R. Burattini et Kb. Campbell, EFFECTIVE DISTRIBUTED COMPLIANCE OF THE CANINE DESCENDING AORTA ESTIMATED BY MODIFIED T-TUBE MODEL, The American journal of physiology, 264(6), 1993, pp. 1977-1987
To estimate descending thoracic aortic compliance in anesthetized open
-chest dogs, a modified T-tube arterial model was used. This model con
sists of two uniform and lossless elastic tubes, one representing arte
ries going toward the head and upper limbs and the other (body tube) r
epresenting descending aortic circulation to the trunk and lower limbs
. Each tube terminates with a generalized first-order low-pass filter
load. Pressure and flow in the ascending aorta and flow in the upper d
escending aorta were measured and used to estimate model parameters. U
sing the estimated model parameters, we calculated the pressure wavesh
ape at the termination of the body tube. Comparison of this model-pred
icted pressure with pressure measured in the abdominal aorta near the
origin of renal arteries suggested that the end of the body tube (effe
ctive reflecting site of the body circulation) corresponds to this maj
or branching site of the abdominal aorta. To calculate the length of t
he body tube, we used aortic pulse wave velocity estimated from the me
asurements of pressure in ascending and abdominal aorta. Calculated bo
dy tube length averaged 30.3 +/- 2.8 cm and approximated the measured
length (30.6 +/- 3.0 cm) of the aorta from the arch to the region of t
he origin of renal arteries. Compliance of the body tube averaged 123
+/- 20 x 10(-6) g-1.cm4.s2 and was interpreted as the descending thora
cic aortic compliance. The ratio of this compliance to the body tube l
ength gave an estimate of the effective distributed compliance, i.e.,
the compliance per unit length that would be observed in the absence o
f tapering. This ratio averaged 4.10 +/- 0.86 x 10(-6) g-1.cm3.s2 and
fell in between the values of local aortic compliance independently es
timated along the descending thoracic aorta from measurements of press
ure and diameter. Thus tube compliance resulted in a physically identi
fiable property. This property was contrasted with the ill-defined eff
ective compliances of the terminal loads.