TY - JOUR
T1 - A method for the analysis of turbulence measured in the canine aorta with hot-film anemometer.
AU - Yamaguchi, T.
AU - Yoshikawa, T.
AU - Kikkawa, S.
AU - Sugawara, M.
PY - 1980
Y1 - 1980
N2 - A method for analyzing the turbulence phenomena in the aorta is presented. The blood velocity measured with a hot-film anemometer in the canine ascending aorta is referred in the discussion. All the experimental data were recorded on magnetic tape and processed on a digital computer after analog-to-digital conversion for the analysis. The turbulence velocity is defined as the difference between a sample velocity recording and the ensemble average of sample recordings. To discriminate the fluid dynamical fluctuations from physiological deviations, we used a threshold to exclude recordings with extraordinary amplitude and waveform due to the arrhythmia of the heart from the ensemble of the sample velocity recordings. Small deviations of the recordings due to respiratory changes were corrected with a coefficient which equates the time integral of each individual velocity recording to that of the ensemble average velocity. The mean turbulence intensity was calculated as the square root of the time mean of the ensemble average square of turbulent velocity during deceleration phase of the ensemble average velocity. The mean turbulence intensity defined above is shown to be related closely to the maximum of ensemble average velocity in each dog.
AB - A method for analyzing the turbulence phenomena in the aorta is presented. The blood velocity measured with a hot-film anemometer in the canine ascending aorta is referred in the discussion. All the experimental data were recorded on magnetic tape and processed on a digital computer after analog-to-digital conversion for the analysis. The turbulence velocity is defined as the difference between a sample velocity recording and the ensemble average of sample recordings. To discriminate the fluid dynamical fluctuations from physiological deviations, we used a threshold to exclude recordings with extraordinary amplitude and waveform due to the arrhythmia of the heart from the ensemble of the sample velocity recordings. Small deviations of the recordings due to respiratory changes were corrected with a coefficient which equates the time integral of each individual velocity recording to that of the ensemble average velocity. The mean turbulence intensity was calculated as the square root of the time mean of the ensemble average square of turbulent velocity during deceleration phase of the ensemble average velocity. The mean turbulence intensity defined above is shown to be related closely to the maximum of ensemble average velocity in each dog.
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U2 - 10.9746/sicetr1965.16.913
DO - 10.9746/sicetr1965.16.913
M3 - Article
AN - SCOPUS:0018936813
SN - 0453-4654
VL - 16
SP - 913
EP - 918
JO - TRANS. SOC. INSTRUM. & CONTROL ENGRS., JAPAN
JF - TRANS. SOC. INSTRUM. & CONTROL ENGRS., JAPAN
IS - 6 , 1980
ER -