def __init__(self, fpath):
""" Visualisation and data extraction from pyxe data object/hdf5 file.
Builds on the PeakAnalysis class, allowing for the 1d/2d vizualisation
of 1d/2d/3d data acquisition arrays. Provides functionality for
array re-alignment (flipping, swapping axes, re-centering). Also
allows for data to be saved to a text file.
Args:
fpath (str): Path to pyxe hdf5 file.
"""
self.fpath = fpath
with h5py.File(fpath, 'r') as f:
self.ndim, self.d1, self.d2, self.d3 = data_extract(f, 'dims')
self.q, self.I, self.phi = data_extract(f, 'raw')
self.peaks, self.peaks_err = data_extract(f, 'peaks')
self.fwhm, self.fwhm_err = data_extract(f, 'fwhm')
self.strain, self.strain_err = data_extract(f, 'strain')
self.strain_tensor = data_extract(f, 'tensor')[0]
self.E, self.v, self.G = data_extract(f, 'material')
self.stress_state, self.analysis_state = data_extract(f, 'state')
self.detector = detector_extract(f)
if self.stress_state is None:
self.stress_eqn = None
else:
p_strain = self.stress_state == 'plane strain'
self.stress_eqn = plane_strain if p_strain else plane_stress
def __init__(self, fpath):
""" Visualisation and data extraction from pyxe data object/hdf5 file.
Builds on the PeakAnalysis class, allowing for the 1d/2d vizualisation
of 1d/2d/3d data acquisition arrays. Provides functionality for
array re-alignment (flipping, swapping axes, re-centering). Also
allows for data to be saved to a text file.
Args:
fpath (str): Path to pyxe hdf5 file.
"""
self.fpath = fpath
with h5py.File(fpath, 'r') as f:
self.ndim, self.d1, self.d2, self.d3 = data_extract(f, 'dims')
self.q, self.I, self.phi = data_extract(f, 'raw')
self.peaks, self.peaks_err = data_extract(f, 'peaks')
self.fwhm, self.fwhm_err = data_extract(f, 'fwhm')
self.strain, self.strain_err = data_extract(f, 'strain')
self.strain_tensor = data_extract(f, 'tensor')[0]
self.E, self.v, self.G = data_extract(f, 'material')
self.stress_state, self.analysis_state = data_extract(f, 'state')
self.detector = detector_extract(f)
if self.stress_state is None:
self.stress_eqn = None
else:
p_strain = self.stress_state == 'plane strain'
self.stress_eqn = plane_strain if p_strain else plane_stress
def __init__(self, fpath):
""" Analysis class for the calculation of peaks and strain.
The analysis is based around two peak fitting methods - single peak
and Pawley refinement. The Pawley refinement requires a more complete
description of the constituent material/phases and returns a lattice
parameter, whereas the single peak analysis returns a particular
lattice spacing, d0, or rather the reciprocal equivalent, q0.
The strain analysis follows naturally from this via a simple strain
calculation (e = delta_a / a0), with the variation in strain wrt.
azimuthal position allowing for the computation of the full strain
tensor (e_xx, e_yy, e_xy).
It is then possible to finalise the analytical procedure and calculate
stress, which relies on the material system being in a plane strain
or plane stress state. The in-plane stress state can then be
determined.
Args:
fpath (str): Path to an analyzed (integrated) pyxe hdf5 file
"""
self.fpath = fpath
with h5py.File(fpath, 'r') as f:
self.ndim, self.d1, self.d2, self.d3 = data_extract(f, 'dims')
self.q, self.I, self.phi = data_extract(f, 'raw')
self.peaks, self.peaks_err = data_extract(f, 'peaks')
self.fwhm, self.fwhm_err = data_extract(f, 'fwhm')
self.strain, self.strain_err = data_extract(f, 'strain')
self.strain_tensor = data_extract(f, 'tensor')[0]
self.E, self.v, self.G = data_extract(f, 'material')
self.stress_state, self.analysis_state = data_extract(f, 'state')
self.detector = detector_extract(f)
if self.stress_state is None:
self.stress_eqn = None
else:
p_strain = self.stress_state == 'plane strain'
self.stress_eqn = plane_strain if p_strain else plane_stress
def __init__(self, fpath):
""" Analysis class for the calculation of peaks and strain.
The analysis is based around two peak fitting methods - single peak
and Pawley refinement. The Pawley refinement requires a more complete
description of the constituent material/phases and returns a lattice
parameter, whereas the single peak analysis returns a particular
lattice spacing, d0, or rather the reciprocal equivalent, q0.
The strain analysis follows naturally from this via a simple strain
calculation (e = delta_a / a0), with the variation in strain wrt.
azimuthal position allowing for the computation of the full strain
tensor (e_xx, e_yy, e_xy).
It is then possible to finalise the analytical procedure and calculate
stress, which relies on the material system being in a plane strain
or plane stress state. The in-plane stress state can then be
determined.
Args:
fpath (str): Path to an analyzed (integrated) pyxe hdf5 file
"""
self.fpath = fpath
with h5py.File(fpath, 'r') as f:
self.ndim, self.d1, self.d2, self.d3 = data_extract(f, 'dims')
self.q, self.I, self.phi = data_extract(f, 'raw')
self.peaks, self.peaks_err = data_extract(f, 'peaks')
self.fwhm, self.fwhm_err = data_extract(f, 'fwhm')
self.strain, self.strain_err = data_extract(f, 'strain')
self.strain_tensor = data_extract(f, 'tensor')[0]
self.E, self.v, self.G = data_extract(f, 'material')
self.stress_state, self.analysis_state = data_extract(f, 'state')
self.detector = detector_extract(f)
if self.stress_state is None:
self.stress_eqn = None
else:
p_strain = self.stress_state == 'plane strain'
self.stress_eqn = plane_strain if p_strain else plane_stress
