Nakamura T, Nakajima T, Suzuki N, Arai S, Suwa N
Tohoku J Exp Med. 1976 Jul;119(3):245-56. doi: 10.1620/tjem.119.245.
Pressure-overloaded hypertrophy of the left ventricle (LV) was produced by coarctation of the ascending aorta in 7 dogs. The overall mean weight of the left ventricle (LVW) was 7.86 +/- 1.49 (S.D.) g/kg body weight; (normal, 5.99 +/- 0.70 g/kg: p less than 0.05). After potassium arrest, pressure-volume (P-V) relationships were examined with the left ventricles isolated from the normals and from the dogs of left ventricular hypertrophy (LVH-dogs). In both groups, the P-V relationships could be expressed by an equation deltaV=a-be-cP throughout the range of filling pressure of 2.5 to 35 cmH2O, where deltav was the actual volume change of LV, P intraventricular pressure, and a, b and c constants. A sensitive index of LV stiffness, the half-inflation pressure (h), was defined as 1n (2b/a)/c. In hypertrophied hearts, h was 10.5 +/- 0.7 cmH2O; (normal 8.0 +/- 0.4 cmH2O; P less than 0.001). The ratio of LVW to LVVp=h (the left ventricular volume at h) in hypertrophy, which was related to the LV chamber geometry, was 3.1 +/- 0.6 in contrast with the normal value of 2.0 +/- 0.3. The development of concentric hypertrophy was thus demonstrated. Moreover, h was closely correlated with LVW/LVVp=h in both the normals and the LVH-dogs (r=0.83; p less than 0.01). On the other hand, an index of LV wall stiffness h/LVW/LVVP=h was relatively constant. Therefore, the increase of LV stiffness in the LVH-dogs was attributed to the change in chamber geometry.
通过升主动脉缩窄在7只犬中造成左心室压力超负荷肥大。左心室的总体平均重量(LVW)为7.86±1.49(标准差)g/kg体重;(正常为5.99±0.70 g/kg:p<0.05)。钾停搏后,对从正常犬和左心室肥大犬(LVH犬)分离出的左心室进行压力-容积(P-V)关系研究。在两组中,在2.5至35 cmH₂O的充盈压力范围内,P-V关系可用方程ΔV = a - be⁻ᶜᴾ表示,其中ΔV是左心室的实际容积变化,P是心室内压力,a、b和c为常数。左心室僵硬度的敏感指标半充盈压力(h)定义为ln(2b/a)/c。在肥厚心脏中,h为10.5±0.7 cmH₂O;(正常为8.0±0.4 cmH₂O;P<0.001)。肥厚时与左心室腔几何形状相关的LVW与LVVp = h的比值为3.1±0.6,而正常值为2.0±0.3。由此证实了向心性肥大的发展。此外,在正常犬和LVH犬中,h与LVW/LVVp = h密切相关(r = 0.83;p<0.01)。另一方面,左心室壁僵硬度指标h/LVW/LVVP = h相对恒定。因此,LVH犬左心室僵硬度的增加归因于心腔几何形状的改变。