Step 1: Write the formula for optical path difference introduced by a thin plate.
When a thin plate of thickness \(t\) and refractive index \(\mu\) is introduced in the path of one ray, the extra optical path difference introduced is
\[
\Delta x=(\mu-1)t
\]
Given,
\[
\mu=\frac{13}{7}
\]
and
\[
t=1.4\times 10^{-6}\,\text{m}
\]
Step 2: Calculate the optical path difference.
\[
\Delta x=\left(\frac{13}{7}-1\right)(1.4\times 10^{-6})
\]
\[
\Delta x=\left(\frac{6}{7}\right)(1.4\times 10^{-6})
\]
\[
\Delta x=1.2\times 10^{-6}\,\text{m}
\]
Step 3: Convert wavelength into SI unit.
Given wavelength is
\[
\lambda=480\,\text{nm}
\]
Since,
\[
1\,\text{nm}=10^{-9}\,\text{m}
\]
Therefore,
\[
\lambda=480\times 10^{-9}\,\text{m}
\]
\[
\lambda=4.8\times 10^{-7}\,\text{m}
\]
Step 4: Find the phase difference.
Phase difference introduced is
\[
\Delta \phi=\frac{2\pi}{\lambda}\Delta x
\]
Substituting the values,
\[
\Delta \phi=\frac{2\pi}{4.8\times 10^{-7}}\times 1.2\times 10^{-6}
\]
\[
\Delta \phi=2\pi\times \frac{1.2\times 10^{-6}}{4.8\times 10^{-7}}
\]
\[
\Delta \phi=2\pi\times 2.5
\]
\[
\Delta \phi=5\pi
\]
Step 5: Final conclusion.
Therefore, the phase difference introduced at the position of central maxima is
\[
\boxed{5\pi}
\]