The quest for load‐independent left ventricular chamber properties: Exploring the normalized pressure phase plane

Abstract

The pressure phase plane (PPP), defined by dP(t)/dt versus P(t) coordinates has revealed novel physiologic relationships not readily obtainable from conventional, time domain analysis of left ventricular pressure (LVP). We extend the methodology by introducing the normalized pressure phase plane (nPPP), defined by 0 ≤ P ≤ 1 and −1 ≤ dP/dt ≤ +1. Normalization eliminates load‐dependent effects facilitating comparison of conserved features of nPPP loops. Hence, insight into load‐invariant systolic and diastolic chamber properties and their coupling to load can be obtained. To demonstrate utility, high‐fidelity P(t) data from 14 subjects (4234 beats) was analyzed. P_NR, the nPPP (dimensionless) pressure, where –dP/dt_peak occurs, was 0.61 and had limited variance (7%). The relative load independence of P_NR was corroborated by comparison of PPP and nPPP features of normal sinus rhythm (NSR) and (ejecting and nonejecting) premature ventricular contraction (PVC) beats. PVCs had lower P(t)_max and lower peak negative and positive dP(t)/dt values versus NSR beats. In the nPPP, +dP/dt_peak occurred at higher (dimensionless) P in PVC beats than in regular beats (0.44 in NSR vs. 0.48 in PVC). However, P_NR for PVC versus NSR remained unaltered (P_NR = 0.64; P > 0.05). Possible mechanistic explanation includes a (near) load‐independent (constant) ratio of maximum cross‐bridge uncoupling rate to instantaneous wall stress. Hence, nPPP analysis reveals LV properties obscured by load and by conventional temporal P(t) and dP(t)/dt analysis. nPPP identifies chamber properties deserving molecular and cellular physiologic explanation.

Introduction

The gold standard for characterization of chamber properties utilizes high‐fidelity, micromanometric left ventricular (LV) pressures (P) as a function of time. The usual parameters include: maximum and minimum LV pressures (P_max and P_min), peak positive and peak negative rate of change of pressure (+dP/dt_peak and –dP/dt_peak), diastatic pressure, and end‐diastolic pressure (EDP). For isovolumic relaxation (IVR) characterization, P from just after –dP/dt_peak to just before mitral valve opening is fit using a 2 or 3 parameter assumed exponential relationship (Weiss et al. ) which includes the time constant of isovolumic relaxation τ (Matsubara et al. ). LVP during the remaining >95% of the cardiac cycle is usually not analyzed.

Eucker et al. () adopted the phase plane analysis method familiar in nonlinear dynamics (Strogatz ) to analyze LVP in the pressure phase plane (PPP) (Eucker et al. ). The oscillatory nature of P during the cardiac cycle generates closed PPP loops (analogs of limit cycles) allowing visualization of dP/dt versus P relation especially during the isovolumic phases when dP/dt reaches its respective systolic and diastolic maxima. PPP analysis has been used to characterize LV relaxation using various mathematical assumptions (Leite‐Moreira et al. ; Chung and Kovács , ; Senzaki and Kass ). Senzaki and Kass () fit the IVR segment in the PPP using a logistic model (parameter τ_L) and showed that it provides a better fit to curved segments than the linear fit (τ) provided by the exponential model. PPP analysis of IVR has also led to a predictive, causal kinematic model, where P(t) is the solution to the equation of motion of a damped oscillator (three parameters) allowing for fit of the model predicted solution from before –dP/dt_peak to MVO (Chung and Kovács ). PPP analysis provides a way to visualize spatiotemporal differences in LV hemodynamics (Ghosh and Kovács ) during IVR. It has also led to the development of a load independent index of IVR (Shmuylovich and Kovács ). Here, we extend PPP analysis and introduce the normalized pressure phase plane (nPPP) defined by −1 ≤ dP/dt ≤ 1, 0 ≤ P ≤ 1. Thus normalization eliminates load‐dependent components of P and dP/dt and retains intrinsic contraction and relaxation features of the loops and helps to elucidate and characterize their differences and similarities.

Specifically, we focus on the values of normalized (dimensionless) pressure during isovolumic contraction (IVC) at +dP/dt_peak (P_NC) and during IVR at −dP/dt_peak (P_NR). Additionally, we analyze loops of normal sinus rhythm (NSR) and premature ventricular contraction (PVC) beats within and among subjects. In our exploration of the normalized pressure phase plane we hypothesize that nPPP analysis will elucidate novel chamber properties.

Method

Derivation of normalized P and dP/dt contours

For each cardiac cycle, LVP was normalized according to:$${\mathrm{P}}_N(t)=\frac{(\mathrm{P}(t)-{\mathrm{P}}_{\min })}{({\mathrm{P}}_{\max }-{\mathrm{P}}_{\min })}$$which assures that P_min = 0 and P_max = 1. Figure A and B illustrate three beats before and after normalization.

The LV dP/dt was normalized according $${\mathrm{P}}_N(t)=\frac{(\mathrm{P}(t)-{\mathrm{P}}_{\min })}{({\mathrm{P}}_{\max }-{\mathrm{P}}_{\min })}$$yielding –dP/dt_peak = −1 and +dP/dt_peak = +1 for each beat. Results are illustrated in Figure C and D with normalized loops in Figure E and F.

Inclusion criteria and data acquisition

We analyzed 17 datasets from our Cardiovascular Biophysics Laboratory database of simultaneous echocardiographic and high‐fidelity hemodynamic recordings. Group clinical characteristics are listed in Table  (14 subjects) and Table  (three subjects). Prior to data acquisition, each subject provided signed, informed consent for participation in accordance with the Institutional Review Board (Human Research Protection Office) of Washington University School of Medicine. The criteria for data selection included: normal LV ejection fraction, normal sinus rhythm, absence of valvular abnormalities and the absence of wall‐motion abnormalities or bundle branch block on the ECG. None of the subjects (in Table ) had a history of coronary artery disease or myocardial infarction. Subjects in the PVC analysis part of the study were selected from the database using the criterion that they had a significant number of PVC beats to enable statistical analysis. One subject in the PVC analysis group (Table ) had a history of coronary artery disease/myocardial infarction and low ejection fraction. All patients underwent elective cardiac catheterization at the request of a referring cardiologist to establish the presence or absence of suspected coronary artery disease.

Subject demographics (n = 14)

Parameter	Mean ± SD
Age (years)	62 ± 9
Gender	7M/7F
Height (cm)	167 ± 9
Weight (lb)	182 ± 43
BMI (kg/m2)	29.7 ± 7.8
EDP (mm Hg)	18 ± 3
ESP (mm Hg)	105 ± 7
Ejection fraction (%)	72 ± 8
No. of beats	302 ± 43
Hypertension	7 (50%)

Values are mean ± standard deviation or number (% of total subjects).

Subject demographics for intrasubject (n = 3) PVC analysis

	Subject B1	Subject B2	Subject B3
Age (years)	43	63	56
Gender	M	M	M
Ejection fraction (%)	81	24	54
Height (cm)	196	183	170
Weight (lb)	335	206	165
BMI (kg/m2)	40	28	26
EDP (mm Hg)	17	15	10
Hypertension	+	+	−
CAD/previous MI	−	+	−
Total NSR beats	150	232	210
Total PVC beats	9 (NE)	78 (E)	17 (E)

+/– denote presence or absence of condition. NE, nonejecting PVC; E, ejecting PVC.

Our method of high‐fidelity, multichannel micromanometric LVP and simultaneous echocardiography recording has been previously detailed (Chung and Kovács ; Shmuylovich and Kovács ; Ghosh and Kovács ). Briefly, simultaneous LV pressure and aortic root pressure measurements were obtained using a 6‐F triple transducer pigtail‐tipped pressure–volume conductance catheter (SSD‐1034; Millar Instruments, Houston, TX). The signal was amplified and calibrated via standard transducer control units (TC‐510; Millar Instruments). Catheter placement was achieved by using fluoroscopy to cross the aortic valve, noting that both (distal and mid) pressure channels displayed LV pressure waveforms while the proximal (3rd) sensor displayed aortic root pressures. Pressure signals were input to clinical monitoring systems (Quinton Diagnostics, Bothell, WA or GE Healthcare, Milwaukee, WI) and a custom personal computer via a research interface (Sigma‐5DF; CD Leycom, Zoetermeer, The Netherlands) at a sampling rate of 250 Hz. Conductance signals were stored but were not used in this study. Ejection fraction was computed from the calibrated ventriculogram (33 mL of contrast at 11 mL/sec, via 6F pigtail catheter (Cordis Corporation, NJ) immediately after hemodynamic recording.

Hemodynamic data analysis

Pressure was converted for analysis via a custom Matlab script (Matlab 6.0; MathWorks, Natick, MA). Data sets were smoothed digitally by using a five‐point average to suppress noise in the derivative (Shmuylovich and Kovács ; Ghosh and Kovács ), attenuating 50% of signal at 40 Hz and 90% above 60 Hz, followed by calculation of continuous dP/dt versus time t from the smoothed data. For each beat, EDP and –dP/dt_peak were extracted from PPP or equivalent time domain contours for both pressure signals.

From the nPPP, the P_NC and P_NR were obtained as shown in Figure  using a custom MATLAB script. For all subjects, the mean value of P_max, P_min +dP/dt_peak, and –dP/dt_peak, pressure at +dP/dt_peak (P_C), pressure at –dP/dt_peak (P_R), P_NC and P_NR were calculated and saved.

We selected three subjects' datasets for PVC analysis. PVCs were first identified from ECG recordings and then classified as ejecting PVCs (E‐PVC) or nonejecting PVCs (NE‐PVC) by comparing LVP to the simultaneous aortic root pressure. If the LV pressure and the aortic root pressure recordings intersected and the aortic pressure showed a rise and fall concordant with the LV pressure it was classified as E‐PVC otherwise it was classified as NE‐PVC as shown in Fig . For the subjects the mean value of P_max, P_min, +dP/dt_peak, –dP/dt_peak, P_C, and P_R were calculated for NSR beats as well as E‐PVC beats and NE‐PVC beats. Mean values for P_NC and P_NR in NSR, E‐PVC and NE‐PVC beats were calculated.

Statistical analysis

The mean, standard deviation (SD), maximum and minimum values were calculated for the points of interest in the regular PPP and nPPP. In addition, to determine variation we calculated the coefficient of variation, defined as the ratio of standard deviation to the mean value of the parameter, (as shown in Table ) expressed as a percentage for the 14 subjects included in the intersubject analysis. To compare NSR and PVC features we used the Student's two‐tailed t‐test to determine statistical significance, with P < 0.05 denoting significance.

Group values (n = 14) of hemodynamic parameters

Parameter	Mean	SD	Min	Max	Variation
Pmax (mm Hg)	137	17	119	165	12.1%
Pmin (mm Hg)	9.3	3	3.6	13.4	29.7%
dP/dtmax (mm Hg/sec)	1257	136	1062	1531	10.8%
dP/dtmin (mm Hg/sec)	−1496	182	−1834	−1266	12.2%
PC (mm Hg)	61	6	49	72	9.6%
PR (mm Hg)	87	10	75	104	11.3%
PNC (dimensionless)	0.41	0.04	0.34	0.48	10.5%
PNR (dimensionless)	0.61	0.04	0.56	0.69	6.6%
EDP (mm Hg)	18	3	13	23	17.9%
ESP (mm Hg)	105	7	93	116	6.9%
nEDP (dimensionless)	0.07	0.02	0.03	0.1	27.1%
nESP (dimensionless)	0.76	0.07	0.64	0.9	8.9%

Coefficient of variation is defined in . SD, Standard deviation.

Results

Table  shows the subject characteristics for the 14 subjects. Table  provides the mean, SD, minimum, maximum, and the coefficient of variation values of the points of interest in the regular PPP and nPPP based on 4234 cardiac cycles. By definition, normalization reduced the variation in P_max, P_min, +dP/dt_peak, and –dP/dt_peak to 0. The variation of P_C (9.6%) changed slightly compared with P_NC (10.5%) while the variation P_NR (6.6%) decreased compared with P_R (11.3%). The variation of both nEDP (27.1%) and nESP (8.9%) increased in comparison to EDP (17.9%) and ESP (6.9%). Among all these P_NR had the lowest variation. To illustrate intersubject variation in PPP loop shape and features Figure A shows individual, superimposed beats from three subjects. Figure B shows same beats in the nPPP, illustrating the effect of normalization in eliminating the differences in Figure A.

To investigate nPPP features and determine the effect of normalization on P_NR, we compared NSR beats to E‐PVCs and NE‐PVCs in the same subject. We selected three datasets that had significant number of PVCs to permit statistical analysis. Table  shows the clinical characteristics. Figure  shows PPP and nPPP for a NSR and E‐PVC beat in the same subject. For clarity, Figure C and D magnifies the P_NC and P_NR portions of Figure B. As these figures illustrate, normalization aids in visualizing features masked by the differences in P_max, P_min, +dP/dt_peak, and –dP/dt_peak. In Subject B1 (see Table ) we compared NE‐PVCs to NSR beats. In concordance with previous results (Carroll et al. ), we found that P_max, +dP/dt_peak, and –dP/dt_peak were significantly lower in magnitude in the PVC beats (P < 0.01). While P_R was statistically different between the two types of beats (P < 0.001); P_NR was not statistically different (P = 0.09). In subjects B2 and B3 (Table ), we compared NSR beats to E‐PVC beats but not to NE‐PVCs because of limited numbers. Similar to subject B1, we found that in B2 and B3, P_max, +dP/dt_peak, and –dP/dt_peak were much lower in magnitude in the PVC beats (P < 0.0001). Also P_R was statistically different between the two types of beats; the value of P_NR was not statistically different (P = 0.09 and P = 1). This suggests that P_NR remains essentially unaltered between NSR and PVC beats. The mean value of P_NR (0.64) in the three datasets with PVCs was comparable to the value of P_NR (0.61) obtained from the first part of the study analyzing 14 datasets. While P_C did not differ between NSR and PVC due to large intrasubject variation (12.3%), P_NR did not differ in spite of the low beat to beat variation (6.3%) indicating a much smaller distribution of P_NR values in NSR and PVC beats. The mean values of the hemodynamic parameters of the PPP and the nPPP in NSR and PVC beats are given in Table  along with measures of statistical significance.

Mean hemodynamic parameters in NSR versus PVC analysis subjects

Parameter	Subject B1	Subject B2	Subject B3
NSR	PVC	NSR	PVC	NSR	PVC
Pmax (mm Hg)	116	101	140	127	132	922
Pmin (mm Hg)	11	11	12	12	9	8
dP/dtmax (mm Hg/sec)	996	758	1190	1026	1007	6522
dP/dtmin (mm Hg/sec)	−1121	−8611	−1169	−1019	−1136	−584
PC (mm Hg)	61	52	73	73	53	47
PR (mm Hg)	73	61	99	88	87	60
PNC	0.47	0.45	0.48	0.53	0.36	0.46
PNR	0.63	0.59	0.67	0.66	0.63	0.63
EDP (mm Hg)	16	‐NA‐	16	‐NA‐	16	‐NA‐
ESP (mm Hg)	106	‐NA‐	123	‐NA‐	89	‐NA‐

The number of beats is given in Table .

⁵P < 0.01.

⁶P < 0.0001.

List of Abbreviations and units of measurement

Abbreviation	Full Term	Unit
PPP	Pressure phase plane	‐NA‐
P	Left ventricular pressure	mm Hg
dP/dt	Time rate of change of LV pressure	mm Hg/sec
Pmin	Minimum LV pressure	mm Hg
Pmax	Maximum LV pressure	mm Hg
+dP/dtpeak	Peak positive dP/dt	mm Hg/sec
−dP/dtpeak	Peak negative dP/dt	mm Hg/sec
PC	Pressure at +dP/dtpeak	mm Hg
PR	Pressure at –dP/dtpeak	mm Hg
EDP	End‐diastolic pressure	mm Hg
ESP	End‐systolic pressure	mm Hg
nPPP	Normalized pressure phase plane	‐NA‐
PNC	Normalized pressure at +dP/dtpeak	Dimensionless
PNR	Normalized pressure at −dP/dtpeak	Dimensionless
nEDP	Normalized end‐diastolic pressure	Dimensionless
nESP	Normalized end‐systolic pressure	Dimensionless
NSR	Normal Sinus Rhythm	‐NA‐
E‐PVC	Ejecting premature ventricular contraction	‐NA‐
NE‐PVC	Nonejecting premature ventricular contraction	‐NA‐
IVR	Isovolumic relaxation	‐NA‐
IVC	Isovolumic contraction	‐NA‐

Discussion

Normalization of diastolic physiologic data has been employed in a different context previously. Klotz et al. () proposed a method to estimate the end‐diastolic pressure–volume relationships by normalizing LV volumes. They found that normalization generated end‐diastolic pressure–volume curves having the same shape across different species and pathologies.

The phase plane method has been used in biological and physiological systems (Paniflov and Hogeweg ; Keener and Sneyd ). LV pressure phase plane analysis, a component of 4‐dimensional physiologic hyperspace (Eucker et al. ), has been previously employed (Eucker et al. ; Chung et al. ; Chung and Kovács ) to identify new cardiac cycle features. In the quest to identify load‐independent chamber properties we explored LV hemodynamics in the nPPP. Normalization maps the variable maximum and minimum pressure and dP/dt limits of consecutive beats to the same values and thereby removes loading effects while contraction and relaxation related loop shape features are retained. We evaluated IVC and IVR loop features in different subjects to characterize differences and similarities. We also compared NSR beats to PVCs in three subjects. Both studies showed that P_NR remains essentially invariant while other nPPP points of interest varied significantly. Hence, nPPP analysis indicates that P_NR is closely conserved.

Load dependence of LV relaxation

Chamber relaxation is known to be determined in part by cross‐bridge uncoupling and other load‐dependent mechanisms (Katz ; Karliner et al. ; Brutsaert et al. ; Gaasch et al. ; Hori et al. ; Eichhorn et al. ; Chemla et al. ; Janssen ; Senzaki and Kass ). Cross‐bridge uncoupling requires dissociation of Ca²⁺ from troponin and its sequestration in the sarcoplasmic reticulum (Bers ; Rice and de Tombe ). Increased afterload, quantified by end‐systolic pressure or volume has a slowing effect on the rate of pressure decay during IVR (Chemla et al. ). Other studies have reported that in normal hearts IVR is load independent while failing hearts show increased load sensitivity (Starling et al. ; Little ; Prabhu ). In failing hearts, –dP/dt_peak is lower than in normal hearts (Prabhu ) and its cause remains uncertain.

Intersubject comparison of nPPP

To determine if nPPP can characterize chamber properties that are minimally load dependent or are load independent, we analyzed data from 14 subjects (302 beats/subject, 4234 beats total; Table ). Normalization eliminated the intersubject variance of P_max, P_min, +dP/dt_peak, and –dP/dt_peak. Normalization did not alter the variation of pressure at which +dP/dt_peak occurs (P_C variance = 10% vs. P_NC variance = 11%), but it did decrease the variation of pressure at which –dP/dt_peak occurs (Table ) (P_R variance = 11%, vs. P_NR variance = 6.6%). Thus, in contrast to IVC, normalization generated a much smaller variation in P_NR during IVR. This is illustrated in Figure  comparing PPP (left) and nPPP (right) in three selected subjects.

As EDP and ESP depend on preload and afterload, respectively, we normalized these indexes, which generated increased variation in the nPPP. The observed increase in variation can be understood by considering at least two effects which influence variation. First, the amplitude of pressure oscillation for each beat, that is, its pressure range and second, the intrinsic contraction/relaxation mechanics. Normalizing removes absolute value effects of pressure without altering intrinsic mechanism effects that determine loop features. Hence the observed increase after normalization suggests that the intrinsic mechanism effects (that determine EDP and ESP) between subjects have higher variation which had been masked by the pressure range variation in PPP.

Hemodynamics of premature ventricular contractions

PVCs provide natural (in contrast to pharmacologic) beat‐to‐beat load variation. Many studies have utilized PVCs to characterize load effects in contraction and relaxation. Carroll et al. () studied IVR during PVCs and found that PVCs enhance shortening and augment restoring forces producing a smaller end‐systolic chamber. PVCs also delay inactivation and prolong relaxation, generating increased values of τ while impairing LV filling (Stoddard et al. ). PVCs have also been employed to more extensively validate a load independent index of diastolic function (Boskovski et al. ).

Effect of normalization on PVC hemodynamics

We exploited PVC generated load variation to assess load‐dependent features in the PPP and the nPPP. Information on the PVC datasets is given in Table  and Table . Figure A shows a NSR and E‐PVC beat in the PPP and Figure B shows the same beats in nPPP. As seen in the figure, E‐PVC has lower values of P_max, +dP/dt_peak, and –dP/dt_peak. P_C was not significantly different between NSR and PVC beats although large beat‐to‐beat variation in each subject was present. P_R was significantly lower in PVCs in all the three subjects (P < 0.001).

The value of P_NR was not significantly different among the three subjects between NSR and PVC beats. This revealed that there is essentially no change in the dimensionless pressure at which the peak rate of pressure decay occurred in both NSR and PVC beats. This value is comparable to the value of P_NR obtained from the first part of the study (Table , P_NR = 0.61). P_NC on the other hand was higher in E‐PVC compared with NSR. Hence unlike contraction, which shows changes in the rate of pressure rise as a function of pressure in PVCs, the rate of pressure decay as a function of pressure is essentially unchanged during IVR in PVCs suggesting a (relatively) conserved intrinsic relaxation mechanism.

Physiological significance of normalization and possible mechanism

LV contraction and relaxation involves actin–myosin cross‐bridge coupling and uncoupling regulated by Ca²⁺ bound to troponin (Baker et al. ; Bombardini ; de Tombe et al. ) and further modulated by the loading conditions involving pressure and its variation. Studies have attempted to understand the contribution of load as factors in contraction and relaxation (Brutsaert et al. ; Hori et al. ; Starling et al. ; Little ; Prabhu ) by physiologic, pharmacologic, or surgical interventions to modify load and evaluate response.

Some of the factors determining these intrinsic mechanisms include calcium cycling, sarcomere kinetics, mitochondrial (ATP) function, extracellular matrix, etc. The similar variation of P_C and P_NC (Table ) suggests that its variation is determined by factors other than load. On the other hand, the reduced variation of P_NR as compared to P_R suggests that its variation is load dependent but the intrinsic mechanism that constrains P_NR to be in the 0.61–0.64 range is conserved. This underscores that nPPP is not merely a scaled down version of the regular PPP. Rather normalization removes P and dP/dt magnitude effects while maintaining shape‐based features.

Maintenance of shape‐based features was borne out by the intrasubject PVC analysis. The value of P_NR was similar in NSR and PVC beats within and across subjects (Table ). Its value was also similar to the value reported in the intersubject analysis (Table ). This permits the inference that intrinsic relaxation mechanisms are more (tightly regulated) conserved than intrinsic contraction mechanisms. Moreover, contractility and the associated value of P_NC in NSR and E‐PVC beats is governed by the beat‐to‐beat variation of preload and afterload while in NE‐PVCs it is primarily determined by the Frank–Starling Law and the timing of the PVC relative to the prior beat. Hence, an nPPP based prediction is that because of the beat‐to‐beat variation of load, we expect P_NC to have larger variation than P_NR. Our observations corroborate this prediction. Sarcomere kinetics is a major determinant of relaxation mechanisms (Piroddi et al. ; Stehle et al. ). Two features of sarcomere kinetics likely to have a bearing on the limited variation of P_NR include (Little et al. ) – (1) kinetics of Ca²⁺ binding and dissociation from troponin and (2) cross‐bridge attachment/detachment and subsequent sarcomere shortening/lengthening. The relative constancy of P_NR suggests that the ratio of maximum rate of cross‐bridge dissociation to instantaneous pressure (force, wall stress) at which that maximum dissociation rate takes place is tightly constrained. This preliminary, proof of concept study demonstrates the utility of PPP normalization in elucidating novel LV diastolic properties.

Limitations

The main limitations pertain to data acquisition. As noted previously (Ghosh and Kovács ), calibration, catheter placement, and orientation with respect to the LV axis may have a slight effect on pressure recordings. However, calibration offsets the pressure by a constant value which should not affect the normalization process. Calibration and drift are mitigated by pre‐ and postcalibration of transducers to zero hydrostatic pressure in a 37°C saline bath. Other issues involving signal processing have been addressed previously (Chung and Kovács ; Shmuylovich and Kovács ; Ghosh and Kovács ). Noisy beats were not analyzed. Moreover, the large (average) number of beats studied in every subject (302) mitigates the effect of noise to an acceptable degree.

As this is a proof of concept study, the number of datasets analyzed is necessarily limited although the 4234 cardiac cycles analyzed mitigates that limitation to an acceptable degree. Although eight of the datasets analyzed in this study have been previously analyzed for different purposes (16), repeat analysis using a different method (normalization) to test a different hypothesis (load independence of phase plane loop features) is appropriate. Relative physiologic uniformity is achieved as a result of enrollment criteria (normal ejection fraction, no coronary artery disease or myocardial infarctions, no diabetes). P and dP/dt values were not very different (<50% variation in P_max, +dP/dt_peak, P_C, and P_R values). This limitation is mitigated by the second part of the study where we compared NSR to PVC beats in the same subject. The PPP in PVC is much smaller and has a different shape from a NSR PPP (Fig. ; Chung and Kovács ). In spite of this, P_NR remained an essentially conserved feature among the three subjects. However, we only studied PVCs in three subjects, which is insufficient to draw definitive conclusions regarding trends. Hence, additional studies are needed to elucidate the magnitude of these changes and differentiate between the changes in E‐PVCs versus NE‐PVCs. Further work in the PPP and physiologic hyperspace is needed involving a greater sample size and specific pathophysiologic states.

Conclusions

We introduce the nPPP for LV hemodynamic analysis. Normalization removes beat‐to‐beat and intersubject variation in P and dP/dt limits and thereby, minimizes load effects. We tested applicability in ~4400 beats in 14 subjects. In the nPPP, the variation of P_NR, the (dimensionless) pressure at which –dP/dt_peak was inscribed, was very substantially reduced. Comparison of NSR beats to both ejecting and nonejecting beats PVCs revealed that P_NR remained tightly controlled. The observed near constancy of P_NR reveals a new aspect of the physiology of diastole and indicates the existence of intrinsic (intracellular) IVR mechanisms for which a possible mechanism is discussed. Thus, nPPP analysis elucidates novel LV chamber properties, and identifies potential research targets in need of molecular and cellular physiologic explanation.

Acknowledgments

The assistance of the staff of the Cardiovascular Procedure Center at Barnes‐Jewish Hospital at Washington University Medical Center is gratefully acknowledged. The comments and suggestions of anonymous reviewers are gratefully acknowledged.

Conflict of Interest

None declared.