--- title: Oersted field status: partial doc_kind: reference audience: user owner: fullmag-public-docs --- (public-docs-physics-interactions-oersted-field-root)= # Oersted field Fullmag exposes two physically and numerically distinct Oersted-field families: 1. `OerstedCylinder`: an analytic infinite cylindrical conductor with prescribed current. 2. `OerstedField(source=...)`: a field derived from a named solved current transport with an explicit circuit-closure contract. They must not share one undifferentiated capability status. (physics-oersted-field-problem-statement)= ## Physical problem This page is the public physical and authoring contract for the interaction. It separates authored semantics, planner resolution, executable backend lanes, and scientific qualification. (physics-oersted-field-governing-equations)= ## Governing equations ### Analytic cylindrical conductor For signed current $I$ along unit axis $\hat{\mathbf a}$, let $\boldsymbol\rho$ be the perpendicular displacement from the conductor axis, $\rho=|\boldsymbol\rho|$, and $\hat{\boldsymbol\phi}=\hat{\mathbf a}\times\boldsymbol\rho/\rho$. For a uniform current density inside radius $R$, ```{math} :label: eq-public-oersted-field-oersted-cylinder \mathbf H_{\mathrm{oe}}(\rho) = \begin{cases} \dfrac{I\rho}{2\pi R^2}\hat{\boldsymbol\phi}, & 0\le\rho