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. Author manuscript; available in PMC: 2023 Nov 1.
Published in final edited form as: J Thorac Cardiovasc Surg. 2021 Jun 30;164(5):1365–1375. doi: 10.1016/j.jtcvs.2021.05.049

Association of diameter and wall stresses of tricuspid aortic valve ascending thoracic aortic aneurysms

Axel Gomez a, Zhongjie Wang a, Yue Xuan a, Michael D Hope b, David A Saloner b, Julius M Guccione a, Liang Ge a, Elaine E Tseng a
PMCID: PMC8716675  NIHMSID: NIHMS1728468  PMID: 34275618

Abstract

Objective:

Ascending thoracic aortic aneurysms carry a risk of acute type A dissection. Elective repair guidelines are designed around size thresholds, but the 1-dimensional parameter of maximum diameter cannot predict acute events in small aneurysms. Biomechanically, dissection can occur when wall stress exceeds strength. Patient-specific ascending thoracic aortic aneurysm wall stresses may be a better predictor of dissection. Our aim was to compare wall stresses in tricuspid aortic valve–associated ascending thoracic aortic aneurysms based on diameter.

Methods:

Patients with tricuspid aortic valve–associated ascending thoracic aortic aneurysm and diameter 4.0 cm or greater (n = 221) were divided into groups by 0.5-cm diameter increments. Three-dimensional geometries were reconstructed from computed tomography images, and finite element models were developed taking into account prestress geometries. A fiber-embedded hyperelastic material model was applied to obtain longitudinal and circumferential wall stress distributions under systolic pressure. Median stresses with interquartile ranges were determined. The Kruskal–Wallis test was used for comparisons between size groups.

Results:

Peak longitudinal wall stresses for tricuspid aortic valve–associated ascending thoracic aortic aneurysm were 290 (265-323) kPa for size 4.0 to 4.4 cm versus 330 (296-359) kPa for 4.5 to 4.9 cm versus 339 (320-373) kPa for 5.0 to 5.4 cm versus 318 (293-351) kPa for 5.5 to 5.9 cm versus 373 (363-449) kPa for 6.0 cm or greater (P = 8.7e-8). Peak circumferential wall stresses were 460 (421-543) kPa for size 4.0 to 4.4 cm versus 503 (453-569) kPa for 4.5 to 4.9 cm versus 549 (430-588) kPa for 5.0 to 5.4 cm versus 540 (471-608) kPa for 5.5 to 5.9 cm versus 596 (506-649) kPa for 6.0 cm or greater (P = .0007).

Conclusions:

Circumferential and longitudinal wall stresses are higher as diameter increases, but size groups had large overlap of stress ranges. Wall stress thresholds based on aneurysm wall strength may be a better predictor of patient-specific risk of dissection than diameter in small ascending thoracic aortic aneurysms.

Keywords: ascending thoracic aortic aneurysms, finite element analysis, tricuspid aortic valve

Graphical Abstract

graphic file with name nihms-1728468-f0001.jpg

Longitudinal wall stress profile of small TAV-aTAA with high aortic root stress.


Ascending thoracic aortic aneurysm (aTAA) is often indolent and asymptomatic until dissection or rupture occurs. aTAA has a dissection or rupture rate of approximately 2% to 3% per year.1 Aortic dissection and rupture are often fatal events in many patients before reaching the hospital, but still carry an approximately 25% operative mortality in patients undergoing emergency surgery.2 Annual incidence of dissection increases with aortic size and approaches 4% and 10% when greater than 5.5 and 6.0 cm, respectively.3 aTAA surgical repair is offered when maximum diameter reaches 5.5 cm or greater, with earlier intervention if rapid growth rate, family history of dissection, personal history of connective tissue disorder, or concurrent surgical aortic valve replacement is present.4 Current elective aTAA repair guidelines balance the risks of surgical intervention versus the risks of dissection. These diameter-based guidelines designed around numeric cutoffs use diameter as a surrogate for aneurysm wall stress based on the law of Laplace. However, diameter-based guidelines have failed to capture most small aTAAs at high risk of acute aortic events. Data from the International Registry of Acute Aortic Dissection as well as our data showed that approximately 60% of type A dissections had a diameter less than 5.5 cm, and approximately 40% had a diameter less than 5 cm at the time of the event.5,6 Thus, acute aortic dissection is a complex hemodynamic event that is not well captured by diameter alone. There is unmet clinical need to develop an innovative approach to better predict acute aortic events and guide well-timed aTAA surgical repair.

From a biomechanical standpoint, dissection and rupture represent mechanical failure of the aortic wall. Mechanical failure can occur when wall stresses exceed wall strength.7 The law of Laplace linearly relates wall stress to both diameter and luminal pressure for spherical or cylindrical structures. However, aTAAs have complex geometries, and Laplace’s law fails to accurately predict true aTAA wall stress. Fundamentally, this imperfect clinical correlation between aortic size and acute aortic events stems from using this simplified method to assess wall stress and thus patient-specific risk of dissection. Actual patient-specific aTAA wall stresses can be accurately calculated from 3-dimensional (3D) computational models using finite element analysis (FEA),8,9 because wall stresses and failure strength are otherwise impossible to directly measure in vivo. FEA has successfully been applied to aTAAs and have shown that aortic regions with high wall stresses coincide with regions where initial intimal tears are observed.6,10,11 Studying aTAA wall stress profiles could improve detection of patients at high risk of acute aortic events and guide clinical decision-making. We have previously investigated wall stress versus diameter for a surgical threshold of less than 5 cm versus 5 cm or greater for both bicuspid aortic valve (BAV) and tricuspid aortic valve (TAV)-associated aTAAs because of our preference for operating on BAV at 5 cm or greater.12 That study had one of the largest sample sizes of aTAA FEA studies. In this study, we chose to focus only on TAV-aTAAs to determine wall stress magnitudes in relation to maximum aortic size and the impact of a 5.5-cm surgical threshold.

MATERIALS AND METHODS

Study Population

Patients with TAV-aTAAs and measured diameter 4.0 cm or greater by computed tomography (CT) scan at San Francisco Veterans Affairs Medical Center between June 2007 and June 2020 were studied. We excluded patients with a BAV confirmed by echocardiography, CT, or surgery. This study was approved by the Committee on Human Research at University of California San Francisco Medical Center and Institutional Review Board at San Francisco Veterans Affairs Medical Center.

Tricuspid Aortic Valve–Associated Ascending Thoracic Aortic Aneurysm Geometry Reconstruction

De-identified CT scans were used to construct computational 3D models of TAV-aTAAs. Models included aortic regions from the left ventricular outflow tract (LVOT) to the mid-thoracic descending aorta. For each patient, CT images were imported into MeVisLab software (MeVis Medical Solutions AG, Bremen, Germany) for image segmentation to obtain a model of the aTAA surface. The surface data were imported into TrueGrid software (version 3.1.3; XYZ Scientific, Inc, Livermore, Calif) to create a geometric mesh model that was discretized into elements that resemble building blocks. Geometric meshes had 3 layers to reflect the intima, media, and adventitia layers with a total of 11,202 hexahedral elements. Meshes were imported into LS-DYNA R10 (LSTC Inc, Livermore, Calif) for finite element (FE) simulations and analysis.

Finite Element Simulations

When obtaining CT images, the aorta was under in vivo physiologic blood pressure conditions. Therefore, our initial models had a geometry that corresponded to systemic pressure and we corrected for prestresses to obtain a zero-pressure geometry suitable for FE simulations using a modified update-Lagrangian method.13,14 FE simulations on TAV-aTAAs were done with a validated fiber-embedded hyperelastic material built and previously described by our group.14 Averaged TAV-aTAA material properties were applied based on previous biaxial stretch testing.15 The aortic wall was assumed to be incompressible, uniform, and hyperelastic. Aortic wall thickness was set at 1.8 mm, derived from our prior aneurysm experimental studies.15 We fixed translational motion at the LVOT, 20 mm proximal to the aortic annulus, and at the mid-descending thoracic aorta, while rotational motion was unconstrained. These boundary conditions allowed for aortic motion with the cardiac cycle while accounting for restraints from the ligamentum arteriosum. The aortic root is a dynamic structure with the cardiac cycle causing displacement. Fixation at the LVOT did allow 3D displacement of the aortic root and aTAA as our particular regions of interest. TAV-aTAA models were subjected to physiologic luminal arterial pressures. The inner lumen was first pressurized to 80 mm Hg. The cardiac cycle was then simulated by gradually increasing luminal pressure from 80 to 120 mm Hg over 300 ms followed by decreasing luminal pressure to 80 mm Hg over 500 ms. Video 1 shows the process of geometry reconstruction and FE simulations. Reproducibility was demonstrated with 2 investigators independently re-constructing TAV-aTAA models and performing FE simulations for a subset of 24 subjects.

Statistical Methods and Data Analysis

TAV-aTAA models were divided into 5 distinct groups based on the maximal diameter reported on their corresponding CTs. The groups were defined by aortic diameters of 4.0 to 4.4 cm, 4.5 to 4.9 cm, 5.0 to 5.4 cm, 5.5 to 5.9 cm, and 6.0 cm or greater. Statistical analysis was performed using 99th-percentile wall stresses, which have been shown to be more accurate by avoiding inhomogeneity in the mesh.16 Peak wall stresses will refer to 99th-percentile wall stresses. Peak wall stresses were calculated for both longitudinal and circumferential directions. Differences in peak stress between directions were studied with the paired samples t test. The relationship of peak stress with aneurysm diameter was studied with the Kruskal–Wallis test to account for the non-normality of stresses in the different size groups. This analysis considered the whole aTAA model (ie, from the aortic annulus to the beginning of aortic arch). Secondary analyses on individual aortic regions were also performed, that is, sinuses of Valsalva (SOV), sinotubular junction (STJ), and ascending aorta (AscAo). Differences in peak stresses between blood pressures of 120 and 95 mm Hg were studied with the Wilcoxon signed-rank test. Continuous variables are reported as median with interquartile range. Categorical variables are reported with count and percentages. Statistical analyses were performed using R (http://www.r-project.org). A flow diagram of the study methodology and primary outcomes is represented in Figure 1.

FIGURE 1.

FIGURE 1.

Flow diagram representing TAV-aTAA sample population (first row), followed by stratification of patients into distinct groups by maximal aneurysm diameter (second row), schematic of aTAA model reconstruction and wall stress simulations (third row), measured peak circumferential (fourth row) and longitudinal (fifth row) wall stresses, and observed relationships between aneurysm peak wall stresses and diameter (sixth row).

RESULTS

Patient Demographics

A total of 221 TAV-aTAA veterans were included in the current study with a median diameter of 4.5 cm. The majority of patients were male (97.3%) with a median age of 70 years. Hypertension and hyperlipidemia were the most common comorbidities, and veterans had a median 16 pack-year smoking history. Cardiovascular risk factors were distributed similarly among different aneurysm size groups with the exception of male sex (P = .030). Table 1 presents demographic information.

TABLE 1.

Tricuspid aortic valve ascending thoracic aortic aneurysm population characteristics

Characteristic 4.0-4.4 cm (n = 100) 4.5-4.9 cm (n = 77) 5.0-5.4 cm (n = 21) 5.5-5.9 cm (n = 13) ≥ 6.0 cm (n = 10) All (n = 221) P value
Diameter (cm) 4.2 (4.1-4.3) 4.7 (4.6-4.8) 5.1 (5.0-5.3) 5.6 (5.5-5.7) 6.0 (6.1-6.5) 4.5 (4.3-4.8) 3.17e-40
Age (y) 70 (66-74) 70 (66-74) 67 (63-72) 67 (63-73) 56 (55-73) 70 (65-74) .11
Male sex 97 (97.0%) 77 (100%) 20 (95%) 11 (85%) 10 (100%) 215 (97%) .030
Smoking (pack-y) 20 (0-45) 15 (0.5-40) 15 (0-43) 20 (3-30) 2 (0-25) 16 (0-40) .73
Hypertension 78 (78.0%) 65 (84.4%) 18 (85.7%) 10 (76.9%) 7 (70.0%) 178 (80.5%) .68
Diabetes 13 (13.0%) 21 (27.3%) 5 (23.8%) 2 (15.4%) 1 (10.0%) 42 (19.0%) .15
Hyperlipidemia 74 (74.0%) 57 (74.0%) 14 (66.7%) 8 (61.5%) 7 (70.0%) 160 (72.4%) .85
CAD 21 (21.0%) 18 (23.4%) 7 (33.3%) 3 (23.1%) 3 (30.0%) 52 (23.5%) .79
PVD 13 (13.0%) 12 (15.6%) 0 (0%) 0 (0%) 10 (100%) 26 (11.8%) .22
COPD 27 (27.0%) 21 (27.3%) 5 (23.8%) 1 (7.7%) 3 (30.0%) 57 (25.8%) .64
CVA 5 (5.0%) 9 (11.7%) 2 (9.5%) 2 (15.4%) 0 (0%) 18 (8.1%) .35
CKD 8 (8.0%) 14 (18.2%) 3 (14.3%) 1 (7.7%) 1 (10.0%) 27 (12.2%) .33
Carotid stenosis 1 (1.0%) 2 (2.6%) 2 (9.5%) 1 (7.7%) 1 (10.0%) 7 (3.2%) .15
Arrhythmia 29 (29.0%) 41 (53.2%) 11 (52.4%) 4 (30.8%) 1 (10.0%) 86 (38.9%) .64
MI 8 (8.0%) 5 (6.5%) 0 (0%) 2 (15.4%) 0 (0%) 15 (6.8%) .40
LVEF (%) 60 (57-65) 61 (55-65) 60 (56-64) 63 (59-69) 57 (51-61) 56 (60-65) .53
CHF 8 (8.0%) 7 (9.1%) 2 (9.5%) 2 (15.4%) 0 (0%) 19 (8.6%) .77
NYHA class I 1 (1.0%) 6 (7.8%) 1 (4.8%) 1 (7.7%) 0 (0%) 9 (4.1%) .20
NYHA class II 4 (4.0%) 0 (0%) 1 (4.8%) 0 (0%) 0 (0%) 5 (2.3%) .37
NYHA class III 3 (3.0%) 1 (1.3%) 0 (0%) 1 (7.7%) 0 (0%) 5 (2.3%) .55
NYHA class IV 0 (0%) 0 (0%) 0 (0%) 0 (0%) 0 (0%) 0 (0%) NA
Hemodialysis 1 (1.0%) 1 (1.3%) 0 (0%) 0 (0%) 0 (0%) 2 (0.9%) .97
Prior PCI 9 (9.0%) 4 (5.2%) 2 (9.5%) 0 (0%) 1 (10.0%) 16 (7.2%) .69
Prior cardiac surgery 9 (9.0%) 9 (11.7%) 2 (9.5%) 0 (0%) 1 (10%) 21 (9.5%) .67

CAD, Coronary artery disease; PVD, peripheral vascular disease; COPD, chronic obstructive pulmonary disease; CVA, cerebrovascular accident; CKD, chronic kidney disease; MI, myocardial infarction; LVEF, left ventricular ejection fraction; CHF, congestive heart failure; NYHA, New York Heart Association; NA, not available; PCI, percutaneous coronary intervention.

Circumferential Tricuspid Aortic Valve–Associated Ascending Thoracic Aortic Aneurysm Wall Stresses by Diameter

Subjects were distributed into size groups based on maximal diameter. The number of aneurysms in groups 4.0 to 4.4 cm, 4.5 to 4.9 cm, 5.0 to 5.4 cm, 5.5 to 6.0 cm, and 6.0 cm or greater were 100, 77, 21, 13, and 10, respectively. At systolic pressure, peak circumferential wall stresses were 460 (421-543) kPa for size 4.0 to 4.4 cm, 503 (453-569) kPa for 4.5 to 4.9 cm, 549 (430-569) kPa for 5.0 to 5.4 cm, 540 (471-608) kPa for 5.5 to 5.9 cm, and 596 (506-649) kPa for 6.0 cm or greater (Table 2). Circumferential peak wall stresses increased with diameter (P = .0008) (Figure 2, A). The same trend was present for individual aTAA anatomic regions (Figure 2, B-D). Peak circumferential wall stresses for AscAo, STJ, and SOV are reported in Table 2. When diameter was evaluated as a continuous variable, the correlation of peak circumferential wall stresses to diameter was r = 0.26 (P = 7.4e-5) for whole aTAA, r = 0.61 (P < 2.2e-16) for AscAo, r = 0.40 (P = 3.7e-10) for STJ, and r = 0.46 (P = 1.8e-13) for SOV, respectively.

TABLE 2.

Circumferential tricuspid aortic valve ascending thoracic aortic aneurysm peak wall stress

4.0-4.4 cm (n = 100) 4.5-4.9 cm (n = 77) 5.0-5.4 cm (n = 21) 5.5-5.9 cm (n = 13) ≥6.0 cm (n = 10) P value
Whole aTAA (kPa) 460 (421-543) 503 (453-569) 549 (430-588) 540 (471-608) 596 (506-649) .0008
SOV (kPa) 377 (334-432) 429 (385-488) 424 (371-453) 454 (415-499) 552 (516-627) 1.6e-8
STJ (kPa) 449 (388-501) 512 (464-589) 534 (439-554) 626 (541-754) 573 (503-622) 1.3e-8
AscAo (kPa) 316 (290-340) 347 (322-365) 358 (342-415) 424 (400-462) 413 (389-466) 2.6e-15

aTAA, Ascending thoracic aortic aneurysm; SOV, sinuses of Valsalva; STJ, sinotubular junction; AscAo, ascending aorta.

FIGURE 2.

FIGURE 2.

Relationship between peak circumferential wall stress and diameter group for whole aneurysm (A), SOV (B),STJ (C), and AscAo (D) in TAV-aTAA. Median (horizontal line), 25th and 75th percentiles (box), range (whiskers), and observations (dots).

Longitudinal Tricuspid Aortic Valve–Associated Ascending Thoracic Aortic Aneurysm Wall Stress by Diameter

At systolic pressure, peak longitudinal wall stresses were 290 (265-323) kPa for size 4.0 to 4.4 cm, 330 (296-359) kPa for 4.5 to 4.9 cm, 339 (320-373) kPa for 5.0 to 5.4 cm, 318 (293-351) kPa for 5.5 to 5.9 cm, and 373 (363-449) kPa for 6.0 cm or greater (Table 3). Longitudinal peak wall stresses increased with diameter (P = 8.7e-8) (Figure 3, A). The same trend was present on individual aTAA anatomic regions (Figure 3, B-D). Peak longitudinal wall stresses for AscAo, STJ, and SOV are reported in Table 3. When diameter was evaluated as a continuous variable, the correlation of peak longitudinal wall stresses to diameter was r = 0.38 (P = 2.1e-9) for whole aTAA, r = 0.51 (P = 3.4e-16) for AscAo, r = 0.52 (P < 2.2e-16) for STJ, and r = 0.52 (P < 2.2e-16) for SOV, respectively. Representative wall stress profiles are shown in Figure 4.

TABLE 3.

Longitudinal tricuspid aortic valve ascending thoracic aortic aneurysm peak wall stress

4.0-4.4 cm (n = 100) 4.5-4.9 cm (n = 77) 5.0-5.4 cm (n = 21) 5.5-5.9 cm (n = 13) ≥6.0 cm (n = 10) P value
Whole aTAA (kPa) 290 (265-323) 330 (296-359) 339 (320-373) 318 (293-351) 373 (363-449) 8.7e-8
SOV (kPa) 295 (263-333) 337 (307-366) 339 (317-380) 359 (320-437) 435 (421-463) 6.6e-10
STJ (kPa) 206 (184-251) 255 (223-286) 284 (229-299) 318 (277-349) 330 (299-413) 2.1e-11
AscAo (kPa) 176 (157-193) 194 (182-213) 225 (203-245) 227 (218-251) 248 (223-256) 8.5e-13

aTAA, Ascending thoracic aortic aneurysm; SOV, sinuses of Valsalva; STJ, sinotubular junction; AscAo, ascending aorta.

FIGURE 3.

FIGURE 3.

Relationship between peak longitudinal wall stress and diameter group for whole aneurysm (A), SOV (B), STJ (C), and AscAo (D) in TAV-aTAA. Median (horizontal line), 25th and 75th percentiles (box), range (whiskers), and observations (dots).

FIGURE 4.

FIGURE 4.

Characteristic TAV-aTAA wall stress profiles by diameter group in both circumferential and longitudinal directions. Color bar displays the relation of figure colors to wall stress magnitude in kPa. Location of highest wall stress are indicated by a black arrow.

Circumferential Versus Longitudinal Tricuspid Aortic Valve–Associated Ascending Thoracic Aortic Aneurysm Wall Stress

Peak wall stresses for TAV-aTAAs were greater in the circumferential than longitudinal direction (494 [432-577] vs 313 [280-352] kPa, P < 2.2e-16). The same relationship was true for TAV-aTAAs size 4.0 to 4.4 cm (460 [421-543] vs 290 [265-323] kPa, P < 2.2e-16), size 4.5 to 4.9 cm (503 [453-569] vs 330 [296-359] kPa, P = 2.5e-14), size 5.0 to 5.4 cm (549 [430-569] vs 339 [320-373] kPa, P = 9.5e-7), size 5.5 to 5.9 cm (540 [471-608] vs 318 [293-351] kPa, P = .0002), and size 6.0 cm or greater (596 [506-649] vs 373 [363-449] kPa, P = .002).

Reproducibility of wall stress results was tested with 2 investigators independently reconstructing TAV-aTAA models and performing FE simulations for a 11% subset of patients (n = 24) of the current study. Circumferential TAV-aTAA peak wall stresses were 486 (449-524) kPa versus 477 (427-521) kPa for investigators 1 and 2, respectively (P = .09). Longitudinal peak wall stresses were 329 (298-341) kPa versus 306 (262-345) kPa for investigator 1 and 2, respectively (P = .24).

Impact of Blood Pressure Reduction on Tricuspid Aortic Valve Ascending Thoracic Aortic Aneurysm Wall Stresses

For a subset of TAV-aTAAs (n = 96) with a median diameter 4.4 (4.1-4.8) cm, overall peak circumferential wall stresses were greater at a blood pressure of 120 mm Hg than 95 mm Hg (444 [385-511] vs 358 [316-412] kPa, P < 2.2e-16). Peak longitudinal wall stresses were also greater at a blood pressure of 120 mm Hg than 95 mm Hg (283 [257-312] vs 238 [213-260] kPa, P < 2.2e-16).

DISCUSSION

In this study, we found that the magnitudes of TAV-aTAA peak wall stress increase with diameter in both circumferential and longitudinal directions. However, aTAA diameter groups had a wide distribution of stresses resulting in a large overlap between different groups. The same findings remained true when considering stresses limited to the SOV, STJ, or AscAo. These findings are consistent with the concept that dissection risk increases with diameter in a population level. However, we found that even small aneurysms can experience wall stresses as large as aneurysms that met surgical size criteria for operation, and some small aneurysms may have large enough wall stress magnitudes to predispose to acute aortic events. These aTAA cases would otherwise have been deemed to be at low risk of dissection or rupture based on diameter alone. Conversely, some patients who would be offered surgical repair based on diameter-based surgical guidelines had wall stresses that were so low and similar to small size aneurysms that they may not be predisposed to dissection.

Finite Element Analyses Studies in Literature

Our findings are consistent with other smaller finite element studies in the literature. Trabelsi and colleagues17 reported that peak wall stress was only loosely correlated with diameter (ρ = 0.53) in a cohort of 5 patients with patient-specific material properties.17 Of interest, the rupture risk index, defined as the ratio of peak to failure stress, was not positively correlated with diameter (ρ = −0.29), suggesting diameter is inadequate to predict dissection. Martin and colleagues18 found that peak systolic wall stress was unrelated to diameter (P = .08) in a group of 27 aneurysms. Notably, they found the diameter risk ratio (defined as aTAA diameter at systole over diameter preceding failure), a metric to capture dissection/rupture risk, missed any observable relation with maximum diameter, but correlated instead with peak wall stress. These findings support wall stress as a superior predictor of dissection or aortic events. Nonetheless, both of these studies were limited by a small sample size, which increases the risk of type II error. Both studies also prevented secondary analysis of TAV-aTAAs exclusively. Similar findings have been described by our group. In an early study, we observed that in TAV-aTAAs, both circumferential and longitudinal systolic wall stresses had moderate correlations with diameter (r = 0.71 and 0.68, respectively). These correlations were stronger than their bicuspid counterparts.9 This study was also limited by a small sample size (n = 18) and aneurysm geometries that excluded SOV and LVOT potentially influencing wall stress values based upon boundary conditions. Our subsequent study with approximately 100 aTAAs addressed these limitations and found a correlation of wall stress with diameter that was improved for large aneurysms size 5 cm or greater than those less than 5 cm.12 However, the correlation was poor to moderate in either group. This observation remained true when studying TAV-aTAAs alone. This study corroborates our findings with a larger study focused on TAV-aTAAs. Overall peak aTAA wall stresses correlated poorly with diameter with r correlation coefficients of 0.26 and 0.38 for circumferential and longitudinal directions, respectively. Similar to our new findings, our previous study demonstrated a large overlap of stresses between less than 5 cm and 5 cm or greater aTAAs. Our current FE study adds to our prior work by examining a larger cohort of aTAAs, double the prior study, and specifically focused on TAV-associated aTAAs (n = 221) to examine diameters incrementally by every 0.5 cm and understand the impact of the 5.5 cm diameter cutoff for aneurysm repair on wall stresses. Of interest, studies have previously proposed and evaluated index diameter metrics including diameter/height and diameter/body surface area as patient-specific predictors of aneurysm dissection and rupture.3 On the basis of these updated guidelines, future studies could evaluate if index diameter metrics provide a better correlation with wall stress.

Biomechanics of Acute Type A Aortic Dissection

In theory from a biomechanical standpoint, aortic dissection may occur from failure of the aortic intimal layer due to high wall stresses versus wall strength.7 Wall strength cannot be determined in vivo as it requires destructive tissue testing from human aTAA surgical specimens. An alternative would be to assess the relationship between in vivo distensibility (aortic stiffness) and ex vivo failure mechanics. Pichamuthu and colleagues19 studied the failure mechanics of TAV versus BAV-ATAAs with uniaxial tensile testing. BAV-aTAA wall strength was found to be greater than that of TAV-aTAA in both circumferential and longitudinal directions. Others found that BAV-aTAA strength was equal to stronger than TAV-aTAAs.20-22 In both BAV and TAV aneurysms, circumferential tensile strength was approximately twice the strength in the longitudinal direction. Although circumferential stresses are significantly greater than longitudinal stresses, the lower longitudinal strength in relationship to circumferential strength explains the reason why dissection entry tears begin transversely.23 Gleason’s group19 reported a longitudinal tensile strength of 54N/cm2 (540 kPa). Tensile strength in relation to wall stress could estimate dissection or rupture risk. One of our small aTAAs with size 4.5 cm already exceeded this strength value. Notably, our results were calculated assuming normal blood pressure (120/80 mm Hg). However, hypertension of varying severity was prevalent (80%) in our cohort. Using a quick nonpatient-specific calculation based on Laplace’s law, patients with aTAAs with peak longitudinal wall stress greater than 462 kPa could reach a stress of 540 kPa when experiencing a systolic pressure of 140 mm Hg. Applied to our cohort, this would include 5% of aTAAs size 4.5 to 5.4 cm and 18% of size 5.5 cm or greater. Close follow-up and prospective investigation of patients with approximately 462 kPa longitudinal stress might be considered to assess a potential surgical wall stress threshold. In this study, we also showed for a group of small aneurysms that blood pressure reduction from 120 to 95 mm Hg resulted in a 20% reduction in longitudinal wall stresses. A 20% wall stress reduction decreased peak longitudinal wall stresses to less than 462 kPa in all but one of our aTAAs less than 5.5 cm. These results emphasize the benefit of blood pressure reduction as a means to reduce aneurysm wall stress and risk of dissection. Although the complexity of dissection may involve the patterns of blood pressure and tissue remodeling over time, the beauty of patient-specific aTAA biomechanics is that as long as the parameters are known, such as changes in blood pressure, aTAA geometry, and in vivo distensibility (as a surrogate for wall strength), then patient-specific simulations over time could provide understanding of when an individual patient transitions from low to higher risk of dissection.

We could also apply epidemiological rates of dissection to our cohort as another means of estimating a surgical stress threshold. Based on a cohort of approximately 800 aTAAs, Zafar and colleagues3 reported annual type A dissection rates for the same size groups we used in the current study and found dissection rates of 1.2% for size 4.0 to 4.4 cm, 2.0% for 4.5 to 4.9 cm, 1.8% for 5.0 to 5.4 cm, 3.5% for 5.5 to 5.9 cm, and 9.6% for 6.0 cm or greater.3 By matching dissection rates to corresponding percentiles of longitudinal wall stress in the same diameter groups, we hypothesize that TAV-aTAAs with longitudinal peak wall stress of at least 457 kPa would be at high risk of dissection events. The percentage of TAV-aTAAs with peak longitudinal wall stresses above this stress threshold were 0% for size 4.0 to 4.4 cm, 3.9% for 4.5 to 4.9 cm, 9.5% for 5.0 to 5.4 cm, 7.7% for 5.5 to 5.9 cm, and 30% for 6.0 cm or greater in our cohort. A surgical wall stress threshold of approximately 450 kPa would be congruent with both the epidemiologic dissection data and failure data available at present.24-26 To better define a surgical threshold, a comprehensive biomechanical study of wall failure properties in relation to the wall stresses specific to aTAA considering all aortic subregions would be beneficial.

Of interest, a recent study found that aTAAs that dissected and had predissection imaging (n = 7), experienced higher longitudinal wall stresses than age and size-matched controls with the location of the entry tear matching regions of increased stress.27 In our study, we found that a group of TAV-aTAAs less than 5.5 cm experience longitudinal wall stresses similar in magnitude to aneurysms 5.5 cm or greater. These findings remained true when studying aneurysms as a whole or by specific aortic regions (ie, STJ, SOV, AscAo). Celi and Berti28 noted that small aneurysms can have large stress values when aneurysm eccentricity is present. Taken together, these observations have the following clinical implications. ATAA wall stresses are dependent on the whole 3D geometry rather than a single maximal diameter value. Small aneurysms that experience large longitudinal stresses could be at high risk of dissection explaining the acute events that occur in aneurysms not meeting surgical repair guidelines.5,6,29 Determining patient-specific TAV-aTAA biomechanics through computational models may further help determine dissection risk and need for elective aTAA surgery despite less than 5.5 cm size.

The use of FEA and wall stresses as tools to assist surgical decision making will require prospective validation in clinical studies. In the present study, we have shown that diameter is poorly correlated to wall stress and that the law of LaPlace is inadequate in these complex geometries. The underlying natural history studies from which the guidelines were based used diameter as a surrogate for wall stress and developed the size thresholds using patients who had already dissected. The limited studies that have captured predissection diameters in patients whose imaging was performed within 2 years of dissection have shown diameters in the 4.3- to 4.5-cm range.27,29 As such, a prospective study of patients with nonsurgical sized aneurysms followed regularly for clinical events and correlated with not only wall stresses but also diameter and other parameters is needed to fundamentally improve on existing guidelines. Although we did not show a correlation of wall stresses to clinical events in this study, Emerel and colleagues27 demonstrated that increased longitudinal wall stresses correlated with intimal tear location. Thus, our study requires future patient follow-up for clinical events.

Study Limitations

Our cohort is heavily weighted to the male population reflective of the veteran population. Ninety-eight percent of our subjects were men with a long history of smoking and high rates of hypertension, hyperlipidemia, and other cardiovascular risk factors. These results may not be reflective of women or civilian populations with different risk profiles. Although our limitation is that the relation of wall stress and dissection risk is not directly established, others have shown a direct correlation of increased longitudinal wall stresses with intimal tear in dissection.27 Our study requires continued patient follow-up for clinical events. In addition, our model has multiple assumptions. TAV-aTAA was assumed to be homogenous, while regional variations in thickness and mechanical properties do exist. Current CT modalities are insufficient to accurately resolve aTAA wall thickness but are the most commonly used imaging techniques. Even cine magnetic resonance imaging, which we have used in a few patients to resolve wall thickness only for research purposes, measures thickness at 1 plane rather than through the entire aTAA region. Thickness used here was based on average ex vivo aTAA tissue thickness, which upon FEA simulation to systemic pressure provided in vivo aTAA wall thickness. Average TAV-ATAA material properties were used, which provide reasonable estimation of patient-specific wall stresses since we demonstrated previously that there were no significant differences in FEA results among simulations using patient-specific, group-averaged, and population-based literature material properties.30 Whole wall properties were used, and the impact of incorporating differences in wall layers material properties27 can be explored in the future. Longitudinal motion was fixed at the LVOT and mid-thoracic descending aorta while cardiac motion during the cardiac cycle does occur. These assumptions can influence simulation results. The present study did not consider fluid-structure interactions or blood flow patterns such as higher velocity and skewed retrograde and helical flow of aneurysmal aorta, which was beyond the scope of this project.31,32 Wall shear stresses were not considered because they are 5 orders of magnitude lower than wall stress due to blood pressure with respect to dissection or rupture risk.33 Wall shear stresses and helical flows are most commonly perturbed in BAV-aTAA, and that population was excluded in this study.

CONCLUSIONS

We described patient-specific TAV-aTAA wall stresses by size and found that circumferential and longitudinal stresses increase with diameter with a large overlap of ranges between small and large aneurysms. Some of our patients with small aTAA are potentially at higher dissection risk, consistent with studies reporting large proportion of dissection events occurring in patients with aneurysms less than 5.5 cm. Wall stresses were effectively reduced with blood pressure reduction, emphasizing the importance of medical therapy to reduce risk. This study highlights the potential utility of patient-specific aTAA wall stresses in relation to wall strength to understand dissection risk and assist decision-making of elective surgical aTAA repair.

Supplementary Material

video supplement

VIDEO 1. Schematic of study methodology displaying image segmentation of a representative TAV-aTAA, inner surface reconstruction (yellow), geometric mesh development with anatomic regions defined in color, and longitudinal wall stress profile with location of peak stress identified by filled arrow. Video also shows representative cardiac cycle simulation results for TAV-aTAA diameter groups. Color bar displays the relation of figure colors to wall stress magnitude in kPa. Video available at: https://www.jtcvs.org/article/S0022-5223(21)00909-0/fulltext.

Download video file (4.8MB, mp4)
supplemental figure

CENTRAL MESSAGE.

Some small TAV-aTAAs have peak wall stresses comparable to those of large aneurysms and are potentially at high risk of acute type A dissection.

PERSPECTIVE.

Type A dissection frequently occurs below aneurysm repair size thresholds. Diameter is a poor predictor of wall stress and thus dissection risk in aneurysms. Using patient-specific models, we found a subset of small aneurysms experiencing substantial wall stresses. FEA could be used to understand dissection risk and assist decision-making of elective surgical aTAA repair.

Acknowledgments

This study was funded by the National Institutes of Health (NIH) R01HL119857-01A1 (L.G.), the American Heart Association Postdoctoral fellowship 20POST35211107 (Z.W.), and NIH K25HL150408 (Y.X.). This study was funded by NIH R01HL119857-01A1 (L.G., E.E.T.). CHR approval: 13-10932, 10-03594.

Abbreviations and Acronyms

AscAo

ascending aorta

aTAA

ascending thoracic aortic aneurysm

BAV

bicuspid aortic valve

CT

computed tomography

FEA

finite element analysis

LVOT

left ventricular outflow tract

SOV

sinuses of Valsalva

STJ

sinotubular junction

TAV

tricuspid aortic valve

3D

3-dimensional

Footnotes

Conflict of Interest Statement

The authors reported no conflicts of interest.

The Journal policy requires editors and reviewers to disclose conflicts of interest and to decline handling or reviewing manuscripts for which they may have a conflict of interest. The editors and reviewers of this article have no conflicts of interest.

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Associated Data

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Supplementary Materials

video supplement

VIDEO 1. Schematic of study methodology displaying image segmentation of a representative TAV-aTAA, inner surface reconstruction (yellow), geometric mesh development with anatomic regions defined in color, and longitudinal wall stress profile with location of peak stress identified by filled arrow. Video also shows representative cardiac cycle simulation results for TAV-aTAA diameter groups. Color bar displays the relation of figure colors to wall stress magnitude in kPa. Video available at: https://www.jtcvs.org/article/S0022-5223(21)00909-0/fulltext.

Download video file (4.8MB, mp4)
supplemental figure

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