Nodal carbon potential quantifies the carbon emissions embodied in each unit of electricity at a bus. It links active-power flow, branch carbon flow, and load-side carbon responsibility. In a coordinated transmission-distribution-microgrid system, bidirectional power exchange causes the carbon intensity at the point of common coupling (PCC) to vary with operating conditions. Reverse flows and near-zero active-power-flow branches alter the effective carbon-flow paths and may render the nodal-carbon-potential equations ill-conditioned or rank deficient. This paper combines a state-dependent PCC boundary, effective propagation topology, and rank-based solution for coordinated transmission–distribution–microgrid systems. Time-series power-flow results are first used to identify the PCC exchange state and update the carbon intensity of a dynamic boundary virtual source. Branch directions are then corrected according to actual active-power flows, and near-zero-flow branches are removed to construct a directed effective carbon-flow topology. Finally, singular-value decomposition diagnoses equation degeneration and determines the effective rank, after a rank-adaptive Moore-Penrose pseudoinverse gives the nodal-carbon-potential solution. The proposed method updates the PCC carbon potential with the power-exchange state and the carbon-flow paths with actual branch flows. It also maintains numerical stability at degenerate operating points.
No takes yet. Share an insight, caveat, or question.
Gui et al. (2026) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: