2022
DOI: 10.3390/s22207784
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A Review of Recent Advances in Vital Signals Monitoring of Sports and Health via Flexible Wearable Sensors

Abstract: In recent years, vital signals monitoring in sports and health have been considered the research focus in the field of wearable sensing technologies. Typical signals include bioelectrical signals, biophysical signals, and biochemical signals, which have applications in the fields of athletic training, medical diagnosis and prevention, and rehabilitation. In particular, since the COVID-19 pandemic, there has been a dramatic increase in real-time interest in personal health. This has created an urgent need for f… Show more

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Cited by 35 publications
(21 citation statements)
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“…Electrocardiography (ECG) and heart rate (HR) are the main signals used to evaluate cardiac status during sport [ 7 ]. The ECG represents cardiac electrical activity and HR is the number of times the heart beats within a one-minute period [ 8 ].…”
Section: Introductionmentioning
confidence: 99%
“…Electrocardiography (ECG) and heart rate (HR) are the main signals used to evaluate cardiac status during sport [ 7 ]. The ECG represents cardiac electrical activity and HR is the number of times the heart beats within a one-minute period [ 8 ].…”
Section: Introductionmentioning
confidence: 99%
“…Sensors that monitor bioelectrical signals, motion data and biochemical markers play an important role in the management of personal health. It has become possible to monitor vital signs thanks to the development of various flexible wearable sensors (Anikwe et al , 2022; Koydemir and Ozcan, 2018; Sun et al , 2022). Inertial sensors are partnered with flexible wearable strain sensors to improve training outcomes and minimize injuries during physical activity.…”
Section: Introductionmentioning
confidence: 99%
“…In case of fibers, the ideal geometry is cylindrical with radial m, the rubber elasticity converting any tensile strain 𝜖 zz = ΔL L * > 0 along the fiber (the ẑ-direction; the original fiber length is L * and the length change ΔL) into a compression of the radius r and thus of p, giving a blue shift of 𝜆 0 away from its relaxed-state maximum value 𝜆 * 0 . [15] The Bragg reflection takes place symmetrically around the 𝜆 given by Equation (1) over a bandwidth equal to Δ𝜆 = pΔn nh (2) where Δn nh is the birefringence in the absence of helix (nh: nonhelical). A decrease in p, as expected if ϵ zz > 0, thus leads not only to a reduction in 𝜆 0 but also to a narrowing of the reflection band.…”
Section: Introductionmentioning
confidence: 99%