Traktor/myenv/Lib/site-packages/mpmath/calculus/optimization.py

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2024-05-26 05:12:46 +02:00
from __future__ import print_function
from copy import copy
from ..libmp.backend import xrange
class OptimizationMethods(object):
def __init__(ctx):
pass
##############
# 1D-SOLVERS #
##############
class Newton:
"""
1d-solver generating pairs of approximative root and error.
Needs starting points x0 close to the root.
Pro:
* converges fast
* sometimes more robust than secant with bad second starting point
Contra:
* converges slowly for multiple roots
* needs first derivative
* 2 function evaluations per iteration
"""
maxsteps = 20
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if len(x0) == 1:
self.x0 = x0[0]
else:
raise ValueError('expected 1 starting point, got %i' % len(x0))
self.f = f
if not 'df' in kwargs:
def df(x):
return self.ctx.diff(f, x)
else:
df = kwargs['df']
self.df = df
def __iter__(self):
f = self.f
df = self.df
x0 = self.x0
while True:
x1 = x0 - f(x0) / df(x0)
error = abs(x1 - x0)
x0 = x1
yield (x1, error)
class Secant:
"""
1d-solver generating pairs of approximative root and error.
Needs starting points x0 and x1 close to the root.
x1 defaults to x0 + 0.25.
Pro:
* converges fast
Contra:
* converges slowly for multiple roots
"""
maxsteps = 30
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if len(x0) == 1:
self.x0 = x0[0]
self.x1 = self.x0 + 0.25
elif len(x0) == 2:
self.x0 = x0[0]
self.x1 = x0[1]
else:
raise ValueError('expected 1 or 2 starting points, got %i' % len(x0))
self.f = f
def __iter__(self):
f = self.f
x0 = self.x0
x1 = self.x1
f0 = f(x0)
while True:
f1 = f(x1)
l = x1 - x0
if not l:
break
s = (f1 - f0) / l
if not s:
break
x0, x1 = x1, x1 - f1/s
f0 = f1
yield x1, abs(l)
class MNewton:
"""
1d-solver generating pairs of approximative root and error.
Needs starting point x0 close to the root.
Uses modified Newton's method that converges fast regardless of the
multiplicity of the root.
Pro:
* converges fast for multiple roots
Contra:
* needs first and second derivative of f
* 3 function evaluations per iteration
"""
maxsteps = 20
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if not len(x0) == 1:
raise ValueError('expected 1 starting point, got %i' % len(x0))
self.x0 = x0[0]
self.f = f
if not 'df' in kwargs:
def df(x):
return self.ctx.diff(f, x)
else:
df = kwargs['df']
self.df = df
if not 'd2f' in kwargs:
def d2f(x):
return self.ctx.diff(df, x)
else:
d2f = kwargs['df']
self.d2f = d2f
def __iter__(self):
x = self.x0
f = self.f
df = self.df
d2f = self.d2f
while True:
prevx = x
fx = f(x)
if fx == 0:
break
dfx = df(x)
d2fx = d2f(x)
# x = x - F(x)/F'(x) with F(x) = f(x)/f'(x)
x -= fx / (dfx - fx * d2fx / dfx)
error = abs(x - prevx)
yield x, error
class Halley:
"""
1d-solver generating pairs of approximative root and error.
Needs a starting point x0 close to the root.
Uses Halley's method with cubic convergence rate.
Pro:
* converges even faster the Newton's method
* useful when computing with *many* digits
Contra:
* needs first and second derivative of f
* 3 function evaluations per iteration
* converges slowly for multiple roots
"""
maxsteps = 20
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if not len(x0) == 1:
raise ValueError('expected 1 starting point, got %i' % len(x0))
self.x0 = x0[0]
self.f = f
if not 'df' in kwargs:
def df(x):
return self.ctx.diff(f, x)
else:
df = kwargs['df']
self.df = df
if not 'd2f' in kwargs:
def d2f(x):
return self.ctx.diff(df, x)
else:
d2f = kwargs['df']
self.d2f = d2f
def __iter__(self):
x = self.x0
f = self.f
df = self.df
d2f = self.d2f
while True:
prevx = x
fx = f(x)
dfx = df(x)
d2fx = d2f(x)
x -= 2*fx*dfx / (2*dfx**2 - fx*d2fx)
error = abs(x - prevx)
yield x, error
class Muller:
"""
1d-solver generating pairs of approximative root and error.
Needs starting points x0, x1 and x2 close to the root.
x1 defaults to x0 + 0.25; x2 to x1 + 0.25.
Uses Muller's method that converges towards complex roots.
Pro:
* converges fast (somewhat faster than secant)
* can find complex roots
Contra:
* converges slowly for multiple roots
* may have complex values for real starting points and real roots
http://en.wikipedia.org/wiki/Muller's_method
"""
maxsteps = 30
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if len(x0) == 1:
self.x0 = x0[0]
self.x1 = self.x0 + 0.25
self.x2 = self.x1 + 0.25
elif len(x0) == 2:
self.x0 = x0[0]
self.x1 = x0[1]
self.x2 = self.x1 + 0.25
elif len(x0) == 3:
self.x0 = x0[0]
self.x1 = x0[1]
self.x2 = x0[2]
else:
raise ValueError('expected 1, 2 or 3 starting points, got %i'
% len(x0))
self.f = f
self.verbose = kwargs['verbose']
def __iter__(self):
f = self.f
x0 = self.x0
x1 = self.x1
x2 = self.x2
fx0 = f(x0)
fx1 = f(x1)
fx2 = f(x2)
while True:
# TODO: maybe refactoring with function for divided differences
# calculate divided differences
fx2x1 = (fx1 - fx2) / (x1 - x2)
fx2x0 = (fx0 - fx2) / (x0 - x2)
fx1x0 = (fx0 - fx1) / (x0 - x1)
w = fx2x1 + fx2x0 - fx1x0
fx2x1x0 = (fx1x0 - fx2x1) / (x0 - x2)
if w == 0 and fx2x1x0 == 0:
if self.verbose:
print('canceled with')
print('x0 =', x0, ', x1 =', x1, 'and x2 =', x2)
break
x0 = x1
fx0 = fx1
x1 = x2
fx1 = fx2
# denominator should be as large as possible => choose sign
r = self.ctx.sqrt(w**2 - 4*fx2*fx2x1x0)
if abs(w - r) > abs(w + r):
r = -r
x2 -= 2*fx2 / (w + r)
fx2 = f(x2)
error = abs(x2 - x1)
yield x2, error
# TODO: consider raising a ValueError when there's no sign change in a and b
class Bisection:
"""
1d-solver generating pairs of approximative root and error.
Uses bisection method to find a root of f in [a, b].
Might fail for multiple roots (needs sign change).
Pro:
* robust and reliable
Contra:
* converges slowly
* needs sign change
"""
maxsteps = 100
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if len(x0) != 2:
raise ValueError('expected interval of 2 points, got %i' % len(x0))
self.f = f
self.a = x0[0]
self.b = x0[1]
def __iter__(self):
f = self.f
a = self.a
b = self.b
l = b - a
fb = f(b)
while True:
m = self.ctx.ldexp(a + b, -1)
fm = f(m)
sign = fm * fb
if sign < 0:
a = m
elif sign > 0:
b = m
fb = fm
else:
yield m, self.ctx.zero
l /= 2
yield (a + b)/2, abs(l)
def _getm(method):
"""
Return a function to calculate m for Illinois-like methods.
"""
if method == 'illinois':
def getm(fz, fb):
return 0.5
elif method == 'pegasus':
def getm(fz, fb):
return fb/(fb + fz)
elif method == 'anderson':
def getm(fz, fb):
m = 1 - fz/fb
if m > 0:
return m
else:
return 0.5
else:
raise ValueError("method '%s' not recognized" % method)
return getm
class Illinois:
"""
1d-solver generating pairs of approximative root and error.
Uses Illinois method or similar to find a root of f in [a, b].
Might fail for multiple roots (needs sign change).
Combines bisect with secant (improved regula falsi).
The only difference between the methods is the scaling factor m, which is
used to ensure convergence (you can choose one using the 'method' keyword):
Illinois method ('illinois'):
m = 0.5
Pegasus method ('pegasus'):
m = fb/(fb + fz)
Anderson-Bjoerk method ('anderson'):
m = 1 - fz/fb if positive else 0.5
Pro:
* converges very fast
Contra:
* has problems with multiple roots
* needs sign change
"""
maxsteps = 30
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if len(x0) != 2:
raise ValueError('expected interval of 2 points, got %i' % len(x0))
self.a = x0[0]
self.b = x0[1]
self.f = f
self.tol = kwargs['tol']
self.verbose = kwargs['verbose']
self.method = kwargs.get('method', 'illinois')
self.getm = _getm(self.method)
if self.verbose:
print('using %s method' % self.method)
def __iter__(self):
method = self.method
f = self.f
a = self.a
b = self.b
fa = f(a)
fb = f(b)
m = None
while True:
l = b - a
if l == 0:
break
s = (fb - fa) / l
z = a - fa/s
fz = f(z)
if abs(fz) < self.tol:
# TODO: better condition (when f is very flat)
if self.verbose:
print('canceled with z =', z)
yield z, l
break
if fz * fb < 0: # root in [z, b]
a = b
fa = fb
b = z
fb = fz
else: # root in [a, z]
m = self.getm(fz, fb)
b = z
fb = fz
fa = m*fa # scale down to ensure convergence
if self.verbose and m and not method == 'illinois':
print('m:', m)
yield (a + b)/2, abs(l)
def Pegasus(*args, **kwargs):
"""
1d-solver generating pairs of approximative root and error.
Uses Pegasus method to find a root of f in [a, b].
Wrapper for illinois to use method='pegasus'.
"""
kwargs['method'] = 'pegasus'
return Illinois(*args, **kwargs)
def Anderson(*args, **kwargs):
"""
1d-solver generating pairs of approximative root and error.
Uses Anderson-Bjoerk method to find a root of f in [a, b].
Wrapper for illinois to use method='pegasus'.
"""
kwargs['method'] = 'anderson'
return Illinois(*args, **kwargs)
# TODO: check whether it's possible to combine it with Illinois stuff
class Ridder:
"""
1d-solver generating pairs of approximative root and error.
Ridders' method to find a root of f in [a, b].
Is told to perform as well as Brent's method while being simpler.
Pro:
* very fast
* simpler than Brent's method
Contra:
* two function evaluations per step
* has problems with multiple roots
* needs sign change
http://en.wikipedia.org/wiki/Ridders'_method
"""
maxsteps = 30
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
self.f = f
if len(x0) != 2:
raise ValueError('expected interval of 2 points, got %i' % len(x0))
self.x1 = x0[0]
self.x2 = x0[1]
self.verbose = kwargs['verbose']
self.tol = kwargs['tol']
def __iter__(self):
ctx = self.ctx
f = self.f
x1 = self.x1
fx1 = f(x1)
x2 = self.x2
fx2 = f(x2)
while True:
x3 = 0.5*(x1 + x2)
fx3 = f(x3)
x4 = x3 + (x3 - x1) * ctx.sign(fx1 - fx2) * fx3 / ctx.sqrt(fx3**2 - fx1*fx2)
fx4 = f(x4)
if abs(fx4) < self.tol:
# TODO: better condition (when f is very flat)
if self.verbose:
print('canceled with f(x4) =', fx4)
yield x4, abs(x1 - x2)
break
if fx4 * fx2 < 0: # root in [x4, x2]
x1 = x4
fx1 = fx4
else: # root in [x1, x4]
x2 = x4
fx2 = fx4
error = abs(x1 - x2)
yield (x1 + x2)/2, error
class ANewton:
"""
EXPERIMENTAL 1d-solver generating pairs of approximative root and error.
Uses Newton's method modified to use Steffensens method when convergence is
slow. (I.e. for multiple roots.)
"""
maxsteps = 20
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
if not len(x0) == 1:
raise ValueError('expected 1 starting point, got %i' % len(x0))
self.x0 = x0[0]
self.f = f
if not 'df' in kwargs:
def df(x):
return self.ctx.diff(f, x)
else:
df = kwargs['df']
self.df = df
def phi(x):
return x - f(x) / df(x)
self.phi = phi
self.verbose = kwargs['verbose']
def __iter__(self):
x0 = self.x0
f = self.f
df = self.df
phi = self.phi
error = 0
counter = 0
while True:
prevx = x0
try:
x0 = phi(x0)
except ZeroDivisionError:
if self.verbose:
print('ZeroDivisionError: canceled with x =', x0)
break
preverror = error
error = abs(prevx - x0)
# TODO: decide not to use convergence acceleration
if error and abs(error - preverror) / error < 1:
if self.verbose:
print('converging slowly')
counter += 1
if counter >= 3:
# accelerate convergence
phi = steffensen(phi)
counter = 0
if self.verbose:
print('accelerating convergence')
yield x0, error
# TODO: add Brent
############################
# MULTIDIMENSIONAL SOLVERS #
############################
def jacobian(ctx, f, x):
"""
Calculate the Jacobian matrix of a function at the point x0.
This is the first derivative of a vectorial function:
f : R^m -> R^n with m >= n
"""
x = ctx.matrix(x)
h = ctx.sqrt(ctx.eps)
fx = ctx.matrix(f(*x))
m = len(fx)
n = len(x)
J = ctx.matrix(m, n)
for j in xrange(n):
xj = x.copy()
xj[j] += h
Jj = (ctx.matrix(f(*xj)) - fx) / h
for i in xrange(m):
J[i,j] = Jj[i]
return J
# TODO: test with user-specified jacobian matrix
class MDNewton:
"""
Find the root of a vector function numerically using Newton's method.
f is a vector function representing a nonlinear equation system.
x0 is the starting point close to the root.
J is a function returning the Jacobian matrix for a point.
Supports overdetermined systems.
Use the 'norm' keyword to specify which norm to use. Defaults to max-norm.
The function to calculate the Jacobian matrix can be given using the
keyword 'J'. Otherwise it will be calculated numerically.
Please note that this method converges only locally. Especially for high-
dimensional systems it is not trivial to find a good starting point being
close enough to the root.
It is recommended to use a faster, low-precision solver from SciPy [1] or
OpenOpt [2] to get an initial guess. Afterwards you can use this method for
root-polishing to any precision.
[1] http://scipy.org
[2] http://openopt.org/Welcome
"""
maxsteps = 10
def __init__(self, ctx, f, x0, **kwargs):
self.ctx = ctx
self.f = f
if isinstance(x0, (tuple, list)):
x0 = ctx.matrix(x0)
assert x0.cols == 1, 'need a vector'
self.x0 = x0
if 'J' in kwargs:
self.J = kwargs['J']
else:
def J(*x):
return ctx.jacobian(f, x)
self.J = J
self.norm = kwargs['norm']
self.verbose = kwargs['verbose']
def __iter__(self):
f = self.f
x0 = self.x0
norm = self.norm
J = self.J
fx = self.ctx.matrix(f(*x0))
fxnorm = norm(fx)
cancel = False
while not cancel:
# get direction of descent
fxn = -fx
Jx = J(*x0)
s = self.ctx.lu_solve(Jx, fxn)
if self.verbose:
print('Jx:')
print(Jx)
print('s:', s)
# damping step size TODO: better strategy (hard task)
l = self.ctx.one
x1 = x0 + s
while True:
if x1 == x0:
if self.verbose:
print("canceled, won't get more excact")
cancel = True
break
fx = self.ctx.matrix(f(*x1))
newnorm = norm(fx)
if newnorm < fxnorm:
# new x accepted
fxnorm = newnorm
x0 = x1
break
l /= 2
x1 = x0 + l*s
yield (x0, fxnorm)
#############
# UTILITIES #
#############
str2solver = {'newton':Newton, 'secant':Secant, 'mnewton':MNewton,
'halley':Halley, 'muller':Muller, 'bisect':Bisection,
'illinois':Illinois, 'pegasus':Pegasus, 'anderson':Anderson,
'ridder':Ridder, 'anewton':ANewton, 'mdnewton':MDNewton}
def findroot(ctx, f, x0, solver='secant', tol=None, verbose=False, verify=True, **kwargs):
r"""
Find an approximate solution to `f(x) = 0`, using *x0* as starting point or
interval for *x*.
Multidimensional overdetermined systems are supported.
You can specify them using a function or a list of functions.
Mathematically speaking, this function returns `x` such that
`|f(x)|^2 \leq \mathrm{tol}` is true within the current working precision.
If the computed value does not meet this criterion, an exception is raised.
This exception can be disabled with *verify=False*.
For interval arithmetic (``iv.findroot()``), please note that
the returned interval ``x`` is not guaranteed to contain `f(x)=0`!
It is only some `x` for which `|f(x)|^2 \leq \mathrm{tol}` certainly holds
regardless of numerical error. This may be improved in the future.
**Arguments**
*f*
one dimensional function
*x0*
starting point, several starting points or interval (depends on solver)
*tol*
the returned solution has an error smaller than this
*verbose*
print additional information for each iteration if true
*verify*
verify the solution and raise a ValueError if `|f(x)|^2 > \mathrm{tol}`
*solver*
a generator for *f* and *x0* returning approximative solution and error
*maxsteps*
after how many steps the solver will cancel
*df*
first derivative of *f* (used by some solvers)
*d2f*
second derivative of *f* (used by some solvers)
*multidimensional*
force multidimensional solving
*J*
Jacobian matrix of *f* (used by multidimensional solvers)
*norm*
used vector norm (used by multidimensional solvers)
solver has to be callable with ``(f, x0, **kwargs)`` and return an generator
yielding pairs of approximative solution and estimated error (which is
expected to be positive).
You can use the following string aliases:
'secant', 'mnewton', 'halley', 'muller', 'illinois', 'pegasus', 'anderson',
'ridder', 'anewton', 'bisect'
See mpmath.calculus.optimization for their documentation.
**Examples**
The function :func:`~mpmath.findroot` locates a root of a given function using the
secant method by default. A simple example use of the secant method is to
compute `\pi` as the root of `\sin x` closest to `x_0 = 3`::
>>> from mpmath import *
>>> mp.dps = 30; mp.pretty = True
>>> findroot(sin, 3)
3.14159265358979323846264338328
The secant method can be used to find complex roots of analytic functions,
although it must in that case generally be given a nonreal starting value
(or else it will never leave the real line)::
>>> mp.dps = 15
>>> findroot(lambda x: x**3 + 2*x + 1, j)
(0.226698825758202 + 1.46771150871022j)
A nice application is to compute nontrivial roots of the Riemann zeta
function with many digits (good initial values are needed for convergence)::
>>> mp.dps = 30
>>> findroot(zeta, 0.5+14j)
(0.5 + 14.1347251417346937904572519836j)
The secant method can also be used as an optimization algorithm, by passing
it a derivative of a function. The following example locates the positive
minimum of the gamma function::
>>> mp.dps = 20
>>> findroot(lambda x: diff(gamma, x), 1)
1.4616321449683623413
Finally, a useful application is to compute inverse functions, such as the
Lambert W function which is the inverse of `w e^w`, given the first
term of the solution's asymptotic expansion as the initial value. In basic
cases, this gives identical results to mpmath's built-in ``lambertw``
function::
>>> def lambert(x):
... return findroot(lambda w: w*exp(w) - x, log(1+x))
...
>>> mp.dps = 15
>>> lambert(1); lambertw(1)
0.567143290409784
0.567143290409784
>>> lambert(1000); lambert(1000)
5.2496028524016
5.2496028524016
Multidimensional functions are also supported::
>>> f = [lambda x1, x2: x1**2 + x2,
... lambda x1, x2: 5*x1**2 - 3*x1 + 2*x2 - 3]
>>> findroot(f, (0, 0))
[-0.618033988749895]
[-0.381966011250105]
>>> findroot(f, (10, 10))
[ 1.61803398874989]
[-2.61803398874989]
You can verify this by solving the system manually.
Please note that the following (more general) syntax also works::
>>> def f(x1, x2):
... return x1**2 + x2, 5*x1**2 - 3*x1 + 2*x2 - 3
...
>>> findroot(f, (0, 0))
[-0.618033988749895]
[-0.381966011250105]
**Multiple roots**
For multiple roots all methods of the Newtonian family (including secant)
converge slowly. Consider this example::
>>> f = lambda x: (x - 1)**99
>>> findroot(f, 0.9, verify=False)
0.918073542444929
Even for a very close starting point the secant method converges very
slowly. Use ``verbose=True`` to illustrate this.
It is possible to modify Newton's method to make it converge regardless of
the root's multiplicity::
>>> findroot(f, -10, solver='mnewton')
1.0
This variant uses the first and second derivative of the function, which is
not very efficient.
Alternatively you can use an experimental Newtonian solver that keeps track
of the speed of convergence and accelerates it using Steffensen's method if
necessary::
>>> findroot(f, -10, solver='anewton', verbose=True)
x: -9.88888888888888888889
error: 0.111111111111111111111
converging slowly
x: -9.77890011223344556678
error: 0.10998877665544332211
converging slowly
x: -9.67002233332199662166
error: 0.108877778911448945119
converging slowly
accelerating convergence
x: -9.5622443299551077669
error: 0.107778003366888854764
converging slowly
x: 0.99999999999999999214
error: 10.562244329955107759
x: 1.0
error: 7.8598304758094664213e-18
ZeroDivisionError: canceled with x = 1.0
1.0
**Complex roots**
For complex roots it's recommended to use Muller's method as it converges
even for real starting points very fast::
>>> findroot(lambda x: x**4 + x + 1, (0, 1, 2), solver='muller')
(0.727136084491197 + 0.934099289460529j)
**Intersection methods**
When you need to find a root in a known interval, it's highly recommended to
use an intersection-based solver like ``'anderson'`` or ``'ridder'``.
Usually they converge faster and more reliable. They have however problems
with multiple roots and usually need a sign change to find a root::
>>> findroot(lambda x: x**3, (-1, 1), solver='anderson')
0.0
Be careful with symmetric functions::
>>> findroot(lambda x: x**2, (-1, 1), solver='anderson') #doctest:+ELLIPSIS
Traceback (most recent call last):
...
ZeroDivisionError
It fails even for better starting points, because there is no sign change::
>>> findroot(lambda x: x**2, (-1, .5), solver='anderson')
Traceback (most recent call last):
...
ValueError: Could not find root within given tolerance. (1.0 > 2.16840434497100886801e-19)
Try another starting point or tweak arguments.
"""
prec = ctx.prec
try:
ctx.prec += 20
# initialize arguments
if tol is None:
tol = ctx.eps * 2**10
kwargs['verbose'] = kwargs.get('verbose', verbose)
if 'd1f' in kwargs:
kwargs['df'] = kwargs['d1f']
kwargs['tol'] = tol
if isinstance(x0, (list, tuple)):
x0 = [ctx.convert(x) for x in x0]
else:
x0 = [ctx.convert(x0)]
if isinstance(solver, str):
try:
solver = str2solver[solver]
except KeyError:
raise ValueError('could not recognize solver')
# accept list of functions
if isinstance(f, (list, tuple)):
f2 = copy(f)
def tmp(*args):
return [fn(*args) for fn in f2]
f = tmp
# detect multidimensional functions
try:
fx = f(*x0)
multidimensional = isinstance(fx, (list, tuple, ctx.matrix))
except TypeError:
fx = f(x0[0])
multidimensional = False
if 'multidimensional' in kwargs:
multidimensional = kwargs['multidimensional']
if multidimensional:
# only one multidimensional solver available at the moment
solver = MDNewton
if not 'norm' in kwargs:
norm = lambda x: ctx.norm(x, 'inf')
kwargs['norm'] = norm
else:
norm = kwargs['norm']
else:
norm = abs
# happily return starting point if it's a root
if norm(fx) == 0:
if multidimensional:
return ctx.matrix(x0)
else:
return x0[0]
# use solver
iterations = solver(ctx, f, x0, **kwargs)
if 'maxsteps' in kwargs:
maxsteps = kwargs['maxsteps']
else:
maxsteps = iterations.maxsteps
i = 0
for x, error in iterations:
if verbose:
print('x: ', x)
print('error:', error)
i += 1
if error < tol * max(1, norm(x)) or i >= maxsteps:
break
else:
if not i:
raise ValueError('Could not find root using the given solver.\n'
'Try another starting point or tweak arguments.')
if not isinstance(x, (list, tuple, ctx.matrix)):
xl = [x]
else:
xl = x
if verify and norm(f(*xl))**2 > tol: # TODO: better condition?
raise ValueError('Could not find root within given tolerance. '
'(%s > %s)\n'
'Try another starting point or tweak arguments.'
% (norm(f(*xl))**2, tol))
return x
finally:
ctx.prec = prec
def multiplicity(ctx, f, root, tol=None, maxsteps=10, **kwargs):
"""
Return the multiplicity of a given root of f.
Internally, numerical derivatives are used. This might be inefficient for
higher order derviatives. Due to this, ``multiplicity`` cancels after
evaluating 10 derivatives by default. You can be specify the n-th derivative
using the dnf keyword.
>>> from mpmath import *
>>> multiplicity(lambda x: sin(x) - 1, pi/2)
2
"""
if tol is None:
tol = ctx.eps ** 0.8
kwargs['d0f'] = f
for i in xrange(maxsteps):
dfstr = 'd' + str(i) + 'f'
if dfstr in kwargs:
df = kwargs[dfstr]
else:
df = lambda x: ctx.diff(f, x, i)
if not abs(df(root)) < tol:
break
return i
def steffensen(f):
"""
linear convergent function -> quadratic convergent function
Steffensen's method for quadratic convergence of a linear converging
sequence.
Don not use it for higher rates of convergence.
It may even work for divergent sequences.
Definition:
F(x) = (x*f(f(x)) - f(x)**2) / (f(f(x)) - 2*f(x) + x)
Example
.......
You can use Steffensen's method to accelerate a fixpoint iteration of linear
(or less) convergence.
x* is a fixpoint of the iteration x_{k+1} = phi(x_k) if x* = phi(x*). For
phi(x) = x**2 there are two fixpoints: 0 and 1.
Let's try Steffensen's method:
>>> f = lambda x: x**2
>>> from mpmath.calculus.optimization import steffensen
>>> F = steffensen(f)
>>> for x in [0.5, 0.9, 2.0]:
... fx = Fx = x
... for i in xrange(9):
... try:
... fx = f(fx)
... except OverflowError:
... pass
... try:
... Fx = F(Fx)
... except ZeroDivisionError:
... pass
... print('%20g %20g' % (fx, Fx))
0.25 -0.5
0.0625 0.1
0.00390625 -0.0011236
1.52588e-05 1.41691e-09
2.32831e-10 -2.84465e-27
5.42101e-20 2.30189e-80
2.93874e-39 -1.2197e-239
8.63617e-78 0
7.45834e-155 0
0.81 1.02676
0.6561 1.00134
0.430467 1
0.185302 1
0.0343368 1
0.00117902 1
1.39008e-06 1
1.93233e-12 1
3.73392e-24 1
4 1.6
16 1.2962
256 1.10194
65536 1.01659
4.29497e+09 1.00053
1.84467e+19 1
3.40282e+38 1
1.15792e+77 1
1.34078e+154 1
Unmodified, the iteration converges only towards 0. Modified it converges
not only much faster, it converges even to the repelling fixpoint 1.
"""
def F(x):
fx = f(x)
ffx = f(fx)
return (x*ffx - fx**2) / (ffx - 2*fx + x)
return F
OptimizationMethods.jacobian = jacobian
OptimizationMethods.findroot = findroot
OptimizationMethods.multiplicity = multiplicity
if __name__ == '__main__':
import doctest
doctest.testmod()