The sound of the thunder takes about \(\displaystyle 0.2\ \text{s}\) extra to cover the same \(\displaystyle 1720\ \text{m}\) once the air cools from \(\displaystyle 22\ ^\circ\text{C}\) to \(\displaystyle 0\ ^\circ\text{C}\).

Section $\displaystyle 10.6.3$ gives the tool: speed \(\displaystyle =\) distance \(\displaystyle \div\) time, used in Example $\displaystyle 10.3$ as distance \(\displaystyle = v \times t\); rearranged, time \(\displaystyle = \dfrac{\text{distance}}{\text{speed}}\).
At \(\displaystyle 22\ ^\circ\text{C}\) the speed is \(\displaystyle 344\ \text{m s}^{-1}\) (Section $\displaystyle 10.6.3$, repeated in the question), so \(\displaystyle t_{22} = \dfrac{1720\ \text{m}}{344\ \text{m s}^{-1}} = 5.00\ \text{s} \).
At \(\displaystyle 0\ ^\circ\text{C}\) the speed is \(\displaystyle 331\ \text{m s}^{-1}\), so \(\displaystyle t_{0} = \dfrac{1720\ \text{m}}{331\ \text{m s}^{-1}} = 5.196\ \text{s} \approx 5.2\ \text{s} \).
The extra time is the difference: \(\displaystyle \Delta t = t_{0} - t_{22} = 5.196\ \text{s} - 5.00\ \text{s} = 0.196\ \text{s} \approx 0.2\ \text{s} \).
Direction check against the chapter: Section $\displaystyle 10.6.3$ states that as the temperature is increased the speed of sound increases, so cooling the air lowers the speed, and a slower wave needs longer for the same distance. The difference therefore has to come out positive and small compared with the \(\displaystyle 5\ \text{s}\) journey itself \(\displaystyle -\) which \(\displaystyle 0.196\ \text{s}\) is.
The book's printed Answer Key gives $\displaystyle 331$ s, which does not agree with Section $\displaystyle 10.6.3$ (nor with the question's own stem): \(\displaystyle 331\) there is the speed of sound in dry air at \(\displaystyle 0\ ^\circ\text{C}\), in \(\displaystyle \text{m s}^{-1}\), not a time. The key entry appears to have copied that speed and re-labelled it as seconds.
Reasoning beyond the chapter, to show the printed figure cannot be rescued by any reading of the question: the entire trip at \(\displaystyle 0\ ^\circ\text{C}\) lasts only \(\displaystyle 5.2\ \text{s}\), so no delay inside this problem can be \(\displaystyle 331\ \text{s}\); and \(\displaystyle 331\ \text{s}\) of travel at roughly \(\displaystyle 340\ \text{m s}^{-1}\) would be \(\displaystyle 331\ \text{s} \times 340\ \text{m s}^{-1} = 112540\ \text{m} \approx 113\ \text{km} \), not the \(\displaystyle 1720\ \text{m}\) the question sets. The chapter's own two speeds settle it the other way, at \(\displaystyle 0.196\ \text{s} \approx 0.2\ \text{s}\).