A) D. 285Hz
We can solve the problem by using the Doppler effect formula:

where
f' is the apparent frequency
v = 340 m/s is the velocity of the sound wave
is the velocity of the observer (the cyclist, in this case), which is negative because the cyclist is moving towards the sound source
is the velocity of the sound source (zero, in this case, since the musician is stationary)
f = 281 Hz is the original frequency
Substituting into the equation, we find:

B) B. 277 Hz
Similarly, we can solve the problem by using the Doppler effect formula:

where
f' is the apparent frequency
v = 340 m/s is the velocity of the sound wave
is the velocity of the observer (the cyclist, in this case), which is now positive because the cyclist is moving away from the sound source
is the velocity of the sound source (zero, in this case, since the musician is stationary)
f = 281 Hz is the original frequency
Substituting into the equation, we find:
