Smart Wearables in Healthcare: Signal Processing, Device Development, and Clinical Applications
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Ludi Wang, Wei Zhou, Ying Xing, Xiaoguang Zhou, "A Novel Neural Network Model for Blood Pressure Estimation Using Photoplethesmography without Electrocardiogram", Journal of Healthcare Engineering, vol. 2018, Article ID 7804243, 9 pages, 2018. https://doi.org/10.1155/2018/7804243
A Novel Neural Network Model for Blood Pressure Estimation Using Photoplethesmography without Electrocardiogram
Abstract
The prevention, evaluation, and treatment of hypertension have attracted increasing attention in recent years. As photoplethysmography (PPG) technology has been widely applied to wearable sensors, the noninvasive estimation of blood pressure (BP) using the PPG method has received considerable interest. In this paper, a method for estimating systolic and diastolic BP based only on a PPG signal is developed. The multitaper method (MTM) is used for feature extraction, and an artificial neural network (ANN) is used for estimation. Compared with previous approaches, the proposed method obtains better accuracy; the mean absolute error is 4.02 ± 2.79 mmHg for systolic BP and 2.27 ± 1.82 mmHg for diastolic BP.
1. Introduction
Blood pressure (BP) is the driving force for the flow of blood through the blood vessels and reflects the cardiovascular health of the human body. At present, hypertension is the most significant risk factor for cardiovascular and cerebrovascular diseases, identified by the World Health Organization [1] as the main cause of death and disability among the elderly. Poorly controlled hypertension increases the risk of heart attacks, strokes, kidney failure, and heart failure.
Table 1 lists the classification criteria for hypertension in adults (age > 18 years). A normal BP for an adult human is 120/80 mmHg. A systolic blood pressure (SBP) of between 140 and 159 mmHg or diastolic blood pressure (DBP) of between 90 and 99 mmHg is defined as the first stage of hypertension, while the second stage is when SBP is higher than 159 mmHg, or DBP is higher than 99 mmHg [2].

Invasive BP measurement has the highest accuracy of several methods available for measuring BP, but it is not widely applied because of its difficulty and high risk. Using Korotkoff sounds to estimate SBP and DBP is another auscultatory measurement, and this has been widely accepted as the gold standard [3, 4]. Despite its high degree of accuracy and reliability, the auscultatory method does not apply to home blood pressure measurement (HBPM) [5], as it requires a treained professional [6]. Furthermore, the mercury sphygmomanometer is gradually being removed from clinical use [6]. Oscillometric blood pressure measurement has become increasingly popular in automated blood pressure measurement devices [7]. This method uses an electronic pressure sensor to observe the pressure oscillation in the cuff, during its gradual deflation from above SBP to below DBP. The oscillation amplitude increases to its maximum value when the cuff pressure reaches the mean arterial pressure and then gradually decreases with subsequent deflation of the cuff pressure [8]. However, it cannot provide continuous beattobeat BP measurement with its periodic features, and it is not appropriate for home healthcare or easing the workload of clinicians at hospitals.
For cuffless BP measurement, the pulse transit time (PTT) method and photoplethysmography (PPG) are widely used techniques [9]. PTT is defined as the time taken for the arterial pulse pressure wave to travel from the aortic valve to the periphery [10], and some researchers have used it to estimate BP indirectly [11]. However, there are two parameters required to calculate PTT, electrocardiogram (ECG), and PPG. As a result, calculation of PPT commonly requires two devices to obtain these two parameters—the ECG is measured at the wrist or chest, and the PPG is measured from the index finger [12].
Wearable pulse rate sensors based on PPG have become increasingly popular, with more than ten companies producing these sensors commercially [13]. To take advantage of this technology, some researchers have experimented with using only a single PPG waveform for estimating BP. A continuous PPG waveform and one single PPG waveform extracted from it are shown in Figure 1. Shin et al. [14] presented a pressure index (PI) extracted from a single PPG signal to estimate BP. Teng et al. [15] extracted four features of PPG signals to find an optimal feature for BP estimation: width of 2/3 pulse amplitude, width of 1/2 pulse amplitude, systolic upstroke time, and diastolic time. This method established a linear regression model and found that systolic upstroke time and diastolic upstroke time from the PPG wave have higher correlations with BP. However, tests show that such a correlation is not always linear. Gao et al. [16] developed a method for BP estimation using the regression support vector machine (RSVM) method, with RBF kernel and discrete wavelet transform, and obtained better performance.
In this paper, a new approach for beattobeat BP estimation based on artificial neural networks (ANNs) is presented. Yi et al. [17] have proved that for BP estimation, ANNs have better performance compared to regression analysis using PTT. The presented method uses a multitaper method (MTM) [18] to obtain the spectral components and combines them with two morphological features of a PPG signal, to constitute the input parameters. For wide representation of possible PPG signal and correspondent beattobeat BP, we extract the signal from the Multiparameter Intelligent Monitoring in Intensive Care (MIMIC) database [19, 20] for network training and testing. The results show that the presented method achieves better performance using only the PPG signal. Figure 2 shows the schematic illustration of presented BP estimation frameworks.
The paper is organized as follows: Section 2 describes the overview of the MIMIC database, Section 3 explains the features extracted from a PPG signal and the presentation of the architecture of the ANN, and Section 4 shows the results using different methods. Finally, the conclusion summarizes the paper proposal and briefly anticipates future work.
2. Data Description
The MIMIC database is a collection of multiparameter recordings from over 90 ICU patients. The data in each case includes signals and periodic measurements obtained from a bedside monitor, as well as clinical data obtained from the patient’s medical record. The recordings vary in length; almost all of them are at least 20 hours, and many are 40 hours or more. In total, the database contains nearly 200 patientdays of realtime signals and accompanying data [21].
The database contains data of ECG (leads I, III, and V), ABP, PAP, PPG, and respiratory signals recorded simultaneously with a 125 Hz sampling rate. In this paper, only the records with both ABP and PPG were extracted. Figure 3 shows an example record.
In total, there are 58,795 valid intervals of PPG signal (subject number is 72) and corresponding BP values for different people and different time instances. In order to avoid overfitting, we use 70% of them for network training, 15% of them for validation, and 15% of them for testing. The training dataset is presented to the network during training, and the network is adjusted according to its error. The validation dataset is used to measure network generalization and to halt training when generalization stops improving. The test dataset has no effect on training and so provides an independent measure of network performance during and after training. The LevenbergMarquardt algorithm was chosen for training the ANN. In this algorithm, training automatically stops when generalization stops improving, as indicated by an increase in the mean square error of the validation samples.
3. ANNBased BP Estimation
3.1. Multitaper Method
The multitaper method (MTM) [22] takes advantage of an extended version of the spectral representation as follows:
In this case, the may contain a number of periodic components in addition to the underlying stationary process as follows: where is a zeromean stationary process with not necessarily constant [18]. The above types of processes, called central stationary or conditional stationary processes, are often referred to as having mixed spectra [23]. For these processes, the expected value of the discrete orthogonal increment process is no longer zero and can be calculated as follows: where is the Dirac delta function. The second central moment of can be obtained as follows:
For processes with mixed spectra, the first moment of gives the deterministic component, while the second central moment of gives the continuous nondeterministic component. The classical method has been centered on the estimation of the second moment of , which gives the continuous component of the spectrum. However, the estimation of the first moment of was initially also required. Major opposition to the classical method is predicated on the fact that there is no separation between the deterministic component and nondeterministic component; spurious peaks in the spectrum can be identified as the deterministic component without an objective criterion for differentiating between real and spurious lines [24].
In the MTM spectral estimation, a useful, yet simple, likelihood ratio test for the significance of periodic components is offered by the multiwindow method. This method makes use of multiple data windows, referred to as “Slepian sequences” and “discrete prolate spheroidal sequences.” They are defined as follows: where N is the number of sampling points of a single PPG wave (the sampling rate is 125 Hz), W is the spectral bandwidth, and are the eigenvalues associated with the Slepian sequences , which can be calculated numerically [25]. After Fourier transformation, the Slepian functions can be calculated as follows:
In the interval , the energy concentration of the above Slepian functions is maximum. Furthermore, the bias from all frequencies is remote from the frequency of the window width times the number of observations, and thus the use of these sequences is very effective in eliminating window leakage [26].
The MTM calculates the expansion or eigen coefficients of input as a first step as follows:
Combining the above equations, the expected value of can be obtained as follows:
At , assuming and thus neglecting the second term in (9), since is highly concentrated in the interval .
By minimizing the residual local squared error, that is, when , the can be estimated. The squared error can be described as follows:
The result is given as follows:
An F test can be used to test for the significance of a line component at , and the location of its maximum value provides an estimation of the line frequency.
In this paper, the periods of interest are nearly as long as the data. Thus, a line component at zero frequency is included and the estimation of from (11) is used as an alternative estimation of the mean, which will result in the preservation of the continuous part of the spectrum at zero frequency [23]. The continuous part of the spectrum can be calculated as follows:
However, according to (4), the spectrum near a significant line component with frequency must be reconstructed, by subtracting the contribution of the line component as follows [27]:
3.2. Feature Extraction
Several spectral and morphological features are used to characterize the single PPG signal. The systolic upstroke time (ST) and diastolic time (DT) presented in [15] are used as the two morphological features. Then the MTM is used to extract the spectral features.
As shown in Figure 4, the dominant frequency of single PPG waveform is mostly focused in the interval of low frequency (0.1~10 Hz).
As a result, this method tries to extract the spectral character in the interval of low frequency (0.1~10 Hz). We calculate the power of every 0.5, 1, 2, 5, and 10 Hz interval. Then, we use them as input separately to determine the optimal number of input parameters, and the results are as listed in Table 2 of Section 4. The best results are obtained when the interval is 0.5 Hz, as presented in Figure 5.

In total, the 22 parameters, including the times of systolic and diastolic parts and spectral features, are used to train the ANN.
3.3. Artificial Neural Network Architecture
There are various ANN architectures for fitting the input data to target, such as counter propagation, learning vector quantization, and radial basis function. Despite good performance, these architectures require large numbers of neurons and cannot be applied in the case of a big training set, due to their substantial memory requirements.
In this paper, PPG features are fed to a multilayer perceptron architecture, which has 22 input neurons (the number of input parameters, as mentioned above) and 2 output neurons, to simultaneously estimate SBP and DBP. This architecture is shown in Figure 6.
4. Experimental Results and Discussion
Figure 7 shows the histograms of the errors, calculated as the difference between real SBP/DBP and the output of the ANN, for the proposed method. The mean difference and standard deviation between the estimated BP and measured BP are −0.0217 ± 4.8950 mmHg for SBP and 0.0975 ± 2.9160 mmHg for DBP.
(a)
(b)
To further evaluate the performance of the presented method, other two BP [15, 16] estimation methods are chosen for comparison in this paper. Table 3 lists the number of subjects in the above studies.
As indicated earlier, performance is assessed on effective records from the MIMIC database and is processed in a MATLAB (MathWorks, Natick, MA, USA) environment. Absolute error and relative error are used to evaluate the performance, which are, respectively, defined as
Table 2 lists the performance results of different numbers of input parameters, and Table 4 lists the results of performance on the test database for the linear regression, RSVMbased method, and ANNbased method with different feature extraction techniques. The results are presented as mean and standard deviation of absolute error and relative error , among reference SBP/DBP and estimated values. For evaluation of the performance of this model in a single individual, test data is divided into individual subsets by index provided by PhysioNet [21] and is used to test performance on each subset, respectively. The estimated performance of the method applied to single individuals is listed in Table 5.

Compared with the other methods, our method has better performance and can be confidently said to provide an effective detection technique for wearable devices and mobile software in the field of hypertension.
5. Conclusion and Future Work
In this study, we propose a noninvasive and beattobeat method of BP estimation determined only from PPG signal. The MTM is used to extract representative features to improve precision and velocity. This is achieved using a typicalstructure feed forward ANN. With the wearable PPG sensor becoming an increasingly popular technology, this method has practical significance as part of a big data solution.
According to the Association for the Advancement of Medical Instrumentation (AAMI), the mean and deviation absolute error between the device and the mercury standard sphygmomanometer can be larger than 5 ± 8 mmHg as well as the number of simultaneous readings agrees within 10 mmHg for 95% or more of the recordings and within 5 mmHg for 85% or more of simultaneous observations [13, 28]. Our future research will investigate how to improve the efficiency of the estimation algorithm, especially in a single individual. We will combine the method with data such as patient age, sex, and previous medical disorders. Hybrid and adaptable methods will also be considered.
Conflicts of Interest
The authors declare that there are no competing interests regarding the publication of this paper.
Acknowledgments
This work is supported by 2015 China Special Fund for GrainScientific Research in Public Interest (201513002).
References
 World Heart Federation, “Hypertension,” August 2017, http://www.worldheartfederation.org/cardiovascularhealth/cardiovasculardiseaseriskfactors/hypertension/?sid=ISI:WoS. View at: Google Scholar
 BC Guidelines & Protocols Advisory Committee, Hypertension – Diagnosis and Management, BC Ministry of Health, 2016.
 J. R. Higgins and S. M. De, “Bloodpressure measurement and classification in pregnancy,” The Lancet, vol. 357, no. 9250, pp. 131–135, 2001. View at: Publisher Site  Google Scholar
 J. Landgraf, S. H. Wishner, and R. A. Kloner, “Comparison of automated oscillometric versus auscultatory blood pressure measurement,” The American Journal of Cardiology, vol. 106, no. 3, pp. 386–388, 2010. View at: Publisher Site  Google Scholar
 T. Ohkubo, Y. Imai, I. Tsuji et al., “Home blood pressure measurement has a stronger predictive power for mortality than does screening blood pressure measurement: a populationbased observation in Ohasama, Japan,” Journal of Hypertension, vol. 16, no. 7, pp. 971–975, 1998. View at: Publisher Site  Google Scholar
 P. K. Lim, S. C. Ng, W. A. Jassim et al., “Improved measurement of blood pressure by extraction of characteristic features from the cuff oscillometric waveform,” Sensors, vol. 15, no. 6, pp. 14142–14161, 2015. View at: Publisher Site  Google Scholar
 T. G. Pickering, J. E. Hall, L. J. Appel et al., “Recommendations for blood pressure measurement in humans and experimental animals. Part 1: blood pressure measurement in humans: a statement for professionals from the Subcommittee of Professional and Public Education of the American Heart Association Council on High Blood Pressure Research,” Hypertension, vol. 45, no. 1, pp. 142–161, 2005. View at: Publisher Site  Google Scholar
 S. Lee, G. Jeon, and G. Lee, “On using maximum a posteriori probability based on a Bayesian model for oscillometric blood pressure estimation,” Sensors, vol. 13, no. 10, pp. 13609–13623, 2013. View at: Publisher Site  Google Scholar
 Z. Taha, L. Shirley, and M. A. M. Razman, “A review on noninvasive hypertension monitoring system by using photoplethysmography method,” Movement, Health & Exercise, vol. 6, no. 1, pp. 47–57, 2017. View at: Google Scholar
 R. P. Smith, J. Argod, J. L. Pepin, and P. A. Levy, “Pulse transit time: an appraisal of potential clinical applications,” Thorax, vol. 54, no. 5, pp. 452–457, 1999. View at: Publisher Site  Google Scholar
 C. Ahlstrom, A. Johansson, F. Uhlin, T. Länne, and P. Ask, “Noninvasive investigation of blood pressure changes using the pulse wave transit time: a novel approach in the monitoring of hemodialysis patients,” Journal of Artificial Organs, vol. 8, no. 3, pp. 192–197, 2005. View at: Publisher Site  Google Scholar
 H. Gesche, D. Grosskurth, G. Küchler, and A. Patzak, “Continuous blood pressure measurement by using the pulse transit time: comparison to a cuffbased method,” European Journal of Applied Physiology, vol. 112, no. 1, pp. 309–315, 2012. View at: Publisher Site  Google Scholar
 W. B. White, A. S. Berson, C. Robbins et al., “National standard for measurement of resting and ambulatory blood pressures with automated sphygmomanometers,” Hypertension, vol. 21, no. 4, pp. 504–509, 1993. View at: Publisher Site  Google Scholar
 H. Shin and S. D. Min, “Feasibility study for the noninvasive blood pressure estimation based on ppg morphology: normotensive subject study,” Biomedical Engineering Online, vol. 16, no. 1, p. 10, 2017. View at: Publisher Site  Google Scholar
 X. F. Teng and Y. T. Zhang, “Continuous and noninvasive estimation of arterial blood pressure using a photoplethysmographic approach,” in Proceedings of the 25th Annual International Conference of the IEEE Engineering in Medicine and Biology Society (IEEE Cat. No.03CH37439), vol. 4, pp. 3153–3156, Cancun, Mexico, 2003. View at: Publisher Site  Google Scholar
 S. C. Gao, P. Wittek, L. Zhao, and W. J. Jiang, “Datadriven estimation of blood pressure using photoplethysmographic signals,” in 2016 38th Annual International Conference of the IEEE Engineering in Medicine and Biology Society (EMBC), pp. 766–769, Orlando, FL, USA, 2016. View at: Publisher Site  Google Scholar
 K. J. Yi, B. Hwan Cho, S. Mi Im, M. Ju Jeon, I. Young Kim, and S. Kim, “Comparative study on artificial neural network with multiple regressions for continuous estimation of blood pressure,” in 2005 IEEE Engineering in Medicine and Biology 27th Annual Conference, pp. 6942–6945, Shanghai, China, 2005. View at: Publisher Site  Google Scholar
 P. Donaldb and A. Walden, Spectral Analysis for Physical Applications, Cambridge University Press, 1998.
 G. B. Moody and R. G. Mark, “A database to support development and evaluation of intelligent intensive care monitoring,” in Computers in Cardiology, 1996, pp. 657–660, Indianapolis, IN, USA, 1996. View at: Publisher Site  Google Scholar
 A. L. Goldberger, L. A. Amaral, L. Glass et al., “PhysioBank, PhysioToolkit, and PhysioNet: components of a new research resource for complex physiologic signals,” Circulation, vol. 101, no. 23, pp. e215–e220, 2000. View at: Publisher Site  Google Scholar
 “MIMIC Database,” August 2017, https://physionet.org/physiobank/database/mimicdb/. View at: Google Scholar
 D. J. Thomson, “Spectrum estimation and harmonic analysis,” Proceedings of the IEEE, vol. 70, no. 9, pp. 1055–1096, 1982. View at: Publisher Site  Google Scholar
 D. J. Thomson, “Time series analysis of Holocene climate data,” Philosophical Transactions of the Royal Society A: Mathematical Physical and Engineering Sciences, vol. 330, no. 1615, pp. 601–616, 1990. View at: Publisher Site  Google Scholar
 D. J. Thomson, “Quadraticinverse spectrum estimates: applications to paleoclimatology,” Philosophical Transactions of the Royal Society A: Mathematical Physical and Engineering Sciences, vol. 332, no. 1627, pp. 539–597, 1990. View at: Publisher Site  Google Scholar
 D. Slepian, “Prolate spheroidal wave functions, fourier analysis, and uncertainty — V: the discrete case,” Bell System Technical Journal, vol. 57, no. 5, pp. 1371–1430, 1978. View at: Publisher Site  Google Scholar
 A. R. Rao and K. Hamed, “Multitaper method of analysis of periodicities in hydrologic data,” Journal of Hydrology, vol. 279, no. 14, pp. 125–143, 2003. View at: Publisher Site  Google Scholar
 Association for the Advancement of Medical Instrumentation, “American national standard for electronic or automated sphygmomanometers,” in ANSI/AAMI SP101992/A1, Arlington, VA, USA, 1996. View at: Google Scholar
 T. Tamura, Y. Maeda, M. Sekine, and M. Yoshida, “Wearable photoplethysmographic sensors—past and present,” Electronics, vol. 3, no. 2, pp. 282–302, 2014. View at: Publisher Site  Google Scholar
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Copyright © 2018 Ludi Wang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.