Module 1 & 2 Calculations Flashcards
If the speed of a wave is c = 1540 m/s and the frequency is 5 MHz, show that the wavelength is λ = 0.31 mm (2 significant figures are adequate). Also determine the period of the wave.
c = f λ λ=c/f λ = 1540/5x10^6Hz = 0.31x10^-3m = 0.31mm
Period (T) = 1/f = 1/5x10^6Hz = 0.2x10^-6s
Sketch the wave front and ray methods of illustrating travelling waves
Draw the concentric circles with ray arrow and wavelength marked. Sketch Huygens wavelets along a front with circles, wavefront and rays.
If the speed of a wave in soft tissue is 1540 m/s what is the wavelength for the following frequencies: 1 MHz, 5 MHz, 10 MHz and 15 MHz? Repeat this calculation for a frequency in the audible range. 1000Hz is in the hearing range.
c = f λ λ = c/f
λ = 1540/1 x 10^6 = 1.54 x 10 ^-3m = 1.54mm
λ = 1540/5 x 10^6 = 0.308 10^-3m = 0.31mm
λ = 1540/10 x 10^6 = 0.154 x 10^-3m = 0.15mm
λ = 1540/15 x 10^6 = 0.102 x 10^-3m = 0.10mm
1000Hz is in the hearing range.
c = f λ λ = c/f
λ = 1540/1000 = 1.54m
Use the idea of Huygens’ principle and wavelets to extend the wave crest pattern in Figure 1.4.
Just draw more concentric circles, each circle (crest) increased in radius by one
wavelength.
Draw two identical sinusoidal waves (like that in Figure 1.1) one above the other and below sketch the time variation of the sum of these two waves. What is the amplitude and relative intensity of the resultant wave compared to the original waves?
The sum of these two original, identical, waves has an amplitude equal to twice that of each original wave, and an intensity equal to four times that of each original wave.
The speed of sound in human soft tissue averages 1540 m/s. Using the powers of ten, re-write this speed using distances in m, cm and mm, and times in s, ms and μs (so 8 ‘new’ expressions).
- 54x10^5cm/s 1.54x10^6mm/s
- 54m/ms 1.54x10-3m/us
- 54x10^2cm/ms 0.15cm/us
- 54x10^3mm/ms 1.54mm/us
1 g of muscle occupies a volume of about 0.95 cm3. What is the density of muscle expressed in kg/m3 and g/cm3?
ρ = m/V ρ = 1/0.95 = 1.05g/cm^3 = 1.05 x 10^-6kg/m^3
What, very roughly, is the wavelength of a diagnostic ultrasound wave in soft tissue? What organs/tissues/structures in the human body are significantly greater than this value (a couple of examples)? What organs/tissues/structures in the human body are significantly smaller than this value (a couple of examples)?
c=fλ λ= c/f = 1540/5x10^6 = 0.31x10^-3m = 0.31mm
All major organs, bones, tendons and muscles are larger than this.
Things smaller than this might include blood and very small microbubbles of air.
Calculate the elapsed time for the echo detection from a structure at a depth of 5cm, assuming the velocity is constant at 1540 m/s.
How would the calculated depth be affected if the overlying tissues had a high fat composition? Provide quantitative estimates to justify your answer.
D = 154000 x ▲t / 2 2D = 154000 x ▲t ▲t = 2D/154000 = 10/154000 = 0.0000649s = 64.9us The calculated depth would appear larger than it is in reality as the speed of sound in fat is slower than it is in most other soft tissues. This means the time elapsed is longer and according to D = 154000 x ▲t / 2 D will appear larger. The speed of sound in fat is 1450m/s rather than the assumed speed of sound in soft tissues which is 1540m/s.
Water = 1.49 x 10^6 kg/m^2/s ST = 1.63 x 10^6kg/m^2/s Bone = 5.7x10^6 Air = 430kg/m^2/s Using the Z values provided determine the reflection and transmission coefficients for interfaces between (average) soft tissue and: (i) air (ii) water (iii) bone
(i) air ( I did this back the front) Air (Z1) = 430kg/m^2/s ST (Z2) = 1.63 x 10^6kg/m^2/s R = Ir/Ii = (Z2 – Z1)2/(Z2 + Z1)2 = (1.63 x 10^6 – 430)^2 / (1.63 x 10^6 + 430)2 = 0.9989 T = It/Ii = 4Z2 Z1 /(Z2 + Z1)2 = 4(1.63 x 10^6) x 430 / 1.63 x 10^6 + 430)^2 = 0.00105
(ii) water (I did this back the front) Water (Z1) = 1.49 x 10^6 kg/m^2/s ST (Z2) = 1.63 x 10^6kg/m^2/s R = Ir/Ii = (Z2 – Z1)2/(Z2 + Z1)2 = (1.63 x 10^6 - 1.49 x 10^6)^2 / (1.63 x 10^6 + 1.49 x 10^6)^2 =0.0020 T = It/Ii = 4Z2 Z1 /(Z2 + Z1)2 = 4 x 1.63 x 10^6 x 1.49 x 10^6 / (1.63 x 10^6 + 1.49 x 10^6) ^2 = 0.9979 (iii) bone ST (Z1) = 1.63 x 10^6 Bone (Z2) = 5.7x10^6 R = Ir/Ii = (Z2 – Z1)2/(Z2 + Z1)2 = (5.7x10^6 – 1.63 x 10^6)^2 / (5.7x10^6 + 1.63 x 10^6)^2 = 0.308 T = It/Ii = 4Z2 Z1 /(Z2 + Z1)2 = 4x5.7x10^6x1.63 x 10^6 / (5.7x10^6 + 1.63 x 10^6)^2 = 0.6916
The amplitude of a CW decreases by a factor of 3. By how much does the intensity of the wave change?
I = const.A^2 A = 3
I = const.3^2
I = const.9
Const. = I/9
Therefore, I has decreased by a factor of 9.
Express the intensity ratios below in dB:
(a) Ix/Io = 1/2
(b) Ix/Io = 1/4
(c) Ix/Io = 1/10
(d) Ix/Io = 1/100
(e) Ix/Io = 4
Using dB = 10 log10 (Ix/Io)
(a) Ix/Io = 1/2 dB = -3
(b) Ix/Io = 1/4 dB = -6
(c) Ix/Io = 1/10 dB = -10
(d) Ix/Io = 1/100 dB = -20
(e) Ix/Io = 4 dB = 6
Express the amplitude ratios below in dB:
(a) Ax/Ao = 1/2
(b) Ax/Ao = 1/10
(c) Ax/Ao = 10
dB = 10 log10(Ax/Ao)2 = 20 log10 (Ax/Ao)
(a) Ax/Ao = 1/2 dB = -6
(b) Ax/Ao = 1/10 dB = -20
(c) Ax/Ao = 10 dB = 20
Estimate the attenuation loss and the corresponding intensity ratio for a 7MHz sound wave with a maximum depth of field of 4 cm.
Repeat this for a maximum depth of field of 6cm and 8 cm.
Attenuation loss = 0.7 x f x 2D dB f is in MHz and D is in cm
= 0.7 x 7 x 2 x 4 =39.2dB
dB = 10 log10 (Ix/I0)
-39.2 = 10 log Ix/I0 Hence Ix/I0 = inverse log (-39.2/10) = 0.00012 = 1.2 x 10^-4
*must remember dB is negative when calculating in terms of attenuation loss
= 0.7 x 7 x 2 x 6 =58.8dB
dB = 10 log10 (Ix/I0)
-58.8 = 10 log Ix/I0 Hence Ix/I0 = inverse log (-58.8/10) = 0.0000013 = 1.3x10^-6
= 0.7 x 7 x 2 x 8 =78.4dB
dB = 10 log10 (Ix/I0)
-78.4 = 10 log Ix/I0 Hence Ix/I0 = inverse log (-78.4/10) = 0.000000014 = 1.4x10^-8
Here you can see that as the distance increases the intensity ratio decreases very rapidly.
Estimate the attenuation loss for a sound wave of frequency 1 MHz with a maximum depth of field of 4 cm.
Repeat this for sound wave frequencies of 5MHz and 10MHz.
Attenuation loss = 0.7 x f x 2D dB = 0.7 x 1 x (2x4) dB = 5.6dB = 0.7 x 5 x (2x4) dB = 28dB = 0.7 x 10 x (2x4) dB = 56dB This shows that the higher the frequency the higher the attenuation, and the lower the signal received back at the transducer.