Measuring combustion response by a forced oscillation method

1972 ◽  
Author(s):  
R. BROWN ◽  
J. ERICKSON ◽  
W. BABCOCK
Author(s):  
V. Mikhaltsevitch ◽  
M. Lebedev ◽  
R. Chavez ◽  
M. Pervukhina ◽  
S. Glubokovskikh ◽  
...  

1987 ◽  
Vol 57 (7) ◽  
pp. 315-318
Author(s):  
Seiichi Yasuda ◽  
Junichi Masuda ◽  
Hiromasa Sekiguchi ◽  
Masao Nagano ◽  
Hirozumi Morishige ◽  
...  

1983 ◽  
Vol 76 (3special) ◽  
pp. 1023-1030
Author(s):  
Yukimoto Horibe ◽  
Shigenobu Iwata ◽  
Tadao Nishimura ◽  
Masao Naito ◽  
Teiji Okada ◽  
...  

1964 ◽  
Vol 1 (5) ◽  
pp. 304-305 ◽  
Author(s):  
ROBERT A. KILGORE ◽  
BENJAMIN T. AVERETT

1974 ◽  
Vol 1974 (136) ◽  
pp. 163-171
Author(s):  
Seiji Takezawa ◽  
Ryoichi Kojima ◽  
Masao Takekawa

2019 ◽  
Vol 87 ◽  
pp. 68-87 ◽  
Author(s):  
Charles Lorenzini ◽  
Alexandre Sanfelice Bazanella ◽  
Luís Fernando Alves Pereira ◽  
Gustavo R. Gonçalves da Silva

1993 ◽  
Vol 120 (1) ◽  
pp. 73-84 ◽  
Author(s):  
T. GOTOH ◽  
H. UNNO ◽  
N. SHIRAGAMI ◽  
H. HONDA ◽  
Y. NAOKI

1986 ◽  
Vol 61 (3) ◽  
pp. 873-880 ◽  
Author(s):  
J. H. Bates ◽  
M. Decramer ◽  
W. A. Zin ◽  
A. Harf ◽  
J. Milic-Emili ◽  
...  

Relaxed expirations were obtained from five anesthetized dogs under control conditions and during various rates of intravenous infusion of histamine. All volume vs. time curves obtained from 20 ms to 2 s after the start of expiration were poorly described by a single exponential function but were fitted very well by a biexponential function. The resistance of the respiratory system as a function of frequency from 2 to 26 Hz was also determined by the forced oscillation method in the same dogs. Three two-compartment models of the respiratory system were identified from the exponentials fitted to the relaxed expiration data, and the one that had the most plausible parameter values under control conditions consisted of a homogeneous lung compartment connected to a viscoelastic compartment. Although a two-compartment model is arguably appropriate for describing relaxed expirations in normal dogs, physiological considerations suggest that there should be more than two interacting components with histamine infusion. We cannot identify all these components from our data, however. The equivalent complex impedance of the respiratory system was also calculated from the biexponential curves and showed significant variation in resistance over the frequency range from 0 to 2 Hz and negligible variation above 2 Hz. The calculated resistances at 2 Hz were consistently higher than those obtained by the forced oscillation method, which may be due to the nonlinear behavior of the respiratory system during relaxed expiration. We conclude that the single-breath and forced oscillation methods should be viewed as providing complimentary information about respiratory resistance.


1991 ◽  
Vol 70 (1) ◽  
pp. 143-151 ◽  
Author(s):  
B. Louis ◽  
A. Harf ◽  
H. Lorino ◽  
D. Isabey

Determination of the frequency response of pneumotachographs is needed whenever they are used to measure high-frequency flows, such as in the forced oscillation method. When screen and capillary pneumotachographs are calibrated using an adiabatic compression in a closed box as a reference impedance, they can be adequately described by a series of inertial-resistive elements. However, this type of reference impedance strongly differs from the actual respiratory impedance (ZL). We studied the frequency response of pneumotachographs up to 250 Hz in reference to the impedance of a compressible gas oscillating in a long tube, taken as a more generalizable model of actual ZL. We found that, with this device, the series resistance-inertance models fail to describe the frequency response of the pneumotachograph. However, when compressible effects in the pneumotachograph are taken into account by adding to the resistive models a compliance (Cpn) corresponding to the compression in half of the inner volume of the pneumotachograph, the agreement with experiments becomes satisfactory. Gas compression-related phenomena were demonstrated to be negligible only when the parameter omega Cpn magnitude of ZL is much smaller than 1 (omega pulsation). Results obtained in normal humans have shown that such a correction is required above 100 Hz. Similar correction at lower frequency might also be necessary in cases of large respiratory impedance (e.g., babies, subjects with pathological lungs, and intubated subjects).


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