AJP - Heart Calcium Transients and Cell-Sarcomere
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Am J Physiol Heart Circ Physiol 292: H2712-H2720, 2007. First published January 12, 2007; doi:10.1152/ajpheart.01068.2006
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E-wave deceleration time may not provide an accurate determination of LV chamber stiffness if LV relaxation/viscoelasticity is unknown

Leonid Shmuylovich and Sándor J. Kovács

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 ({Delta}Pavg/{Delta}Vavg) is an important diastolic function index. An E-wave-based determination of {Delta}Pavg/{Delta}Vavg (Little WC, Ohno M, Kitzman DW, Thomas JD, Cheng CP. Circulation 92: 1933–1939, 1995) predicted that deceleration time (DT) determines stiffness as follows: {Delta}Pavg/{Delta}Vavg = N({pi}/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 {Delta}Pavg/{Delta}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: H178–H187, 1987) with stiffness (k) and relaxation/viscoelasticity (c) parameters. Because the predicted linear relation between k and {Delta}Pavg/{Delta}Vavg has been validated, we reexpress the DT-stiffness ({Delta}Pavg/{Delta}Vavg) relation of Little et al. as follows: DTk {approx} Formula. Using the kinematic model, we derive the general DT-chamber stiffness/viscoelasticity relation as follows: DTk,c = Formula(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 {Delta}Pavg/{Delta}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



Address for reprint requests and other correspondence: S. J. Kovács, Cardiovascular Biophysics Laboratory, Washington Univ. Medical Center, 660 South Euclid Ave., Box 8086, St. Louis, MO 63110 (e-mail: sjk{at}wuphys.wustl.edu)




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