A few more comments. In a previous post, I suggested that it was best to treat gravity as a fictitious force, rather than a real force. This is a rather subtle point, involving Einstein's equivalence principle, and could be argued. But "Einstein's elevator" is routinely used to explain General Relativity, henceforth GR, and why GR only has one sort of mass rather than two separate sorts of masses in Newton's theory. The two sorts of masses in Newton's theory are gravitational mass and inertial mass, and Newton's theory provides no explanation of why they should always be the same, while Einstein's theory assumes they are the same.
When we look closely at Einstein's elevator, we see that the force stretching the spring is actually not a real force, but a fictitious force. The real force is applied to one end of the spring. The other end of the spring applies a force to accelerate the mass.
This is good as far as it goes, but it doesn't go far enough, in my opinion. Many of the more interesting predictions of GR simply do not have a natural interpretation as a "force". One example of this is gravitational time dilation. Forces and time dilation are two different things, that are apparently unrelated. But there is a deeper connection, which can be seen by understanding the geometric version of the theory.
Another example of such a phenomenon that doesn't have a natural interpretation as a force are the predictions of GR of the changes in spatial geometry that occur near large masses (with a suitable definition of terms, most notably a definition of spatial geometry that involves splitting a static space-time geometry into a static spatial geometry and some notion of time).
Basically, attempting to unnaturally force all the predictions of GR into the paradigm of a "force" is not natural to the theory, and will lead to an incomplete understanding of the predictions of the theory. Some aspects of gravity are more amenable than others to a 'force' interpretation, but many interesting aspects of the theory are best explained from the geometrical viewpoint.
Fully understanding the geometrical viewpoint of GR is no easy task. But it has its rewards if one follows through. It is possible to understand some aspects of GR without understanding it's geometrical viewpoint, but generally such understandings are limited and incomplete.