| Literature DB >> 22163496 |
Rodrigo Pérez1, Úrsula Costa, Marc Torrent, Javier Solana, Eloy Opisso, César Cáceres, Josep M Tormos, Josep Medina, Enrique J Gómez.
Abstract
Here an inertial sensor-based monitoring system for measuring and analyzing upper limb movements is presented. The final goal is the integration of this motion-tracking device within a portable rehabilitation system for brain injury patients. A set of four inertial sensors mounted on a special garment worn by the patient provides the quaternions representing the patient upper limb's orientation in space. A kinematic model is built to estimate 3D upper limb motion for accurate therapeutic evaluation. The human upper limb is represented as a kinematic chain of rigid bodies with three joints and six degrees of freedom. Validation of the system has been performed by co-registration of movements with a commercial optoelectronic tracking system. Successful results are shown that exhibit a high correlation among signals provided by both devices and obtained at the Institut Guttmann Neurorehabilitation Hospital.Entities:
Keywords: biomechanical model; inertial sensors; motion tracking; neurorehabilitation; upper limb
Mesh:
Year: 2010 PMID: 22163496 PMCID: PMC3231046 DOI: 10.3390/s101210733
Source DB: PubMed Journal: Sensors (Basel) ISSN: 1424-8220 Impact factor: 3.576
Figure 1.Schematic view of the motion capture system.
Figure 2.System integration box.
Figure 3.Robot manipulator approach.
Figure 4.Schematic view of the inertial sensor location.
Figure 5.Marker model.
Figure 6.Serving water from a jar ADL setup.
Figure 7.Calibration setup.
Figure 8.Test garment along with BTS markers for co-registration.
Figure 9.Synchronization signals.
Results of pure movement co-registrations.
| 0.997 | 13.2 | |
| 0.992 | 13.6 | |
| 0.994 | 13.4 | |
| 0.895 | 13.6 | |
| 0.842 | 20.9 | |
| 0.718 | 17.25 | |
| 0.994 | 61 | |
| 0.995 | 59.9 | |
| 0.995 | 60.45 | |
| 0.992 | 10 | |
| 0.976 | 1.6 | |
| 0.984 | 5.8 | |
| 0.962 | 24.5 | |
| 0.974 | 23.7 | |
| 0.968 | 24.1 | |
| 0.980 | 10.8 | |
| 0.995 | 12.5 | |
| 0.987 | 11.65 |
Results of serving from a jar co-registrations.
| 0.998 | 13.5 | 0.905 | 6.3 | 0.849 | 28 | 0.980 | 18.8 | 0.960 | 10.6 | 0.960 | 25.7 | |
| 0.992 | 14.6 | 0.909 | 8.5 | 0.884 | 27.2 | 0.982 | 17 | 0.840 | 13.3 | 0.897 | 27.2 | |
| 0.995 | 13.8 | 0.895 | 7.8 | 0.830 | 28.1 | 0.977 | 19.3 | 0.956 | 10.8 | 0.916 | 26.1 | |
| 0.995 | 14.2 | 0.909 | 7 | 0.877 | 29.3 | 0.977 | 18.8 | 0.942 | 11.4 | 0.897 | 29.8 | |
| 0.996 | 13 | 0.921 | 7.6 | 0.824 | 31.8 | 0.980 | 19.1 | 0.927 | 12.4 | 0.948 | 25.6 | |
| 0.995 | 13.82 | 0.908 | 7.44 | 0.853 | 28.88 | 0.979 | 18.6 | 0.925 | 11.7 | 0.924 | 26.88 | |
Results after calibration for pure internal rotation movements.
| 0.998 | 0.27 | 60.9 | |
| 0.996 | 0.81 | 59.9 | |
| 0.997 | 0.54 | 60.4 |
Figure 10.Transfer function that models test garment noise (modeled with a second-order polynomial function).
Figure 11.(a) Internal rotation signals provided by both systems after calibration. (b) Internal rotation signals provided by both systems without calibration.