1. Introduction
Traffic congestion throughout the United States (US) has reached unprecedented levels, a phenomenon primarily attributable to evolving travel patterns in which traffic delays have permeated midday periods, midweek timeframes, and weekends, extending beyond traditional weekday peak hours [
1]. According to INRIX’s 2024 Global Traffic Scorecard, the US national cost of congestion has risen to
$74 billion in forfeited time and productivity, with drivers in New York City and Chicago each losing 102 h per year, ranking both cities closely behind Istanbul, and the New York metropolitan area alone incurring an estimated
$9.5 billion in economic losses [
2]. In this context, the present study concerns non-recurrent congestion (NRC), namely the unpredictable delay caused by random disruptive events such as incidents, adverse weather, and special events, as distinguished from recurrent congestion (RC), which arises predictably from routine peak period demand. The detection framework developed herein is based on a Physics-Informed Neural Network (PINN), a deep learning model whose training is constrained by the governing equations of traffic flow theory; both concepts are elaborated on in the sections that follow.
Effective mitigation of these substantial economic consequences necessitates the precise identification and quantification of delay mechanisms. Transportation analyses differentiate between recurring and non-recurring congestion, noting that roughly half of all congestion is caused by unpredictable, non-recurring disruptions [
3,
4]. These non-recurring events include traffic incidents, adverse weather conditions, road construction zones, and special events. Crucially, these unexpected factors introduce highly variable and unpredictable travel times, compelling both travelers and freight shippers to allocate excessive buffer time, which ultimately results in lost resources [
3].
Skabardonis et al. [
5] define non-recurrent congestion as the extra delay on freeway segments caused by unpredictable and random events that disrupt normal traffic flow. This type of delay results from incidents such as accidents, breakdowns, or from special events, lane closures, and bad weather. Essentially, non-recurrent congestion is the additional delay that occurs beyond the regular, predictable delay, which would happen in the absence of the specific disruptive event.
Non-recurrent congestion profoundly impacts transportation systems by adding significant variability to operations and increasing overall delay. Since congestion delay is a random quantity with a large statistical “tail”, reliance on single-day measurements or instrumented probe vehicles to estimate delay is considered highly misleading. Non-recurrent events cause a marked reduction in travel time reliability; analysis of the I-210 corridor showed that the 90th percentile travel time increased by approximately 8 min under incident conditions. Empirical studies further demonstrate that non-recurrent delay accounts for a substantial portion of the total delay, contributing between 13% and 30% of the total congestion delay during peak periods in the corridors examined [
5]. In specific case studies, such as the I-880 corridor, each incident during the PM shift was found to contribute an average of 383.8 to 486.1 vehicle-hours of delay [
6]. The cumulative effect of these delays is a severe economic burden.
Despite the disclosed substantial impacts of non-recurrent congestion (NRC), its accurate analysis is hindered by significant methodological and data-related challenges. A primary conceptual problem is the difficulty in separating non-recurrent delays from recurrent delays. Furthermore, quantifying the impact of an event is complex because it requires estimating the exact spatial and temporal region of impact, which is often difficult when the time and location data for the incident lack the necessary accuracy. There are also subtle questions of compounding causation that complicate analysis, such as determining how to attribute delay when adverse weather concurrently increases both the number of incidents and the baseline recurrent delay [
5]. Additionally, implementing detailed measurement methodologies statewide is constrained by the fact that comprehensive data, including detailed incident records, special event data, and precise lane closure information, are not routinely available [
7].
Numerous methodologies have been developed for identifying NRC and traffic anomalies, which can be broadly classified into four categories: statistical analysis, data clustering, machine learning, and traffic flow modeling. As detailed in
Section 2, each category faces fundamental challenges, including the difficulty of defining objective thresholds between recurrent and non-recurrent congestion, sensitivity to measurement noise, the scarcity of ground truth NRC labels, and, for purely data-driven models, the risk of producing results detached from established traffic flow theory [
8,
9,
10,
11,
12,
13,
14].
The objective of this research is to develop and evaluate an NRC detection method that requires neither labeled incident data nor subjective thresholds calibrated per site, by grounding the detection baseline in traffic flow theory. The underlying premise is that a model constrained by the physics of normal traffic flow cannot reproduce non-recurrent disruptions, so significant deviations between observed and physics-estimated traffic states signal an NRC event. This premise admits a natural interpretation in terms of symmetry: recurrent congestion preserves the day-to-day temporal symmetry of traffic patterns, whereas a non-recurrent event constitutes a local symmetry breaking that the physics-constrained residual is designed to expose.
This research proposes a robust framework for non-recurrent traffic congestion by leveraging Physics-Informed Neural Networks (PINNs) to establish a physically consistent baseline of normal traffic behavior. By treating the traffic stream as a continuous fluid-like system, the PINN acts as an expert estimator that identifies anomalies by measuring the divergence between observed sensor data and the theoretically plausible traffic state. The mathematical foundation of this approach is rooted in the Lighthill–Whitham–Richards (LWR) model, which defines traffic dynamics through the conservation of mass equation. This first-order partial differential equation (PDE) describes the evolution of traffic density, k, over time, t, and space, x.
To ensure the model remains accurate across diverse flow conditions, a two-regime fundamental diagram is utilized to define the flow–density relationship. The detection of non-recurrent congestion is subsequently executed through a rigorous analysis of the model residuals. Because PINN is trained to represent the most plausible and normal traffic state for a given location and time, its output serves as a high-fidelity benchmark for typical flow. When real-time observed traffic states deviate significantly from the PINN’s estimated density, the resulting anomaly score—defined as the absolute difference between observation and estimation—signals a breakdown in the expected physical process. Since recurrent bottlenecks are already accounted for within the physical constraints and historical training of the model, a high residual indicates an external event that cannot be explained by standard traffic physics. Consequently, this methodology allows for the rapid identification of incidents, providing traffic management centers with a more accurate and automated tool for incident response and urban mobility optimization.
The contributions of this study are threefold. First, to the best of the authors’ knowledge, this is the first application of a PINN to non-recurrent congestion detection: whereas prior PINN studies in transportation employ the network as a traffic state estimator to reconstruct unobserved conditions, the present framework repurposes the PINN as a physically constrained baseline of normal traffic behavior, against which anomalies are identified through residual analysis. Second, the framework requires neither labeled incident data nor site-specific congestion thresholds, addressing two limitations that pervade existing NRC detection methods. Third, a differentiable two-regime fundamental diagram combining the Greenshields and Underwood models is embedded in the physics loss, enabling the baseline to remain accurate across both free-flow and congested regimes.
The rest of this paper is organized as follows.
Section 2 reviews the literature on NRC detection across four methodological categories and highlights the research gaps this study addresses.
Section 3 introduces the proposed PINN framework, including the LWR-based physics formulation, the two-regime fundamental diagram, and the considerations for loss weighting and hyperparameters.
Section 4 describes the case study site and data.
Section 5 presents the model parameters and NRC detection results, and
Section 6 concludes with key findings and directions for future research.
4. Case Study
This section presents a case study to evaluate the performance of the proposed PINN-based NRC detection method formulated in
Section 3.
This study selects a 12 km segment on the outer loop (i.e., westbound direction) of the Seoul Ring Expressway in Korea between the Howon IC and the 2nd Nogosan Tunnel, as shown in
Figure 2. The chosen segment has 17 permanent data collection stations that capture traffic data, such as count, speed, and occupancy. The selected segment includes three tunnels (i.e., 1st Nogosan Tunnel, 2nd Nogosan Tunnel, and Sapaesan Tunnel), where non-recurrent congestion plays a critical role in congestion and incident management. Furthermore, the interchange (i.e., Songchoo IC) located in the segment often causes unstable traffic flow due to heavy weaving traffic. Along the westbound travel direction, station 3620 is located immediately downstream of the Howon IC, stations 3621, 3622, and 3624 are located within the Sapaesan Tunnel, and station 3633 is located between the Sapaesan Tunnel and the Songchoo IC. The corridor was selected for this proof-of-concept evaluation owing to the availability of high-resolution sensor data covering the entire segment.
This study employs 15 min interval traffic data collected from each data collection station over a period of 6 months from 1 January 2022 to 30 June 2022. The data is obtained from the data portal of Korea Expressway Corp. The data collection stations capture traffic count (q in veh/hour), speed (u in km/hour), and occupancy (o in %). Thus, density (k in veh/km) is estimated using the fundamental equation.
Figure 3,
Figure 4,
Figure 5 and
Figure 6 display hourly speed–density plots, in which each panel aggregates the corresponding 15 min observations, from four selected locations over 24-h: Sapaesan Tunnel (Station ID 3622), Songchoo IC (Station ID 3634), 1st Nogosan Tunnel (Station ID 3638), and 2nd Nogosan Tunnel (Station ID 3645). It is noted that the shaded panels in each figure indicate peak periods (i.e., 7–9 a.m. and 5–7 p.m.). Compared to Nogosan Tunnels (1st and 2nd), as shown in
Figure 3 and
Figure 4, traffic flow in the Sapaesan Tunnel and Songchoo IC during peak hours (i.e., 7~9 a.m. and 5~7 p.m.) appears slightly unstable. This unstable traffic likely results from upstream shockwaves caused by merging and diverging traffics in and around Songchoo IC.
For model training and evaluation, the dataset was divided temporally. The 15 min interval traffic data collected from 1 January to 30 June 2022 (i.e., 181 days), corresponding to 295,392 observations (=181 days × 96 intervals/day × 17 sensor stations), were used to train the PINN baseline. The data collected on 1 July 2022 (i.e., 1632 observations) were held out entirely from training and used to evaluate the NRC detection performance reported in
Section 5. The data were obtained from the open data portal of the Korea Expressway Corporation, which publishes traffic measurements from the permanent detection stations along the corridor, and no additional processing was applied beyond the density estimation described above.
5. Results
Table 2 summarizes the parameters that were used to build the final model. Physics weight is a parameter used to balance the impact of the physics part of PINN to the model training. The physics samples parameter is the number of data points for time, t, and location, x, that are used to randomly choose physics inputs to calculate the physics loss. Depending on how to combine both physics weight and physics samples, the performance of PINN varies. For instance, limited physics samples with very small physics weights would likely cause the PINN model to ignore the physics part, resulting in a final model that would resemble a pure neural network model. On the other hand, excessively large physics samples with relatively high physics weight might cause the model to focus more on the physics part, which could result in the final model lacking a neural network nature.
As aforementioned, this research employs a two-regime traffic state framework for the physics part of PINN: (1) Underwood model for heavy traffic state and (2) Greenshields model for low–moderate traffic state. Through an in-depth data analysis, 17.0 veh/km is identified as the density threshold for distinguishing between heavy and low–moderate traffic state regimes. Furthermore, the jam density and the optimal density are also estimated by using a curve-fitting technique, as shown in
Table 1. Likewise, the free-flow speeds for both models are also estimated to be 97.1 km/h and 144.8 km/hour for the Greenshields model and Underwood model, respectively.
The parameters in
Table 2 were determined in two groups through a calibration process. The traffic stream parameters, including the jam density, the optimal density, and the free-flow speeds of the two regimes, were calibrated by least squares curve fitting of the two-regime fundamental diagram to the six-month speed–density observations, and the density threshold separating the two regimes (i.e., 17.0 veh/km) was identified from the observed transition in the speed–density relationship. It should be noted that the fitted free-flow speed of the Underwood model (i.e., 144.8 km/h) exceeds that of the Greenshields model (i.e., 97.1 km/h) because, in the Underwood formulation, the free-flow speed is a curve-fitting parameter obtained by extrapolating the congested regime data to zero density rather than an observable travel speed, and values exceeding the physical free-flow speed are typical when the model is fitted to congested regime observations. The network hyperparameters, including the numbers of hidden layers and neurons, the learning rate, the batch size, the number of epochs, the physics weight, and the number of physics collocation samples, were selected through preliminary sensitivity experiments in which candidate configurations were compared based on validation loss and the stability of the physics residual during training, following the considerations described in
Section 3.2.2 and
Section 3.2.3.
All experiments were conducted on a workstation equipped with an Intel Core Ultra 9 285 CPU (24 cores), 64 GB of memory, and an NVIDIA RTX PRO 6000 GPU, running Ubuntu 24.04 with PyTorch and CUDA 13.0. Training the final model (i.e., 5000 epochs with a batch size of 4096 and 10,000 physics collocation samples) required approximately 5.5 h. Once trained, generating the baseline density for a new observation interval requires only a forward pass, executing in well under one second for all seventeen stations, which is negligible relative to the 15 min data collection cycle. The modest computational footprint indicates that the framework can be operated, and periodically retrained, on standard hardware available to traffic management centers without specialized infrastructure.
Figure 7 presents the evolution of the total loss over the training epochs. The total loss decreased rapidly during the initial stage of training, and it became stabilized well from the epoch 1623, confirming that the model remained stable throughout training rather than being optimized away.
Upon the completion of the model training, the traffic data collected on 1 July 2022 (i.e., the held out evaluation day, see
Section 4) are applied to predict traffic states.
Figure 8 shows the 24 h density result at the sensor station located between the Sapaesan Tunnel and the Songchoo IC (i.e., Station ID 3633) obtained from the final model. The dots in blue indicate the actual density collected from the sensor and the red curve means the density predicted by the PINN model.
Based on the prediction results, non-recurrent congestion is identified when the traffic condition (i.e., density) recorded by the sensor exceeds the predicted model’s tolerance level (τ). In this research, the tolerance level is set at 1.5 or 150% of the predictions, meaning that if the observed density exceeds the predicted density by 50%, it is considered non-recurrent congestion. The adopted value is grounded in the fitted parameters of the fundamental diagram. Since the estimated normal peak period density ranges from approximately 22 to 27 veh/km and the fitted optimal density is 24.9 veh/km, a state flagged at this tolerance necessarily lies well beyond the capacity density, on the congested branch of the fundamental diagram, which is a physically oversaturated condition that cannot be produced by recurrent equilibrium flow. Lower tolerance values (e.g., 1.2 or 1.3) would flag states within the plausible neighborhood of the capacity point, where measurement noise and routine peak period variability reside. The magnitude is also consistent with the threshold conventions employed in the NRC detection literature [
8,
9] and with the multiple normal variation logic of the residual-based monitoring schemes reviewed in
Section 2.4. It should be noted that the tolerance level is an operator-adjustable parameter reflecting an agency’s preferred balance between detection sensitivity and false alarms, and a formal calibration of the tolerance level against ground-truth incident records is planned as part of the expanded case study described in
Section 6.
Figure 9,
Figure 10,
Figure 11 and
Figure 12 show the cases of non-recurrent congestion detected, which are marked with dashed circles.
Regarding the sensitivity of the detection outcome to the tolerance level, the detected events in
Table 3 exhibit peak observed to predicted density ratios of 2.00 (station 3620), 1.92 (station 3621), 1.68 (station 3622), and 1.50 (station 3624). The three sustained events at stations 3620 through 3622 would therefore remain detected for any tolerance level up to 1.68, well above the adopted value, whereas the brief excursion at station 3624 lies at the margin of the criterion. Increasing the tolerance thus prunes marginal, short-duration excursions first while retaining the pronounced events, which is the intended behavior of the tolerance parameter; a full sensitivity evaluation at lower tolerance levels, quantifying additional detections and false alarms, requires ground truth incident records and is included in the expanded evaluation described in
Section 6.
It should be emphasized that the proposed framework, as evaluated here, constitutes a proof of concept demonstrating the feasibility of physics-informed, residual-based anomaly detection, rather than a fully validated operational incident detection system; operational deployment would require the quantitative validation and calibration steps outlined in
Section 6.
As demonstrated in
Figure 9,
Figure 10,
Figure 11 and
Figure 12, the proposed method successfully isolated non-recurrent incidents from the background noise of daily recurrent traffic. Excessive density increases are observed at stations 3620, 3621, and 3622 between 3:00 p.m. and 4:45 p.m. on 1 July 2022. It is worth noting that station 3620 is located immediately downstream of the Howon IC and stations 3621, 3622, and 3624 are located within the Sapaesan Tunnel (see
Section 4); tunnel sections are among the locations where recurrent and non-recurrent congestion co-occur and where fixed-threshold methods struggle. The normal traffic state during this period, estimated by the model trained with the past six months of data, ranges from approximately 22 veh/km to 27 veh/km. Thus, such abnormally high density should be treated as non-recurrent traffic congestion.
Table 3 summarizes the detected events, listing each event with its station, location, time window, baseline density, peak observed density, and flag status. A purely data-driven neural network lacking the physics constraint would be expected to fit such density excursions as normal patterns, consistent with the overfitting behavior documented for unconstrained models in the traffic state estimation literature [
29,
30,
31]; a formal ablation comparison is planned as part of the expanded evaluation (see
Section 6).
The detection capability demonstrated above can be explained from two complementary perspectives. From the standpoint of traffic flow theory, the two congestion types are physically distinct phenomena. Recurrent congestion arises from demand exceeding capacity at fixed bottlenecks, and the resulting traffic states, however dense, evolve along the equilibrium manifold defined by the fundamental diagram and satisfy the LWR conservation law. Non-recurrent congestion, by contrast, originates from a sudden reduction in capacity (e.g., a blocked lane or a stalled vehicle), which produces density profiles that violate the equilibrium relationship embedded in the model. Because the PINN baseline is constrained to remain on the physically admissible manifold, recurrent congestion is reproduced and thus absorbed, while capacity collapse states are unreproducible by construction and surface as large residuals. The detection signal is therefore not a statistical judgment of rarity but a physical judgment of implausibility. In the language of symmetry, recurrent congestion preserves the temporal symmetry of the daily traffic pattern and remains consistent with the conservation law, whereas a non-recurrent event breaks this symmetry locally; the anomaly score can thus be interpreted as a measure of local symmetry breaking relative to the physically symmetric baseline.
From the machine learning perspective, the physics loss functions as a strong inductive bias. It regularizes the network toward solutions consistent with the conservation law, preventing the overfitting behavior in which an unconstrained model would absorb anomalous observations into its learned representation of normal conditions, which is the failure mode that undermines purely data-driven anomaly detectors trained without labels. The physics constraint also substitutes for labeled data: the model requires only raw sensor measurements, sidestepping the scarcity and imbalance of incident labels that complicate supervised deep learning approaches [
14,
19].
These properties translate directly into practical implications for traffic management centers. The framework operates on standard 15 min detector data already collected by most agencies; it requires no per site threshold calibration, since the baseline adapts to each location’s recurrent patterns through training; the residual is physically interpretable (i.e., expressed in vehicles per kilometer above the plausible state), which supports operator trust and alarm triage; and the single operator-adjustable parameter maps transparently onto an agency’s preferred balance between sensitivity and false alarms. In an operational deployment, residuals exceeding the tolerance at consecutive intervals or at adjacent stations, as observed at stations 3620 through 3622, would trigger incident verification protocols, enabling faster response than the manual monitoring of speed maps. This method therefore provides traffic management centers with a dependable and automated instrument for incident response, functioning as a digital twin of a roadway’s standard operational capacity to facilitate prompt and proactive incident management strategies.
6. Concluding Remarks
This research addresses the critical challenge of identifying non-recurrent congestion (NRC), which accounts for approximately half of all urban traffic delays and results in billions of dollars in lost productivity. Existing methodologies often struggle to distinguish between predictable recurrent patterns and unpredictable incidents due to measurement noise, inherent modeling errors, and a pervasive lack of ground-truth data. By proposing a Physics-Informed Neural Network (PINN) framework, this study establishes a novel diagnostic tool that fuses the universal approximation capabilities of deep learning with the established physical laws of macroscopic traffic flow theory.
Central to this approach is the integration of the Lighthill–Whitham–Richards (LWR) model as a latent state estimator, which creates a physically consistent baseline of normal traffic behavior by ensuring that estimates are strictly governed by the conservation of mass. To accurately represent the traffic stream across varying conditions, the methodology incorporates a two-regime fundamental diagram that utilizes the Greenshields model for free-flow regimes and transitions to the Underwood model to capture the complex, non-linear behavior of congested states. To prevent the model from purely memorizing anomalies as normal patterns, a self-adaptive weighting strategy was implemented to balance empirical data-driven loss with the physics-based residual. This optimization process forces the model to fill data gaps with physically plausible interpolations rather than relying solely on statistical fitting.
The detection of non-recurrent congestion is ultimately realized by measuring the divergence (i.e., residual) between real-time sensor observations and the PINN’s estimated density. Because recurrent bottlenecks are already accounted for within the model’s physical constraints and historical training, significant physical outliers are flagged as incidents. The main innovative aspect of this work is flipping the usual role of the PINN. Instead of estimating unobserved traffic states, the physics-constrained network acts as a highly accurate reference for normal operation. This way, deviations that cannot be explained physically, rather than statistically identified outliers, become the signal for detection. Viewed through the lens of symmetry, moreover, the framework detects non-recurrent congestion as a local breaking of the temporal symmetry of recurrent traffic patterns, with the conservation law providing the invariant structure against which such breaking becomes measurable.
Empirical validation via a case study on the Seoul Ring Expressway segment in Korea demonstrated the efficacy of this approach; by setting a tolerance level of 150% of the predicted density, the system successfully isolated non-recurrent incidents from the background noise of daily recurrent traffic. This methodology provides traffic management centers with a robust and automated tool for incident response, acting as a digital twin of a roadway’s normal operating capacity to enable immediate and proactive incident management strategies.
While the current case study scale is sufficient for conducting a proof-of-concept test that explores the applicability of the proposed idea, it is essential to evaluate the performance of the proposed PINN-based NRC detection method under more diverse traffic conditions to ensure the model’s robustness. The present results should accordingly be read as establishing feasibility rather than operational readiness. The immediate next steps include acquiring ground truth incident records to enable a formal quantitative evaluation (e.g., precision, recall, F1 score, false alarm rate, and detection delay), calibrating the tolerance level against such records, and conducting comparative benchmarking against representative baselines, including an identically configured neural network without the physics loss, sequence models such as LSTM, autoencoder-based anomaly detectors, and statistical outlier methods. In addition, the expanded case study will include an interchange-focused evaluation by extending the study corridor to cover more interchanges, since interchanges are simultaneously subject to recurrent congestion and highly exposed to non-recurrent events.