Step 1: Set up the Doppler picture with wind.
Source and observer approach each other, so the heard frequency rises. With wind present, sound travels in an effective medium, so we use \[ f' = f\left(\frac{v_{eff} + v_o}{v_{eff} - v_s}\right). \]
Step 2: Convert speeds to $ms^{-1}$.
Using $1\,kmph = \tfrac{5}{18}\,ms^{-1}$: source $v_s = 31\times\tfrac{5}{18} \approx 8.61\,ms^{-1}$, observer $v_o = 23\times\tfrac{5}{18} \approx 6.39\,ms^{-1}$, wind $v_w = 5\times\tfrac{5}{18} \approx 1.39\,ms^{-1}$.
Step 3: Fix the effective sound speed.
The wind blows from observer toward the source, opposite to the sound's travel from source to observer, so it reduces the effective speed: $v_{eff} = 340 - 1.39 \approx 338.6\,ms^{-1}$.
Step 4: Build the numerator and denominator.
Numerator $v_{eff} + v_o = 338.6 + 6.39 = 344.99$. Denominator $v_{eff} - v_s = 338.6 - 8.61 = 329.99$.
Step 5: Compute the apparent frequency.
$f' = 660\times \dfrac{345}{330} = 660\times 1.0454 \approx 690\,Hz$.
Step 6: Conclude.
Both motions raise the pitch and the wind makes only a small change, giving about $690\,Hz$, which is option (3).
\[ \boxed{f' \approx 690\,Hz} \]