“Reality” of length contraction in SR vs. Bell's spaceship paradox I read John Rennie's answer to "Reality" of length contraction in SR. He concludes about the length of a stick and length contraction that

... it's just that due to the rotation in spacetime we are viewing the
  two ends at different times.

This answer seems to describe it similarly:

In a relatively moving frame, the coordinate length of the rod is
  smaller than the proper length.

Both answers sound to me as if length contraction is a matter of the observer's "relativistic perspective" alone.
Does this not contradict the (afaik accepted) explanation of Bell's spaceship paradox, according to which the thread between the spaceships breaks? I  construe the breaking thread as evidence that length contraction is not only a matter of the observer's "relativistic perspective", but that contraction is "real" in the moving system.
Can someone piece together the "relative perspective only" and "breaking thread" views? If the answer includes some "there is acceleration in the spaceship paradox", it would be great to learn how this is relevant.
 A: Some four-positions
We consider two points in the frame $S'$ which is moving relative to the frame $S$ at speed $v$. In the coordinates of $S'$, these points have four-positions
\begin{equation}
\mathbf{x}_A' = (t_A',x_A')^\intercal, \quad \mathbf{x}_B' = (t_B',x_B')^\intercal.
\end{equation}
The proper distance between these points is given by
\begin{equation}
\Delta s^2 = -\Delta t^{\prime 2} + \Delta x^{\prime 2}.
\end{equation}
Expanding the primed coordinates in terms of the unprimed coordinates, using the Lorentz transformations, we have
\begin{equation}
-(t_A'-t_B')^2 + (x'_A-x'_B)^2 = -(\gamma(t_A-vx_A)-\gamma(t_B-vx_B))^2 + (\gamma(x_A - v t_A) - \gamma(x_B - vt_B))^2,
\end{equation}
where we have deliberately not expanded out the brackets, so that we recall that the left squares and right squares correspond on both sides of the equation.
Bell's spaceships
Now we can state the Bell spaceship problem as follows. Consider two spaceships that are uniformly accelerated in $S$ so that the distance between them in $S$ remains constant. Between them lies a string that just spans the distance. The question is whether the string will break due to this acceleration. 
Mathematically we return to our four-position analysis. We wish to define a length $L' := x_A'-x_B'$ in $S'$ and so we are required to set $t_A'=t_B'$. This cancels the left-hand square on both sides of the equation. To define a length in $S$ we must do the same, defining $L := x_A - x_B$ at $t_A = t_B$. Crucially, we now set $L$ to be constant. This implies that $L'$, i.e. the distance that the observer in $S'$ experiences, as $L' = \gamma L$. We see that the distance between these two points from the point of view of $S'$ increases as the velocity increases. Note that there is no rod here, just two-comoving points and two perspectives on their absolute distance. To see length contraction, we simply fix $L'$ as the proper distance. This means that $L$ is going to see the rod obeying $L = L'/\gamma$.
Discussion
The solution to the paradox comes when we realise that fixing the distance $L$ is going to cause real stress on the object when it wants to contract, at least from the point of view of $S$. This fixing in $S$ would be viewed in $S'$ as the gradual distancing of the two spaceships as the they accelerate, causing equal stress and equally causing the string to break. The entire paradox does not crucially rely on accelerating frames. The hidden statement of the paradox is in the rewording of the setup: 
What happens to a rod if we boost it to a velocity without allowing it to contract?
Bell found that many physicists did not have good intuition for this  situation and put it down to the fact that they had never been taught what I call the 'ether intuition'. That is to say that relativity can be consistently understood by invoking an ether which is a preferred state of rest but entirely undetectable. This ether imposes physical length contraction that can have physical effects like breaking the string. Both interpretations of relativity provide the same result but Bell argued that the former could provide pedagogical power.
A: The answer is easy enough. The spaceships are accelerating, so their rest frame is not the frame in which the distance between them (ie the fixed length of the string) is set. The problem goes away if you say that the two rockets accelerate in such a way that the proper distance between them stays constant- in that case the string won't break. But the proper distance seems to become smaller and smaller in any inertial reference frame from which their accelerating motion is viewed. If you want to fix the distance between them in such an other frame, even though they are accelerating, you must increase the proper distance between them, and hence the string snaps.
To avoid conceptual traps in connection with SR it is a good idea to try to bear in mind that its effects are entirely reciprocal. If an object appears length contracted because it is passing us at speed, we seem length contracted by exactly the same amount from its perspective. In our own rest frame our dimensions are unchanged, and so are its in its rest frame. If you remember that in connection with Bell's spaceship paradox you will realise that if the rope is to break it must be because the spaceships are getting further apart in their own frame.
A: Math might not lie, but math can't tell the difference between duration contraction and length contraction. The final answer is the same.
If an object travels from A to B and accelerates, the trip gets shorter. Not distance shorter, duration shorter. This is where the confusion arises. Length contraction is real, but it's not the contraction of physical length. It's length contraction of duration.
Time dilation means less time passes on the clock of a traveller moving at relativistic speeds. At 87% of light speed, it's 50% slower than normal. For the traveler, a ten year journey, only takes 5 years. The distance doesn't change, only the duration from the traveller's perspective. It's real. Both are real. The clock on the traveler ship will confirm that the trip only took 5 years, but, it's a clock, not an odometer. 
