physics-equationAvailable
Modified nodal analysis
KCL rows are augmented with branch-current unknowns for voltage sources, inductors, controlled sources, ports, and ideal op-amp constraints.
Reference contract
| Field | Value | Description |
|---|---|---|
| differentiability | exact-ad | — |
| entity_dimension | global | — |
| latex | \mathbf C(\mathbf p)\dot{\mathbf x}+\mathbf g(\mathbf x,\mathbf p,\mathbf u,t)=\mathbf 0 | — |
| mathml | <math display="block"><mrow><mi>C</mi><mover><mi>x</mi><mo>.</mo></mover><mo>+</mo><mi>g</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>p</mi><mo>,</mo><mi>u</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>=</mo><mn>0</mn></mrow></math> | — |
| name | Modified nodal analysis | — |
| section | governing-equation | — |
KCL rows are augmented with branch-current unknowns for voltage sources, inductors, controlled sources, ports, and ideal op-amp constraints.
Contract
| Property | Value |
|---|---|
| differentiability | exact-ad |
| entity_dimension | global |
| latex | \mathbf C(\mathbf p)\dot{\mathbf x}+\mathbf g(\mathbf x,\mathbf p,\mathbf u,t)=\mathbf 0 |
| mathml | <math display="block"><mrow><mi>C</mi><mover><mi>x</mi><mo>.</mo></mover><mo>+</mo><mi>g</mi><mo>(</mo><mi>x</mi><mo>,</mo><mi>p</mi><mo>,</mo><mi>u</mi><mo>,</mo><mi>t</mi><mo>)</mo><mo>=</mo><mn>0</mn></mrow></math> |
| name | Modified nodal analysis |
| section | governing-equation |