940 lines
35 KiB
Python
940 lines
35 KiB
Python
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import pytest
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from functools import lru_cache
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from numpy.testing import (assert_warns, assert_,
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assert_allclose,
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assert_equal,
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assert_array_equal,
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suppress_warnings)
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import numpy as np
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from numpy import finfo, power, nan, isclose, sqrt, exp, sin, cos
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from scipy import optimize
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from scipy.optimize import (_zeros_py as zeros, newton, root_scalar,
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OptimizeResult)
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from scipy._lib._util import getfullargspec_no_self as _getfullargspec
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# Import testing parameters
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from scipy.optimize._tstutils import get_tests, functions as tstutils_functions
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TOL = 4*np.finfo(float).eps # tolerance
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_FLOAT_EPS = finfo(float).eps
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bracket_methods = [zeros.bisect, zeros.ridder, zeros.brentq, zeros.brenth,
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zeros.toms748]
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gradient_methods = [zeros.newton]
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all_methods = bracket_methods + gradient_methods
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# A few test functions used frequently:
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# # A simple quadratic, (x-1)^2 - 1
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def f1(x):
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return x ** 2 - 2 * x - 1
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def f1_1(x):
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return 2 * x - 2
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def f1_2(x):
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return 2.0 + 0 * x
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def f1_and_p_and_pp(x):
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return f1(x), f1_1(x), f1_2(x)
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# Simple transcendental function
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def f2(x):
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return exp(x) - cos(x)
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def f2_1(x):
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return exp(x) + sin(x)
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def f2_2(x):
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return exp(x) + cos(x)
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# lru cached function
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@lru_cache
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def f_lrucached(x):
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return x
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class TestScalarRootFinders:
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# Basic tests for all scalar root finders
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xtol = 4 * np.finfo(float).eps
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rtol = 4 * np.finfo(float).eps
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def _run_one_test(self, tc, method, sig_args_keys=None,
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sig_kwargs_keys=None, **kwargs):
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method_args = []
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for k in sig_args_keys or []:
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if k not in tc:
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# If a,b not present use x0, x1. Similarly for f and func
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k = {'a': 'x0', 'b': 'x1', 'func': 'f'}.get(k, k)
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method_args.append(tc[k])
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method_kwargs = dict(**kwargs)
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method_kwargs.update({'full_output': True, 'disp': False})
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for k in sig_kwargs_keys or []:
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method_kwargs[k] = tc[k]
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root = tc.get('root')
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func_args = tc.get('args', ())
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try:
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r, rr = method(*method_args, args=func_args, **method_kwargs)
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return root, rr, tc
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except Exception:
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return root, zeros.RootResults(nan, -1, -1, zeros._EVALUEERR, method), tc
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def run_tests(self, tests, method, name, known_fail=None, **kwargs):
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r"""Run test-cases using the specified method and the supplied signature.
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Extract the arguments for the method call from the test case
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dictionary using the supplied keys for the method's signature."""
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# The methods have one of two base signatures:
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# (f, a, b, **kwargs) # newton
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# (func, x0, **kwargs) # bisect/brentq/...
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# FullArgSpec with args, varargs, varkw, defaults, ...
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sig = _getfullargspec(method)
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assert_(not sig.kwonlyargs)
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nDefaults = len(sig.defaults)
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nRequired = len(sig.args) - nDefaults
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sig_args_keys = sig.args[:nRequired]
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sig_kwargs_keys = []
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if name in ['secant', 'newton', 'halley']:
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if name in ['newton', 'halley']:
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sig_kwargs_keys.append('fprime')
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if name in ['halley']:
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sig_kwargs_keys.append('fprime2')
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kwargs['tol'] = self.xtol
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else:
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kwargs['xtol'] = self.xtol
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kwargs['rtol'] = self.rtol
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results = [list(self._run_one_test(
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tc, method, sig_args_keys=sig_args_keys,
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sig_kwargs_keys=sig_kwargs_keys, **kwargs)) for tc in tests]
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# results= [[true root, full output, tc], ...]
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known_fail = known_fail or []
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notcvgd = [elt for elt in results if not elt[1].converged]
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notcvgd = [elt for elt in notcvgd if elt[-1]['ID'] not in known_fail]
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notcvged_IDS = [elt[-1]['ID'] for elt in notcvgd]
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assert_equal([len(notcvged_IDS), notcvged_IDS], [0, []])
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# The usable xtol and rtol depend on the test
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tols = {'xtol': self.xtol, 'rtol': self.rtol}
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tols.update(**kwargs)
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rtol = tols['rtol']
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atol = tols.get('tol', tols['xtol'])
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cvgd = [elt for elt in results if elt[1].converged]
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approx = [elt[1].root for elt in cvgd]
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correct = [elt[0] for elt in cvgd]
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# See if the root matches the reference value
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notclose = [[a] + elt for a, c, elt in zip(approx, correct, cvgd) if
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not isclose(a, c, rtol=rtol, atol=atol)
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and elt[-1]['ID'] not in known_fail]
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# If not, evaluate the function and see if is 0 at the purported root
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fvs = [tc['f'](aroot, *tc.get('args', tuple()))
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for aroot, c, fullout, tc in notclose]
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notclose = [[fv] + elt for fv, elt in zip(fvs, notclose) if fv != 0]
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assert_equal([notclose, len(notclose)], [[], 0])
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method_from_result = [result[1].method for result in results]
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expected_method = [name for _ in results]
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assert_equal(method_from_result, expected_method)
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def run_collection(self, collection, method, name, smoothness=None,
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known_fail=None, **kwargs):
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r"""Run a collection of tests using the specified method.
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The name is used to determine some optional arguments."""
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tests = get_tests(collection, smoothness=smoothness)
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self.run_tests(tests, method, name, known_fail=known_fail, **kwargs)
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class TestBracketMethods(TestScalarRootFinders):
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@pytest.mark.parametrize('method', bracket_methods)
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@pytest.mark.parametrize('function', tstutils_functions)
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def test_basic_root_scalar(self, method, function):
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# Tests bracketing root finders called via `root_scalar` on a small
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# set of simple problems, each of which has a root at `x=1`. Checks for
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# converged status and that the root was found.
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a, b = .5, sqrt(3)
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r = root_scalar(function, method=method.__name__, bracket=[a, b], x0=a,
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xtol=self.xtol, rtol=self.rtol)
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assert r.converged
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assert_allclose(r.root, 1.0, atol=self.xtol, rtol=self.rtol)
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assert r.method == method.__name__
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@pytest.mark.parametrize('method', bracket_methods)
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@pytest.mark.parametrize('function', tstutils_functions)
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def test_basic_individual(self, method, function):
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# Tests individual bracketing root finders on a small set of simple
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# problems, each of which has a root at `x=1`. Checks for converged
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# status and that the root was found.
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a, b = .5, sqrt(3)
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root, r = method(function, a, b, xtol=self.xtol, rtol=self.rtol,
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full_output=True)
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assert r.converged
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assert_allclose(root, 1.0, atol=self.xtol, rtol=self.rtol)
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@pytest.mark.parametrize('method', bracket_methods)
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def test_aps_collection(self, method):
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self.run_collection('aps', method, method.__name__, smoothness=1)
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@pytest.mark.parametrize('method', [zeros.bisect, zeros.ridder,
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zeros.toms748])
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def test_chandrupatla_collection(self, method):
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known_fail = {'fun7.4'} if method == zeros.ridder else {}
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self.run_collection('chandrupatla', method, method.__name__,
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known_fail=known_fail)
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@pytest.mark.parametrize('method', bracket_methods)
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def test_lru_cached_individual(self, method):
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# check that https://github.com/scipy/scipy/issues/10846 is fixed
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# (`root_scalar` failed when passed a function that was `@lru_cache`d)
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a, b = -1, 1
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root, r = method(f_lrucached, a, b, full_output=True)
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assert r.converged
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assert_allclose(root, 0)
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class TestNewton(TestScalarRootFinders):
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def test_newton_collections(self):
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known_fail = ['aps.13.00']
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known_fail += ['aps.12.05', 'aps.12.17'] # fails under Windows Py27
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for collection in ['aps', 'complex']:
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self.run_collection(collection, zeros.newton, 'newton',
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smoothness=2, known_fail=known_fail)
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def test_halley_collections(self):
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known_fail = ['aps.12.06', 'aps.12.07', 'aps.12.08', 'aps.12.09',
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'aps.12.10', 'aps.12.11', 'aps.12.12', 'aps.12.13',
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'aps.12.14', 'aps.12.15', 'aps.12.16', 'aps.12.17',
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'aps.12.18', 'aps.13.00']
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for collection in ['aps', 'complex']:
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self.run_collection(collection, zeros.newton, 'halley',
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smoothness=2, known_fail=known_fail)
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def test_newton(self):
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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x = zeros.newton(f, 3, tol=1e-6)
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assert_allclose(f(x), 0, atol=1e-6)
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x = zeros.newton(f, 3, x1=5, tol=1e-6) # secant, x0 and x1
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assert_allclose(f(x), 0, atol=1e-6)
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x = zeros.newton(f, 3, fprime=f_1, tol=1e-6) # newton
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assert_allclose(f(x), 0, atol=1e-6)
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x = zeros.newton(f, 3, fprime=f_1, fprime2=f_2, tol=1e-6) # halley
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assert_allclose(f(x), 0, atol=1e-6)
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def test_newton_by_name(self):
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r"""Invoke newton through root_scalar()"""
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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r = root_scalar(f, method='newton', x0=3, fprime=f_1, xtol=1e-6)
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assert_allclose(f(r.root), 0, atol=1e-6)
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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r = root_scalar(f, method='newton', x0=3, xtol=1e-6) # without f'
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assert_allclose(f(r.root), 0, atol=1e-6)
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def test_secant_by_name(self):
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r"""Invoke secant through root_scalar()"""
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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r = root_scalar(f, method='secant', x0=3, x1=2, xtol=1e-6)
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assert_allclose(f(r.root), 0, atol=1e-6)
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r = root_scalar(f, method='secant', x0=3, x1=5, xtol=1e-6)
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assert_allclose(f(r.root), 0, atol=1e-6)
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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r = root_scalar(f, method='secant', x0=3, xtol=1e-6) # without x1
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assert_allclose(f(r.root), 0, atol=1e-6)
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def test_halley_by_name(self):
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r"""Invoke halley through root_scalar()"""
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for f, f_1, f_2 in [(f1, f1_1, f1_2), (f2, f2_1, f2_2)]:
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r = root_scalar(f, method='halley', x0=3,
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fprime=f_1, fprime2=f_2, xtol=1e-6)
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assert_allclose(f(r.root), 0, atol=1e-6)
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def test_root_scalar_fail(self):
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message = 'fprime2 must be specified for halley'
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with pytest.raises(ValueError, match=message):
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root_scalar(f1, method='halley', fprime=f1_1, x0=3, xtol=1e-6) # no fprime2
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message = 'fprime must be specified for halley'
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with pytest.raises(ValueError, match=message):
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root_scalar(f1, method='halley', fprime2=f1_2, x0=3, xtol=1e-6) # no fprime
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def test_array_newton(self):
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"""test newton with array"""
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def f1(x, *a):
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b = a[0] + x * a[3]
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return a[1] - a[2] * (np.exp(b / a[5]) - 1.0) - b / a[4] - x
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def f1_1(x, *a):
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b = a[3] / a[5]
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return -a[2] * np.exp(a[0] / a[5] + x * b) * b - a[3] / a[4] - 1
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def f1_2(x, *a):
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b = a[3] / a[5]
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return -a[2] * np.exp(a[0] / a[5] + x * b) * b**2
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a0 = np.array([
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5.32725221, 5.48673747, 5.49539973,
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5.36387202, 4.80237316, 1.43764452,
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5.23063958, 5.46094772, 5.50512718,
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5.42046290
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])
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a1 = (np.sin(range(10)) + 1.0) * 7.0
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args = (a0, a1, 1e-09, 0.004, 10, 0.27456)
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x0 = [7.0] * 10
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x = zeros.newton(f1, x0, f1_1, args)
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x_expected = (
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6.17264965, 11.7702805, 12.2219954,
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7.11017681, 1.18151293, 0.143707955,
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4.31928228, 10.5419107, 12.7552490,
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8.91225749
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)
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assert_allclose(x, x_expected)
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# test halley's
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x = zeros.newton(f1, x0, f1_1, args, fprime2=f1_2)
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assert_allclose(x, x_expected)
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# test secant
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x = zeros.newton(f1, x0, args=args)
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assert_allclose(x, x_expected)
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def test_array_newton_complex(self):
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def f(x):
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return x + 1+1j
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def fprime(x):
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return 1.0
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t = np.full(4, 1j)
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x = zeros.newton(f, t, fprime=fprime)
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assert_allclose(f(x), 0.)
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# should work even if x0 is not complex
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t = np.ones(4)
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x = zeros.newton(f, t, fprime=fprime)
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assert_allclose(f(x), 0.)
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x = zeros.newton(f, t)
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assert_allclose(f(x), 0.)
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def test_array_secant_active_zero_der(self):
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"""test secant doesn't continue to iterate zero derivatives"""
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x = zeros.newton(lambda x, *a: x*x - a[0], x0=[4.123, 5],
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args=[np.array([17, 25])])
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assert_allclose(x, (4.123105625617661, 5.0))
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def test_array_newton_integers(self):
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# test secant with float
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x = zeros.newton(lambda y, z: z - y ** 2, [4.0] * 2,
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args=([15.0, 17.0],))
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assert_allclose(x, (3.872983346207417, 4.123105625617661))
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# test integer becomes float
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x = zeros.newton(lambda y, z: z - y ** 2, [4] * 2, args=([15, 17],))
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assert_allclose(x, (3.872983346207417, 4.123105625617661))
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def test_array_newton_zero_der_failures(self):
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# test derivative zero warning
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assert_warns(RuntimeWarning, zeros.newton,
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lambda y: y**2 - 2, [0., 0.], lambda y: 2 * y)
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# test failures and zero_der
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with pytest.warns(RuntimeWarning):
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results = zeros.newton(lambda y: y**2 - 2, [0., 0.],
|
||
|
lambda y: 2*y, full_output=True)
|
||
|
assert_allclose(results.root, 0)
|
||
|
assert results.zero_der.all()
|
||
|
assert not results.converged.any()
|
||
|
|
||
|
def test_newton_combined(self):
|
||
|
def f1(x):
|
||
|
return x ** 2 - 2 * x - 1
|
||
|
def f1_1(x):
|
||
|
return 2 * x - 2
|
||
|
def f1_2(x):
|
||
|
return 2.0 + 0 * x
|
||
|
|
||
|
def f1_and_p_and_pp(x):
|
||
|
return x**2 - 2*x-1, 2*x-2, 2.0
|
||
|
|
||
|
sol0 = root_scalar(f1, method='newton', x0=3, fprime=f1_1)
|
||
|
sol = root_scalar(f1_and_p_and_pp, method='newton', x0=3, fprime=True)
|
||
|
assert_allclose(sol0.root, sol.root, atol=1e-8)
|
||
|
assert_equal(2*sol.function_calls, sol0.function_calls)
|
||
|
|
||
|
sol0 = root_scalar(f1, method='halley', x0=3, fprime=f1_1, fprime2=f1_2)
|
||
|
sol = root_scalar(f1_and_p_and_pp, method='halley', x0=3, fprime2=True)
|
||
|
assert_allclose(sol0.root, sol.root, atol=1e-8)
|
||
|
assert_equal(3*sol.function_calls, sol0.function_calls)
|
||
|
|
||
|
def test_newton_full_output(self, capsys):
|
||
|
# Test the full_output capability, both when converging and not.
|
||
|
# Use simple polynomials, to avoid hitting platform dependencies
|
||
|
# (e.g., exp & trig) in number of iterations
|
||
|
|
||
|
x0 = 3
|
||
|
expected_counts = [(6, 7), (5, 10), (3, 9)]
|
||
|
|
||
|
for derivs in range(3):
|
||
|
kwargs = {'tol': 1e-6, 'full_output': True, }
|
||
|
for k, v in [['fprime', f1_1], ['fprime2', f1_2]][:derivs]:
|
||
|
kwargs[k] = v
|
||
|
|
||
|
x, r = zeros.newton(f1, x0, disp=False, **kwargs)
|
||
|
assert_(r.converged)
|
||
|
assert_equal(x, r.root)
|
||
|
assert_equal((r.iterations, r.function_calls), expected_counts[derivs])
|
||
|
if derivs == 0:
|
||
|
assert r.function_calls <= r.iterations + 1
|
||
|
else:
|
||
|
assert_equal(r.function_calls, (derivs + 1) * r.iterations)
|
||
|
|
||
|
# Now repeat, allowing one fewer iteration to force convergence failure
|
||
|
iters = r.iterations - 1
|
||
|
x, r = zeros.newton(f1, x0, maxiter=iters, disp=False, **kwargs)
|
||
|
assert_(not r.converged)
|
||
|
assert_equal(x, r.root)
|
||
|
assert_equal(r.iterations, iters)
|
||
|
|
||
|
if derivs == 1:
|
||
|
# Check that the correct Exception is raised and
|
||
|
# validate the start of the message.
|
||
|
msg = 'Failed to converge after %d iterations, value is .*' % (iters)
|
||
|
with pytest.raises(RuntimeError, match=msg):
|
||
|
x, r = zeros.newton(f1, x0, maxiter=iters, disp=True, **kwargs)
|
||
|
|
||
|
def test_deriv_zero_warning(self):
|
||
|
def func(x):
|
||
|
return x ** 2 - 2.0
|
||
|
def dfunc(x):
|
||
|
return 2 * x
|
||
|
assert_warns(RuntimeWarning, zeros.newton, func, 0.0, dfunc, disp=False)
|
||
|
with pytest.raises(RuntimeError, match='Derivative was zero'):
|
||
|
zeros.newton(func, 0.0, dfunc)
|
||
|
|
||
|
def test_newton_does_not_modify_x0(self):
|
||
|
# https://github.com/scipy/scipy/issues/9964
|
||
|
x0 = np.array([0.1, 3])
|
||
|
x0_copy = x0.copy() # Copy to test for equality.
|
||
|
newton(np.sin, x0, np.cos)
|
||
|
assert_array_equal(x0, x0_copy)
|
||
|
|
||
|
def test_gh17570_defaults(self):
|
||
|
# Previously, when fprime was not specified, root_scalar would default
|
||
|
# to secant. When x1 was not specified, secant failed.
|
||
|
# Check that without fprime, the default is secant if x1 is specified
|
||
|
# and newton otherwise.
|
||
|
res_newton_default = root_scalar(f1, method='newton', x0=3, xtol=1e-6)
|
||
|
res_secant_default = root_scalar(f1, method='secant', x0=3, x1=2,
|
||
|
xtol=1e-6)
|
||
|
# `newton` uses the secant method when `x1` and `x2` are specified
|
||
|
res_secant = newton(f1, x0=3, x1=2, tol=1e-6, full_output=True)[1]
|
||
|
|
||
|
# all three found a root
|
||
|
assert_allclose(f1(res_newton_default.root), 0, atol=1e-6)
|
||
|
assert res_newton_default.root.shape == tuple()
|
||
|
assert_allclose(f1(res_secant_default.root), 0, atol=1e-6)
|
||
|
assert res_secant_default.root.shape == tuple()
|
||
|
assert_allclose(f1(res_secant.root), 0, atol=1e-6)
|
||
|
assert res_secant.root.shape == tuple()
|
||
|
|
||
|
# Defaults are correct
|
||
|
assert (res_secant_default.root
|
||
|
== res_secant.root
|
||
|
!= res_newton_default.iterations)
|
||
|
assert (res_secant_default.iterations
|
||
|
== res_secant_default.function_calls - 1 # true for secant
|
||
|
== res_secant.iterations
|
||
|
!= res_newton_default.iterations
|
||
|
== res_newton_default.function_calls/2) # newton 2-point diff
|
||
|
|
||
|
@pytest.mark.parametrize('kwargs', [dict(), {'method': 'newton'}])
|
||
|
def test_args_gh19090(self, kwargs):
|
||
|
def f(x, a, b):
|
||
|
assert a == 3
|
||
|
assert b == 1
|
||
|
return (x ** a - b)
|
||
|
|
||
|
res = optimize.root_scalar(f, x0=3, args=(3, 1), **kwargs)
|
||
|
assert res.converged
|
||
|
assert_allclose(res.root, 1)
|
||
|
|
||
|
@pytest.mark.parametrize('method', ['secant', 'newton'])
|
||
|
def test_int_x0_gh19280(self, method):
|
||
|
# Originally, `newton` ensured that only floats were passed to the
|
||
|
# callable. This was indadvertently changed by gh-17669. Check that
|
||
|
# it has been changed back.
|
||
|
def f(x):
|
||
|
# an integer raised to a negative integer power would fail
|
||
|
return x**-2 - 2
|
||
|
|
||
|
res = optimize.root_scalar(f, x0=1, method=method)
|
||
|
assert res.converged
|
||
|
assert_allclose(abs(res.root), 2**-0.5)
|
||
|
assert res.root.dtype == np.dtype(np.float64)
|
||
|
|
||
|
|
||
|
def test_gh_5555():
|
||
|
root = 0.1
|
||
|
|
||
|
def f(x):
|
||
|
return x - root
|
||
|
|
||
|
methods = [zeros.bisect, zeros.ridder]
|
||
|
xtol = rtol = TOL
|
||
|
for method in methods:
|
||
|
res = method(f, -1e8, 1e7, xtol=xtol, rtol=rtol)
|
||
|
assert_allclose(root, res, atol=xtol, rtol=rtol,
|
||
|
err_msg='method %s' % method.__name__)
|
||
|
|
||
|
|
||
|
def test_gh_5557():
|
||
|
# Show that without the changes in 5557 brentq and brenth might
|
||
|
# only achieve a tolerance of 2*(xtol + rtol*|res|).
|
||
|
|
||
|
# f linearly interpolates (0, -0.1), (0.5, -0.1), and (1,
|
||
|
# 0.4). The important parts are that |f(0)| < |f(1)| (so that
|
||
|
# brent takes 0 as the initial guess), |f(0)| < atol (so that
|
||
|
# brent accepts 0 as the root), and that the exact root of f lies
|
||
|
# more than atol away from 0 (so that brent doesn't achieve the
|
||
|
# desired tolerance).
|
||
|
def f(x):
|
||
|
if x < 0.5:
|
||
|
return -0.1
|
||
|
else:
|
||
|
return x - 0.6
|
||
|
|
||
|
atol = 0.51
|
||
|
rtol = 4 * _FLOAT_EPS
|
||
|
methods = [zeros.brentq, zeros.brenth]
|
||
|
for method in methods:
|
||
|
res = method(f, 0, 1, xtol=atol, rtol=rtol)
|
||
|
assert_allclose(0.6, res, atol=atol, rtol=rtol)
|
||
|
|
||
|
|
||
|
def test_brent_underflow_in_root_bracketing():
|
||
|
# Testing if an interval [a,b] brackets a zero of a function
|
||
|
# by checking f(a)*f(b) < 0 is not reliable when the product
|
||
|
# underflows/overflows. (reported in issue# 13737)
|
||
|
|
||
|
underflow_scenario = (-450.0, -350.0, -400.0)
|
||
|
overflow_scenario = (350.0, 450.0, 400.0)
|
||
|
|
||
|
for a, b, root in [underflow_scenario, overflow_scenario]:
|
||
|
c = np.exp(root)
|
||
|
for method in [zeros.brenth, zeros.brentq]:
|
||
|
res = method(lambda x: np.exp(x)-c, a, b)
|
||
|
assert_allclose(root, res)
|
||
|
|
||
|
|
||
|
class TestRootResults:
|
||
|
r = zeros.RootResults(root=1.0, iterations=44, function_calls=46, flag=0,
|
||
|
method="newton")
|
||
|
|
||
|
def test_repr(self):
|
||
|
expected_repr = (" converged: True\n flag: converged"
|
||
|
"\n function_calls: 46\n iterations: 44\n"
|
||
|
" root: 1.0\n method: newton")
|
||
|
assert_equal(repr(self.r), expected_repr)
|
||
|
|
||
|
def test_type(self):
|
||
|
assert isinstance(self.r, OptimizeResult)
|
||
|
|
||
|
|
||
|
def test_complex_halley():
|
||
|
"""Test Halley's works with complex roots"""
|
||
|
def f(x, *a):
|
||
|
return a[0] * x**2 + a[1] * x + a[2]
|
||
|
|
||
|
def f_1(x, *a):
|
||
|
return 2 * a[0] * x + a[1]
|
||
|
|
||
|
def f_2(x, *a):
|
||
|
retval = 2 * a[0]
|
||
|
try:
|
||
|
size = len(x)
|
||
|
except TypeError:
|
||
|
return retval
|
||
|
else:
|
||
|
return [retval] * size
|
||
|
|
||
|
z = complex(1.0, 2.0)
|
||
|
coeffs = (2.0, 3.0, 4.0)
|
||
|
y = zeros.newton(f, z, args=coeffs, fprime=f_1, fprime2=f_2, tol=1e-6)
|
||
|
# (-0.75000000000000078+1.1989578808281789j)
|
||
|
assert_allclose(f(y, *coeffs), 0, atol=1e-6)
|
||
|
z = [z] * 10
|
||
|
coeffs = (2.0, 3.0, 4.0)
|
||
|
y = zeros.newton(f, z, args=coeffs, fprime=f_1, fprime2=f_2, tol=1e-6)
|
||
|
assert_allclose(f(y, *coeffs), 0, atol=1e-6)
|
||
|
|
||
|
|
||
|
def test_zero_der_nz_dp(capsys):
|
||
|
"""Test secant method with a non-zero dp, but an infinite newton step"""
|
||
|
# pick a symmetrical functions and choose a point on the side that with dx
|
||
|
# makes a secant that is a flat line with zero slope, EG: f = (x - 100)**2,
|
||
|
# which has a root at x = 100 and is symmetrical around the line x = 100
|
||
|
# we have to pick a really big number so that it is consistently true
|
||
|
# now find a point on each side so that the secant has a zero slope
|
||
|
dx = np.finfo(float).eps ** 0.33
|
||
|
# 100 - p0 = p1 - 100 = p0 * (1 + dx) + dx - 100
|
||
|
# -> 200 = p0 * (2 + dx) + dx
|
||
|
p0 = (200.0 - dx) / (2.0 + dx)
|
||
|
with suppress_warnings() as sup:
|
||
|
sup.filter(RuntimeWarning, "RMS of")
|
||
|
x = zeros.newton(lambda y: (y - 100.0)**2, x0=[p0] * 10)
|
||
|
assert_allclose(x, [100] * 10)
|
||
|
# test scalar cases too
|
||
|
p0 = (2.0 - 1e-4) / (2.0 + 1e-4)
|
||
|
with suppress_warnings() as sup:
|
||
|
sup.filter(RuntimeWarning, "Tolerance of")
|
||
|
x = zeros.newton(lambda y: (y - 1.0) ** 2, x0=p0, disp=False)
|
||
|
assert_allclose(x, 1)
|
||
|
with pytest.raises(RuntimeError, match='Tolerance of'):
|
||
|
x = zeros.newton(lambda y: (y - 1.0) ** 2, x0=p0, disp=True)
|
||
|
p0 = (-2.0 + 1e-4) / (2.0 + 1e-4)
|
||
|
with suppress_warnings() as sup:
|
||
|
sup.filter(RuntimeWarning, "Tolerance of")
|
||
|
x = zeros.newton(lambda y: (y + 1.0) ** 2, x0=p0, disp=False)
|
||
|
assert_allclose(x, -1)
|
||
|
with pytest.raises(RuntimeError, match='Tolerance of'):
|
||
|
x = zeros.newton(lambda y: (y + 1.0) ** 2, x0=p0, disp=True)
|
||
|
|
||
|
|
||
|
def test_array_newton_failures():
|
||
|
"""Test that array newton fails as expected"""
|
||
|
# p = 0.68 # [MPa]
|
||
|
# dp = -0.068 * 1e6 # [Pa]
|
||
|
# T = 323 # [K]
|
||
|
diameter = 0.10 # [m]
|
||
|
# L = 100 # [m]
|
||
|
roughness = 0.00015 # [m]
|
||
|
rho = 988.1 # [kg/m**3]
|
||
|
mu = 5.4790e-04 # [Pa*s]
|
||
|
u = 2.488 # [m/s]
|
||
|
reynolds_number = rho * u * diameter / mu # Reynolds number
|
||
|
|
||
|
def colebrook_eqn(darcy_friction, re, dia):
|
||
|
return (1 / np.sqrt(darcy_friction) +
|
||
|
2 * np.log10(roughness / 3.7 / dia +
|
||
|
2.51 / re / np.sqrt(darcy_friction)))
|
||
|
|
||
|
# only some failures
|
||
|
with pytest.warns(RuntimeWarning):
|
||
|
result = zeros.newton(
|
||
|
colebrook_eqn, x0=[0.01, 0.2, 0.02223, 0.3], maxiter=2,
|
||
|
args=[reynolds_number, diameter], full_output=True
|
||
|
)
|
||
|
assert not result.converged.all()
|
||
|
# they all fail
|
||
|
with pytest.raises(RuntimeError):
|
||
|
result = zeros.newton(
|
||
|
colebrook_eqn, x0=[0.01] * 2, maxiter=2,
|
||
|
args=[reynolds_number, diameter], full_output=True
|
||
|
)
|
||
|
|
||
|
|
||
|
# this test should **not** raise a RuntimeWarning
|
||
|
def test_gh8904_zeroder_at_root_fails():
|
||
|
"""Test that Newton or Halley don't warn if zero derivative at root"""
|
||
|
|
||
|
# a function that has a zero derivative at it's root
|
||
|
def f_zeroder_root(x):
|
||
|
return x**3 - x**2
|
||
|
|
||
|
# should work with secant
|
||
|
r = zeros.newton(f_zeroder_root, x0=0)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
# test again with array
|
||
|
r = zeros.newton(f_zeroder_root, x0=[0]*10)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
|
||
|
# 1st derivative
|
||
|
def fder(x):
|
||
|
return 3 * x**2 - 2 * x
|
||
|
|
||
|
# 2nd derivative
|
||
|
def fder2(x):
|
||
|
return 6*x - 2
|
||
|
|
||
|
# should work with newton and halley
|
||
|
r = zeros.newton(f_zeroder_root, x0=0, fprime=fder)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
r = zeros.newton(f_zeroder_root, x0=0, fprime=fder,
|
||
|
fprime2=fder2)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
# test again with array
|
||
|
r = zeros.newton(f_zeroder_root, x0=[0]*10, fprime=fder)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
r = zeros.newton(f_zeroder_root, x0=[0]*10, fprime=fder,
|
||
|
fprime2=fder2)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
|
||
|
# also test that if a root is found we do not raise RuntimeWarning even if
|
||
|
# the derivative is zero, EG: at x = 0.5, then fval = -0.125 and
|
||
|
# fder = -0.25 so the next guess is 0.5 - (-0.125/-0.5) = 0 which is the
|
||
|
# root, but if the solver continued with that guess, then it will calculate
|
||
|
# a zero derivative, so it should return the root w/o RuntimeWarning
|
||
|
r = zeros.newton(f_zeroder_root, x0=0.5, fprime=fder)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
# test again with array
|
||
|
r = zeros.newton(f_zeroder_root, x0=[0.5]*10, fprime=fder)
|
||
|
assert_allclose(r, 0, atol=zeros._xtol, rtol=zeros._rtol)
|
||
|
# doesn't apply to halley
|
||
|
|
||
|
|
||
|
def test_gh_8881():
|
||
|
r"""Test that Halley's method realizes that the 2nd order adjustment
|
||
|
is too big and drops off to the 1st order adjustment."""
|
||
|
n = 9
|
||
|
|
||
|
def f(x):
|
||
|
return power(x, 1.0/n) - power(n, 1.0/n)
|
||
|
|
||
|
def fp(x):
|
||
|
return power(x, (1.0-n)/n)/n
|
||
|
|
||
|
def fpp(x):
|
||
|
return power(x, (1.0-2*n)/n) * (1.0/n) * (1.0-n)/n
|
||
|
|
||
|
x0 = 0.1
|
||
|
# The root is at x=9.
|
||
|
# The function has positive slope, x0 < root.
|
||
|
# Newton succeeds in 8 iterations
|
||
|
rt, r = newton(f, x0, fprime=fp, full_output=True)
|
||
|
assert r.converged
|
||
|
# Before the Issue 8881/PR 8882, halley would send x in the wrong direction.
|
||
|
# Check that it now succeeds.
|
||
|
rt, r = newton(f, x0, fprime=fp, fprime2=fpp, full_output=True)
|
||
|
assert r.converged
|
||
|
|
||
|
|
||
|
def test_gh_9608_preserve_array_shape():
|
||
|
"""
|
||
|
Test that shape is preserved for array inputs even if fprime or fprime2 is
|
||
|
scalar
|
||
|
"""
|
||
|
def f(x):
|
||
|
return x**2
|
||
|
|
||
|
def fp(x):
|
||
|
return 2 * x
|
||
|
|
||
|
def fpp(x):
|
||
|
return 2
|
||
|
|
||
|
x0 = np.array([-2], dtype=np.float32)
|
||
|
rt, r = newton(f, x0, fprime=fp, fprime2=fpp, full_output=True)
|
||
|
assert r.converged
|
||
|
|
||
|
x0_array = np.array([-2, -3], dtype=np.float32)
|
||
|
# This next invocation should fail
|
||
|
with pytest.raises(IndexError):
|
||
|
result = zeros.newton(
|
||
|
f, x0_array, fprime=fp, fprime2=fpp, full_output=True
|
||
|
)
|
||
|
|
||
|
def fpp_array(x):
|
||
|
return np.full(np.shape(x), 2, dtype=np.float32)
|
||
|
|
||
|
result = zeros.newton(
|
||
|
f, x0_array, fprime=fp, fprime2=fpp_array, full_output=True
|
||
|
)
|
||
|
assert result.converged.all()
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize(
|
||
|
"maximum_iterations,flag_expected",
|
||
|
[(10, zeros.CONVERR), (100, zeros.CONVERGED)])
|
||
|
def test_gh9254_flag_if_maxiter_exceeded(maximum_iterations, flag_expected):
|
||
|
"""
|
||
|
Test that if the maximum iterations is exceeded that the flag is not
|
||
|
converged.
|
||
|
"""
|
||
|
result = zeros.brentq(
|
||
|
lambda x: ((1.2*x - 2.3)*x + 3.4)*x - 4.5,
|
||
|
-30, 30, (), 1e-6, 1e-6, maximum_iterations,
|
||
|
full_output=True, disp=False)
|
||
|
assert result[1].flag == flag_expected
|
||
|
if flag_expected == zeros.CONVERR:
|
||
|
# didn't converge because exceeded maximum iterations
|
||
|
assert result[1].iterations == maximum_iterations
|
||
|
elif flag_expected == zeros.CONVERGED:
|
||
|
# converged before maximum iterations
|
||
|
assert result[1].iterations < maximum_iterations
|
||
|
|
||
|
|
||
|
def test_gh9551_raise_error_if_disp_true():
|
||
|
"""Test that if disp is true then zero derivative raises RuntimeError"""
|
||
|
|
||
|
def f(x):
|
||
|
return x*x + 1
|
||
|
|
||
|
def f_p(x):
|
||
|
return 2*x
|
||
|
|
||
|
assert_warns(RuntimeWarning, zeros.newton, f, 1.0, f_p, disp=False)
|
||
|
with pytest.raises(
|
||
|
RuntimeError,
|
||
|
match=r'^Derivative was zero\. Failed to converge after \d+ iterations, '
|
||
|
r'value is [+-]?\d*\.\d+\.$'):
|
||
|
zeros.newton(f, 1.0, f_p)
|
||
|
root = zeros.newton(f, complex(10.0, 10.0), f_p)
|
||
|
assert_allclose(root, complex(0.0, 1.0))
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize('solver_name',
|
||
|
['brentq', 'brenth', 'bisect', 'ridder', 'toms748'])
|
||
|
def test_gh3089_8394(solver_name):
|
||
|
# gh-3089 and gh-8394 reported that bracketing solvers returned incorrect
|
||
|
# results when they encountered NaNs. Check that this is resolved.
|
||
|
def f(x):
|
||
|
return np.nan
|
||
|
|
||
|
solver = getattr(zeros, solver_name)
|
||
|
with pytest.raises(ValueError, match="The function value at x..."):
|
||
|
solver(f, 0, 1)
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize('method',
|
||
|
['brentq', 'brenth', 'bisect', 'ridder', 'toms748'])
|
||
|
def test_gh18171(method):
|
||
|
# gh-3089 and gh-8394 reported that bracketing solvers returned incorrect
|
||
|
# results when they encountered NaNs. Check that `root_scalar` returns
|
||
|
# normally but indicates that convergence was unsuccessful. See gh-18171.
|
||
|
def f(x):
|
||
|
f._count += 1
|
||
|
return np.nan
|
||
|
f._count = 0
|
||
|
|
||
|
res = root_scalar(f, bracket=(0, 1), method=method)
|
||
|
assert res.converged is False
|
||
|
assert res.flag.startswith("The function value at x")
|
||
|
assert res.function_calls == f._count
|
||
|
assert str(res.root) in res.flag
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize('solver_name',
|
||
|
['brentq', 'brenth', 'bisect', 'ridder', 'toms748'])
|
||
|
@pytest.mark.parametrize('rs_interface', [True, False])
|
||
|
def test_function_calls(solver_name, rs_interface):
|
||
|
# There do not appear to be checks that the bracketing solvers report the
|
||
|
# correct number of function evaluations. Check that this is the case.
|
||
|
solver = ((lambda f, a, b, **kwargs: root_scalar(f, bracket=(a, b)))
|
||
|
if rs_interface else getattr(zeros, solver_name))
|
||
|
|
||
|
def f(x):
|
||
|
f.calls += 1
|
||
|
return x**2 - 1
|
||
|
f.calls = 0
|
||
|
|
||
|
res = solver(f, 0, 10, full_output=True)
|
||
|
|
||
|
if rs_interface:
|
||
|
assert res.function_calls == f.calls
|
||
|
else:
|
||
|
assert res[1].function_calls == f.calls
|
||
|
|
||
|
|
||
|
def test_gh_14486_converged_false():
|
||
|
"""Test that zero slope with secant method results in a converged=False"""
|
||
|
def lhs(x):
|
||
|
return x * np.exp(-x*x) - 0.07
|
||
|
|
||
|
with pytest.warns(RuntimeWarning, match='Tolerance of'):
|
||
|
res = root_scalar(lhs, method='secant', x0=-0.15, x1=1.0)
|
||
|
assert not res.converged
|
||
|
assert res.flag == 'convergence error'
|
||
|
|
||
|
with pytest.warns(RuntimeWarning, match='Tolerance of'):
|
||
|
res = newton(lhs, x0=-0.15, x1=1.0, disp=False, full_output=True)[1]
|
||
|
assert not res.converged
|
||
|
assert res.flag == 'convergence error'
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize('solver_name',
|
||
|
['brentq', 'brenth', 'bisect', 'ridder', 'toms748'])
|
||
|
@pytest.mark.parametrize('rs_interface', [True, False])
|
||
|
def test_gh5584(solver_name, rs_interface):
|
||
|
# gh-5584 reported that an underflow can cause sign checks in the algorithm
|
||
|
# to fail. Check that this is resolved.
|
||
|
solver = ((lambda f, a, b, **kwargs: root_scalar(f, bracket=(a, b)))
|
||
|
if rs_interface else getattr(zeros, solver_name))
|
||
|
|
||
|
def f(x):
|
||
|
return 1e-200*x
|
||
|
|
||
|
# Report failure when signs are the same
|
||
|
with pytest.raises(ValueError, match='...must have different signs'):
|
||
|
solver(f, -0.5, -0.4, full_output=True)
|
||
|
|
||
|
# Solve successfully when signs are different
|
||
|
res = solver(f, -0.5, 0.4, full_output=True)
|
||
|
res = res if rs_interface else res[1]
|
||
|
assert res.converged
|
||
|
assert_allclose(res.root, 0, atol=1e-8)
|
||
|
|
||
|
# Solve successfully when one side is negative zero
|
||
|
res = solver(f, -0.5, float('-0.0'), full_output=True)
|
||
|
res = res if rs_interface else res[1]
|
||
|
assert res.converged
|
||
|
assert_allclose(res.root, 0, atol=1e-8)
|
||
|
|
||
|
|
||
|
def test_gh13407():
|
||
|
# gh-13407 reported that the message produced by `scipy.optimize.toms748`
|
||
|
# when `rtol < eps` is incorrect, and also that toms748 is unusual in
|
||
|
# accepting `rtol` as low as eps while other solvers raise at 4*eps. Check
|
||
|
# that the error message has been corrected and that `rtol=eps` can produce
|
||
|
# a lower function value than `rtol=4*eps`.
|
||
|
def f(x):
|
||
|
return x**3 - 2*x - 5
|
||
|
|
||
|
xtol = 1e-300
|
||
|
eps = np.finfo(float).eps
|
||
|
x1 = zeros.toms748(f, 1e-10, 1e10, xtol=xtol, rtol=1*eps)
|
||
|
f1 = f(x1)
|
||
|
x4 = zeros.toms748(f, 1e-10, 1e10, xtol=xtol, rtol=4*eps)
|
||
|
f4 = f(x4)
|
||
|
assert f1 < f4
|
||
|
|
||
|
# using old-style syntax to get exactly the same message
|
||
|
message = fr"rtol too small \({eps/2:g} < {eps:g}\)"
|
||
|
with pytest.raises(ValueError, match=message):
|
||
|
zeros.toms748(f, 1e-10, 1e10, xtol=xtol, rtol=eps/2)
|
||
|
|
||
|
|
||
|
def test_newton_complex_gh10103():
|
||
|
# gh-10103 reported a problem when `newton` is pass a Python complex x0,
|
||
|
# no `fprime` (secant method), and no `x1` (`x1` must be constructed).
|
||
|
# Check that this is resolved.
|
||
|
def f(z):
|
||
|
return z - 1
|
||
|
res = newton(f, 1+1j)
|
||
|
assert_allclose(res, 1, atol=1e-12)
|
||
|
|
||
|
res = root_scalar(f, x0=1+1j, x1=2+1.5j, method='secant')
|
||
|
assert_allclose(res.root, 1, atol=1e-12)
|
||
|
|
||
|
|
||
|
@pytest.mark.parametrize('method', all_methods)
|
||
|
def test_maxiter_int_check_gh10236(method):
|
||
|
# gh-10236 reported that the error message when `maxiter` is not an integer
|
||
|
# was difficult to interpret. Check that this was resolved (by gh-10907).
|
||
|
message = "'float' object cannot be interpreted as an integer"
|
||
|
with pytest.raises(TypeError, match=message):
|
||
|
method(f1, 0.0, 1.0, maxiter=72.45)
|