TY - JOUR
T1 - E-wave deceleration time may not provide an accurate determination of LV chamber stiffness if LV relaxation/viscoelasticity is unknown
AU - Shmuylovich, Leonid
AU - Kovács, Sándor J.
PY - 2007/6
Y1 - 2007/6
N2 - Average left ventricular (LV) chamber stiffness (ΔP avg/ΔVavg) is an important diastolic function index. An E-wave-based determination of ΔPavg/ΔVavg (Little WC, Ohno M, Kitzman DW, Thomas JD, Cheng CP. Circulation 92: 1933-1939, 1995) predicted that deceleration time (DT) determines stiffness as follows: ΔPavg/ΔVavg = N(π/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 ΔPavg/ ΔVavg 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 ΔPavg/ΔVavg has been validated, we reexpress the DT-stiffness (ΔPavg/ΔVavg) relation of Little et al. as follows: DTk ≈ π/(2 √k). Using the kinematic model, we derive the general DT-chamber stiffness/viscoelasticity relation as follows: DTk,c = π/(2 √k) + c/(2k) (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 ΔPavg/ΔVavg 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.
AB - Average left ventricular (LV) chamber stiffness (ΔP avg/ΔVavg) is an important diastolic function index. An E-wave-based determination of ΔPavg/ΔVavg (Little WC, Ohno M, Kitzman DW, Thomas JD, Cheng CP. Circulation 92: 1933-1939, 1995) predicted that deceleration time (DT) determines stiffness as follows: ΔPavg/ΔVavg = N(π/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 ΔPavg/ ΔVavg 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 ΔPavg/ΔVavg has been validated, we reexpress the DT-stiffness (ΔPavg/ΔVavg) relation of Little et al. as follows: DTk ≈ π/(2 √k). Using the kinematic model, we derive the general DT-chamber stiffness/viscoelasticity relation as follows: DTk,c = π/(2 √k) + c/(2k) (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 ΔPavg/ΔVavg 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.
KW - Diastole
KW - Echocardiography
KW - Mathematical modeling
UR - http://www.scopus.com/inward/record.url?scp=34447548916&partnerID=8YFLogxK
U2 - 10.1152/ajpheart.01068.2006
DO - 10.1152/ajpheart.01068.2006
M3 - Article
C2 - 17220184
AN - SCOPUS:34447548916
SN - 0363-6135
VL - 292
SP - H2712-H2720
JO - American Journal of Physiology - Heart and Circulatory Physiology
JF - American Journal of Physiology - Heart and Circulatory Physiology
IS - 6
ER -