Respuesta :
A) A. 380 kHz
To clerly see the image of the fetus, the wavelength of the ultrasound must be 1/4 of the size of the fetus, therefore
[tex]\lambda=\frac{1}{4}(1.6 cm)=0.4 cm=0.004 m[/tex]
The frequency of a wave is given by
[tex]f=\frac{v}{\lambda}[/tex]
where
v is the speed of the wave
[tex]\lambda[/tex] is the wavelength
For the ultrasound wave in this problem, we have
v = 1500 m/s is the wave speed
[tex]\lambda=0.004 m[/tex] is the wavelength
So, the frequency is
[tex]f=\frac{1500 m/s}{0.004 m}=3.75\cdot 10^5 Hz=375 kHz \sim 380 kHz[/tex]
B) B. f(c+v)/c−v
The formula for the Doppler effect is:
[tex]f'=\frac{v\pm v_r}{v\pm v_s}f[/tex]
where
f' is the apparent frequency
v is the speed of the wave
[tex]v_r[/tex] is the velocity of the receiver (positive if the receiver is moving towards the source, negative if it is moving away from the source)
[tex]v_s[/tex] is the speed of the source (positive if the source is moving away from the receiver, negative if it is moving towards the receiver)
f is the original frequency
In this problem, we have two situations:
- at first, the ultrasound waves reach the blood cells (the receiver) which are moving towards the source with speed
[tex]v_r = +v[/tex] (positive)
- then, the reflected waves is "emitted" by the blood cells (the source) which are moving towards the source with speed
[tex]v_s = -v[/tex]
also
v = c = speed of sound in the blood
So the formula becomes
[tex]f'=\frac{c + v}{v - v_s}f[/tex]
C. A. The gel has a density similar to that of skin, so very little of the incident ultrasonic wave is lost by reflection
The reflection coefficient is
[tex]R=\frac{(Z_1 -Z_2)^2}{(Z_1+Z_2)^2}[/tex]
where Z1 and Z2 are the acoustic impedances of the two mediums, and R represents the fraction of the wave that is reflected back. The acoustic impedance Z is directly proportional to the density of the medium, [tex]\rho[/tex].
In order for the ultrasound to pass through the skin, Z1 and Z2 must be as close as possible: therefore, a gel with density similar to that of skin is applied, in order to make the two acoustic impedances Z1 and Z2 as close as possible, so that R becomes close to zero.