This study revealed that a PEAR1/HIF‐1α/ glycolysis/lactate/H3K18la positive feedback loop in PMVECs that drives the development of S‐ALI. Mechanistically, PEAR1 mediates the binding of HIF‐1α to AARS1, leading to the lactylation of HIF‐1α, the primary lactylation site of which is K172.
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Sensors Layout Optimization Design of Rocket Sled Test System. [PDF]
Qian H, Wang W, Zhao X, Jiang Y.
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Baseline Ventricular-Arterial Coupling Modifies Left Atrial Pressure Response to Venoarterial Extracorporeal Membrane Oxygenation In Vitro. [PDF]
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Assessing left atrial systolic contribution via pressure-volume loops in murine HFpEF. [PDF]
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Chest compression synchronized ventilation versus chest compression superimposed by sustained inflation in asphyxiated newborn piglets: a randomized animal trial. [PDF]
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Enhanced external counter pulsation as a novel therapy to maintain cardiac output during hemodialysis: a preliminary randomized controlled study. [PDF]
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One of the problems that has to be solved in order to improve the accuracy of the results obtained in ground facilities is that of support interference, especially in regard to dynamic test data. While the dynamic sting interference has been well documented for hypersonic flow, it is generally only expected at transonic speeds in the cases where the ...
L.E. Ericsson, J.P. Reding
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The simulation of unsteady transonic flow and the stability of a transonic boundary layer
Journal of Applied Mathematics and Mechanics, 2005The authors discuss modification of a model (see \textit{O. S. Ryzhov} [Sov. Phys. Dokl. 22(1977), 537--539 (1978; Zbl 0359.76036)]) for investigation of free nonstationary visco-nonviscous interaction at transonic velocities. The model modification consists in taking into account a singular term of transonic extension and allows to refine the Lin ...
Bogdanov, A. N., Diesperov, V. N.
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Analysis of nonlinear transonic blockage in unsteady transonic flows
28th Fluid Dynamics Conference, 1997Numerical simulation of the oscillation of strong to weak shocks in a Laval nozzle, due to downstream static pressure sinusoidal fluctuations, is presented. The strong shock motion is mainly harmonic. However, static pressure signals, recorded near the shock/boundary layer interaction and on the axis downstream of the shock, show several higher modes ...
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