and the kinematics (i.e. the motion). And for simplicity let's start with Newtonian gravity and only consider cases where M>>m (i.e. a small particle in the gravitational field of a big planet).
Dynamics: The particle is acted on by a force F = GMm/r². The mass of the particle does determine the force on the particle, so a particle with m=0 should have no force. But how do we measure this force? It turns out that this force is impossible to measure directly, we can use a scale to weigh the object, but what this actually measures is the normal force not the force of gravity. Since we cannot measure this force then how do we know it is given by F = GMm/r²? We know because of the kinematics, i.e. on a scale we measure the normal force, the object is kinematically stationary, so there must be a gravitational force cancelling out the normal force.
Kinematics: The particle undergoes an acceleration of a = GM/r² if it is free to move. So a free particle of m=0 should (according to Newtonian theory) undergo the same acceleration as any other free particle. We can measure this acceleration directly, so in some sense, this acceleration is the primary effect of gravity and the force is a secondary or presumed effect. Now, since we can directly measure the acceleration of a massless particle let's work backwards and see what the force should be. We can use F = ma = 0 GM/r² = 0. So from the kinematics, despite the fact that the particle is accelerating, the force is 0, i.e. it does not take any force to accelerate a massless particle, they have no inertia. So this kinematic result is consistent with the dynamics above.
GR: Now, there is one big problem with all of the above, and that is that all massless objects travel at c where relativistic considerations are obviously important. So it turns out that the Newtonian approximation is off by a factor of 2. I don't want to get too far into the details, but in GR gravity is not considered a real force at all. Instead, the observed kinematics are attributed to curved spacetime rather than to any force. In other words, free particles, like a satellite, travel in (locally) straight lines called geodesics through a (globally) curved spacetime. There is no force of gravity, so there really are no dynamics, and the path of the particle depends on the curvature of the underlying spacetime and not on the mass of the particle. Therefore, massless free particles also travel on these geodesics so their path is (globally) curved just like everything else. Again, the kinematics do not depend on the mass of the particle.