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Resolve numerical instability in chemical_potential - #1726
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## main #1726 +/- ##
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- Hits 7946 7945 -1
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My suspicion is that you're running into the same issue discussed in astropy/astropy#9721. I'd suggest exploring something like... @validate_quantities(
n_e={"can_be_negative": False, "pass_equivalent_units": True},
T={"can_be_negative": False, "equivalencies": u.temperature_energy()},
)
def chemical_potential(n_e: u.m**-3, T: u.K) -> u.dimensionless_unscaled:
# deBroglie wavelength
lambdaDB = thermal_deBroglie_wavelength(T)
# degeneracy parameter
degen = (np.cbrt(n_e) * lambdaDB).to(u.dimensionless_unscaled)**3
...Using |
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@JaydenR2305 Can you add the same changes you made in #1727, sans change log entry, to this PR? If all the checks pass, then I'd be comfortable merging #1727 without all of its checks passing. |
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Looks like 5.0 still uses |
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You are correct, see my comment #1727 (comment). |
rocco8773
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In the docstring, can you make the executive decision to either consistently use the subscript
"... where
If we keep the subscript, then we at least need to explain what it means.
rocco8773
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Do you know which section in Bontiz discusses the chemical potential? If so, can you included in the first line of the docstring Notes section?
Good call! I added the specific equation number from Bonitz and improved the overall explanation. The documentation was somewhat vague on how the calculation is performed so I tried to make things more explicit |
namurphy
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LGTM! It looks like you addressed all of @rocco8773's comments, and I only have a very minor suggestion for the changelog entry. I'm happy to get this merged soon. Thank you for doing this!
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Cool, I've never heard of the BFGS algorithm. I have some reading up to do! Thanks for digging into this! |
| self.n_e_fail = 1e23 * u.cm**-3 | ||
| self.T = 11604 * u.K | ||
| self.True1 = 6.133671348607095e-11 | ||
| self.True1 = 0 |
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Add another test where the result is non-zero.
Co-authored-by: Nick Murphy <namurphy@cfa.harvard.edu>
…enR2305/PlasmaPy into chemical-potential-stability
| Changed `~plasmapy.formulary.quantum.chemical_potential` to use the | ||
| Broyden-Fletcher-Goldfarb-Shanno algorithm to implicitly solve for beta. |
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| Changed `~plasmapy.formulary.quantum.chemical_potential` to use the | |
| Broyden-Fletcher-Goldfarb-Shanno algorithm to implicitly solve for beta. | |
| Changed `~plasmapy.formulary.quantum.chemical_potential` to use the | |
| Broyden-Fletcher-Goldfarb-Shanno algorithm to implicitly solve for | |
| the β(\ :math:`= 1/(k_B T)`\ ) parameter. |
Only so beta is not mistaken for the plasma beta, which would likely be common in this community.
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Whoops, that shouldn't say beta anyways. It should be the dimensionless chemical potential
| The definition for the ideal chemical potential is implicit, so it must | ||
| be obtained numerically by solving for the Fermi integral for values | ||
| of chemical potential approaching the degeneracy parameter. Since values | ||
| returned from the `~plasmapy.formulary.mathematics.Fermi_integral` | ||
| are complex, a nonlinear Levenberg-Marquardt least squares method is | ||
| used to iteratively approach a value of :math:`μ` which minimizes | ||
| :math:`I_{1/2}(β μ_a^{ideal}) - χ_a` | ||
| are complex, the Broyden–Fletcher–Goldfarb–Shanno algorithm is | ||
| used to iteratively approach a value of :math:`μ^{ideal}` which minimizes | ||
| :math:`\lvert I_{1/2}(β μ^{ideal}) - χ \rvert`. |
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I'm thinking as a follow up PR, it would be good to break out the code for the ideal chemical potential into its own function. @JaydenR2305 What do you think about this and would you be willing to do it? Again, this would be a followup PR and I'm not suggesting to do it in this PR.
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Sure. That means this function would just be a wrapper for that function multiplied by beta?
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Yeah, in the end that would be the case.
| def test_knowns(n_e, T, expected_beta): | ||
| """ | ||
| Tests Fermi_integral for expected value. | ||
| Tests chemical_potential for expected value. | ||
| """ | ||
| methodVal = chemical_potential(self.n_e, self.T) | ||
| testTrue = u.isclose(methodVal, self.True1, rtol=1e-16, atol=0.0) | ||
| errStr = f"Chemical potential value should be {self.True1} and not {methodVal}." | ||
| methodVal = chemical_potential(n_e, T).value | ||
| testTrue = np.isclose(methodVal, expected_beta, rtol=1e-16, atol=0.0) | ||
| errStr = ( | ||
| f"Chemical potential value should be {expected_beta} and not {methodVal}." | ||
| ) | ||
| assert testTrue, errStr |
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Can you add another assert to ensure the returned unit is dimensionless_unscaled? It'll likely look something like...
assert testTrue, errStr
assert chemical_potential.unit == u.dimensionless_unscaledAlso, could you please refactor this to meet PEP8 naming standards? e.g. methodVal -> method_val
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Looks good to me! Thank you for working on this.
This one attempts to use the :wikipedia: role, though I'll need to check that it works.

Currently, for reasonable electron densities (~1e10 cm^-3 - 1e20 cm^-3),
chemical_potentialreturns a number extremely close to zero (~1e-16). This behavior is reasonable and expected. However, there are some occasions where the current least squares regression method will return an abnormally large value, demonstrating numerical instability. This instability can sometimes cause the docstring test to failI propose we use some alternative to a least squares method. The method tested in the figures is the Broyden–Fletcher–Goldfarb–Shanno algorithm. The figures were generated at 11000 Kelvin using the two different methods to calculate the chemical potential, and the resulting residual.
For densities greater than 1e20 cm^-3, the graphs produce identical results
The first regime is where the chemical potential is ~0. The algorithms generally agree on zero but sometimes the least squares method produces unexpected results

The residuals for both functions are the same suggesting they have an approximately equal error

Both algorithms produce the same results for electron densities greater than 1e20

docstrings.