Skip to main content
. Author manuscript; available in PMC: 2022 Aug 1.
Published in final edited form as: J Comput Phys. 2022 Aug;463:111266. doi: 10.1016/j.jcp.2022.111266

Fig. 8.

Fig. 8

Behavior of the Klotz EDPVR relation is shown for varying end-diastolic PV-points. First, Veddat was varied while keeping peddat constant and vice versa. Normalized curves match for alternating Veddat (left) while curves for alternating peddat (right) differ in shape.