Selected Solutions
v = 331 m/s (1 + (T - 273 K)/273 K)1/2 = (331 m/s)(1 + (295 K - 273 K)/273 K)1/2 = 344 m/s
Please note that the equation in the book is poorly written and should be re-written as above. Since the echo took 3.0 s to return, this means that the sound took 1.5 s to reach the mountain. At 344 m/s, this means that the mountain is
d = (344 m/s)(1.5 s) = 516 m
l' = l + vs/f
This corresponds to a frequency that is given by
f' = v/l' = f v/(v + vs)
This is the frequency relative to still air. As the bicyclist moves through this wave, she hears a frequency that is increased above this still air frequency by
f'' = f'(v + vo)/v = f (v + vo)/(v + vs)
If we use the fact that 3vo = vs, we get
f'' = f (v + vo)/(v + 3vo)
Solving this for vo, we get
f'' (v + 3vo)
= f (v + vo)
vo
(3f'' - f) = v (f - f'')
vo
= v (f - f'')/(3f'' - f) = 345 m/s (25/805) = 10.7 m/s
Since the car is moving 3 times faster, the speed of the car is 32.1 m/s.
fn = n v/(2L)
where v is the speed of sound, n=1,2,3,..., and L is the length of the tube. For the fundemental frequency, we set n = 1. This means that the length of the pipe can be found by solving for L, i.e.
L = v/(2f1) = (345 m/s)/(523.2 Hz) = .659 m
When we close off one end, we impose a node at one end and change the resonant frequencies by
fn = n v/(4L)
If f3 = 261.6 Hz, then we can solve for the length of the pipe by
L = 3v/(4f3) = (1035 m/s)/(1046 Hz) = .989 m.