|
|
||||||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Cardiovascular Biophysics Laboratory, Washington University School of Medicine, St. Louis, Missouri
Submitted 29 September 2006 ; accepted in final form 8 January 2007
Average left ventricular (LV) chamber stiffness (
Pavg/
Vavg) is an important diastolic function index. An E-wave-based determination of
Pavg/
Vavg (Little WC, Ohno M, Kitzman DW, Thomas JD, Cheng CP. Circulation 92: 19331939, 1995) predicted that deceleration time (DT) determines stiffness as follows:
Pavg/
Vavg = N(
/DT)2 (where N is constant), which implies that if the DTs of two LVs are indistinguishable, their stiffness is indistinguishable as well. We observed that LVs with indistinguishable DTs may have markedly different
Pavg/
Vavg values determined by simultaneous echocardiography-catheterization. To elucidate the mechanism by which LVs with indistinguishable DTs manifest distinguishable chamber stiffness, we use a validated, kinematic E-wave model (Kovács SJ, Barzilai B, Perez JE. Am J Physiol Heart Circ Physiol 252: H178H187, 1987) with stiffness (k) and relaxation/viscoelasticity (c) parameters. Because the predicted linear relation between k and
Pavg/
Vavg has been validated, we reexpress the DT-stiffness (
Pavg/
Vavg) relation of Little et al. as follows: DTk
. Using the kinematic model, we derive the general DT-chamber stiffness/viscoelasticity relation as follows: DTk,c =
(where c and k are determined directly from the E-wave), which reduces to DTk when c << k. Validation involved analysis of 400 E-waves by determination of five-beat averaged k and c from 80 subjects undergoing simultaneous echocardiography-catheterization. Clinical E-wave DTs were compared with model-predicted DTk and DTk,c. Clinical DT was better predicted by stiffness and relaxation/viscoelasticity (r2 = 0.84, DT vs. DTk,c) jointly rather than by stiffness alone (r2 = 0.60, DT vs. DTk). Thus LVs can have indistinguishable DTs but significantly different
Pavg/
Vavg if chamber relaxation/viscoelasticity differs. We conclude that DT is a function of both chamber stiffness and chamber relaxation viscoelasticity. Quantitative diastolic function assessment warrants consideration of simultaneous stiffness and relaxation/viscoelastic effects.
echocardiography; mathematical modeling; diastole
| HOME | HELP | FEEDBACK | SUBSCRIPTIONS | ARCHIVE | SEARCH | TABLE OF CONTENTS |
| Visit Other APS Journals Online |