| Literature DB >> 32462091 |
Monika Petelczyc1, Jan Jakub Gierałtowski1, Barbara Żogała-Siudem2, Grzegorz Siudem1.
Abstract
An observational error of heart rate variability (HRV) may arise from many factors, such as a limited sampling frequency, QRS complexes detection process, preprocessing procedures and others. In our study, we focused on the first two origins of measurement error. We introduced a model of observational error and suggested universal descriptors for the assessment of its resultant magnitude in terms of time, frequency as well as nonlinear parameters. For this purpose, we applied Monte Carlo simulations which showed that the most sensitive to observational error are: pNN50 (the proportion of pairs of successive RR intervals that differ by more than 50 ms) and markers obtained from frequency analysis. On the other hand, the most resistant are other time domain parameters as well as the short and long-term slopes of Detrended Fluctuation Analysis (DFA). We postulate that the observational error should be considered in population studies, when different recorders are used in the research centres. Additionally, in the case of patients with similar etiology of disease but with different heart rhythms abnormalities the scatter of HRV parameters will also be observed due to the subject's the time series variability.Entities:
Keywords: Biomedical engineering; Cardiology; Error approximation; Monte Carlo methods; Signal processing
Year: 2020 PMID: 32462091 PMCID: PMC7240322 DOI: 10.1016/j.heliyon.2020.e03984
Source DB: PubMed Journal: Heliyon ISSN: 2405-8440
Figure 1The computations for RR intervals of ECG file no. 101 from MIT-BIH Arrhythmia Database [10]. Each box-plot represents 1000 values of α2 parameter obtained from the time series with added Gaussian noise (MC simulation). The Gaussian noise has zero mean and standard deviation σ given in milliseconds. Horizontal dotted line marks the parameter α2 for the original recording.
The ratios of the total error p ± SD for the HRV parameters with increasing magnitude of observational error σ. The p values in the table are normalised and presented in %, following Eq. (2). The results are obtained from the MC simulations repeated 103 times for each signal of the MIT BIH Database separately.
| HRV parameter | ||||
|---|---|---|---|---|
| MeanRR | 0.005 ± 0.0005 | 0.01 ± 0.001 | 0.01 ± 0.001 | 0.02 ± 0.002 |
| SDRR | 0.07 ± 0.06 | 0.21 ± 0.19 | 0.3 ± 0.28 | 0.66 ± 0.66 |
| RMSSD | 0.13 ± 0.15 | 0.4 ± 0.51 | 0.58 ± 0.75 | 1.3 ± 1.78 |
| pRR50 | 1.98 ± 2.37 | 4.14 ± 5.09 | 5.94 ± 8.77 | 15.0 ± 24.3 |
| 0.13 ± 0.10 | 0.32 ± 0.30 | 0.42 ± 0.43 | 0.83 ± 0.97 | |
| 0.15 ± 0.11 | 0.34 ± 0.25 | 0.44 ± 0.34 | 0.79 ± 0.67 | |
| ApEn | 1.37 ± 1.23 | 2.27 ± 2.26 | 3.04 ± 3.09 | 6.13 ± 6.02 |
| SampEn | 1.79 ± 1.45 | 2.79 ± 2.39 | 3.71 ± 3.21 | 7.47 ± 6.42 |
| LF | 12.89 ± 21.56 | 25.86 ± 32.53 | 28.88 ± 35.42 | 37.94 ± 41.97 |
| HF | 4.69 ± 5.44 | 10.49 ± 11.47 | 11.39 ± 12.00 | 14.85 ± 15.22 |
| LF/HF | 18.04 ± 28.20 | 36.86 ± 45.13 | 41.35 ± 49.46 | 54.51 ± 59.66 |