You need to learn to walk before you can learn to run, inflector. Physics students really should learn about Newtonian mechanics in general and Newton's shell theorem in particular before delving into general relativity. There are many ways to prove Newton's shell theorem.
- Use Newton's convoluted geometric arguments. One word: Yech.
- Integrate the Newton's expression for gravitational acceleration over a ring and then integrate that over the sphere. This is a rather messy double vector integral. Still yech.
- Integrate the gravitational potential and find that it is constant inside a sphere. A freshman in college could do this integral.
- Invoke Gauss law for gravitation and be done with it. Easy, but freshman don't know Gauss' law for gravitation.
With option 3 it is easy to show that the gravitational potential inside a spherical shell, while constant, is not the same as the gravitational potential at some point outside of and far removed from the shell.
General relativity must agree with Newtonian mechanics in the domain in which Newtonian mechanics has been well-tested. This is the domain of smallish masses, smallish relative velocities, and not-so-small distances between masses. Note that one of the key post-dictions of general relativity, the relativistic precession of Mercury, is a combination of a not-so-small, a not-so-small relative velocity, and somewhat small distances. Even then, the difference between Newtonian mechanics and general relativity is very, very small.
Regarding the two wikipedia statements you cited regarding the equivalence principle: First off, it's wikipedia. No justification, no explanation, no math, just raw statements. Do learn to take things in wikipedia about controversial subjects or science beyond that taught to freshmen with a big grain of salt.
The first statement applies to clocks in a spaceship. Suppose a spaceship is accelerating and has two clocks in it, one near the tail and one near the nose. That acceleration results in the equivalent of a gravitational potential difference between the clocks. The clock in the nose will be time dilated compared to the clock in the tail of the rocket.
The second statement misses the mark in my mind. In particular, it is missing the word "local". Comparing conditions inside a spherical shell of mass to those outside the shell is not a local experiment.