How did Trinity Rodman's observed-role agreement change across the 2021–2026 NWSL regular seasons?
Trinity Rodman's observed-role agreement increased from 89.5% in 2021 to 90.9% in 2026. The model evaluated 22 2026 starts and found 2 depth tensions. The most frequent alternative observed role was inverted winger in 1 starts.
Trinity Rodman's observed-role agreement increased from 89.5% in 2021 to 90.9% in 2026. The model evaluated 22 2026 starts and found 2 depth tensions. The most frequent alternative observed role was inverted winger in 1 starts.
What mattersEvidence-backed summary
- Modeled
Trinity Rodman's observed-role agreement increased from 89.5% in 2021 to 90.9% in 2026. The model evaluated 22 2026 starts and found 2 depth tensions. The most frequent alternative observed role was inverted winger in 1 starts.
The sequence distinguishes Trinity Rodman's listed position from the model's read of on-ball behavior and shows how the relation changed across seasons.
Full table ↓ Selected evidence from Workflow evidence. Season Starts As assigned Role tensions° Most frequent alternative role° Alternative-role starts° Agreement %° Confidence° 2021 19 17 2 inverted winger 2 89.5 0.76 2022 16 12 4 attacking wing-back 1 75 0.78 2023 19 15 4 inverted winger 2 78.9 0.82 2024 20 18 2 inverted winger 1 90 0.83 2025 9 6 3 inverted winger 2 66.7 0.74 2026 22 20 2 inverted winger 1 90.9 0.86
Exact evidence located
Every claim points to exact returned rows and fields; semantic verification is not claimed.
The evidence
Site-owned records returned by this workflow. The Dossier renderer preserves their values and scope.
Workflow evidence
Trinity Rodman's observed-role model output by NWSL regular season.
| 2021 | 19 | 17 | 2 | inverted winger | 2 | 89.5 | 0.76 |
| 2022 | 16 | 12 | 4 | attacking wing-back | 1 | 75 | 0.78 |
| 2023 | 19 | 15 | 4 | inverted winger | 2 | 78.9 | 0.82 |
| 2024 | 20 | 18 | 2 | inverted winger | 1 | 90 | 0.83 |
| 2025 | 9 | 6 | 3 | inverted winger | 2 | 66.7 | 0.74 |
| 2026 | 22 | 20 | 2 | inverted winger | 1 | 90.9 | 0.86 |