Hanya Shizuo
J Heart Valve Dis. 2015 May;24(3):280-5.
To date, no study has determined the specified Bernoulli constant (K) and validated the simplified Bernoulli equation for semilunar valve stenosis by simultaneous measurement of peak jet flow velocity and maximum pressure gradient in humans.
Using multisensor catheters, the relationship between the peak jet flow velocity (V) and maximum-pressure gradient (max-PG) across the stenosis were analyzed, and K-values calculated for patients with pulmonary (n = 37) and aortic (n = 6) valve stenosis, who were stratified by max-PG into two groups: max-PG 50 mmHg (n = 28; group A) and those with max-PG > 50 mmHg (n = 15; group B).
The specified constant K obtained for max-PG with peak jet flow velocity squared (V2) was 3.9, which was very close to the simplified Bernoulli constant (= 4.0), with a wide distribution in K-value for max-PG (median [interquartile range]: 3.9 [3.0-4.5]). Although there were no significant differences in specified K-values between two groups (p = 0.216), the values of K were significantly more widely scattered in group A than in group B (3.4 [2.5-4.8] versus 4.1 [3.8-4.4]; p < 0.001).
The study results confirmed that, the more severe the stenosis the better suited the simplified Bernoulli constant (K = 4.0) could be for assessing semilunar valve stenosis. This result is consistent with the fluid-mechanical theorem that the kinetic energy of the jet (1/2) ρV92) (= 4.0V(2)) produced by the stenosis disappears completely only downstream of the severe semilunar valve stenosis.
迄今为止,尚无研究通过同时测量人体半月瓣狭窄处的峰值射流流速和最大压力阶差来确定特定的伯努利常数(K)并验证简化伯努利方程用于半月瓣狭窄的情况。
使用多传感器导管,分析狭窄处峰值射流流速(V)与最大压力阶差(max - PG)之间的关系,并计算肺动脉瓣狭窄患者(n = 37)和主动脉瓣狭窄患者(n = 6)的K值,这些患者按max - PG分层为两组:max - PG≤50 mmHg(n = 28;A组)和max - PG>50 mmHg(n = 15;B组)。
由峰值射流流速平方(V²)得到的max - PG的特定常数K为3.9,非常接近简化伯努利常数(= 4.0),max - PG的K值分布较广(中位数[四分位间距]:3.9 [3.0 - 4.5])。尽管两组之间特定K值无显著差异(p = 0.216),但A组K值的离散度明显大于B组(3.4 [2.5 - 4.8] 对 4.1 [3.8 - 4.4];p < 0.001)。
研究结果证实,狭窄越严重,简化伯努利常数(K = 4.0)越适合用于评估半月瓣狭窄。该结果与流体力学定理一致,即狭窄产生的射流动能(1/2)ρV²(= 4.0V²)仅在严重半月瓣狭窄下游完全消失。