Answer:

Step-by-step explanation:
The change of frecuency of sound due to the movement of the source is colled Doppler Effect.
As James (the source) is running toward the wall, the frecuency reaching the wall (so the eco sound) will be higher than the source. In this case the frecuency at the wall will be:

where
is the speed of source, 2 m/s
and
is the speed of sound, given that we have wind movind the air in the opposite direction respect to the wall, the speed of sound would be:
Replacing the values:

Now the wall becames the new source, and James (the observer is aproaching the source), for an observer aproaching the source the new frecuency will be:

Now the waves are traveling in the direction of wind, so the velocity of sound will be:
Replacing:
