Another way to solve this is by solving the nodes' current equations.
First redraw the circuit, number the nodes and their voltages, then write the nodes' equations and solve \$R_{12} = x R = 10x \Omega\$, the resistance asked for.
![schematic](https://cdn.statically.io/img/i.sstatic.net/TCtzM.png)
simulate this circuit – Schematic created using CircuitLab
The sum of currents going into every node is zero.
$$ \frac{U_1}{xR} + \frac{U_3-U_1}{R} + \frac{U_4-U_1}{3R} = 0 \\
\frac{U_3}{3R} + \frac{U4}{R} + \frac{-U_1}{xR} = 0 \\
\frac{U_1-U_3}{R} +\frac{U_4-U_3}{2R} + \frac{-U_3}{3R} = 0 \\
\frac{U_1-U_4}{3R} + \frac{U_3-U_4}{2R} + \frac{-U4}{R} = 0
$$
Recognize that \$U_1\$ is the driving voltage and therefore has to end up at the right hand side of the equations.
$$ \begin{align}
\frac{U_3}{R} + \frac{U_4}{3R} &= -\frac{U_1}{xR} + \frac{U_1}{R} + \frac{U_1}{3R} \\
\frac{U_3}{3R} + \frac{U_4}{R} &= \frac{U_1}{xR} \\
-\frac{U_3}{R} -\frac{U_3}{2R} - \frac{U_3}{3R} +\frac{U_4}{2R} &= -\frac{U_1}{R} \\
\frac{U_3}{2R} -\frac{U_4}{3R} -\frac{U_4}{2R} -\frac{U_4}{R} &= - \frac{U_1}{3R}
\end{align}
$$
Multiply the top \$2\$ equations with \$3xR\$ and the bottom \$2\$ with \$6R\$ to get
$$ \begin{align}
3 x U_3 + x U_4 &= ( -3 + 3x + x ) U_1 \\
x U_3 + 3 x U_4 &= 3 U_1 \\
( - 6 - 3 - 2 ) U_3 + 3 U_4 &= - 6 U_1 \\
3 U_3 + ( - 2 - 3 - 6 ) U_4 &= - 2 U_1
\end{align}
$$
and after regrouping
$$ \begin{align}
3 x U_3 + x U_4 &= ( 4 x - 3 ) U_1 \\
x U_3 + 3 x U_4 &= 3 U_1 \\
11 U_3 - 3 U_4 &= 6 U_1 \\
3 U_3 - 11 U_4 &= - 2 U_1
\end{align}
$$
The top 2 equations give \$ -8xU_4 = (4x - 12) U_1 \$, or
$$ 2 U_4 = ( 3/x - 1 ) U_1 $$
and the lower 2 equations give \$ 112 U_4 = 40 U_1 \$, or
$$ 2 U_4 = \frac{40}{56} U_1 = \frac{5}{7} U_1 $$
Subracting those two equations which express \$U_4\$ in \$U_1\$ from each other, gives \$ 0 = (3/x - 1 - \frac{5}{7}) U_1 \$, or
$$ x = 2 - \frac{1}{4} $$
Hence the equivalent resistance between terminals \$ 1 \$ and \$ 2 \$ equals \$ R_{12} = 17.50 \Omega \$. (How exciting...)