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Unlike closure mechanisms for laser or EDM machining, pulsed water jet manufacturing does not currently have any. The reason is timing; nothing tracks the chamber resonance quickly enough. Although FFT analysis requires 30–50 ms, control of a HAPOS (hydrodynamic acoustic pulse oscillatory system) operation up to 450 MPa has to be kept below 10 ms of inference budget. The answer is our 12-layer physics-guided CNN (PG-CNN) which reads the resonance frequency f rez directly from a model’s raw pressure signals (100 kHz, Hann-windowed, N = 4096 samples). Training runs in two stages. First we pre-train on 2400 synthetic spectra from a validated Helmholtz model (Δ f = 6.4% against the five-element HAPOS); we then fine-tune on 129 quality-screened experimental spectra (out of 312 planned acquisition slots) over 5–25 MPa, using discriminative learning rates and early stopping. The dilated convolutions (kernel K = 7, dilations {1, 2, 4}) cover a 1.69 ms receptive field; attention pooling then selects the time segments. Within PG-SAD, the fixed transfer constant k̃ rkk = 9.41·10 − 4 gives way to a learnable function k rkk ( p , g ) under heteroscedastic constraints. On the held-out set ( n = 240) the PG-CNN reaches 98.2% accuracy inside a ± 50 Hz band with MAE = 23.4 Hz ( R 2 = 0.998), while PG-SAD lowers the mean absolute frequency error to 12.8 Hz at F1 = 0.97. After ONNX/TensorRT optimisation, a Jetson Xavier NX delivers 6.2 ms inference (161 FPS at 15 W), well within the τ ≈ 50 ms time constant of plunger pumps. This physics–CNN bridge is what supplies the sensing layer that closed-loop control and predictive maintenance of pulsed water jet cells have been missing.
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Kušnerová et al. (2026) studied this question.
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