A frequency response identification method for discrete-time processes with cyclic steady state conditions

Automatica ◽  
2014 ◽  
Vol 50 (12) ◽  
pp. 3260-3267 ◽  
Author(s):  
Kyungsu Kim ◽  
Yu Jin Cheon ◽  
In-Beum Lee ◽  
Jietae Lee ◽  
Su Whan Sung
2014 ◽  
Vol 24 (6) ◽  
pp. 1002-1014 ◽  
Author(s):  
Kyung Hwan Ryu ◽  
Si Nae Lee ◽  
Chang-Mo Nam ◽  
Jietae Lee ◽  
Su Whan Sung

2012 ◽  
Vol 45 (15) ◽  
pp. 331-336
Author(s):  
Yu Jin Cheon ◽  
Hyunjoo Kim ◽  
Kyung Su Kim ◽  
Kyung Hwan Ryu ◽  
In-Beum Lee ◽  
...  

AIChE Journal ◽  
2011 ◽  
Vol 57 (12) ◽  
pp. 3429-3435 ◽  
Author(s):  
Yu Jin Cheon ◽  
Su Whan Sung ◽  
Jietae Lee ◽  
Cheol Ho Je ◽  
In-Beum Lee

1997 ◽  
Vol 273 (4) ◽  
pp. F625-F634 ◽  
Author(s):  
H. E. Layton ◽  
E. Bruce Pitman ◽  
Leon C. Moore

A mathematical model was used to investigate the filter properties of the thick ascending limb (TAL), that is, the response of TAL luminal NaCl concentration to oscillations in tubular fluid flow. For the special case of no transtubular NaCl backleak and for spatially homogeneous transport parameters, the model predicts that NaCl concentration in intratubular fluid at each location along the TAL depends only on the fluid transit time up the TAL to that location. This exact mathematical result has four important consequences: 1) when a sinusoidal component is added to steady-state TAL flow, the NaCl concentration at the macula densa (MD) undergoes oscillations that are bounded by a range interval envelope with magnitude that decreases as a function of oscillatory frequency; 2) the frequency response within the range envelope exhibits nodes at those frequencies where the oscillatory flow has a transit time to the MD that equals the steady-state fluid transit time (this nodal structure arises from the establishment of standing waves in luminal concentration, relative to the steady-state concentration profile, along the length of the TAL); 3) for any dynamically changing but positive TAL flow rate, the luminal TAL NaCl concentration profile along the TAL decreases monotonically as a function of TAL length; and 4) sinusoidal oscillations in TAL flow, except at nodal frequencies, result in nonsinusoidal oscillations in NaCl concentration at the MD. Numerical calculations that include NaCl backleak exhibit solutions with these same four properties. For parameters in the physiological range, the first few nodes in the frequency response curve are separated by antinodes of significant amplitude, and the nodes arise at frequencies well below the frequency of respiration in rat. Therefore, the nodal structure and nonsinusoidal oscillations should be detectable in experiments, and they may influence the dynamic behavior of the tubuloglomerular feedback system.


Automatica ◽  
1993 ◽  
Vol 29 (2) ◽  
pp. 523-526 ◽  
Author(s):  
Irwin W. Sandberg ◽  
Lilian Y. Xu

1994 ◽  
Vol 116 (3) ◽  
pp. 550-553 ◽  
Author(s):  
Chung-Wen Chen ◽  
Jen-Kuang Huang

This paper proposes a new algorithm to estimate the optimal steady-state Kalman filter gain of a linear, discrete-time, time-invariant stochastic system from nonoptimal Kalman filter residuals. The system matrices are known, but the covariances of the white process and measurement noises are unknown. The algorithm first derives a moving average (MA) model which relates the optimal and nonoptimal residuals. The MA model is then approximated by inverting a long autoregressive (AR) model. From the MA parameters the Kalman filter gain is calculated. The estimated gain in general is suboptimal due to the approximations involved in the method and a finite number of data. However, the numerical example shows that the estimated gain could be near optimal.


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