| Literature DB >> 34233715 |
Sylvia Krupickova1,2,3, Suzan Hatipoglu2, Giovanni DiSalvo1,3, Inga Voges1,2, Daniel Redfearn1, Sandrine Foldvari1, Christian Eichhorn1,2, Sian Chivers1, Filippo Puricelli2, Grazia Delle-Donne1, Courtney Barth1, Dudley J Pennell2,3, Sanjay K Prasad2,3, Piers E F Daubeney4,5.
Abstract
BACKGROUND: Cardiovascular magnetic resonance (CMR) derived fractal analysis of the left ventricle (LV) has been shown in adults to be a useful quantitative measure of trabeculation with high reproducibility and accuracy for the diagnosis of LV non-compaction (LVNC). The aim of this study was to investigate the utility and feasibility of fractal analysis in children.Entities:
Keywords: Children; Fractal analysis; Left ventricular noncompaction
Year: 2021 PMID: 34233715 PMCID: PMC8265058 DOI: 10.1186/s12968-021-00778-5
Source DB: PubMed Journal: J Cardiovasc Magn Reson ISSN: 1097-6647 Impact factor: 5.364
Fig. 1A Cardiovascular Magnetic Resonance (CMR) Trabecular Fractal Analysis using OsiriX Plugin (MATLAB graphical user interface). B Example of segmentation using fractal plug-in in a patient with left ventricular non-compaction (LVNC)
Demographics data of the 3 studied groups (LVNC, hypertrabeculation and normal controls), N = 84
| Variable | LVNC (N = 28) | Hypertrabeculation (N = 28) | Normal (N = 28) |
|---|---|---|---|
| Age (years) | 14(4) | 12(3) p = 0.098* | 13(3) p = 0.512** |
| Male/Female | 16/12 | 18/10 p = 0.594* | 18/10 p = 1.000** |
| Weight (kg) | 51(18) | 47(16) p = 0.238* | 49(17) p = 0.422** |
| Height (cm) | 156 (22) | 154(16) p = 0.550* | 156(19) p = 0.617** |
| BSA (m2) | 1.48 (0.35) | 1.41(0.31) p = 0.321* | 1.45(0.35). p = 0.461** |
| Fractal global | 1.345(0.053) | 1.252(0.034) p < 0.001* | 1.158(0.038) p < 0.001** |
| Fractal max | 1.475(0.041) | 1.346(0.027) p < 0.001* | 1.259(0.043) p < 0.001** |
| Petersen | 2.8(0.4) | 1.8(0.2) p < 0.001* | 1.1(0.1) p < 0.001** |
| Jacquier | 0.35(0.10) | 0.19(0.07) p < 0.001* | 0.14(0.08). p = 0.012** |
| LVEDVI (ml/m2) | 67(15) | 67(11) p = 0.658* | 65(11) p = 0.870** |
| LVESVI (ml/m2) | 27(11) | 24(7) p = 0.566* | 22(5) p = 0.522** |
| LVSVI (ml/m2) | 40(9) | 43(8) p = 0.209* | 43(8) p = 0.837** |
| LVEF (%) | 61(11) | 65(7) p = 0.189* | 66(5) p = 0.594** |
| LV mass (g/m2)a | 96(18) | 82(15) p = 0.002* | 69(10) p < 0.001** |
Mean (SEM)
*Wilcoxon test comparing LVNC and hypertrabeculation groups
**Wilcoxon test comparing hypertrabeculation group and normal controls
aTrabeculations were included in the global LV mass for our volumetric analysis, therefore the difference in LV mass index between groups is significant
BSA body surface area, LV left ventricular, LVEDVI left ventricular end-diastolic volume index, LVEF left ventricular ejection fraction, LVESVI left ventricular end-systolic volume index, LVNC left ventricular non-compaction, LVSVI left ventricular stroke volume index
Fig. 2Global (A) and maximum fractal dimension (FD) (B) in all studied subjects. Violin plots show the distribution of global (A) and maximum FD (B) in the LVNC, hyper-trabeculated group and controls. There was no overlap between the LVNC and hyper-trabeculated/ normal groups for mean maximum FD. Both global and maximum FD were higher in the LVNC group than in the hyper-trabeculation group (p < 0.001) and controls (p < 0.001). Mean ± SEM
Fig. 3Distribution of maximum fractal dimension (FD) within the LV for the LVNC, hyper-trabeculation and normal groups. The LVNC group (A) had a different pattern of maximum FD distribution when compared to the hyper-trabeculated group (B) and normal (C). There was an increase in maximum FD from base to apex in the LVNC group [maximum FD at apex 1.467 (0.035)] whereas the hyper-trabeculated and normal groups showed highest maximum FD in the middle third of the LV [1.327 (0.025), 1.251 (0.042), respectively]
Maximum fractal dimension in the LV basal, mid and apical third in all 3 study groups
| LVNC | Hypertrabeculation | Controls | |
|---|---|---|---|
| Basal third | 1.274 (0.078) | 1.179 (0.082) p < 0.001* | 1.140 (0.088) p = 0.078** |
| Mid third | 1.394 (0.082) | ||
| Apical third | 1.316 (0.058) p < 0.001* | 1.195 (0.074) p < 0.001** |
Highest maximum fractal dimension in each study group is highlighted in bold
Mean (SEM)
*Wilcoxon test comparing LVNC and hypertrabeculation groups
**Wilcoxon test comparing hypertrabeculation and control groups
Fig. 4Bland Altman graphs showing the intraobserver variability for all 3 methods—Fractal analysis (A), Petersen (B) and Jacquier (C). Fractal analysis showed the best intraobserver variability from all 3 methods [intraclass correlation coefficient (ICC) 0.99, 95% CI 0.98, 1.00]. The Petersen method had more intraobserver variability than the fractal method (ICC 0.95, 95% CI 0.90, 0.98) and the Jacquier method showed the worst intraobserver variability (ICC 0.82, 95% CI 0.63, 0.92)
Fig. 5Bland Altman graphs showing the interobserver variability for all 3 methods—Fractal analysis (A), Petersen (B) and Jacquier (C). Interobserver variability was better using the fractal method (ICC 0.97, 95% CI 0.95, 0.99), and considerably more using the Petersen (ICC 0.92, 95% CI 0.83, 0.96) and Jacquier methods (ICC 0.74, 95% CI 0.45, 0.88)