I have found the following unit-distance embedding of the cubic symmetric graph $F_{42}A$ with $D_7$ symmetry. (Gerbracht's embedding on the MathWorld page for cubic symmetric graphs is only of $C_7$ symmetry; for embeddings of other cubic symmetric graphs see my Shibuya repository.)

Let the blue vertex above have coordinates $(a,\frac12)$, which with $D_7$ symmetry determines the rest of the graph. $a$ must satisfy the following sextic over $\mathbb Q[t]$: $$256 a^{6} + a^{5} \left(16 t^{5} - 320 t^{3} + 304 t\right) + a^{4} \left(- 16 t^{2} - 144\right) + a^{3} \left(- 32 t^{5} + 656 t^{3} - 912 t\right) + a^{2} \left(- 4 t^{4} + 112 t^{2} - 188\right) + a \left(7 t^{5} - 136 t^{3} + 57 t\right) - t^{4} + 13 t^{2} + 14=0\tag1$$ where $t=\tan\frac\pi7$. This suggests that there should be six algebraically related $D_7$ embeddings, but the above polynomial has only two real roots, leading to two embeddings: the one above and the one below.

In the spirit of what I did at the end of this other answer, I want to see whether I can factor $(1)$ further to obtain a quadratic whose roots are the two real solutions for $a$ ($a=0.27455\dots$ in the first picture and $a=1.24353\dots$ in the second). Normally I would use GAP's DecomPoly for this, but it only accepts polynomials over $\mathbb Q$ and not any extension of it, and certainly feeding it the degree-$36$ polynomial that $a$ satisfies over $\mathbb Q$* would take too long.
How can I find or show non-existence of a factorisation of $(1)$ over an extension of $\mathbb Q[t]$ in a reasonable amount of time?
*$_{68719476736 a^{36} - 532575944704 a^{34} + 1975684956160 a^{32} - 4512936886272 a^{30} + 7013413158912 a^{28} - 8394446471168 a^{26} + 8723128909824 a^{24} - 7969139851264 a^{22} + 6247085506560 a^{20} - 4187786313728 a^{18} + 2514551767040 a^{16} - 1412168695808 a^{14} + 697307058176 a^{12} - 259585758208 a^{10} + 65704151296 a^{8} - 10689048384 a^{6} + 1029214816 a^{4} - 48560176 a^{2} + 790321}$
The resolvent method for determining Galois groups works over any field – not just $\mathbb Q$ – and is enough to solve this question. To illustrate how consider coordinate values $a$ and $b$ in the following unit-distance embedding of $F_{56}A$ with $D_{14}$ symmetry:
$a$ and $b$ satisfy $$a^{4} \left(16 t^{4} + 16 t^{2}\right) - 64 a^{3} t^{3} + a^{2} \left(- 8 t^{4} + 24 t^{2}\right) + 16 a t + t^{4} + 5 t^{2} - 4=0\\ b^{4} \left(16 t^{4} + 16 t^{2}\right) + 64 b^{3} t^{3} + b^{2} \left(- 8 t^{4} + 24 t^{2}\right) - 16 b t + t^{4} + 5 t^{2} - 4=0$$ where $t=\tan\frac\pi{14}$. To compute the resolvent polynomial in $\mathbb Q[t][y]$ exactly I use Stauduhar's method of computing its coefficients numerically to high precision and "rounding" them to the nearest element in $\mathbb Q[t]$ – where rounding means applying an integer relation algorithm. Concretely, using mpmath and SymPy for the resolvent of the $a$-polynomial with respect to $x_1-x_2$:
$P$ at the end is the exact resolvent polynomial, and the last lines of the program's output are Singular commands to factor the resolvent in $\mathbb Q[t]$.
The orbit-length partition corresponding to $x_1-x_2$ is $(4,8)$. Now I can consult Soicher and McKay (1985), p. 277 for the possible Galois groups of the $a$-polynomial; the only possibility for degree $4$ and partition $(4,8)$ is $D_4$, the dihedral group of order $8$. Checking LMFDB then shows that the $a$-polynomial splits over a quadratic extension of $\mathbb Q[t]$, which in this case is $\mathbb Q[t,u=\sqrt{-21t^4+98t^2+71}]$. Indeed the $b$-polynomial also splits over $\mathbb Q[t,u]$ and $$z_1=2\sqrt{14(31t^5u-20t^4-154t^3u+104t^2+87tu-68)}\qquad z_2=7t(t^2-3)^2-4u$$ $$a=\frac{z_1+z_2}{64}\qquad b=\frac{z_1-z_2}{64}$$
Returning to the original question, I compute the resolvent of $(1)$ with respect to $x_1+x_2$:
then factor:
The orbit-length partition is $(15)$; Soicher and McKay indicate that the Galois group is one of $PSL(2,5),PGL(2,5),A_6,S_6$. However, LMFDB shows that none of these four groups allow subfields, so the conclusion is that $(1)$ has no factorisation over an extension of $\mathbb Q[t]$. Indeed, the results of further resolvent tests with respect to $p_\Delta=\prod_{i<j}(x_i-x_j)$ and $x_1+x_2+x_3+p_\Delta$ (cf. this "tutorial" by Curtis Bright) shows that the Galois group of $(1)$ over $\mathbb Q[t]$ is exactly $S_6$.