- #1
rwooduk
- 762
- 59
On the surface, the equation is simply the peak rarefractional pressure divided by the root of the applied frequency:
##MI = \frac{P_{ra}}{\sqrt{f}}##
But the pressure is reduced/derated by an attenuation factor/coefficient that is dependent on depth and frequency e.g. ##0.3 \ dB / (cm \cdot MHz)##
An example calculation is given in the paper "Tutorial paper: thermal and mechanical indices". Where it takes a 4 MHz pulse, at 6cm, 2 Mpa, ##0.3 \ dB / (cm \cdot MHz)## and says the MI would be (2*0.44)/SQRT(4) = 0.44. I can't get the 0.44 because the dimensional analysis with units doesn't seem right.
##MI = \frac{MPa}{\sqrt{MHz}}\cdot \frac{dB}{cm\cdot MHz}##
I can easily calculate the attenuation, which is simply the attenuation coefficient multiplied by distance and frequency. Which for his example is 7.2 dB, I can also calculate intensity from this from I = I * 10^(-dB/10), but still don't get the 0.44.
Am I overcomplicating things?
##MI = \frac{P_{ra}}{\sqrt{f}}##
But the pressure is reduced/derated by an attenuation factor/coefficient that is dependent on depth and frequency e.g. ##0.3 \ dB / (cm \cdot MHz)##
An example calculation is given in the paper "Tutorial paper: thermal and mechanical indices". Where it takes a 4 MHz pulse, at 6cm, 2 Mpa, ##0.3 \ dB / (cm \cdot MHz)## and says the MI would be (2*0.44)/SQRT(4) = 0.44. I can't get the 0.44 because the dimensional analysis with units doesn't seem right.
##MI = \frac{MPa}{\sqrt{MHz}}\cdot \frac{dB}{cm\cdot MHz}##
I can easily calculate the attenuation, which is simply the attenuation coefficient multiplied by distance and frequency. Which for his example is 7.2 dB, I can also calculate intensity from this from I = I * 10^(-dB/10), but still don't get the 0.44.
Am I overcomplicating things?