You've written
$$ ((uw_1*(2*sl*f_1)^2) / 386.4)/tl_1 - ((uw_1*(2*sl*f_2)^2) / 386.4)/tl_1 = ((uw_2*(2*sl*f_3)^2) / 386.4)/tl_2 - ((uw_2*(2*sl*f_4)^2) / 386.4)/tl_2 $$
which I find hard to read. I'm going to replace "sl" with "S", and $uw_1$, etc., with $u_1$, and $tl_1$ with $T_1$, etc., to get
$$
((u_1*(2*S*f_1)^2) / 386.4)/T_1 - ((u_1*(2*S*f_2)^2) / 386.4)/T_1 = ((u_2*(2*S*f_3)^2) / 386.4)/T_2 - ((u_2*(2*S*f_4)^2) / 386.4)/T_2
$$
And since you've asked to solve for $u_2$, I'm going to assume $u_1$ is known. First, let's multiply both sides by $T_1 T_2$ and do some cancelling:
$$
T_2((u_1*(2*S*f_1)^2) / 386.4) - T_2((u_1*(2*S*f_2)^2) / 386.4)= T_1 ((u_2*(2*S*f_3)^2) / 386.4) - T_1((u_2*(2*S*f_4)^2) / 386.4)
$$
Now we can expand $(2*S*f_1)^2$ into $4 S^2 f_1^2$, and let $Q = 4S^2$, because it appears so often. Now we have
$$
T_2((u_1Qf_1^2) / 386.4) - T_2((u_1Qf_2^2) / 386.4)= T_1 ((u_2Qf_3^2) / 386.4) - T_1((u_2*Qf_4^2) / 386.4)
$$
Phew! It fits on one line now. Now let's factor out some stuff:
$$
(T_2 \cdot u_1 \cdot Q)
\left[ \frac{f_1^2}{ 386.4} - \frac{f_2^2}{ 386.4} \right]= (T_1 \cdot u_2 \cdot Q) \left[ \frac{f_3^2}{386.4}- \frac{f_4^2)}{386.4} \right].
$$
Multiply through by $386.4$ to get rid of it everywhere:
$$
(T_2 \cdot u_1 \cdot Q)
\left[f_1^2 - f_2^2 \right]= (T_1 \cdot u_2 \cdot Q) \left[ f_3^2-f_4^2 \right].
$$
Do a little division:
$$
(T_2 \cdot u_1 \cdot Q)
\frac{\left[f_1^2 - f_2^2 \right]}{ \left[ f_3^2-f_4^2 \right]}= (T_1 \cdot u_2 \cdot Q).
$$
Divide both sides by $Q$:
$$
(T_2 \cdot u_1 )
\frac{\left[f_1^2 - f_2^2 \right]}{ \left[ f_3^2-f_4^2 \right]}= (T_1 \cdot u_2 ).
$$
and then by $T_1$:
$$
(\frac{T_2}{T_1} \cdot u_1 )
\frac{\left[f_1^2 - f_2^2 \right]}{ \left[ f_3^2-f_4^2 \right]}=u_2 .
$$
That wasn't so bad, was it?
$\times$. – Shaun Jul 29 '17 at 15:14