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This repository was archived by the owner on Sep 4, 2024. It is now read-only.
As we assume that all masses are binary (either 1, or 0), that means, one can implement [semi-explicit differential algebraic equations](https://en.wikipedia.org/wiki/Differential-algebraic_system_of_equations) with
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this node dynamics type.
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$rhsdescription
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``f`` is represented by `rhs` field of `OrdinaryNodeDynamics`.
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- the general signature of `rhs` is
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```Julia
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rhs(dint_dt::AbstractVector,
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u::Complex,
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i::Complex,
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int::AbstractVector,
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t,
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)::Complex
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```
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- Input
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- `u` is the complex voltage ``u``
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- `i` is the complex current ``i``
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- `int` is the array of internal variables ``y_1, \dots, y_n``
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- `t` is the time ``t``
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- Output
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- the (complex) return value describes ``\frac{du}{dt}``
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- `rhs` writes values in `dint_dt` describing the left-hand side ``\frac{dy_1}{dt}, \dots, \frac{dy_n}{dt}``
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