This section presents the development of the robotic manufacturing cell and the two complementary research activities investigated in this work. The first concerns the initial development of a numerical pipeline for automated trajectory generation, intended to reduce the programming effort required when adapting the cell to different duct geometries. The second focuses on the development and experimental validation of the cutting and welding processes through the fabrication and mechanical characterization of representative thermoplastic composite components.
4.2. Initial Trajectory-Generation Pipeline
Automated robot trajectory generation is an important component of a flexible manufacturing cell intended for low-volume production involving substantial part variability. In this work, a numerical pipeline is developed to generate manufacturing trajectories directly from the CAD geometry of fluid-transfer ducts, thereby reducing the amount of manual robot programming required for each new component. The approach processes a three-dimensional CAD model and generates a discrete sequence of robot poses describing both the position and local orientation (Yaw, Pitch, Roll) required along the manufacturing trajectory. The resulting trajectory is subsequently transferred to RoboDK for simulation, validation, and robot-code generation. The proposed trajectory-generation pipeline consists of the following main steps:
- 1.
Importing the three-dimensional model from a STEP file;
- 2.
Extracting the relevant geometric primitives from the model;
- 3.
Computing an Oriented Bounding Box (OBB) based on the part geometry;
- 4.
Generating the welding plane and its associated normal vector;
- 5.
Redefining the global reference frame according to the part geometry;
- 6.
Discretizing the central trajectory of the part;
- 7.
Defining the local orientation at each trajectory point;
- 8.
Adapting the generated trajectory for Robot 1 and Robot 2; and
- 9.
Exporting the resulting trajectory to the offline programming environment for validation, simulation, and robot-code post-processing.
Figure 7 highlights the three key steps of the path generation algorithm. It is important to note that the main components of a discrete path can be defined using the Frenet frame formulation. Each discrete point along the trajectory is represented by a 3D position coordinate (x,y,z) and an orientation defined by three orthogonal unit vectors (tangent, normal, and binormal), forming a local coordinate system at each point along the robot path. This discretization can be expressed using the following 4×4 transformation matrix
:
where
represents the position of the
kth trajectory point, while
,
, and
are three-dimensional unit vectors defining the tangent, normal, and binormal directions, respectively. These vectors form the rotation matrix
and therefore define the local orientation associated with each trajectory point. The resulting sequence of homogeneous transformations provides the pose information required for subsequent trajectory adaptation, simulation, and robot-program generation.
4.3. Development and Validation of the Cutting and Welding Processes
The second component of this work concerns the fabrication and experimental validation of parts produced using the robotic cell. Four part configurations were considered, encompassing both straight (2D) and curved (3D) reinforced thermoplastic ducts, as well as foam-based duct components.
Figure 8 presents the three-dimensional model of a representative reinforced thermoplastic duct. Each duct consists primarily of two half-shells, denoted R1 and R2, which are handled by Robots R1 and R2, respectively.
Dual-arm manipulation is used to cooperatively position and assemble the two half-shells within the multi-station robotic cell. Accurate control of the relative pose between the two manipulators is particularly important during laser welding and during the associated approach, positioning, and repositioning motions. As illustrated in
Figure 9, a Master–Follower control strategy is used, with Robot R1 acting as the guiding robot and Robot R2 following the coordinated motion. Each manipulator holds one half-shell while the two components are positioned to form the complete duct and expose the interfaces required for welding.
Additional manufacturing processes, including cutting, ultrasonic welding, and thermal coating, are coordinated within the robotic cell, although the two robots do not necessarily execute identical tasks or sequences. Using nominal welding parameters of 100 W and 12 mm/s, testing was extended to 3D ducts. After minor adjustments to robot speed and tooling clearance, successful fabrication of 3D geometries was achieved. To validate the automated workflow, a 3D Polyetherimide (PEI) duct with SPUD and three reinforced thermoplastic ducts were repeatedly produced in fully automatic mode without human intervention or process-related downtime. These results confirm the feasibility of the approach for both 2D and 3D reinforced thermoplastic duct manufacturing.
The robotic cell uses laser transmission welding (LTW) with a near-infrared (NIR) laser to locally heat the joint interface. As illustrated in
Figure 10, the laser radiation passes through the semi-transparent layer and is absorbed by the underlying absorbing (black) layer. The resulting localized heating raises the temperature at the interface and enables fusion of the thermoplastic material under applied contact pressure.
The influence of welding parameters was initially investigated using 2D duct specimens. Laser power and robot travel speed were varied to determine operating conditions providing adequate mechanical resistance of the welded joint. Four specimens were tested for each parameter combination using an INSTRON 5980 Series universal testing machine at a crosshead displacement rate of 0.08 in/min. Tensile loading was applied to the welded specimens, and the breaking load of the joint was used as the primary metric for comparing welding conditions.
The results are typically expressed in terms of stress
and strain
. Equations
2 and
3 provide these values. Stress (
) is calculated by dividing the applied force (F) by the original cross-sectional area perpendicular to the load direction (
), while strain (
) is the ratio of the elongation (l -
) to the initial length (
).
Figure 11 summarizes the experimental workflow. First, the dual-arm robotic cell manufactures the duct specimens using selected combinations of robot travel speed and NIR laser power. The resulting parts are then visually inspected to identify apparent welding defects. Finally, the ducts are sectioned into specimens for mechanical testing, and the resulting breaking loads are recorded for analysis.
Figure 12 displays the average breaking strength (in KN) of the tested samples under various operating parameters. Each curve corresponds to a different laser power. Among the tested conditions, a laser power of 100 W combined with a travel speed of 12 mm/s produced the highest average breaking load, approximately 1.5 kN. These parameters were therefore selected as the nominal welding conditions for subsequent experiments.
Increasing laser power beyond this point likely leads to excessive heating and thermal degradation of the polymer matrix, resulting in reduced weld shear strength. These results indicate that thermal degradation dominates at higher power levels, emphasizing the importance of maintaining a delicate balance between sufficient fusion and overheating. This highlights the narrow processing window of thermoplastic laser welding and the need for precise control of both power and travel speed. In the air leak test procedure, the duct is installed on the test bench and gradually pressurized in 2.5 psi steps, starting at 2.5 psi and increasing up to a maximum of 15 psi. At each step, the duct is inspected by spraying a soap-water solution on its surface to detect leaks, indicated by the formation of air bubbles as shown in
Figure 13. This stepwise method helps assess how leakage evolves under increasing pressure and ensures the welded joints remain structurally sound.
The tests demonstrate that 2D ducts withstand the maximum pressure of 15 psi without showing significant degradation. However, as pressure increases, some leakage is observed. While the setup in
Figure 13 does not allow precise measurement of leakage rates at constant pressure, it provides an initial qualitative indication of the parts ability to maintain initial pressure. In the aerospace industry, performance requirements, particularly those related to the leakage rate of polymer ducts, can vary considerably. These thresholds depend on the specific function of the duct within the aircraft, as well as the technical specifications set by each manufacturer. Leakage rates are typically expressed in cubic feet per minute per square foot (cfm/ft²), following an air leakage standard provided by the industrial partner. This standard is derived from a proprietary, application-specific context that remains undisclosed.
Leakage evaluation tests are conducted using the same test bench, starting with an initial internal pressure of 2.5 psi. The air supply is then shut off, and the pressure decay over time is recorded. This data is used in the ideal gas law to estimate the volume of air lost.
Figure 14 shows a graph of the internal pressure drop over time. Due to minor inconsistencies during setup, the initial pressure could not be fixed precisely at 2.5 psi; instead, a starting average pressure of 2.8 psi was recorded at time zero.
Figure 15 shows the final outcome of a reinforced thermoplastic 3D fluid transfer duct produced using the selected welding parameters.The foam cutting station also presented challenges due to material behavior during the cutting process. The force generated by the interaction between the oscillating blade and the foam caused deformation and tearing in the cutting area, rather than producing a clean cut.
Figure 16 a) shows the foam half-shell preform before cutting, while
Figure 16 b) illustrates the desired final sections for both Robot R1 and Robot R2. Despite multiple trials involving adjustments of cutting parameters such as speed, tooling design, and robot offset clean cuts could not be achieved in the robot cell.
Figure 17 highlights the effects of cutting forces on 3D-shaped foam. Due to its softness and flexibility, the foam cannot withstand the localized pressure from the blade, which exceeds its minimal elastic deformation threshold, resulting in tearing rather than clean separation.
Several potential causes of the cutting failure were investigated. The oscillating blade was replaced to exclude blade wear as the primary cause, and the cutting tool was redesigned to improve guidance and support of the foam during the operation. Adjustments to robot speed and tool offset were also evaluated. Despite these modifications, sufficiently clean and repeatable cuts could not be achieved using the oscillating-blade configuration.
An alternative cutting method based on a heated Nichrome wire was therefore investigated.
Figure 18 presents the corresponding experimental setup. Joule heating of the wire enables the foam to be separated with substantially lower mechanical cutting forces, thereby reducing deformation of the compliant workpiece.
Preliminary manual experiments produced cleaner and more consistent cuts than those obtained with the oscillating blade. The proposed setup includes a thermocouple for temperature monitoring, while the main controllable process parameters include electrical current, applied voltage, wire tension, and robot travel speed. Maintaining sufficient and stable wire tension is particularly important to limit wire deformation and reduce the risk of breakage during cutting.
Different Nichrome wire diameters were evaluated, with a 36-gauge wire (0.19 mm diameter) providing the most promising results among the tested configurations. Further investigation is required to determine the appropriate compromise between wire mechanical strength, thermal response, and cutting resistance. The effect of the resulting surface quality on subsequent assembly and welding performance also remains to be quantified. Future work will therefore focus on characterizing the effects of wire diameter, electrical current, and robot travel speed on cutting quality and on the mechanical performance of the resulting welded joints.