v = ÖB/r for a liquid. v = ÖB/r= Ö2.8
x 1010Pa/1.36 x 104kg/m3 = 1.4km/s.
(a) Solve for the intensity. b
= (10db)logI/I0 10b/10dB
= I/I0 I = I010b/10dB Solve
for P0. For T = 20.0°C, v = 343m/s. P0/2rv
= I
= I010b/10dB P0 = Ö2rvI010b/10dB
= Ö2(1.20kg/m3)(343m/s)(10W/m2)10120.0dB/10dB
= 28.7N/m2. (b) F
= P0A = (28.7N/m2)(0.550 x 10-4m2)
= 1.58mN.
fn = nv/2L for a pipe open at both ends
and v = 343m/s for T = 20.0°C. Find L. f1
= v/2L L = v/2f1
= (343m/s)/2(130.8Hz)
= 1.31m.
fbeat = Df =3(64.5Hz) -
196.0Hz = 0.2Hz.
(a) A source and an observer are traveling toward each other (vs
> 0, vo < 0) fo = [(1 - v0/v)/(1
- v0s/v)] ffs = {[1 -
(-0.50)]/(1 - 0.5}}(1.0kHz) = 3.0KHz.
(b) A source and an observer are traveling away from each other (vs
< 0, vo > 0) fo = [(1- 0.50)/(1
+ 0.50)](1.0kHz) = 330Hz.
(c) A source and an observer are traveling in the same direction (vs
< 0, vo < 0) fo = [(1 - 0.50)/(1
- 0.50)](1.0kHz) = 1.0kHz.
Use the result of Problem 31 for the frequency of reflected waves during
angiodynography fbeat = Df = fr
- f = ( 1 + vcell>/vsound)/(1 - vcell/vsound)f
- f = (5.0 x 10Hz)[(1 + 0.1m/s/15700m/s)/(1 - 0.10m/s/1570m/s) - 1} = 640Hz.
Problem 31 result: