# Optimization of an Accelerometer and Gyroscope-Based Fall Detection Algorithm

Authors: Quoc T. Huynh; Uyen D. Nguyen; Lucia B. Irazabal; Nazanin Ghassemian; Binh Q. Tran
Journal: Journal of Sensors
 (2015)

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## Abstract

Falling is a common and significant cause of injury in elderly adults (>65 yrs old), often leading to disability and death. In the USA, one in three of the elderly suffers from fall injuries annually. This study’s purpose is to develop, optimize, and assess the efficacy of a falls detection algorithm based upon a wireless, wearable sensor system (WSS) comprised of a 3-axis accelerometer and gyroscope. For this study, the WSS is placed at the chest center to collect real-time motion data of various simulated daily activities (i.e., walking, running, stepping, and falling). Tests were conducted on 36 human subjects with a total of 702 different movements collected in a laboratory setting. Half of the dataset was used for development of the fall detection algorithm including investigations of critical sensor thresholds and the remaining dataset was used for assessment of algorithm sensitivity and specificity. Experimental results show that the algorithm detects falls compared to other daily movements with a sensitivity and specificity of 96.3% and 96.2%, respectively. The addition of gyroscope information enhances sensitivity dramatically from results in the literature as angular velocity changes provide further delineation of a fall event from other activities that may also experience high acceleration peaks.


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## Body

## 1. Introduction

Fall events are the most significant cause of injury in the elderly. Falls result in many disabling fractures that could eventually lead to death due to complications such as infection or pneumonia. In the United States, more than one-third of elderly people over 65 years old fall at least once per year [1]. In 2008, hospital emergency rooms treated over 2.1 million nonfatal fall injuries among older adults of which 25% were hospitalized. Unfortunately, with age, chances of falling increases and injuries are exacerbated. Injuries due to falls for those over 85 years old were four times greater than in adults aged 65 to 74. Further, once a person falls, they are likely to fall again.While falls in the elderly have a direct health effect, another key effect is related to financial costs associated with the incident. In 2000, costs associated with falls in the elderly were estimated by the CDC to be approximately $20 billion and to increase to $54.9 billion by 2020 [2]. Half of elderly fallers are not able to get up by themselves [3]. On average, elderly fallers lie helplessly for more than 10 minutes with 3% waiting for more than one hour before receiving assistance [4]. Theselong lies often result in hospitalizations, institutionalization, and high morbidity-mortality rates. Research by Bertera et al. [5] has shown that the elderly are interested in new technologies that support their health, independence, and safety, especially as it supports their desire to age-in-place [6].Personal Emergency Response Systems (PERS) have been developed to facilitate calling for help after a fall event. However, in severe cases of an emergency, the individual may not be able to activate the PERS alarm. Recent reports show that 80% of elderly persons who were unable to get up after a fall did not use their PERS device to call for help [7, 8]. For this reason, automatic fall detection is an active area of research. Many falls research strategies using accelerometers primarily utilize changes in acceleration magnitude to determine falls. When the acceleration exceeds a critical threshold, the fall is detected [9, 10]. These systems successfully detect falls with sensitivities greater than 85% and specificities between 88 and 94%. However, focusing only on large acceleration can result in many false positives as other activities such as sitting, running, and jumping may also result in large peak accelerations. For example, Huynh et al. [11] have shown that average peak acceleration during running (2.3–2.8 g) overlaps with the range observed during falls (2.4–5.4 g). This overlap reduces the specificity (i.e., detection of false positives) of purely accelerometer-based algorithms.Other fall detection algorithms rely on detection of body orientation (i.e., prone) after a fall. However, these strategies may be affected by activities with similar postures (i.e., sleeping, reclining) and are less effective when a person’s fall posture is not horizontal. Furthermore, additional studies have used complex algorithms such as support vector machine (SVM) [12] and Markov models [13] to detect falls. The robustness of these systems has not been demonstrated. They are also limited by excessive use of computational resources and cannot respond in real-time. While computational complexities can potentially be offloaded to cloud-based services, real-time and continuous access to the cloud may be unreliable especially in rural communities.Unlike other prior works, this project proposes using a combination of accelerometer and gyroscope sensors for robust fall detection. While the accelerometer provides valuable information regarding body inertial changes due to impact, the gyroscope provides unique information regarding the body’s rotational velocity during a fall event. A fall event produces both high acceleration and angular velocity, the combination of which is not observed during normal daily activities. The thrust of this work is to develop and optimize an algorithm for robust fall detection while simultaneously optimizing sensitivity and specificity.


## 2. Methodology

In prior studies [11], our team has developed a wireless sensor system and an algorithm to identify fall events from other daily activities such as walking, running, sitting, and climbing stairs. The system includes a wireless sensor system (WSS) comprised of a 3-axis accelerometer and gyroscope. Figure 1 shows the overall schematic of system. The WSS transmits and receives real-time accelerometer and gyro data during the fall. The detection algorithm is based on a simple threshold detection method using accelerometer thresholds found in the literature. Gyroscope threshold was determined experimentally using preliminary data collected.Figure 1
The schematic of wireless sensors system.


### 2.1. Wireless Sensor System (WSS)

The wireless sensor system (Figure2) contains a sensor module (Figure 2(a)), Micro Control Unit (MCU), and Wi-Fi module to sense body orientation and activity data, control data flow, and transmit/receive data, respectively. The WSS is placed at the center of chest (Figure 2(c)).Figure 2
Fall detection system: (a) sensor module (6 DOF), (b) wireless sensor system (WSS), (c) system attached on center chest.
(a)
(b)
(c)


#### 2.1.1. Sensor Module

Since our system uses both acceleration and angular velocity to detect falls, we choose to use the 6-DOF module with small size and power requirements. It includes a triaxial accelerometer ADXL345 and a triaxial gyroscope ITG3200 (Figure2(a)). Acceleration measurement range of ADXL345, with 13-bit resolution and 4 mg/LSB, is up to ±16 g. Additionally, the ITG-3200 gyroscope can capture the angular velocity between ±2000°/sec. Both sensors are connected with the MCU via I2C digital interface port.


#### 2.1.2. Micro Control Unit (MCU) Module

The MCU for the control system is an LPC 1786 (NXP semiconductors), an ARM Cortex-M3 32-bit based microcontroller specifically designed for embedded applications requiring a high level of integration and low power dissipation. The chip can operate up to 100 MHz CPU frequency. In addition, the UART interface provides the sampling frequency up to 4 Mb/s.


#### 2.1.3. Wireless Module

The Wifly RN131 module is a stand-alone Wi-Fi module operating at a fully integrated 2.4 GHz and providing an IP stack with IEEE 802.11 b/g standard. The RN131 can operate with communication speed up to 11 Mbps. Due to its small form factor and extremely low power consumption, it is perfect for mobile wireless applications with portable battery operated devices. Additionally, its UART hardware interfaces for connecting with MCU can operate up to 1 Mbps data rate.


#### 2.1.4. Collection Program

The data collection program is written in Matlab (Mathworks, Inc., Natick, MA) to receive, display, and analyze real-time acceleration and angular velocity data from the WSS [11]. The program also stores data for later analyses.


### 2.2. Fall Detection Algorithm

The parameters used in analyses are similar to those proposed in previous studies [10, 14]. The total sum acceleration vector, Acc, containing both static and dynamic acceleration components, is calculated from sampled data using(1)Acc=(Ax)2+(Ay)2+Az2,where Ax, Ay, and Az are the accelerations (g) in the x, y, and z directions. Similarly, angular velocity is calculated from sampled data as indicated in the following:(2)ω=(ωx)2+(ωy)2+ωz2,where ωx, ωy, and ωz are angular velocities in x, y, and z directions.When stationary, the acceleration magnitude, Acc, from triaxial accelerometer is constant (+1 g), and angular velocity is 0°/s. When the subject falls, the acceleration is rapidly changing and the angular velocity produces a variety of signals along fall direction. Critical thresholds in the acceleration and angular velocity are then used for determining a fall event. These critical thresholds are defined and derived as follows [15].(i)
Lower fall threshold (LFT): local minima for the Acc resultant of each recorded activity are referred to as the signal lower peak values (LPVs). The LFTacc for the acceleration signals is set at the level of the smallest magnitude lower fall peak (LFP) recorded.(ii)
Upper fall threshold (UFT): local maxima for the Acc resultant of each recorded activity are referred to as the signal upper peak values (UPVs). The UFT for each of the acceleration (UFTacc) and the angular velocity (UFTgyro) signals are set at the level of the lowest upper fall peak (UFP) recorded for the Acc and ω, respectively. The UFTacc is related to the peak impact force experienced by the body segment during the impact phase of the fall.Fall detection algorithms using accelerometers are normally divided into two groups, one based onLFTacc comparison and the other based on UFTacc comparison. Although past research has achieved some significant results, accuracy of these strategies is still below desired levels. Bourke et al. [15] used LFTacc and UFTacc and found the sensitivity and specificity of performance to be 83.33% and 67.08%, respectively.In this study, we use bothLFTacc and UFTacc in combination with the UFTgyro for fall detection. We determine the LFT and UFT for both the acceleration and angular velocity based on collected experimental data. Our proposed algorithm is shown in Figure 3. First, the instantaneous acceleration magnitude, Acc, is computed and compared to the LFTacc. When Acc falls below the LFTacc threshold, data from the next 0.5 s, period referred to as fall window, is compared to the UFT for both the acceleration and angular velocity vector. The fall window period was obtained from the literature [16, 17]. Within the fall window, if both magnitudes of acceleration and angular velocity are above the UFTacc and UFTgyro, respectively, then a fall is detected. If only one or neither is observed, a fall is not indicated.Figure 3
Combined accelerometer and gyroscope detection schema.Robustness of the proposed algorithm is evaluated by measuring sensitivity and specificity typically defined as(3)Sensitivity=No.TPNo.TP+No.FN,Specificity=No.TNNo.TN+No.FP,where the following happen.(i)
# True positive (No.TP): fall occurs; device detects it.(ii)
# False positive (No.FP): device detects fall; fall did not occur.(iii)
# True negative (No.TN): normal movement (i.e., no fall); device does not declare a fall.(iv)
# False negative (No.FN): fall occurs; device does not detect it.Difficulty lies in determining the optimal thresholds for LFTacc, UFTacc, and UFTgyro. Improperly low threshold selection may lead to increased occurrences of false positives detected during daily activities, resulting in lower specificity. Alternatively, too stringent threshold selection may cause failure of fall detection altogether leading to increased false negatives and decreased system sensitivity.Many algorithms determine the thresholds experimentally [18]. Likewise, this study determines these thresholds for optimal sensitivity and specificity. To optimize thresholds, sensitivity and specificity are calculated for all possible thresholds values from experimental data. The sensitivity is inversely related with specificity in the sense that sensitivity increases as specificity decreases across various thresholds. The receiver operating characteristic (ROC; Figure 4) curve displays the tradeoff between the sensitivity (y-axis) and specificity (x-axis). The optimal threshold is the point that can provide the minimum distance between the point (0, 1) and itself [19]. The distance is defined in (4), where SN, SP are the sensitivity and specificity, respectively, as follows:(4)dT=1-SN2+SP2.Figure 4
The ROC curve. Optimal threshold shown as minimum distance,d, to point (0, 1) where sensitivity (SN) and specificity (SP) are 100% and 100%, respectively. False positive rate equals 1 − specificity as an algorithm that results in 100% false positive has 0% specificity and one that has 0% false positive rate results in 100% specificity.


### 2.3. Experimental and Procedure

To collect falls data for development and optimization of the falls algorithm, experiments were performed on 27 young healthy subjects (male and female, age from 18 to 28 years, weight from 50 to 90 kg, and height from 154.5 to 180.0 cm) and 9 middle-age subjects (age from 38 to 56 years, weight from 55 to 87 kg, and height from 160.0 to 185.0 cm) at The Catholic University of America (Washington, DC). The research protocol was approved by the Human Subjects/Institutional Review Board (IRB) Committee. The WSS was attached to the center of the chest of each subject, determined as optimal location by our previous study [20]. Each subject was asked to perform movements such as standing, walking, sitting down/standing up, step, and run and 4 different falls tests, forward, backward, and right/left sideway fall. Falls were conducted onto a 36-inch high jump cushion to prevent injury.


## 2.1. Wireless Sensor System (WSS)

The wireless sensor system (Figure2) contains a sensor module (Figure 2(a)), Micro Control Unit (MCU), and Wi-Fi module to sense body orientation and activity data, control data flow, and transmit/receive data, respectively. The WSS is placed at the center of chest (Figure 2(c)).Figure 2
Fall detection system: (a) sensor module (6 DOF), (b) wireless sensor system (WSS), (c) system attached on center chest.
(a)
(b)
(c)


### 2.1.1. Sensor Module

Since our system uses both acceleration and angular velocity to detect falls, we choose to use the 6-DOF module with small size and power requirements. It includes a triaxial accelerometer ADXL345 and a triaxial gyroscope ITG3200 (Figure2(a)). Acceleration measurement range of ADXL345, with 13-bit resolution and 4 mg/LSB, is up to ±16 g. Additionally, the ITG-3200 gyroscope can capture the angular velocity between ±2000°/sec. Both sensors are connected with the MCU via I2C digital interface port.


### 2.1.2. Micro Control Unit (MCU) Module

The MCU for the control system is an LPC 1786 (NXP semiconductors), an ARM Cortex-M3 32-bit based microcontroller specifically designed for embedded applications requiring a high level of integration and low power dissipation. The chip can operate up to 100 MHz CPU frequency. In addition, the UART interface provides the sampling frequency up to 4 Mb/s.


### 2.1.3. Wireless Module

The Wifly RN131 module is a stand-alone Wi-Fi module operating at a fully integrated 2.4 GHz and providing an IP stack with IEEE 802.11 b/g standard. The RN131 can operate with communication speed up to 11 Mbps. Due to its small form factor and extremely low power consumption, it is perfect for mobile wireless applications with portable battery operated devices. Additionally, its UART hardware interfaces for connecting with MCU can operate up to 1 Mbps data rate.


### 2.1.4. Collection Program

The data collection program is written in Matlab (Mathworks, Inc., Natick, MA) to receive, display, and analyze real-time acceleration and angular velocity data from the WSS [11]. The program also stores data for later analyses.


## 2.1.1. Sensor Module

Since our system uses both acceleration and angular velocity to detect falls, we choose to use the 6-DOF module with small size and power requirements. It includes a triaxial accelerometer ADXL345 and a triaxial gyroscope ITG3200 (Figure2(a)). Acceleration measurement range of ADXL345, with 13-bit resolution and 4 mg/LSB, is up to ±16 g. Additionally, the ITG-3200 gyroscope can capture the angular velocity between ±2000°/sec. Both sensors are connected with the MCU via I2C digital interface port.


## 2.1.2. Micro Control Unit (MCU) Module

The MCU for the control system is an LPC 1786 (NXP semiconductors), an ARM Cortex-M3 32-bit based microcontroller specifically designed for embedded applications requiring a high level of integration and low power dissipation. The chip can operate up to 100 MHz CPU frequency. In addition, the UART interface provides the sampling frequency up to 4 Mb/s.


## 2.1.3. Wireless Module

The Wifly RN131 module is a stand-alone Wi-Fi module operating at a fully integrated 2.4 GHz and providing an IP stack with IEEE 802.11 b/g standard. The RN131 can operate with communication speed up to 11 Mbps. Due to its small form factor and extremely low power consumption, it is perfect for mobile wireless applications with portable battery operated devices. Additionally, its UART hardware interfaces for connecting with MCU can operate up to 1 Mbps data rate.


## 2.1.4. Collection Program

The data collection program is written in Matlab (Mathworks, Inc., Natick, MA) to receive, display, and analyze real-time acceleration and angular velocity data from the WSS [11]. The program also stores data for later analyses.


## 2.2. Fall Detection Algorithm

The parameters used in analyses are similar to those proposed in previous studies [10, 14]. The total sum acceleration vector, Acc, containing both static and dynamic acceleration components, is calculated from sampled data using(1)Acc=(Ax)2+(Ay)2+Az2,where Ax, Ay, and Az are the accelerations (g) in the x, y, and z directions. Similarly, angular velocity is calculated from sampled data as indicated in the following:(2)ω=(ωx)2+(ωy)2+ωz2,where ωx, ωy, and ωz are angular velocities in x, y, and z directions.When stationary, the acceleration magnitude, Acc, from triaxial accelerometer is constant (+1 g), and angular velocity is 0°/s. When the subject falls, the acceleration is rapidly changing and the angular velocity produces a variety of signals along fall direction. Critical thresholds in the acceleration and angular velocity are then used for determining a fall event. These critical thresholds are defined and derived as follows [15].(i)
Lower fall threshold (LFT): local minima for the Acc resultant of each recorded activity are referred to as the signal lower peak values (LPVs). The LFTacc for the acceleration signals is set at the level of the smallest magnitude lower fall peak (LFP) recorded.(ii)
Upper fall threshold (UFT): local maxima for the Acc resultant of each recorded activity are referred to as the signal upper peak values (UPVs). The UFT for each of the acceleration (UFTacc) and the angular velocity (UFTgyro) signals are set at the level of the lowest upper fall peak (UFP) recorded for the Acc and ω, respectively. The UFTacc is related to the peak impact force experienced by the body segment during the impact phase of the fall.Fall detection algorithms using accelerometers are normally divided into two groups, one based onLFTacc comparison and the other based on UFTacc comparison. Although past research has achieved some significant results, accuracy of these strategies is still below desired levels. Bourke et al. [15] used LFTacc and UFTacc and found the sensitivity and specificity of performance to be 83.33% and 67.08%, respectively.In this study, we use bothLFTacc and UFTacc in combination with the UFTgyro for fall detection. We determine the LFT and UFT for both the acceleration and angular velocity based on collected experimental data. Our proposed algorithm is shown in Figure 3. First, the instantaneous acceleration magnitude, Acc, is computed and compared to the LFTacc. When Acc falls below the LFTacc threshold, data from the next 0.5 s, period referred to as fall window, is compared to the UFT for both the acceleration and angular velocity vector. The fall window period was obtained from the literature [16, 17]. Within the fall window, if both magnitudes of acceleration and angular velocity are above the UFTacc and UFTgyro, respectively, then a fall is detected. If only one or neither is observed, a fall is not indicated.Figure 3
Combined accelerometer and gyroscope detection schema.Robustness of the proposed algorithm is evaluated by measuring sensitivity and specificity typically defined as(3)Sensitivity=No.TPNo.TP+No.FN,Specificity=No.TNNo.TN+No.FP,where the following happen.(i)
# True positive (No.TP): fall occurs; device detects it.(ii)
# False positive (No.FP): device detects fall; fall did not occur.(iii)
# True negative (No.TN): normal movement (i.e., no fall); device does not declare a fall.(iv)
# False negative (No.FN): fall occurs; device does not detect it.Difficulty lies in determining the optimal thresholds for LFTacc, UFTacc, and UFTgyro. Improperly low threshold selection may lead to increased occurrences of false positives detected during daily activities, resulting in lower specificity. Alternatively, too stringent threshold selection may cause failure of fall detection altogether leading to increased false negatives and decreased system sensitivity.Many algorithms determine the thresholds experimentally [18]. Likewise, this study determines these thresholds for optimal sensitivity and specificity. To optimize thresholds, sensitivity and specificity are calculated for all possible thresholds values from experimental data. The sensitivity is inversely related with specificity in the sense that sensitivity increases as specificity decreases across various thresholds. The receiver operating characteristic (ROC; Figure 4) curve displays the tradeoff between the sensitivity (y-axis) and specificity (x-axis). The optimal threshold is the point that can provide the minimum distance between the point (0, 1) and itself [19]. The distance is defined in (4), where SN, SP are the sensitivity and specificity, respectively, as follows:(4)dT=1-SN2+SP2.Figure 4
The ROC curve. Optimal threshold shown as minimum distance,d, to point (0, 1) where sensitivity (SN) and specificity (SP) are 100% and 100%, respectively. False positive rate equals 1 − specificity as an algorithm that results in 100% false positive has 0% specificity and one that has 0% false positive rate results in 100% specificity.


## 2.3. Experimental and Procedure

To collect falls data for development and optimization of the falls algorithm, experiments were performed on 27 young healthy subjects (male and female, age from 18 to 28 years, weight from 50 to 90 kg, and height from 154.5 to 180.0 cm) and 9 middle-age subjects (age from 38 to 56 years, weight from 55 to 87 kg, and height from 160.0 to 185.0 cm) at The Catholic University of America (Washington, DC). The research protocol was approved by the Human Subjects/Institutional Review Board (IRB) Committee. The WSS was attached to the center of the chest of each subject, determined as optimal location by our previous study [20]. Each subject was asked to perform movements such as standing, walking, sitting down/standing up, step, and run and 4 different falls tests, forward, backward, and right/left sideway fall. Falls were conducted onto a 36-inch high jump cushion to prevent injury.


## 3. Results

Figure5 shows a typical example of the acceleration and angular velocity signals while performing different daily activities. Corresponding instances when the acceleration and angular velocity values exceed LFTacc, UFTacc, and UFTgyro during the various daily activities such as standing, running, sitting up, lying down, walking, stepping, and falling are also shown below the raw signals. During a fall event (~10 sec), the acceleration signal decreases from 1 g to cross below LFTacc and, within 0.5 s, acceleration and angular velocity increase to cross above UFTacc and UFTgyro, almost simultaneously. With rigorous activities such as running, the peak of accelerations can reach critical LFTacc and UFTacc thresholds indicative of a fall event. However, the confirmatory UFTgyro threshold is never reached. For events such as lying down or sitting up, the UFTgyro threshold is triggered, but the acceleration conditions are not met. Thus, the combination accelerometer and gyroscope sensor system complement one another for a more robust fall detection algorithm.Figure 5
Display of Acc andω for various activities: standing, running, sitting up, lying down, standing up, walking up steps, and falling. Also shown are the thresholds for UFTacc, LFTacc, and UFTgyro to determine a fall event. Lastly, events detected that satisfy each of the algorithm components are shown at the bottom. A fall event is denoted when all 3 thresholds are detected within the fall window.From the experimental data collected, a subset of the data (18 subjects) is analyzed to identifyLFTacc and UFTacc of acceleration and UFTgyro of angular velocity. After that, the remaining data is used for validation to determine the sensitivity and specificity of the algorithm. The mean and standard deviation values of minimum and maximum of acceleration and maximum of angular velocity are statistically for 90% and 99% confidence levels. Table 1 shows the mean and standard error for LFTacc, UFTacc, and UFTgyro as well as values for 90% and 99% upper and lower confidence levels.Table 1
Summary of critical threshold values for LFTacc, UFTacc, and UFTgyro including mean ± standard error, threshold values at upper and lower 90% confidence limits and at 99% upper and lower confidence limit.
LFTacc (g)
UFTacc (g)
UFTgyro (°/s)
Mean ± standard error
0.18 ± 0.06
3.27 ± 0.38
382.1 ± 98.9
Lower 90% limit
0.10
2.77
254.52
Upper 90% limit
0.27
3.76
509.61
Lower 99% limit
0.03
2.37
151.69
Upper 99% limit
0.33
4.16
612.43To improve system accuracy, theupper confidence limit between 90% and 99% (0.27 g–0.33 g) for LFTacc and thelower confidence limit between 90% and 99% (2.37 g–2.77 g) of UFTacc and UFTgyro (151.7–254.5°/s) are used for the fall detection algorithm. To optimize the thresholds used for the final algorithm, the proposed algorithm is run at different levels for the ranges specified of LFTacc, UFTacc, and UFTgyro and sensitivity and specificity values are calculated for the combined algorithm. Figure 6 shows a spatial mapping of sensitivity and specificity of system in the range of LFTacc (0.2 g–0.4 g) and UFTacc (2 g-3 g) of acceleration. As expected, there is a tradeoff between sensitivity and specificity with sensitivity increasing while specificity decreases, and vice versa. The optimized algorithm simultaneously maximizes both measures.Figure 6
Graphical relationship between sensitivity and specificity with varying values ofLFTacc and UFTacc.Because this study’s goal is to develop a fall detection system with targeted accuracy over 90% for both sensitivity and specificity, three thresholds were initially chosen ofLFTacc, UFTacc, and UFTgyro 0.26 g, 2.77 g, and 254.5°/s, respectively, based upon individual analyses from experimental data. Each threshold is then varied for the ranges above and sensitivity and specificity are calculated. From the ROC curves, the optimal threshold is chosen which minimizes distance d in Figure 4.Figure7 shows the sensitivity versus threshold values for (a) UFTgyro, (b) LFTacc, and (c) UFTacc, respectively, and the corresponding ROC curves ((d)–(f)). The optimal threshold for correctly identifying a fall or nonfall is determined by minimizing distance d in the ROC curves. For angular velocity (Figures 7(a) and 7(d)), this minimized distance d is 0.063 and occurs when UFTgyro is 240°/s, corresponding to sensitivity of 95.5% and specificity of 97.1% (100% − specificity = 2.9%). Similarly, Figures 7(b) and 7(e) represent the change of the sensitivity and specificity and ROC curves when LFTacc is varied. The minimized distance dT is 0.062 corresponding to an LFT range between 0.30 g and 0.35 g and results in 96% sensitivity and 95% specificity. Lastly, Figures 7(c) and 7(f) show the optimal UFTacc threshold (dT=0.059) of 2.4 g with corresponding sensitivity and specificity values of 94.9% and 97.5%, respectively.Figure 7
Representative curves of sensitivity versus threshold values (1st row) for (a)UFTgyro, (b) LFTacc, and (c) UFTacc and corresponding ROC curves (2nd row; (d)–(f)). Minimum distance point, d, is shown in each ROC curve with sensitivity (~95%).
(a)
(b)
(c)
(d)
(e)
(f)Table2 provides a summary of results for fall sensitivity and specificity without (i.e., accelerometer only) and with inclusion of gyroscope information. In this table, critical thresholds for LFT and UFT are set at two confidence levels, 90% and 99%. Since thresholds are set to desired confidence levels, no optimization strategy is implemented. Results show increasing confidence level from 90% to 99% increases sensitivity from 83.56% to 98.75%, as expected, while dramatically decreasing specificity (from 96.12% to 75.93%) of accelerometer only algorithms. These results are similar to findings by others [9, 10]. Addition of gyroscope information improves specificity by the ability to differentiate falls from other rigorous efforts. This is achieved with slightly diminished sensitivity compared to accelerometer only methods.Table 2
Fall algorithm sensitivity and specificitywithout and with gyroscope while critical thresholds are set at 90% and 99% confidence levels.
Accelerometerwithout gyro
Accelerometerwith gyro
Confidence level
90%
99%
90%
99%
Sensitivity
83.56%
98.75%
81.37%
96.55%
Specificity
96.12%
75.93%
99.38%
89.50%When critical thresholds are established and optimized using ROC analyses, one is able to achieve improved specificity while simultaneously achieving high levels of sensitivity for algorithms utilizing accelerometer only and with a combined accelerometer and gyroscope strategy (Table3). For the combined accelerometer and gyroscope sensor plus optimization strategy, sensitivity and specificity for fall detection were 96.3% and 96.2%, respectively.Table 3
Fall algorithm sensitivity and specificity without and with gyroscope with ROC optimization strategy implemented.
Accelerometerwithout gyro
Accelerometerwith gyro
Sensitivity
97.36%
96.3%
Specificity
82.72%
96.2%


## 4. Discussion

This study investigates a wireless sensor system that combines measures of acceleration and angular velocity of body to detect and differentiate falls from daily activities. In this study, 36 subjects performed four different types of falls as well as daily activities for a total of 9 different activities. Half the experimental dataset was used to develop and train the algorithm and to determine critical thresholds, while the other half was used to validate and test the final fall detection algorithm.Tolkiehn et al. [21] reported results of an accelerometer only algorithm of 83.3% sensitivity and 79.1% specificity to detect falls. Chen et al. [22] reported achieving 94% specificity with their fall detection algorithm, but with low sensitivity (76%). Bourke et al. [23] recently proposed an algorithm with high sensitivity (97%), but with a cost of lower specificity (83%). Others have shown similar tradeoff between achieving high specificity [88–94%] and decreased detection of falls (sensitivity = 85%) [9, 10, 24].In this study, following an optimization schema using ROC curves and iterative analyses of sensitivity and specificity, we were able to determine critical thresholds forLFTacc, UFTacc, and UFTgyro that simultaneously result in high sensitivity and specificity of fall detection. These optimized values were 0.30 g–0.35 g, 2.4 g, and 240°/s, respectively. Results demonstrate the effectiveness of the combinedaccelerometer with gyroscope algorithm that is optimized for sensitivity and specificity compared to traditionalaccelerometer only strategies of fall detection. The optimized, combined sensor schema achieves both high sensitivity (96.3%) and high specificity (96.3%), simultaneously, much higher than prior results reported in the literature. The increased sensitivity is achieved by inclusion of gyroscope information which provides valuable additional information on body rotation in order to differentiate a fall event from other high impact activities such as running and jumping. The optimization strategy results in dramatic increases in specificity while only slightly sacrificing fall detection sensitivity.The addition of gyroscope information reduces the occurrence of false positives resulting from rigorous activities such as running and jumping. While these activities produce high acceleration peaks similar to a fall, rotational angular velocities are much lower than seen in fall events and therefore are not triggered by the proposed algorithm. The inclusion of a check for body angular velocity threshold dramatically improves specificity from 82.72% without gyroscope to 96.2% with gyroscope. As there is a tradeoff between sensitivity and specificity, optimization of key thresholds via ROC analyses provides a systematic strategy for maximizing both sensitivity and specificity simultaneously.


## 5. Conclusion and Future Work

Fall detection is an important focus area in elderly care and greatly affects health, wellness, and disability. In this study, an optimized fall detection algorithm was developed using acceleration and angular velocity data collected from a wireless sensor system located in the center chest. Using an optimization approach, critical thresholds are determined through this work that results in robust fall detection. The optimized algorithm was able to detect falls with high sensitivity (96.3%) and specificity (96.2%) compared to prior strategies by other researchers who were able to achieveeither high sensitivityor high specificity, but not both. The methodological approach followed in this effort also provides a systematic approach to selection of critical thresholds for fall detection that simultaneously optimizes both sensitivity and specificity. The proposed method is a simple threshold method and, therefore, is easy to port to wearable, electronic devices or inclusion in other mobile health platforms.One limitation of this study is that the thresholds and algorithms were developed using data obtained from young healthy subjects and, for safety reasons, in a laboratory setting falling onto a cushioned mat. We expect that actual data from elderly individuals falling onto normal hard floors would experience higher peak accelerations and potentially higher angular velocities as these falls would be unexpected. Therefore, we expect theLFTacc, UFTacc, and UFTgyro threshold values from this work would still apply for real-world scenarios. While the system may be effective in detection of falls, it may be less effective in detection ofnear falls another clinically important area of falls research.The system proposed herein is for a dedicated, wearable fall detection sensor system. Integration and deployment of the algorithm onto a smartphone, smartwatch device, or other mobile communication systems would be beneficial not only in detection of a fall, but also in alerting caregivers and other providers to the fall event. In these instances, the critical thresholds for the detection algorithm require further study. We and others have shown peak acceleration measures during a fall event vary considerably with position on the body [16, 20]. Regardless, the proposed strategy of combining accelerometer and gyroscope measures is still expected to result in a robust fall detection algorithm.



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*Source: 452078-2015-04-09.xml*