The hysteresis stage for one channel, in normalized units.
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#include <hysteresis.hpp>
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| void | prepare (double solver_rate_hz) noexcept |
| void | reset () noexcept |
| void | set_character (double drive, double bias) noexcept |
| | drive and bias come from the tape character table; both are re-mapped onto physical constants here rather than being used as gain and offset.
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| double | process (double field) noexcept |
| | One solver step.
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| std::size_t | converged_steps () const noexcept |
| | Diagnostics for the acceptance suite: how often the solver converged inside the iteration cap versus ran out of iterations.
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| std::size_t | capped_steps () const noexcept |
| void | clear_solver_counters () noexcept |
The hysteresis stage for one channel, in normalized units.
◆ capped_steps()
| std::size_t pulp::signal::chardelay::JilesAthertonHysteresis::capped_steps |
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const |
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inlinenoexcept |
◆ clear_solver_counters()
| void pulp::signal::chardelay::JilesAthertonHysteresis::clear_solver_counters |
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inlinenoexcept |
◆ converged_steps()
| std::size_t pulp::signal::chardelay::JilesAthertonHysteresis::converged_steps |
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const |
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inlinenoexcept |
Diagnostics for the acceptance suite: how often the solver converged inside the iteration cap versus ran out of iterations.
◆ prepare()
| void pulp::signal::chardelay::JilesAthertonHysteresis::prepare |
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double | solver_rate_hz | ) |
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inlinenoexcept |
◆ process()
| double pulp::signal::chardelay::JilesAthertonHysteresis::process |
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double | field | ) |
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inlinenoexcept |
One solver step.
Input and output are normalized magnetic field and magnetization respectively.
◆ reset()
| void pulp::signal::chardelay::JilesAthertonHysteresis::reset |
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inlinenoexcept |
◆ set_character()
| void pulp::signal::chardelay::JilesAthertonHysteresis::set_character |
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double | drive, |
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double | bias ) |
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inlinenoexcept |
drive and bias come from the tape character table; both are re-mapped onto physical constants here rather than being used as gain and offset.
drive → a (the anhysteretic shape parameter: smaller a is a steeper approach to saturation, i.e. more saturation for the same field, which is what a drive control should do) bias → c (the reversible fraction: less reversibility means a wider loop and more odd-harmonic content — a worn machine) k and α stay at their published γ-Fe2O3 values. [the mapping CURVES are design parameters; the endpoints they map onto are published]
The documentation for this class was generated from the following file:
- /home/runner/work/pulp/pulp/core/signal/include/pulp/signal/character_delay/hysteresis.hpp