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power_spectrum.py
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power_spectrum.py
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"""
Package: Qtools
Module: power_spectrum
(C) 2020-2022 Andreas H. Nielsen
See README.md for further details.
"""
import numpy as np
from math import pi, sqrt, ceil
from qtools import time_history
from qtools.config import set_module, Info, version
class Spectrum:
"""Base class for Fourier and power spectra.
Attributes
----------
f : 1D NumPy array
Frequency in Hz.
unit : str, optional
Unit of the spectral ordinates (e.g. 'g**2*s'). Used only for plotting.
label : str
A user-defined label.
fmt : str
The line format to be used when plotting this spectrum (see notes on
`fmt` parameter in the `Matplotlib documentation
<https://matplotlib.org/api/_as_gen/matplotlib.pyplot.plot.html>`_).
"""
def __init__(self, f, unit=None, label='_nolegend_', fmt=''):
self.f = f
self.unit = unit
self.label = label
self.fmt = fmt
def setLabel(self, label):
"""Sets the label of the spectrum."""
self.label = str(label)
def setUnit(self, unit):
"""Sets the unit of the spectral ordinates."""
self.label = str(unit)
def setLineFormat(self, fmt):
"""Sets the `fmt` attribute equal to the supplied argument."""
self.fmt = str(fmt)
@set_module('qtools')
class PowerSpectrum(Spectrum):
"""
This class provides attributes and methods for power spectra.
Parameters
----------
f : 1D NumPy array
Frequency in Hz.
Wf : 1D NumPy array
Single-sided power spectral density as a function of frequency (Hz).
unit : str, optional
Unit of the spectral ordinates (e.g. 'g**2*s'). Used only for plotting.
label : str, optional
A user-defined label (inherited from the time history when the
:func:`.calcps` function is used).
fmt : str, optional
The line format to be used when plotting this spectrum (see notes on
`fmt` parameter in the `Matplotlib documentation
<https://matplotlib.org/api/_as_gen/matplotlib.pyplot.plot.html>`_)
Attributes
----------
f : 1D NumPy array
Frequency in Hz.
w : 1D NumPy array.
Circular frequency in rad/s.
Wf : 1D NumPy array
Single-sided power spectral density as a function of frequency (Hz).
Gw : 1D NumPy array
Single-sided power spectral density as a function of circular frequency
(rad/s).
unit : str
Unit of the spectral ordinates (e.g. 'g**2*s'). Used only for plotting.
label : str
A user-defined label (inherited from the time history when the calcps()
method is used).
fmt : str
The line format to be used when plotting this spectrum (see notes on
`fmt` parameter in the `Matplotlib documentation
<https://matplotlib.org/api/_as_gen/matplotlib.pyplot.plot.html>`_).
Notes
-----
In Qtools, the term `power spectrum` is synonymous with `power spectral
density`. All instances of this class contain power spectral densities.
The different frequency measures are related by :math:`\\omega = 2 \\pi f`
where :math:`f` is the frequency in Hz and :math:`\\omega` is the circular
frequency in rad/s. The different spectral densities are related by:
.. math::
W(f) = 2 \\pi G(\\omega)
"""
def __init__(self, f, Wf, unit=None, label='_nolegend_', fmt=''):
Spectrum.__init__(self, f, unit=unit, label=label, fmt=fmt)
self.Wf = Wf
self.w = 2*pi*f
self.Gw = Wf/(2*pi)
def moment(self, n):
"""
Calculates an approximation to the n'th moment of the
power spectrum defined as:
.. math::
\\lambda_{n} = \\int_{0}^{\\infty} \\omega^{n} G(\\omega)d\\omega
where :math:`G(\\omega)` is the one-sided power spectral density
function.
Parameters
----------
n : int
The order of the moment.
Returns
-------
A float approximating the n'th moment.
"""
return np.trapz(self.w**n*self.Gw, x=self.w)
def moments(self, *ns):
"""Calculate multiple moments in one go. See :meth:`moment` for
further information.
Parameters
----------
\*ns : int
One or more integers.
Returns
-------
List
A list of moments whose length is equal to the number of arguments
provided to the method.
"""
return [self.moment(n) for n in ns]
def rms(self):
"""
This method calculates the root mean square from the power spectrum.
"""
return sqrt(self.moment(0))
@set_module('qtools')
class FourierSpectrum(Spectrum):
"""
This class provides attributes and methods for Fourier spectra.
Parameters
----------
f : 1D NumPy array
Frequency in Hz.
X : 1D NumPy array
Complex Fourier amplitudes.
dt : float
Time step.
unit : str, optional
Unit of the spectrum (e.g. 'g'). Used only for plotting.
label : str, optional
A user-defined label (inherited from the time history when the
:func:`.calcfs` function is used)
fmt : str, optional
The line format to be used when plotting this spectrum (see notes on
`fmt` parameter in the `Matplotlib documentation
<https://matplotlib.org/api/_as_gen/matplotlib.pyplot.plot.html>`_)
Attributes
----------
f : 1D NumPy array
Frequency in Hz.
X : 1D NumPy array
Complex Fourier amplitudes.
dt : float
Time step.
unit : str
Unit of the spectrum (e.g. 'g'). Used for plotting.
label : str
A user-defined label (inherited from the time history when the calcps()
method is used).
fmt : str
The line format to be used when plotting this spectrum (see notes on
`fmt` parameter in the `Matplotlib documentation
<https://matplotlib.org/api/_as_gen/matplotlib.pyplot.plot.html>`_).
Notes
-----
The absolute amplitude `|X|` of the spectrum is used for plotting.
"""
def __init__(self, f, X, N, dt, L=0, unit=None, label='_nolegend_', fmt=''):
Spectrum.__init__(self, f, unit=unit, label=label, fmt=fmt)
self.X = X
self.N = N
self.L = L
self.dt = dt
def abs(self):
"""Returns the absolute amplitude as a NumPy array."""
return np.absolute(self.X)
@set_module('qtools')
def calcps(th):
"""
Calculates an estimate of the power spectrum corresponding to a time
history considered as a sample from a stationary and ergodic process.
Parameters
----------
th : an instance of class :class:`.TimeHistory`
The input time history.
Returns
-------
ps : an instance of :class:`.PowerSpectrum`
Notes
-----
The smoothed power spectrum is calculated in accordance with a
procedure described by `Newland (1993)`_.
References
----------
.. _Newland (1993):
Newland, D.E., 1993: *An Introduction to Random Vibrations, Spectral &
Wavelet Analysis*, 3rd Ed., Pearson Education Ltd.
"""
# Initial checks etc.
lbl = th.label if th.label != '_nolegend_' else ''
Info.note('Computing power spectum for time history {}'.format(lbl))
if type(th) != time_history.TimeHistory:
raise TypeError('The th parameter must be specified as an instance of'
' class TimeHistory')
if not th.dt_fixed:
raise ValueError('To compute a power spectrum, a time history must be'
' defined with fixed time step')
if th.ordinate == 'a':
unit = 'm**2/s**3'
elif th.ordinate == 'v':
unit = 'm**2/s'
elif th.ordinate == 'd':
unit = 'm**2*s'
else:
Info.warn('The time history does not represent acceleration, '
'velocity or displacement.')
# Ensure time history has zero mean
th.zero_mean()
# Determine required size of array. This will pad the input th with zeros
# up to first 2**p integer that is greater than th.ndat)
N = th.ndat
p = 1
while N-2**p > 0:
p += 1
M = 2**p
# Execute FFT
Xc = 1/M*np.fft.rfft(th.data, n=M)
K = np.size(Xc)
# Fourier amplitude
X = np.absolute(Xc)
# Durations and frequencies
# NB: the period T of the signal is the duration of the time history plus
# a time step
TL = th.dt*M
T = th.Td+th.dt
f = np.fft.rfftfreq(M, d=th.dt)
# Unsmoothed spectrum
Sk = M/N*TL/(2*pi)*X**2
# Calculate smoothed spectrum
#
# TO DO: Investigate whether smoothing should be done over an interval
# that is proportional to frequency (such that smoothing covers a wider
# frequency band at higher frequencies)
#
# Assume the required bandwidth is 0.5Hz
Be = 0.5
ns = ceil(M*Be*T/(2*N)-0.5)
#Info.note('Smoothing parameter ns = ',ns)
Sw = np.zeros(K)
for k in range(K):
sswkm = 0.0
for m in range(-ns,ns+1):
i = k+m
if i < 0:
sswkm += Sk[-i]
elif i >= 0 and i < K-1:
sswkm += Sk[i]
Sw[k] = 1/(2*ns+1)*sswkm
# Convert to single-sided spectrum
Wf = 4*pi*Sw
Info.end()
# Create and return the spectrum
ps = PowerSpectrum(f, Wf, unit=unit)
ps.setLabel(th.label)
return ps
@set_module('qtools')
def calcfs(th, M=None):
"""
Calculates a Fourier spectrum from a time history.
Parameters
----------
th : an instance of class :class:`.TimeHistory`
The input time history.
M : int
Number of points in the input time history to use. If `M` is smaller
than the length of the input (`th.ndat`), the input is cropped. If it
is larger, the input is padded with zeros. If `M` is not given, the
length of the input along the axis specified by axis is used.
Returns
-------
fs : an instance of :class:`.FourierSpectrum`
Notes
-----
The time history must have fixed time step. The original time history is
recovered exactly (within numerical precision) by using :func:`.calcth`
provided ``M = th.ndat``.
"""
# Initial checks etc.
if type(th) != time_history.TimeHistory:
raise TypeError('The th parameter must be specified as an instance of'
' class TimeHistory')
if not th.dt_fixed:
raise ValueError('To compute a Fourier spectrum, a time history must'
' be defined with fixed time step')
# Determine required size of array
if M is None:
N = th.ndat
else:
N = M
# L is the number of zeros added to the time history
L = N - th.ndat
# Execute FFT
X = 1/N*np.fft.rfft(th.data, n=M)
f = np.fft.rfftfreq(N, d=th.dt)
# Output
Info.note('Converting time history {} into a Fourier'
' spectrum.'.format(th.label))
if L == 0:
Info.note('The original length of the time history is used with'
' {} data points'.format(N))
elif L > 0:
Info.note('Added {} zeros ({:5.2f} sec) to the end of the time'
' history.'.format(L,L*th.dt))
else:
Info.warn('Removed {} data points from the end of the'
' time history.'.format(L))
# Create and return the spectrum
Info.end()
fs = FourierSpectrum(f, X, N, th.dt, L)
fs.setLabel(th.label)
return fs
@set_module('qtools')
def transfer(ps, fn, xi, tfun=0):
"""
Transfers a spectrum from base to in-structure for a SDOF system.
Parameters
----------
ps : a instance of class PowerSpectrum or FourierSpectrum
Input spectum.
fn : float
Center frequency of the transfer function.
xi : float
Damping ratio of the transfer function.
tfun : int, optional
Type of transfer function: see notes below. The default is 0.
Returns
-------
An instance of class PowerSpectrum or FourierSpectrum
Output spectrum.
Notes
-----
The following SDOF transfer functions are supported:
0. Input: total acceleration --> output: relative displacement
1. Input: total acceleration --> output: total acceleration
All transfer functions assume viscous damping.
"""
wn = 2*pi*fn
w = 2*pi*ps.f
if isinstance(ps, PowerSpectrum):
if tfun==0:
if ps.unit=='m**2/s**3':
unit = 'm**2*s'
else:
Info.warn('Could not recognise unit in transfer function.')
unit = None
H2 = 1/((wn**2 - w**2)**2 + (2*xi*wn*w)**2)
elif tfun==1:
unit = ps.unit
H2 = (wn**4 + (2*xi*wn*w)**2)/((wn**2 - w**2)**2 + (2*xi*wn*w)**2)
Wy = H2*ps.Wf
return PowerSpectrum(ps.f, Wy, unit=unit)
if isinstance(ps, FourierSpectrum):
if tfun==0:
if ps.unit=='m/s**2':
unit = 'm'
else:
unit = None
H = -1/(wn**2 - w**2 + 2*1j*xi*wn*w)
elif tfun==1:
H = -(2*1j*xi*wn*w + wn**2)/(wn**2 - w**2 + 2*1j*xi*wn*w)
Y = H*ps.X
return FourierSpectrum(ps.f, Y, ps.N, ps.dt, L=ps.L, unit=unit)
@set_module('qtools')
def savesp(ps, fname, abscissa='f', fmt='%.18e', delimiter=' ',
newline='\n', header='_default_', footer='', comments='# '):
"""Save the spectrum to text file. This function uses
:func:`numpy.savetxt` to perform the output operation. See
documentation for :func:`numpy.savetxt` to understand the full
functionality.
Parameters
----------
ps : an instance of class FourierSpectrum or PowerSpectrum
The spectrum to be saved to file.
fname : str
Filename or file handle. See :func:`numpy.savetxt`.
abscissa : str
If set equal to 'w', then the abscissa will be circular frequency
(in rad/s), otherwise it will be linear frequency (in Hz).
This parameter will be ignored when `ps` is a Fourier spectrum.
For consistency, when ``abscissa == 'w'``, the ordinate will be divided
by :math:`2\\pi`. Default 'f'.
fmt : str or sequence of strs, optional
See :func:`numpy.savetxt`.
delimiter : str, optional
String or character separating columns.
newline : str, optional
String or character separating lines.
header : str, optional
If `header` is not specified, a default header will be generated
by this function. Set ``header = ''`` to avoid any header being
written. All other parameter values will be passed directly to
:func:`numpy.savetxt`.
footer : str, optional
String that will be written at the end of the file.
comments : str, optional
String that will be prepended to the `header` and `footer` strings,
to mark them as comments.
"""
if isinstance(ps, FourierSpectrum):
head0 = 'Fourier '
head2 = 'f [Hz], X [{}]'.format(ps.unit)
out = np.array([ps.f,ps.X])
elif isinstance(ps, PowerSpectrum):
head0 = 'Power '
if abscissa=='f':
head2 = 'f [Hz], Wf [{}]'.format(ps.unit)
out = np.array([ps.f, ps.Wf])
elif abscissa=='w':
head2 = 'w [rad/s], Gw [{}]'.format(ps.unit)
out = np.array([2*pi*ps.f, ps.Sw/(2*pi)])
else:
raise TypeError('Wrong type of object supplied as first argument.')
if header=='_default_':
lbl = ps.label+' ' if ps.label != '_nolegend_' else ''
head1 = head0+'spectrum {}computed by Qtools v. {}\n'.format(lbl,version)
header = head1+head2
np.savetxt(fname, out.T, fmt=fmt, delimiter=delimiter, newline=newline,
header=header, footer=footer, comments=comments)
@set_module('qtools')
def kanai_tajimi(we, wg, xig, G0=1, wc=None, xic=1.0, unit='m**2/s**3'):
"""
Computes the Kanai-Tajimi power spectrum.
Parameters
----------
we : NumPy 1D array
Exicitation frequencies in rad/s.
wg : float
Ground frequency. Typical values are between 15 rad/s (soft ground)
and 40 rad/s (hard ground).
xig : float
Ground damping. Typical values are between 0.3 and 0.6.
G0 : float, optional
Factor used to scale the spectrum. The default is 1.
wc : float, optional
Ground frequency in the Clough & Penzien correction term (see notes
below). If not specified, the correction term is not applied.
xic : float, optional
Ground damping in the Clough & Penzien correction term (see notes
below).
unit : str, optional
Unit of the power spectrum. The default value ('m**2/s**3') is
appropriate for an acceleration spectrum.
Returns
-------
ps : an instance of :class:`.PowerSpectrum`
Notes
-----
This function returns the Kanai-Tajimi power spectrum (see e.g.
`Kramer (1996)`_). Optionally, the correction proposed by `Clough &
Penzien (2003)`_ may be applied. The correction attenuates the spectral
density at low frequencies and ensures that `G(0) = 0`. The parameters
`wc` and `xic` (which Clough & Penzien denote :math:`\\omega_2` and
:math:`\\xi_2`, respectively) must be set appropriately to produce the
desired attenuation. In particular, `wc` should be less than `wg`.
It should be noted that the `n`th spectral moment is infinite (and
therefore meaningless) for `n` >= 2.
References
----------
.. _Kramer (1996):
Kramer, S.L., 1996: *Geotechnical Earthquake Engineering*, Prentice-Hall.
.. _Clough & Penzien (2003):
Clough, R.W., & Penzien, J., 2003: *Dynamics of Structures*, 3rd Edition,
Computers & Structures, Inc.
"""
H1 = (1 + 2*1j*xig*we/wg)/(1 - (we/wg)**2 + 2*1j*xig*we/wg)
if isinstance(wc, float):
H = H1*(we/wc)**2/(1 - (we/wc)**2 + 2*1j*xic*we/wc)
label = 'Kanai-Tajimi (Clough-Penzien)'
else:
H = H1
label = 'Kanai-Tajimi'
ps = PowerSpectrum(we/(2*pi), G0*np.abs(H)**2, unit=unit, label=label)
return ps
@set_module('qtools')
def band_limited(we, wc, bw, G0=1, unit='m**2/s**3'):
"""
Returns a band-limited constant power spectrum.
Parameters
----------
we : NumPy 1D array
Exicitation frequencies in rad/s.
wc : float
Central frequency.
bw : float
Bandwidth.
G0 : float, optional
Factor used to scale the spectrum. The default is 1.
unit : str, optional
Unit of the power spectrum. The default value ('m**2/s**3') is
appropriate for an acceleration spectrum.
Returns
-------
ps : an instance of :class:`.PowerSpectrum`
Notes
-----
This function returns a band-limited power spectrum with constant
amplitude G0. The lower frequency is computed as
`w0` = max(0, `wc` - `bw`/2) and the upper frequency is computed as
`w1` = `wc` + `bw`/2. A warning is issued if `wc` - `bw`/2 < 0.
"""
if wc - bw/2 < 0:
Info.warn('With the supplied parameters, the lower frequency would'
'be less than zero. The lower frequency is set to zero.')
w0 = max(0, wc - bw/2)
w1 = wc + bw/2
Gw = np.where(np.logical_and(we > w0, we < w1), G0, 0)
label = 'Band-limited'
ps = PowerSpectrum(we/(2*pi), 2*pi*Gw, unit=unit, label=label)
return ps