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Article

Energetics of a Novel 3D-Printed Custom Ankle Foot Orthosis in a Population of Individuals with Foot Drop: A Pilot Study

1
Movement Analysis Laboratory and Functional Evaluation of Prostheses, IRCCS Istituto Ortopedico Rizzoli, Via di Barbiano 1/10, 40136 Bologna, Italy
2
Medical Technology Laboratory, IRCCS Istituto Ortopedico Rizzoli, Via di Barbiano 1/10, 40136 Bologna, Italy
3
Independent Researcher, 41126 Modena, Italy
4
CRP Technology, Via Cesare della Chiesa 150/C, 41126 Modena, Italy
5
Department of Information Engineering, University of Padova, Via G. Gradenigo 6/A, 35131 Padova, Italy
*
Author to whom correspondence should be addressed.
Appl. Sci. 2025, 15(11), 5885; https://doi.org/10.3390/app15115885
Submission received: 25 February 2025 / Revised: 30 April 2025 / Accepted: 22 May 2025 / Published: 23 May 2025
(This article belongs to the Special Issue 3D Printing Technologies in Biomedical Engineering)

Abstract

Featured Application

This study provides quantitative evidence on the energetics of 3D-printed custom foot and ankle orthoses for people with foot drop. The outcome of this study highlights the consistency of the mechanical performance of 3D-printed orthoses.

Abstract

Passive Dynamic Ankle–Foot Orthoses (PD-AFOs) are medical devices prescribed to individuals with foot drop, a condition characterized by weakness of the ankle dorsiflexor muscles. PD-AFOs can store and release energy during the stance phase of the gait cycle, while supporting the foot in the swing phase. This study aimed at estimating the energetics of a novel fiberglass-reinforced polyamide custom PD-AFO in a population of mild foot drop patients. Eight PD-AFOs were designed and 3D-printed via selective laser sintering for eight participants with a unilateral foot drop condition. Lower limb kinematics and AFO flexion/extension were recorded during comfortable walking speed via skin marker-based stereophotogrammetry. The stiffness of each AFO was measured via an ad hoc experimental setup. The elastic work performed by the PD-AFO during gait was calculated as the dot product of the calf-shell resisting moment and the rotation angle. The average maximum energy stored by the calf-shell across all PD-AFOs was 0.013 ± 0.005 J/kg. According to this study, 3D-printed custom PD-AFOs made with fiberglass-reinforced polyamide can store some elastic energy, which is released to the ankle during push-off. Further studies should be conducted to assess the effect of this energy return mechanism in improving the gait of individuals with deficits of the ankle plantarflexor muscles.

1. Introduction

Passive Dynamic Ankle–Foot Orthoses (PD-AFOs) are assistive medical devices prescribed for individuals affected by neuro-muscular deficits of the ankle dorsiflexor muscles, usually associated with neurological conditions like cerebral palsy [1,2,3], stroke [4,5,6], and hemiplegia [7,8]. These orthoses aim at restoring physiological ankle kinematics and dynamics by supporting the foot of the affected limb, especially in the swing phase of walking. While standard AFOs are mainly designed to support the foot and ankle in the swing phase of walking, PD-AFOs can also address impairments and deficits of the ankle plantarflexor muscles by incorporating energy-storing and -returning mechanisms into their design. For this purpose, variable-stiffness mechanical springs or the high elastic properties of composite materials have been used to store energy and to mimic the physiological gait pattern [1,3,7,9,10,11]. This ability to store and return energy effectively reduces the reliance on muscle activation, leading to lower energy expenditure and improved gait efficiency. According to Bregman et al. [12], around a 10% decrease in energy cost can be achieved by walking with a PD-AFO. Brehm et al. [13] reported a significant 9% lower net non-dimensional energy cost of walking in a population of children walking with either a posterior leaf spring or a solid ankle–foot orthosis. In the systematic review by Daryabor et al. [14], four studies reported a significant reduction in total and net energy cost using different types of AFOs in people with stroke. Bleyenheuft et al. [15] reported an almost significant reduction in energy cost with either a posterior leaf spring or the articulated Chignon® orthosis during treadmill walking. A significant reduction in energy cost was also reported with a carbon-fiber AFO [16]. The mechanism behind these energy savings is attributed to the ability of PD-AFOs to optimize ankle kinematics and dynamics. PD-AFOs can effectively control ankle plantarflexion and dorsiflexion, reducing excessive ankle movements and promoting more natural gait patterns [17,18]. PD-AFOs can also enhance balance, reduce pain, and improve overall quality of life for individuals with gait impairments. Efficient and comfortable walking result in increased participation in activities of daily living and improved social engagement [19]. It should, though, be highlighted that outcome measures of energy expenditure often differ between studies and AFOs’ performance can be difficult to compare. Normalized oxygen consumption, either in mL/kg/m or mL/kg/min, normalized energy cost in J/kg/m, heart rate, and physiological cost index have all been used to quantify the energetic contribution of dynamic AFOs in different motor tasks. While the net energetic effect of dynamic AFOs is mostly calculated as the difference in energy consumption in gait between AFO and shod (no AFO) conditions, the actual energy stored and released due to the elastic deformation of the orthosis is seldom measured or reported [3].
The adoption of 3D printing technologies in the production of AFOs offers substantial advantages over traditional plaster casting and manual molding manufacturing methods. While the latter are inherently variable and time-consuming, 3D printing enables the creation of highly personalized orthoses through 3D scanning and 3D modeling tools. This digital workflow allows for precise replication of patient anatomy, leading to devices with improved fit and comfort and which can be tailored to individual patient needs [20]. Three-dimensionally printed AFOs have shown comparable or superior biomechanical and kinematic effects to conventional AFOs, including improvements in gait speed and foot plantar pressure [21,22]. The technology offers advantages such as design optimization, reduced labor and production costs, and weight savings [23]. Three-dimensional printing techniques such as fused deposition modeling and selective laser sintering allow for the creation of AFOs with mechanical properties similar to traditional carbon-fiber AFOs [23,24]. Higher satisfaction and comfort have been reported for 3D-printed AFOs compared to conventional ones, particularly in terms of weight and ease of use [21,22]. Furthermore, 3D printing facilitates rapid prototyping and design iterations, allowing for real-time adjustments based on patient feedback or clinical observations. This feature contrasts with the lengthy and iterative nature of traditional orthosis fabrication. The capacity for on-demand production and decentralized manufacturing also enhances accessibility, particularly in remote areas. Additionally, the ability to use a wide variety of materials allows for orthoses to be created with specific mechanical properties which can replicate or improve upon traditional AFOs [24]. The reduction in material waste and the ability to digitally store orthotic designs, thus reducing time and costs in case a replacement AFO is required, also allow for more efficient and less expensive orthotic care.
Recently, a novel 3D-printed PD-AFO made from fiberglass-reinforced polyamide has been developed for individuals with foot drop dissatisfied with off-the-shelf devices. This PD-AFO has been reported to improve gait parameters and ankle kinematics compared to no-AFO conditions and to be more comfortable than standard polypropylene leaf spring AFOs [17]. These AFOs can be individually dimensioned to achieve the desired stiffness and, due to the high properties of the polyamide-based composite material, the calf-shell can sustain large angular displacements without plastic deformation and without the need for torsion springs, e.g., as in [3]. Thus, it is plausible that some elastic energy can be stored and released in the stance phase of gait. While AFOs are designed primarily to prevent excessive plantarflexion during the swing phase, understanding PD-AFO energetics is crucial for optimizing design, especially when ankle plantarflexor muscles are compromised.
Therefore, this pilot study aimed to (1) investigate if any elastic energy is absorbed/released by the novel custom PD-AFO and (2) determine the timing of energy absorption/release during gait. In order to address these aims, the kinematics of the novel 3D-printed dynamic custom AFO were recorded in a population of individuals with foot drop during gait.

2. Materials and Methods

Eight custom PD-AFOs were designed and manufactured for a population of individuals (3F, 5M; age 62.0 ± 13.1 years, BMI 25.8 ± 2.5 kg/m2) affected by unilateral foot drop condition due to compression of the lumbosacral spine. Ethical approval was granted for the study by the local Ethical Committee (0016384, 23 December 2019) and informed consent was signed by all participants in the study.
In all participants, ankle dorsiflexor muscle strength was scored ≤3 according to the Medical Research Council (MRC) scale [25], whereas the ankle plantarflexor muscles strength was scored ≤4. With the exception of ankle dorsiflexion impairment, all participants showed good residual mobility in the affected limb (i.e., they were capable of walking without crutches or other walking aids albeit with compensations at the lower limb joints). The procedure for the design and production of the AFOs has been previously documented by the same authors [26]. In summary, the leg and foot of each participant were scanned in upright double-leg standing using a Kinect-based 3D scanner (Microsoft, Redmond, WA, US). The custom PD-AFOs were designed using Blender (version 4.4, https://www.blender.org/) and aligned to the 3D model of the leg and foot in weight bearing. Anatomical congruence was pursued at the foot plantar surface and at the calf shell to ensure comfort and proper fixation of the AFO to the leg. The calf-shell was aligned to the calf midline, as to be oriented along the anatomical axis of the patient’s tibia. The AFOs were manufactured via selective laser sintering of a fiberglass-reinforced polyamide powder (Windform® GT, CRP Technology, Modena, Italy). This 3D printing technology allows us to obtain parts with a resolution of about 0.1 mm. Since the stiffness of the present AFO is highly sensitive to the cross-section dimensions of the calf-shell, selective laser sintering is critical to the correct optimization of the AFO mechanical properties. The concave shape of the calf-shell increases the moment of inertia of the cross-section, allowing it to bend almost as a rigid body around the X-axis as in Figure 1b, which is designed to be close to the physiological ankle–joint axis [26]. The bending stiffness of the AFO calf-shell in anatomical plantarflexion ( k p) and dorsiflexion ( k d) were measured by applying a 15 deg rotation in both directions using a custom apparatus (Figure 1a) [27].
An 8-camera motion analysis system (Vicon, Oxford UK) was used to track the position of 20 reflective markers placed on relevant body landmarks of the pelvis, femur, tibia, and foot/footwear according to the IOR-gait protocol [28]. Three additional markers were placed on the posterior side of the calf-shell of each custom AFO (Figure 1b). This allowed measuring the relative plantarflexion ( α p) and dorsiflexion ( α d) angles of the AFO calf-shell with respect to the foot. The ISB recommended convention was used to calculate hip, knee, and ankle joint rotations and the AFO calf-shell flexion/extension in gait [29]. Ground reaction forces were sampled at 2000 Hz using two force plates embedded in the floor (Kistler, Winterthur, Switzerland). Ankle power was calculated using force plate and kinematic data and normalized to the participant’s body weight (W/kg). Five walking trials at self-selected speed were recorded for each participant in three conditions: wearing the custom AFO (Figure 1c), wearing an off-the-shelf polypropylene leaf spring AFO (Codivilla Spring, Ottobock, Duderstadt, Germany), and shod (no-AFO). According to the current clinical practice at the authors’ institution, the Codivilla Spring is one of the most recommended off-the-shelf PD-AFOs for individuals with foot drop, when no other significant anatomical alterations are present. Furthermore, the stiffness of the Codivilla Spring is comparable to that of the custom PD-AFOs used here [30]. For each custom AFO, the resisting torque T( α ) in gait can be linearly correlated to the plantarflexion and dorsiflexion angles via the following equations:
T p α = k p × α p
T d α = k d × α d
where subscripts p and d are used to indicate plantarflexion and dorsiflexion directions, respectively. Finally, the AFO work was calculated as the dot product between T( α ) and α as follows:
W p α = T p α × α p
W d α = T d α × α d
where Wp( α ) and Wd( α ) represent the energy absorbed and released by the AFO in the stance phase of walking during ankle plantarflexion and dorsiflexion rotations, respectively. W( α ) is assumed to be positive (energy released) when vectors T( α ) and α have the same direction (plantarflexion or dorsiflexion) and negative (energy absorbed) when they have opposite directions. Work was normalized to the participant’s weight (J/kg).
The non-parametric paired Wilcoxon signed rank test was used to assess the effect of the AFO on kinetic and spatio-temporal parameters (α = 0.05).

3. Results

The measured stiffnesses of the eight custom PD-AFOs were in the range of 0.15–0.23 N*m/deg and 0.10–0.27 N*m/deg in plantarflexion and dorsiflexion, respectively.
Patients walked faster while wearing the PD-AFO with respect to the shod condition (normalized speed AFO = 53.8 ± 14.0 %height/s; normalized speed SHOD = 50.8 ± 15.0 %height/s; p = 0.015). No difference in walking speed was observed with respect to the Codivilla Spring (normalized speed CODIVILLA = 53.6 ± 15.3 %height/s; p > 0.05).
Figure 2a shows the mean temporal profiles (±1SD) of the calf-shell plantarflexion/dorsiflexion angle (deg) during the normalized stance phase duration. Similarly to what is generally observed for ankle motion, plantarflexion of the PD-AFO at early stance is followed by dorsiflexion during midstance and by late-stance plantarflexion. This motion generates a resisting torque due to the PD-AFO stiffnesses kp and kd (Figure 2b).
Figure 3 reports the temporal profiles of the work done by each of the eight custom PD-AFOs during the normalized stance phase duration. In all PD-AFOs, energy was absorbed during the load-acceptance phase (1–15% stance) and at late stance (50–90% stance). Energy was released up to midstance (15–50% stance) and during push-off (80–100% stance). At early stance, the maximum energy absorbed and released by the PD-AFOs was 0.011 ± 0.005 J/kg at 12 ± 2% (t1 in Figure 3) of the stance phase. At late stance, the maximum energy was 0.008 ± 0.007 J/kg at 88 ± 9% (t2 in Figure 3) of the stance phase. The average maximum energy released across the whole stance phase was 0.013 ± 0.005 J/kg.
Figure 4 reports the inter-participant mean ankle power during the normalized stance phase duration in the PD-AFO and shod conditions. Although the difference was not statistically significant (p = 0.06), a trend for reduced maximum normalized ankle power at push-off was observed. This was 1.9 W/kg and 2.0 W/kg, respectively, in the PD-AFO and shod conditions.

4. Discussion

Current advances in 3D printing technologies have enhanced the production of custom orthopedic devices fitting patients’ anatomy and with personalized mechanical properties. While 3D-printed custom orthoses are still more expensive than similar off-the-shell solutions, the costs are increasingly offset by the higher performance and the better comfort. In addition, significant anatomical alterations can only be addressed by such custom devices. PD-AFOs are recommended for individuals with mild foot drop instability, which may also need support in the push-off phase of walking due to weakness or insufficiency of the ankle plantarflexor muscles. While several commercial and custom AFOs are reported in the literature for different lower limb pathologies, only a few studies have investigated the energetics of PD-AFOs with respect to their design and mechanical properties [9,11]. In this study, we aimed at calculating the energetics of a novel custom PD-AFO in a population of individuals with mild foot drop condition.
Quantifying the energetic effects of a novel custom AFO in patients with foot drop is crucial for several reasons. First, this study provides objective, data-driven evidence of the AFO’s energetic contribution to gait dynamics. In vivo biomechanical measurements offer a quantitative assessment of how the device influences patients’ physiological exertion during ambulation, adding instrumental evidence to the subjective evaluations on comfort and ease of use. This is essential for validating the AFO’s potential to enhance functional mobility. Second, by quantifying the AFO’s impact on energy expenditure, clinicians can make informed decisions regarding prescription and customization of the device. Understanding the energetic benefits allows for personalized treatment plans, optimizing design and stiffness properties to maximize patient outcomes. This is particularly vital for patients with chronic conditions, where even small reductions in the metabolic cost per gait cycle can substantially improve quality of life. Furthermore, this study contributes to the broader scientific understanding of AFO interventions. These investigations allow researchers to better correlate AFO design parameters with AFO mechanics in gait and to identify key biomechanical parameters influencing AFO effectiveness. This knowledge can drive the development of more efficient and patient-centered orthotic solutions for foot drop and other gait impairments.
The present PD-AFOs were characterized by relatively low bending stiffness with respect to the average data reported for individuals with similar conditions. While no specific data are available in the literature to establish the correct stiffness of PD-AFOs for different degrees of ankle dorsi/plantarflexion deficits, in this study, a reference stiffness was used and adjusted according to the weight of each participant. Low bending stiffness allows for better foot and ankle dynamics in gait as it minimizes the restraint of the ankle in dorsiflexion, while providing sufficient support to resist passive ankle plantarflexion. A gait analysis study by Kerkum et al. [3] on a population of children with cerebral palsy estimated the net work of a flexible AFO featuring a stiffness in plantarflexion similar to that of the present custom PD-AFO (0.11 ± 0.13 N*m/deg), albeit more rigid in dorsiflexion (0.7 ± 0.2 N*m/deg) by about 0.03 J/kg. Although not directly comparable to what measured here, Bregman et al. reported a positive work of 0.06 W/kg for AFOs with stiffness ranging from 1.4 to 23.5 N*m/deg [12]. Despite the relatively low stiffness of the present PD-AFO, the ankle plantarflexion angle was significantly lower (p < 0.05) in the swing phase when wearing the custom PD-AFO with respect to the shod condition [17]. All participants in this study were affected by a foot drop condition, but only some of them suffered also from mild plantarflexion deficit. These individuals are likely to benefit the most by using low-stiffness PD-AFOs, as excessive rigidity of the calf-shell in plantarflexion would hinder the ankle joint physiological mobility in the push-off phase. Although further validation through a larger clinical trial is warranted, preliminary evidence seems to suggest that individuals with foot drop exhibiting mild plantarflexion weakness may benefit from PD-AFOs characterized by minimal plantarflexion stiffness. Consequently, a subsequent study will be designed to quantify the minimum plantarflexion stiffness of a PD-AFO necessary to provide adequate foot and footwear support during the swing phase of gait.
As far as the outcome of the present energetic analysis, the temporal profiles of the work calculated over the normalized stance phase duration were rather consistent across PD-AFOs (Figure 4). At foot contact, all PD-AFOs absorbed some energy by plantarflexing the calf-shell, which was released to the ankle up to midstance. Subsequently, energy was absorbed to dorsiflex the calf-shell up to about 90% of the stance phase. This energy was released to the ankle at push-off. It is therefore plausible that this, albeit small, amount of energy may be used to improve foot and ankle propulsion at late stance or to decrease the amount of ankle net work required to walk at the same walking speed. Indeed, while the participants walked faster when wearing the PD-AFO with respect to the shod condition, the power released at the ankle was lower, albeit not statistically significant, in the PD-AFO condition. Although a larger dataset is needed to establish a correlation between varying AFO stiffness and gait expenditure relative to ankle plantar flexor deficits, this study provides a foundation for individualized prescription guidelines for AFOs in drop foot conditions.
These results should be critically assessed with respect to some limitations. Since no direct comparison with other custom AFO designs was performed in the same testing conditions, it is difficult to assess how the present low-stiffness design performs with respect to other—more rigid—custom dynamic AFOs. While the outcome of the energetic analysis was rather consistent across participants, the limited sample size prevents the present energetic data to be representative of the varying nature of the foot drop condition. Indeed, a larger foot drop population would allow us to include different walking patterns that may affect the present outcome. In addition, due to its flexibility, the AFO foot plate can also store and release some energy in the push-off phase and during metatarsophalangeal joint dorsiflexion and plantarflexion. Thus, it can be hypothesized that the actual positive work released to the ankle could be larger than what reported in this study by analyzing the energetics of the calf-shell only. Furthermore, no follow-up evaluations were conducted thus the long-term energetics of the PD-AFO, its effect on ankle power, and the biomechanical adaptations or changes in performance following familiarization.

5. Conclusions

The present investigation aimed at quantifying the energetics of a novel 3D-printed custom PD-AFO for foot drop individuals with good residual mobility. While the energy absorbed and released by this PD-AFO is rather small compared to the work produced at the ankle at push-off, a net positive effect on spatio-temporal parameters was observed [17]. Acknowledging the limited clinical translatability of this pilot study due to its small sample size, future research will focus on hypothesis-driven investigations in larger cohorts of individuals with foot drop. These cohorts will be stratified according to the severity of neuro-muscular impairment to elucidate the optimal mechanical properties of custom-made PD-AFOs for enhanced clinical guidance.

Author Contributions

Conceptualization, P.C. and G.R.; methodology, P.C., R.F., M.B., A.Z., M.O. and F.C.; software, P.C., A.Z. and L.Z.; validation, P.C., G.R. and Z.S.; formal analysis, M.B.; investigation, P.C.; resources, F.C. and A.L.; data curation, P.C., G.R. and M.O.; writing—original draft preparation, P.C. and G.R.; writing—review and editing, P.C., G.R., Z.S. and A.L.; visualization, P.C.; supervision, P.C.; project administration, A.L.; funding acquisition, A.L. All authors have read and agreed to the published version of the manuscript.

Funding

This study was partially funded by Ministero della Salute 5 × 1000 (#2024/731146; “Modellazione 3D, Progettazione e Correzione di Deformità Muscolo-scheletriche e Sostituzioni Protesiche”).

Institutional Review Board Statement

The study was conducted in accordance with the Declaration of Helsinki and approved by the local CE-AVEC Ethical Committee (#0016384 on 23 December 2019).

Informed Consent Statement

Informed consent was obtained from all participants involved in the study.

Data Availability Statement

Experimental and kinematic data can be made available upon request.

Acknowledgments

The authors would like to thank Luigi Lena for helping with the figures.

Conflicts of Interest

Author Franco Cevolini was employed by the company CRP Technology (Modena, Italy). The remaining authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Abbreviations

The following abbreviations are used in this manuscript:
PD-AFOPassive Dynamic Ankle–Foot Orthosis

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Figure 1. (a) The testing apparatus used to measure the PD-AFO stiffness (k) by applying a controlled 15 deg rotation in flexion and extension [22]; (b) the PD-AFO calf-shell local reference frame (XAFO, YAFO, ZAFO), based on the position of three reflective markers, allows measuring the PD-AFO flexion/extension angle in gait; (c) gait analysis of one of the participants with foot drop wearing the custom PD-AFO.
Figure 1. (a) The testing apparatus used to measure the PD-AFO stiffness (k) by applying a controlled 15 deg rotation in flexion and extension [22]; (b) the PD-AFO calf-shell local reference frame (XAFO, YAFO, ZAFO), based on the position of three reflective markers, allows measuring the PD-AFO flexion/extension angle in gait; (c) gait analysis of one of the participants with foot drop wearing the custom PD-AFO.
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Figure 2. (a) Mean temporal profiles (±1SD) of the calf-shell plantarflexion/dorsiflexion angle [deg] during normalized stance phase (%). From heel-strike to t1, the calf-shell rotates posteriorly (i.e., the foot plate plantarflexes with respect to the calf-shell); from t1 to t2, the calf-shell rotates anteriorly (i.e., the foot plate dorsiflexes with respect to the calf-shell); from t2 to toe-off, the calf-shell rotates posteriorly back to the neutral position. (b) Temporal profile of the mean (±1SD) AFO resisting moment (N*m) over normalized stance phase (%). The resisting moment in gait was estimated by using the moment/angle relationship following the experimental measurements of AFO stiffness.
Figure 2. (a) Mean temporal profiles (±1SD) of the calf-shell plantarflexion/dorsiflexion angle [deg] during normalized stance phase (%). From heel-strike to t1, the calf-shell rotates posteriorly (i.e., the foot plate plantarflexes with respect to the calf-shell); from t1 to t2, the calf-shell rotates anteriorly (i.e., the foot plate dorsiflexes with respect to the calf-shell); from t2 to toe-off, the calf-shell rotates posteriorly back to the neutral position. (b) Temporal profile of the mean (±1SD) AFO resisting moment (N*m) over normalized stance phase (%). The resisting moment in gait was estimated by using the moment/angle relationship following the experimental measurements of AFO stiffness.
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Figure 3. Each curve represents the work normalized to body weight (J/kg) performed by each of the 8 AFOs over the normalized stance phase (%). From heel-strike to t1, the calf-shell absorbs energy by flexing posteriorly. The calf-shell releases energy from t1 up to the neutral position at midstance and absorbs energy again by flexing anteriorly up to t2. From t2 to toe-off, the calf-shell releases energy by rotating posteriorly back to the neutral position. This work released by the AFO supports ankle plantarflexion in the push-off phase.
Figure 3. Each curve represents the work normalized to body weight (J/kg) performed by each of the 8 AFOs over the normalized stance phase (%). From heel-strike to t1, the calf-shell absorbs energy by flexing posteriorly. The calf-shell releases energy from t1 up to the neutral position at midstance and absorbs energy again by flexing anteriorly up to t2. From t2 to toe-off, the calf-shell releases energy by rotating posteriorly back to the neutral position. This work released by the AFO supports ankle plantarflexion in the push-off phase.
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Figure 4. Mean temporal profiles of body-weight normalized ankle power (W/kg) in the custom AFO, Codivilla Spring, and in shod conditions over normalized stance phase (%).
Figure 4. Mean temporal profiles of body-weight normalized ankle power (W/kg) in the custom AFO, Codivilla Spring, and in shod conditions over normalized stance phase (%).
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MDPI and ACS Style

Caravaggi, P.; Rogati, G.; Baleani, M.; Fognani, R.; Zamagni, L.; Ortolani, M.; Zomparelli, A.; Cevolini, F.; Sawacha, Z.; Leardini, A. Energetics of a Novel 3D-Printed Custom Ankle Foot Orthosis in a Population of Individuals with Foot Drop: A Pilot Study. Appl. Sci. 2025, 15, 5885. https://doi.org/10.3390/app15115885

AMA Style

Caravaggi P, Rogati G, Baleani M, Fognani R, Zamagni L, Ortolani M, Zomparelli A, Cevolini F, Sawacha Z, Leardini A. Energetics of a Novel 3D-Printed Custom Ankle Foot Orthosis in a Population of Individuals with Foot Drop: A Pilot Study. Applied Sciences. 2025; 15(11):5885. https://doi.org/10.3390/app15115885

Chicago/Turabian Style

Caravaggi, Paolo, Giulia Rogati, Massimiliano Baleani, Roberta Fognani, Luca Zamagni, Maurizio Ortolani, Alessandro Zomparelli, Franco Cevolini, Zimi Sawacha, and Alberto Leardini. 2025. "Energetics of a Novel 3D-Printed Custom Ankle Foot Orthosis in a Population of Individuals with Foot Drop: A Pilot Study" Applied Sciences 15, no. 11: 5885. https://doi.org/10.3390/app15115885

APA Style

Caravaggi, P., Rogati, G., Baleani, M., Fognani, R., Zamagni, L., Ortolani, M., Zomparelli, A., Cevolini, F., Sawacha, Z., & Leardini, A. (2025). Energetics of a Novel 3D-Printed Custom Ankle Foot Orthosis in a Population of Individuals with Foot Drop: A Pilot Study. Applied Sciences, 15(11), 5885. https://doi.org/10.3390/app15115885

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