Physics-Refined Spatiotemporal Forecasting on Open-Boundary Hydrologic Graphs
Authors: Haoyang Jiang, Zhengui Wang, Shenghan Gao, Y. Joseph Zhang, Xingquan Zhu, Yi He
Organizations: William & Mary, Williamsburg, VA, USA · Virginia Institute of Marine Science, William & Mary, Gloucester Point, VA, USA · Florida Atlantic University, Boca Raton, FL, USA
Spatiotemporal forecasting on hydrologic graphs is especially prone to instability in open-boundary systems, where the forecast domain exchanges fluxes with an unobserved exterior. In such systems, boundary nodes receive external forcing, e.g., upstream inflows in rivers or tidal signals in coastal regions, that is typically unavailable at prediction time. The absence of this information can compound errors as forecasts unfold in an autoregressive fashion, leading to inferior long-horizon performance. This paper dissects this instability issue by exploring two questions. 1) What boundary forcing enters the forecast domain when information beyond the boundary is missing? 2) How should this forcing propagate through the domain without incurring error amplification under autoregressive rollout? To address both, we propose a new computing framework comprising two key components. First, to compensate for the boundary forcing, our framework learns ghost node proxies from the boundary and interior nodes, striving to approximate unobserved external inputs. Second, to control error accumulation from these learned proxies, we leverage two physics refiners. In particular, one refiner enforces local consistency by aligning ghost proxies with their two-hop neighbors (i.e., boundary nodes and their immediate interiors). The other refiner enhances global stability by correcting the model forecasts through a physics-guided graph neural operator, reducing long-horizon numerical drift. Two real-world hydrologic graphs are employed for empirical evaluation. Comparative results show that our proposal enjoys higher prediction accuracy and long-horizon stability over both learning-based and physics-informed model competitors.
Figures & tables
Fig. 1 : Demonstration of downstream error amplification in the Danube river system [ 2 ] . (a) Boundary nodes regulate the influx of entire network due to unobserved external forcing, and (b) boundary errors propagate and amplify toward downstream under autoregressive rollout in STGNN.
Fig. 2 : Overall pipeline of PRSOBG . For directed graphs (e.g., the Danube river system) and unstructured meshes (e.g., Chesapeake Bay), PRSOBG makes missing open-boundary forcing learnable by constructing ghost-node proxies from boundary–interior dynamics (Sec. III-A ). The proxy is instantiated as one-to-one upstream explicit ghost nodes in directed graphs, and as three mesh-specific ghost variants in unstructured meshes to inject boundary forcing into message passing (Sec. III-B ). During autoregressive rollout, PRSOBG first applies a local boundary refiner to stabilize proxy–boundary consistency (Sec. III-C ), then applies a global physics refiner to regularize propagation, using either an explicit refiner (Sec. III-D1 ) or a convexified semi-implicit refiner (Sec. III-D2 ).
T=6
T=16
T=30
Method
RMSE
Imp.
RMSE
Imp.
RMSE
Imp.
Data-Driven Baselines
STGNN (Backbone)
0.3499
–
0.4147
–
0.5924
–
GRU (Temporal Only)
0.2623
+25.04%
0.3746
+9.67%
0.5529
+6.67%
Ghost-Only STGNN
0.2777
+20.63%
0.3878
+6.49%
0.4836
+18.37%
GraphNODE [ 18 ]
0.3466
+0.94%
0.4104
+1.04%
0.5871
+0.89%
TABLE I : River System under autoregressive rollout with T∈{6,16,30} . Imp. is relative to STGNN (Backbone).
T=6
T=16
T=30
Method
RMSE
Imp.
RMSE
Imp.
RMSE
Imp.
Data-Driven Baselines
STGNN (Backbone)
0.0732
–
0.1797
–
0.2864
–
GRU (Temporal Only)
0.0524
+28.42%
0.1202
+33.11%
0.2108
+26.40%
GraphNODE [ 18 ]
0.0721
+1.50%
0.1743
+3.01%
0.2782
+2.86%
GraphSSM [ 19 ]
0.0705
+3.69%
0.1716
+4.51%
0.2746
+4.12%
TABLE II : Chesapeake Bay under autoregressive rollout with T∈{6,16,30} . Imp. is relative to STGNN (Backbone).
Fig. 3 : Comparison under autoregressive rollout. Across both directed graphs and unstructured meshes, PRSOBG mitigates boundary-induced instability and achieves consistently lower errors than a vanilla STGNN.
Method
Train (rel.)
Inference (rel.)
Memory (rel.)
STGNN
1.00 ×
1.00 ×
1.00 ×
Ghost-Only
1.01 ×
1.01 ×
1.01 ×
Ours-Explicit
1.04 ×
1.03 ×
1.02 ×
Ours-Convexified
1.08 ×
1.08 ×
1.05 ×
TABLE III : Computational cost relative to the STGNN.
Method
Ghost RMSE
Pearson Corr.
VN
0.1018
0.206
Ghost
0.0705
0.961
TABLE IV : Controlled ghost-proxy validation under known upstream forcing ( T=6 ).
Method
RMSE
Imp.
IW
Imp.
STGNN
0.3499
–
0.4423
–
Ghost-Only
0.2777
20.63%
0.2422
45.24%
Ours-Conv.
0.2311
33.95%
0.1770
59.98%
TABLE V : Extreme/high-flow evaluation on River System under autoregressive rollout ( T=6 ).
Change
λreg
Δt
g^
RMSE / %Δ
Default
1.0
1.0
1.0
0.2311 / –
λreg +20%
1.2
1.0
1.0
0.2324 / +0.56%
λreg -20%
0.8
1.0
1.0
0.2322 / +0.47%
Δt +20%
1.0
1.2
1.0
0.2339 / +1.21%
Δt -20%
1.0
0.8
1.0
0.2309 / -0.09%
g^ +20%
1.0
1.0
1.2
0.2364 / +2.29%
TABLE VI : Sensitivity of the Convexified Refiner.
Department of Computer Science and Engineering, Lehigh University, Bethlehem PA 18015, USA · Department of Civil and Environmental Engineering, Lehigh University, Bethlehem2026 PA 18015, USA