Step 1: Understand phase change conditions.
At air--soap interface: reflection from rarer to denser, so phase reversal occurs.
At soap--glass interface: reflection from rarer (soap) to denser (glass), so phase reversal occurs again.
Thus, two phase reversals cancel each other.
Step 2: Condition for reflection maxima at normal incidence.
\[
2nt = m\lambda
\]
Step 3: Adjacent maxima correspond to successive integers.
So for \(\lambda_1 = 420\) nm and \(\lambda_2 = 630\) nm:
\[
2nt = m(420) = (m-1)(630)
\]
Step 4: Solve for \(m\).
\[
m\cdot 420 = (m-1)\cdot 630
\]
\[
420m = 630m - 630
\]
\[
210m = 630
\Rightarrow m = 3
\]
Step 5: Compute thickness \(t\) using \(m=3\).
\[
2nt = 3 \times 420
\]
\[
2(1.4)t = 1260
\Rightarrow 2.8t = 1260
\]
\[
t = \frac{1260}{2.8} = 450 \text{ nm}
\]
Final Answer:
\[
\boxed{450 \text{ nm}}
\]