Given \( h = 4.25 \times 10^{-15} \, \text{eV} \cdot \text{s} \), the frequency of the incident light is related to the energy absorbed by the hydrogen atoms using the equation:
\[
E = h \times f
\]
Where:
- \( E \) is the energy absorbed,
- \( h \) is Planck's constant,
- \( f \) is the frequency of the incident light.
The total emission lines are 6, so the electron must have absorbed energy and jumped from \( n = 1 \) to \( n = 4 \). The energy difference between these levels can be expressed as:
\[
\Delta E = h \times f
\]
Using the formula for the frequency, we calculate:
\[
\Delta E = 13.6 \left[ \frac{1}{4^2} - \frac{1}{2^2} \right] \, \text{eV}
\]
Now solving for the frequency:
\[
f = \frac{12.75 \times 10^{-15}}{4.25 \times 10^{-15}} = 3 \times 10^{15} \, \text{Hz}
\]
Thus, \( x = 12 \).