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- builtins.object
-
- MultiPlotting
- Plotting
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- PlottingSuperstructure
class MultiPlotting(builtins.object) |
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MultiPlotting(crystal_list)
Plotting functions for the Multi-Crystal Object |
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Methods defined here:
- __init__(self, crystal_list)
- Initialize self. See help(type(self)) for accurate signature.
- quick_intensity_cut(self, x_axis_crystal=[[1, 0, 0]], y_axis_crystal=[[0, 1, 0]], centre=[0, 0, 0], q_max=4.0, cut_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity as different sized markers
x_axis = direction along x, in units of the reciprocal lattice (hkl)
y_axis = direction along y, in units of the reciprocal lattice (hkl)
centre = centre of the plot, in units of the reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
E.G. hk plot at L=3 for hexagonal system:
xtl.quick_intensity_cut([1,0,0],[0,1,0],[0,0,3])
hhl plot:
xtl.quick_intensity_cut([1,1,0],[0,0,1],[0,0,0])
- simulate_intensity_cut(self, x_axis_crystal=[[1, 0, 0]], y_axis_crystal=[[0, 1, 0]], centre=[0, 0, 0], q_max=4.0, cut_width=0.05, background=0.0, peak_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity
x_axis_crystal = list of crytal x-directions in (hkl), for each crystal
y_axis_crystal = list of crytal y-directions in (hkl), for each crystal
centre = centre of the plot, in units of the reciprocal lattice (hkl) of crystal 1
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
background = average background value
peak_width = reflection width in A-1
E.G. hk plot at L=3 for hexagonal system (xtl1) with xtl2 oriented with the (110) alond xtl1's (100):
xtls = multi_crystal([xtl1,xtl2])
xtl.simulate_intensity_cut([[1,0,0],[1,1,0]],[[0,1,0],[0,0,1]],[0,0,3])
- simulate_powder(self, energy_kev=8.0, peak_width=0.05, background=0, powder_average=True)
- Generates a powder pattern for multiple phases
see classes_scattering.generate_powder
Data descriptors defined here:
- __dict__
- dictionary for instance variables (if defined)
- __weakref__
- list of weak references to the object (if defined)
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class Plotting(builtins.object) |
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Plotting(xtl)
Plotting functions for the Crystal Object |
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Methods defined here:
- __init__(self, xtl)
- initialise
- axis_reciprocal_lattice_lines(self, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05, axes=None, *args, **kwargs)
- Add lines to the current axis showing the reciprocal lattice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:param axes: None for plt.gca() or axis of choice
:param args: argments to pass to plot function, e.g. linewidth, alpha, color
:return: None
- axis_reciprocal_lattice_points(self, axes=None, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05, **kwargs)
- Add lines to the current axis showing the reciprocal lattice
:param axes: None for plt.gca() or axis of choice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:param kwargs: keyword arguments to pass to plt.plot(..., **kwargs)
:return: None
- axis_reciprocal_lattice_vectors(self, axes=None, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05)
- Add lines to the current axis showing the reciprocal lattice
:param axes: None for plt.gca() or axis of choice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:return: None
- generate_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05, background=0.0, peak_width=0.05)
- Generate a cut through reciprocal space, returns an array with centred reflections
Inputs:
x_axis = direction along x, in units of the reciprocal lattice (hkl)
y_axis = direction along y, in units of the reciprocal lattice (hkl)
centre = centre of the plot, in units of the reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
background = average background value
peak_width = reflection width in A-1
Returns:
Qx/Qy = [1000x1000] array of coordinates
plane = [1000x1000] array of plane in reciprocal space
E.G. hk plane at L=3 for hexagonal system:
Qx,Qy,plane = xtl.generate_intensity_cut([1,0,0],[0,1,0],[0,0,3])
plt.figure()
plt.pcolormesh(Qx,Qy,plane)
plt.axis('image')
- plot_3Dlattice(self, q_max=4.0, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], cut_width=0.05)
- Plot lattice points in 3D
- plot_3Dpolarisation(self, hkl, energy_kev=None, polarisation='sp', azim_zero=[1, 0, 0], psi=0)
- Plots the scattering vectors for a particular azimuth
:param hkl:
:param energy_kev:
:param polarisation:
:param azim_zero:
:param psi:
:return: None
- plot_crystal(self, show_labels=False)
- Plot the atomic cell in 3D
Click and drag to rotate the structure in 3D
Atoms are coloured according to their label
set show_labels=True to show the label of each sphere
- plot_diffractometer_reciprocal_space(self, energy_kev, delta=0, gamma=0)
- Plot diffractometer angles using orientation
:param energy_kev:
:param delta:
:param gamma:
:return: None
- plot_exchange_paths(self, cen_idx, nearest_neighbor_distance=6.6, exchange_type='O', bond_angle=90.0, search_in_cell=True, group_neighbors=True, disp=False)
- Calcualtes exchange paths and adds them to the crystal structure plot
:param cen_idx: index of central ion in xtl.Structure
:param nearest_neighbor_distance: Maximum radius to serach to
:param exchange_type: str or None. Exchange path only incoroporates these elements, or None for any
:param bond_angle: float. Search for exchange ions withing this angle to the bond
:param search_in_cell: Bool. If True, only looks for neighbors within the unit cell
:param group_neighbors: Bool. If True, only shows neighbors with the same bond distance once
:param disp: Bool. If True, prints details of the calcualtion
:return:
- plot_layers(self, layers=None, layer_axis=2, layer_width=0.05, show_labels=False)
- Separate the structure into layers along the chosen axis
and plot the atoms in each layer in a separate figure.
:param layers: list of layers to plot in fractional coordinates, or NOne for automatic determination
:param layer_axis: axis (0,1,2) of direction normal to layers
:param layer_width: distance from layer value to include in plot
:param show_labels: False*/True add text labels
:return:
- plot_ms_azimuth(self, hkl, energy_kev, azir=[0, 0, 1], pv=[1, 0], numsteps=3, peak_width=0.1, full=False, pv1=False, pv2=False, sfonly=True, pv1xsf1=False, log=False)
- Run the multiple scattering code and plot the result
See multiple_scattering.py for more details.
:param xtl: Crystal structure from Dans_Diffraction
:param hkl: [h,k,l] principle reflection
:param energy_kev: calculation energy
:param azir: [h,k,l] reference of azimuthal 0 angle
:param pv: [s,p] polarisation vector
:param numsteps: int: number of calculation steps from energy min to max
:param full: True/False: calculation type: full
:param pv1: True/False: calculation type: pv1
:param pv2: True/False: calculation type: pv2
:param sfonly: True/False: calculation type: sfonly *default
:param pv1xsf1: True/False: calculation type: pv1xsf1?
:param log: log y scale
:return: None
- plot_multiple_scattering(self, hkl, azir=[0, 0, 1], pv=[1, 0], energy_range=[7.8, 8.2], numsteps=60, full=False, pv1=False, pv2=False, sfonly=True, pv1xsf1=False)
- Run the multiple scattering code and plot the result
See multiple_scattering.py for more details.
:param xtl: Crystal structure from Dans_Diffraction
:param hkl: [h,k,l] principle reflection
:param azir: [h,k,l] reference of azimuthal 0 angle
:param pv: [s,p] polarisation vector
:param energy_range: [min, max] energy range in keV
:param numsteps: int: number of calculation steps from energy min to max
:param full: True/False: calculation type: full
:param pv1: True/False: calculation type: pv1
:param pv2: True/False: calculation type: pv2
:param sfonly: True/False: calculation type: sfonly *default
:param pv1xsf1: True/False: calculation type: pv1xsf1?
:return: None
- plot_xray_resonance(self, hkl, energy_kev=None, width=1.0, npoints=200)
- Plot energy scan using x-ray dispersion corrections
:param hkl: list of [h,k,l] reflections
:param energy_kev: float energy in keV to scan around
:param width: float in keV width of scan
:param npoints: int number of poins to calculate
:return: None
- quick_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity as different sized markers
x_axis = direction along x, in units of the reciprocal lattice (hkl)
y_axis = direction along y, in units of the reciprocal lattice (hkl)
centre = centre of the plot, in units of the reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
E.G. hk plot at L=3 for hexagonal system:
xtl.quick_intensity_cut([1,0,0],[0,1,0],[0,0,3])
hhl plot:
xtl.quick_intensity_cut([1,1,0],[0,0,1],[0,0,0])
- simulate_0kl(self, H=0, **kwargs)
- Plots the (H)kl layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_azimuth(self, hkl, energy_kev=None, polarisation='sp', F0=1, F1=1, F2=1, azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_azimuth_nonresonant(self, hkl, energy_kev=None, polarisation='sp', azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_azimuth_resonant(self, hkl, energy_kev=None, polarisation='sp', F0=1, F1=1, F2=1, azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_ewald_coverage(self, energy_kev=8.0, sample_normal=[0, 0, 1], sample_para=[1, 0, 0], phi=0, chi=0, **kwargs)
- NOT FINISHED
Plot ewald space coverage within a particular scattering plane
energy_kev = energy of incident radiation in keV
sample_normal = direction of scattering plane perp to beam direction
sample_para = direction of scattering plane || to beam direction
phi = rotation of lattice about scattering plane verticle
chi = rotation of lattice perpendicular to scattering plane
- simulate_h0l(self, K=0, **kwargs)
- Plots the h(K)l layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_hhl(self, HmH=0, **kwargs)
- Plots the hhl layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_hk0(self, L=0, **kwargs)
- Plots the hk(L) layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05, background=0.0, peak_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity
x_axis = direction along x, in units of the reciprocal lattice (hkl)
y_axis = direction along y, in units of the reciprocal lattice (hkl)
centre = centre of the plot, in units of the reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
background = average background value
peak_width = reflection width in A-1
E.G. hk plot at L=3 for hexagonal system:
xtl.simulate_intensity_cut([1,0,0],[0,1,0],[0,0,3])
hhl plot:
xtl.simulate_intensity_cut([1,1,0],[0,0,1],[0,0,0])
- simulate_polarisation_nonresonant(self, hkl, energy_kev=None, azim_zero=[1, 0, 0], psi=0)
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_polarisation_resonant(self, hkl, energy_kev=None, F0=1, F1=1, F2=1, azim_zero=[1, 0, 0], psi=0)
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_powder(self, energy_kev=None, peak_width=0.01, background=0, powder_average=True)
- Generates a powder pattern, plots in a new figure with labels
see classes_scattering.generate_powder
Data descriptors defined here:
- __dict__
- dictionary for instance variables (if defined)
- __weakref__
- list of weak references to the object (if defined)
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class PlottingSuperstructure(Plotting) |
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PlottingSuperstructure(xtl)
Plotting functions for Superstructure class crystal object
Copies the functions from Plotting, but changes several functions to apply additional actions
This changes the behaviour of the xtl.Plot functions such as xtl.Plot.simulate_hk0()
generate_intensity_cut & simulate_intensity_cut
- Refelctions are symmetrised by the parent symmetry, accounting for multiple superlattice domains
- Generated plots have lines and vectors associated with parent structure
- Effects functions such as xtl.Plot.simulate_hk0() |
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- Method resolution order:
- PlottingSuperstructure
- Plotting
- builtins.object
Methods defined here:
- generate_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05, background=0.0, peak_width=0.05)
- Generate a cut through reciprocal space, returns an array with centred reflections
Inputs:
x_axis = direction along x, in units of the parent reciprocal lattice (hkl)
y_axis = direction along y, in units of the parent reciprocal lattice (hkl)
centre = centre of the plot, in units of the parent reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
background = average background value
peak_width = reflection width in A-1
Returns:
qx/qy = [1000x1000] array of coordinates
plane = [1000x1000] array of plane in reciprocal space
E.G. hk plane at L=3 for hexagonal system:
qx,qy,plane = xtl.generate_intensity_cut([1,0,0],[0,1,0],[0,0,3])
plt.figure()
plt.pcolormesh(qx,qy,plane)
plt.axis('image')
- simulate_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05, background=0.0, peak_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity
x_axis = direction along x, in units of the parent reciprocal lattice (hkl)
y_axis = direction along y, in units of the parent reciprocal lattice (hkl)
centre = centre of the plot, in units of the parent reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
background = average background value
peak_width = reflection width in A-1
E.G. hk plot at L=3 for hexagonal system:
xtl.simulate_intensity_cut([1,0,0],[0,1,0],[0,0,3])
hhl plot:
xtl.simulate_intensity_cut([1,1,0],[0,0,1],[0,0,0])
Methods inherited from Plotting:
- __init__(self, xtl)
- initialise
- axis_reciprocal_lattice_lines(self, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05, axes=None, *args, **kwargs)
- Add lines to the current axis showing the reciprocal lattice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:param axes: None for plt.gca() or axis of choice
:param args: argments to pass to plot function, e.g. linewidth, alpha, color
:return: None
- axis_reciprocal_lattice_points(self, axes=None, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05, **kwargs)
- Add lines to the current axis showing the reciprocal lattice
:param axes: None for plt.gca() or axis of choice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:param kwargs: keyword arguments to pass to plt.plot(..., **kwargs)
:return: None
- axis_reciprocal_lattice_vectors(self, axes=None, x_axis=(1, 0, 0), y_axis=(0, 1, 0), centre=(0, 0, 0), q_max=4.0, cut_width=0.05)
- Add lines to the current axis showing the reciprocal lattice
:param axes: None for plt.gca() or axis of choice
:param x_axis: direction along x, in units of the reciprocal lattice (hkl)
:param y_axis: direction along y, in units of the reciprocal lattice (hkl)
:param centre: centre of the plot, in units of the reciprocal lattice (hkl)
:param q_max: maximum distance to plot to - in A-1
:param cut_width: width in height that will be included, in A-1
:return: None
- plot_3Dlattice(self, q_max=4.0, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], cut_width=0.05)
- Plot lattice points in 3D
- plot_3Dpolarisation(self, hkl, energy_kev=None, polarisation='sp', azim_zero=[1, 0, 0], psi=0)
- Plots the scattering vectors for a particular azimuth
:param hkl:
:param energy_kev:
:param polarisation:
:param azim_zero:
:param psi:
:return: None
- plot_crystal(self, show_labels=False)
- Plot the atomic cell in 3D
Click and drag to rotate the structure in 3D
Atoms are coloured according to their label
set show_labels=True to show the label of each sphere
- plot_diffractometer_reciprocal_space(self, energy_kev, delta=0, gamma=0)
- Plot diffractometer angles using orientation
:param energy_kev:
:param delta:
:param gamma:
:return: None
- plot_exchange_paths(self, cen_idx, nearest_neighbor_distance=6.6, exchange_type='O', bond_angle=90.0, search_in_cell=True, group_neighbors=True, disp=False)
- Calcualtes exchange paths and adds them to the crystal structure plot
:param cen_idx: index of central ion in xtl.Structure
:param nearest_neighbor_distance: Maximum radius to serach to
:param exchange_type: str or None. Exchange path only incoroporates these elements, or None for any
:param bond_angle: float. Search for exchange ions withing this angle to the bond
:param search_in_cell: Bool. If True, only looks for neighbors within the unit cell
:param group_neighbors: Bool. If True, only shows neighbors with the same bond distance once
:param disp: Bool. If True, prints details of the calcualtion
:return:
- plot_layers(self, layers=None, layer_axis=2, layer_width=0.05, show_labels=False)
- Separate the structure into layers along the chosen axis
and plot the atoms in each layer in a separate figure.
:param layers: list of layers to plot in fractional coordinates, or NOne for automatic determination
:param layer_axis: axis (0,1,2) of direction normal to layers
:param layer_width: distance from layer value to include in plot
:param show_labels: False*/True add text labels
:return:
- plot_ms_azimuth(self, hkl, energy_kev, azir=[0, 0, 1], pv=[1, 0], numsteps=3, peak_width=0.1, full=False, pv1=False, pv2=False, sfonly=True, pv1xsf1=False, log=False)
- Run the multiple scattering code and plot the result
See multiple_scattering.py for more details.
:param xtl: Crystal structure from Dans_Diffraction
:param hkl: [h,k,l] principle reflection
:param energy_kev: calculation energy
:param azir: [h,k,l] reference of azimuthal 0 angle
:param pv: [s,p] polarisation vector
:param numsteps: int: number of calculation steps from energy min to max
:param full: True/False: calculation type: full
:param pv1: True/False: calculation type: pv1
:param pv2: True/False: calculation type: pv2
:param sfonly: True/False: calculation type: sfonly *default
:param pv1xsf1: True/False: calculation type: pv1xsf1?
:param log: log y scale
:return: None
- plot_multiple_scattering(self, hkl, azir=[0, 0, 1], pv=[1, 0], energy_range=[7.8, 8.2], numsteps=60, full=False, pv1=False, pv2=False, sfonly=True, pv1xsf1=False)
- Run the multiple scattering code and plot the result
See multiple_scattering.py for more details.
:param xtl: Crystal structure from Dans_Diffraction
:param hkl: [h,k,l] principle reflection
:param azir: [h,k,l] reference of azimuthal 0 angle
:param pv: [s,p] polarisation vector
:param energy_range: [min, max] energy range in keV
:param numsteps: int: number of calculation steps from energy min to max
:param full: True/False: calculation type: full
:param pv1: True/False: calculation type: pv1
:param pv2: True/False: calculation type: pv2
:param sfonly: True/False: calculation type: sfonly *default
:param pv1xsf1: True/False: calculation type: pv1xsf1?
:return: None
- plot_xray_resonance(self, hkl, energy_kev=None, width=1.0, npoints=200)
- Plot energy scan using x-ray dispersion corrections
:param hkl: list of [h,k,l] reflections
:param energy_kev: float energy in keV to scan around
:param width: float in keV width of scan
:param npoints: int number of poins to calculate
:return: None
- quick_intensity_cut(self, x_axis=[1, 0, 0], y_axis=[0, 1, 0], centre=[0, 0, 0], q_max=4.0, cut_width=0.05)
- Plot a cut through reciprocal space, visualising the intensity as different sized markers
x_axis = direction along x, in units of the reciprocal lattice (hkl)
y_axis = direction along y, in units of the reciprocal lattice (hkl)
centre = centre of the plot, in units of the reciprocal lattice (hkl)
q_max = maximum distance to plot to - in A-1
cut_width = width in height that will be included, in A-1
E.G. hk plot at L=3 for hexagonal system:
xtl.quick_intensity_cut([1,0,0],[0,1,0],[0,0,3])
hhl plot:
xtl.quick_intensity_cut([1,1,0],[0,0,1],[0,0,0])
- simulate_0kl(self, H=0, **kwargs)
- Plots the (H)kl layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_azimuth(self, hkl, energy_kev=None, polarisation='sp', F0=1, F1=1, F2=1, azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_azimuth_nonresonant(self, hkl, energy_kev=None, polarisation='sp', azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_azimuth_resonant(self, hkl, energy_kev=None, polarisation='sp', F0=1, F1=1, F2=1, azim_zero=[1, 0, 0])
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_ewald_coverage(self, energy_kev=8.0, sample_normal=[0, 0, 1], sample_para=[1, 0, 0], phi=0, chi=0, **kwargs)
- NOT FINISHED
Plot ewald space coverage within a particular scattering plane
energy_kev = energy of incident radiation in keV
sample_normal = direction of scattering plane perp to beam direction
sample_para = direction of scattering plane || to beam direction
phi = rotation of lattice about scattering plane verticle
chi = rotation of lattice perpendicular to scattering plane
- simulate_h0l(self, K=0, **kwargs)
- Plots the h(K)l layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_hhl(self, HmH=0, **kwargs)
- Plots the hhl layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_hk0(self, L=0, **kwargs)
- Plots the hk(L) layer of reciprocal space
for inputs, see help(xtl.simulate_intensity_cut)
- simulate_polarisation_nonresonant(self, hkl, energy_kev=None, azim_zero=[1, 0, 0], psi=0)
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_polarisation_resonant(self, hkl, energy_kev=None, F0=1, F1=1, F2=1, azim_zero=[1, 0, 0], psi=0)
- Simulate azimuthal scan of resonant x-ray scattering
energy_kev = x-ray energy in keV
polarisation = x-ray polarisation: 'ss',{'sp'},'ps','pp'
F0/1/2 = Resonance factor Flm
azim_zero = [h,k,l] vector parallel to the origin of the azimuth
- simulate_powder(self, energy_kev=None, peak_width=0.01, background=0, powder_average=True)
- Generates a powder pattern, plots in a new figure with labels
see classes_scattering.generate_powder
Data descriptors inherited from Plotting:
- __dict__
- dictionary for instance variables (if defined)
- __weakref__
- list of weak references to the object (if defined)
| |


{{alert.start | date:'medium' }}
Server down for {{(alert.end - alert.start)/1000 | number: 0}} seconds (until
{{alert.end | date:'shortTime' }}).
{{alert.end | date:'MMM d, h:mm:ss a' }}).
{{alert.end | date:'medium' }}).
{{alert.start | date:'medium' }}
Response time was above the threshold ({{alert.threshold | number: 0}} ms) for {{(alert.end - alert.start) / 1000.0 | number: 0}} seconds (until
{{alert.end | date:'shortTime' }}).
{{alert.end | date:'MMM d, h:mm:ss a' }}).
{{alert.end | date:'medium' }}).
The average response time was {{alert.avg | number: 0}} ms.


Waldemar Schneider
FLAVIA IT-Management GmbH
created by "accident"
coordination of distributed system leads to boiler plate
provides tools for distributed systems
based on some netflix components
based on spring boot of course :-)
runnable machines everywhere
create instance one time
make it immutable


getting more chefs in the kitchen
Developing Infrastructure as a Team
Who Am I?
Andrew Gross
Developer at Yipit.com
WHO IS YIPIT?
New York City
24 Employees
15 "Core" Developers
1 Operations Only Developer (me)
Daily Deal Aggregation
E-Commerce Deal Aggregation
The TEchnical Challenges
Data Aggregation and Discovery
Fully Customized Emails at Scale
Image Processing
Personalization
AI
Geolocation
Problem Solving TOols
Python
C
Ruby
Javascript
Django
Flask
Tornado
Chef
AWS
SendGrid
CHEF Stack
Local
-
Berkshelf
-
Vagrant
-
Chef-Solo
-
Minitest
-
Rspec
Chef STACK
PRODUCTION
-
Chef-Client
-
Hosted Chef
-
AWS
-
Chef 10.18.2
-
Chef 11
DevelopMent Style
Cookbook Development
-
Master Chef Repo
-
Git Repo Per Cookbook
-
Application Cookbooks
-
Library Cookbooks
Developers
Developers
Developers
Why do we want
more DEVS IN CHEF?
Go beyond
localhost
Insight into:
Resiliency
Distributed Computing
Automation
Monitoring
State Transitions
Be a true full stack developer
-
Development rigor
-
Testing
-
CI / CD
-
Code Review
-
Versioning
-
Dependency Management
Sneakily reduce my own workload
What's STopping Developers?
Simple Install Wiki
Focus on basic parts of cookbooks
- Recipes
- Templates
- Attributes
Hide the rest
Use a familiar
command wrapper
(
Make,
rake,
fab
)
Java
node
.my_cookbook.my_attribute
Ruby
node[:my_cookbook][:my_attribute]
Python
node['my_cookbook']['my_attribute']
Be Opinionated
Make decisions for them
...because they don't know
(they can change it once they do)
yipit_baseline
- Every Machine
- ssh
- `chef-client` aaS
- .bash_profile
yipit_web
Nginx Version baked in
Devs don't care what version
They just want a working webserver
Chef DSL
Attributes
Library Calls
Easier to Test
Faster to Test
Easier to Reuse
Dirty Secret of Programming Incoming
Developers will cheat
Give them something good to cheat from
Use them for 'low-level' tasks
Developers should be interacting
with org. specific cookbooks
Simple
No (few) Attributes
Short Runlists
Reduce Complexity
Fewer Places to Check for Errors
Lock Cookbook Versions
Some static attributes
Versioned via Git
(w/ Knife Spork)
Endpoint Mappings
Package / Library Versions
Volatile Infrastructure Data
Require Tests for Logic
- RSpec
- simplecov
- Minitest Handler
Logic is anything not Chef DSL
Use It
Gerrit
Phabricator
Github
Comfort allows Investigation
Advancted Topics
- Handlers
- Search
- Dynamic
Configuration
- LWRPs
'Self-Managed' Services
Easier Service Deployment
The Prestige
(AMInator as a Chef Handler)


Balthazar:
How is it going? My name is Maestro Balthazar! I'm a merchant of the Black Anvil Guild. I was a much-sought-after blacksmith in my day but now I spend all of my time studying golems. If you wish to create an item you should go and ask one of my blacksmith friends!
Quest


Hey {{ contributor.get_full_name }},
Please check the amount below and make sure it matches your records. The total is ${{ total|floatformat:2 }}. If you were overpaid in August and have a credit, this is not reflected below. If you have any questions about payroll, including your credit balance, please reply to<EMAIL_ADDRESS>before {{ deadline }}. All payments will be processed by the 20th of this month.
Total: ${{ total|floatformat:2 }}
| Amount | Date | Title / Feature Type |
|---|---|---|
| ${{ contribution.pay|floatformat:2 }} | {{ contribution.content.published|date:"m/d/y" }} |
{{ contribution.content.title|safe }}
{{ contribution.content.feature_type.name }} |
| ${{ line_item.amount|floatformat:2 }} | {{ line_item.payment_date|date:"m/d/y" }} | {{ line_item.note }} |


Ms. Brenda J. DeArmas Ricci is a native of Tampa, Fla. After graduating high school, she left Florida to pursue her undergraduate education at Loyola University in New Orleans, La. Upon getting her bachelor’s degree, she attended Loyola University Law School, where she earned her Juris Doctor in 1981. That same year, she founded the Law Offices of Brenda J. DeArmas Ricci and began official operations in downtown New Orleans.
During the early years of her practice, Ms. DeArmas Ricci had only one employee, Ms. Irma J. Montemayor. In 1981, Ms. Montemayor had already gained many years of experience as a paralegal for another immigration law firm. Moreover, Ms. Montemayor has remained as Ms. DeArmas Ricci’s dedicated paralegal and secretary since the business began operations. They have worked together for over 30 years in the field of immigration law, and they have handled thousands of immigration cases.
After a brief period at 614 Tchoupitoulas St., the practice was moved to the World Trade Center in New Orleans in 1983. The business continued to expand and the staff gained notoriety for its passion and proficient knowledge regarding immigration law.
In 2007, Ms. DeArmas Ricci hired Mr. Parker S. Kornick as her law clerk. In 2009, Mr. Kornick earned his Juris Doctor from Loyola University Law School, and he has remained with the company as an associate attorney concentrating in Immigration Employment Law. Also in 2009, the business relocated to its current location of 400 Poydras St., Suite 2375, New Orleans, La. The company continues to expand by offering a variety of family immigration, employment immigration, tourist visas, temporary work visas, waivers, student visas, translations, EOIR litigation and more.
Copyright © Law Offices of Brenda J. DeArmas Ricci 2017


[%- page.import({ title => 'First steps', section => 'first_steps', description => "How to get started with your first Perl script", keywords => "Perl, Command line, Perl script", }) -%]
After installing Perl you will want to actually run some Perl code. You need to use a command line (Windows, macOS, Unix/Linux) program to do this.
Check you have Perl installed by typing the command below into your command line program: [% WRAPPER code_snippet %]perl -v[% END %]
Now create a 'perl_tests' folder to save your test files into, you will need to be able to find this from the command line.
Open a text editor (Windows, macOS, Unix/Linux) creating a new file with the following content
[% WRAPPER code_chunk -%] [%- PROCESS 'first_steps/01_hello_world.pl' -%] [%- END %]Save this file as plain text into your 'perl_tests' folder, name the file 'hello_world.pl'.
Then run the script from the command line by typing: [% WRAPPER code_snippet %]perl /path/to/perl_tests/hello_world.pl[% END %]
Open the file again and replace NAME, with your name. Save the file.
Run the script again by typing [% WRAPPER code_snippet %]perl /path/to/perl_tests/hello_world.pl[% END %]


Users sign up, login and reset their passwords using the new TEAM Mentor 4.0 User Interface. However, all users are stored in the TEAM Mentor 3.6 Back-end and are managed from the respective UI.
Administrators can manage TEAM Mentor users via the Tbot. Tbot is accessible using TEAM Mentor 3.6 Back-end. Tbot can be accessed via the "Tbot" link in the top right corner of the main user interface. The TEAM Mentor Tbot is only available to Administrator users.
The user management section is under "Users" row in Tbot and of consists of the following links: "Current Users", "New User", and "SSO Token". The "Current Users" link opens a section that lists all current users and their vital statistics.
Clicking further on a user name allows changing the properties of the current user account.
The "New User" link opens a page that allows creating a new user.
Another user management section is available under "Users - Import". This consists of "Import Legacy Users", "Users in CSV", and "User Import CSV". "Import Legacy Users" will help in importing users from TEAM Mentor versions prior to 3.3. "Users in CSV" will output a list of users in the CSV format. "User Import CSV" will allow importing a large amount of users in bulk from a CSV file.
User reporting is available throuth "Users - Analysis" row in Tbot. At this time the following reports are available. "All Users Activities", "All Users Tags", "Users Accounts Expiration", and "Users Mapped by Email". "All Users Activities" provides filterable information on logged user events. These events include user login/logout, however "view article" and "search" do not work at this time. "All Users Tags" show a filtrable list of users and their associated custom tags (see below). "Users Accounts Expiration" shows a list of users grouped by "No Expiration Date" - users with no expiration date, "Not Expired" - users with expiration date in the future, "Not Enabled" - user accounts which are disabled, "Empty Email" - Users which have no email in the email field. Note that these mostly would be legacy users from prior to 3.3 where email was not a required field.
It is possible to tag a user with any Key/Value pair tag. This becomes very useful when an organization has a custom user account scheme that is used to identify the user. For example an organization may have user keys such as "Department", or "Location ID", or "Product Unit" for example. And the corresponding values maybe "Engineering", "NYC-53d" and "Real Time Feed". You may add any key value pair in the "Edit " screen"
By default any user can sign up for access. Upon successful sign up the user access is restricted only by the following two parameters:
Regardless if the the access is allowed for evaluation or not, anonymous user sign-up may not be the desired behavior. To work around the current limitation, please set EvalAccounts_Enabled to true and EvalAccounts_Days to -1. This will still allow users to create accounts, however they will not be usable. If this workaround is implemented only the administrator will be able to create user accounts.
Alternatively to Preventing Users From Signing Up, you may want to enable self signup but have the capability of approving each user. If enabled, right after a user signs up, he or she will get an email from TEAM Mentor stating that their account is in the process of being approved.
At the same time TM administrator will get an email requesting user approval.
To approve the user, TM administrator will need to click on the relevant link in an email. To disapprove the user, administrator can ether ignore the email or specifically go into account management section of Tbot and delete the user. One the TM adminstrator approves the user, the user will get an email stating that their account had been approved and that they can now use the service.
"New Accounts Enabled" setting under TM Security in TMConfig is the main setting that controls this functionality. Access TMConfig by clicking on Tbot in the Admin menu and selecting Edit TMConfig under Admin - Config row. UNCHECK the "New Accounts Enabled" button and "Show Content to Anonymous Users" in order to ENABLE the User Approval Workflow. You may also choose to set the newly created user accounts to never expire, in that case tick "New Accounts Don't Expire" checkbox. Alternatively the "Eval Accounts Days" option controls the expiration date. If the option is set to 30 days for example, the newly created user account will have an expiration date of 30 days from now.
You must also configure the email correctly. See Configuring Email for further information.


The Fault in Our Stars
Hazel and Augustus are two teenagers who share an acerbic wit, a disdain for the conventional, and a love that sweeps them on a journey. Their relationship is all the more miraculous, given that Hazel's other constant companion is an oxygen tank, Gus jokes about his prosthetic leg, and they meet and fall in love at a cancer support group.


We are happy to present an article about Citrus on the German Java portal site JAXenter.de. The article gives a detailed introduction to the framework and describes how Citrus can ease the trouble of integration testing in SOA projects. Read the full article on JAXenter.
The German JavaMagazin (http://www.javamagazin.de) gives a short introduction to the Citrus test framework in its latest issue JavaMagazin 02/2010.


November 2019 security patches roll out for the Pixel 2, 3, 4, and Essential Phone
by Joe FedewaAs we kick off the first full week in November, Google is rolling out a new batch of Android security updates. This month is notable because it marks the end of monthly updates for the original Google Pixel and Pixel XL (RIP). We’ve still got patches for the Pixel 4, Pixel 4 XL, Pixel 3, Pixel 3 XL, Pixel 3a, Pixel 3a XL, Pixel 2, Pixel 2 XL, and Essential Phone, though.
This month, there is a pretty decent list of “Functional patches” for the entire Pixel 2 through Pixel 4. Two fixes, in particular, were included for only the Pixel 4 and Pixel 4 XL. Google previously talked about improvements to the 90Hz “Smooth Display,” and it appears some have been included this month. There’s also a bottom speaker improvement specifically for the Pixel 3.
| Category | Improvements | Devices |
|---|---|---|
| Assistant | Improvements for Google Assistant Hotword | Pixel 2, Pixel 2 XL, Pixel 3, Pixel 3 XL |
| Audio | Improvements for bottom speaker audio quality | Pixel 3 |
| Stability | Additional fixes for some devices stuck during boot | Pixel 3, Pixel 3 XL, Pixel 3a, Pixel 3a XL |
| Keyboards | Additional support for Xbox BT controller mapping | Pixel 2, Pixel 2 XL, Pixel 3, Pixel 3 XL, Pixel 3a, Pixel 3a XL, Pixel 4, Pixel 4 XL |
| Display/Graphics | Smooth Display improvements | Pixel 4, Pixel 4 XL |
| Camera | Camera quality improvements | Pixel 4, Pixel 4 XL |
The OTA files and factory images for the Pixel devices can be found at the links below. Find the Android security files for your device and click “Link” to start the download. This will bring your device up to Android 10 in the process. To flash the update manually without losing all of your data, follow the steps outlined in this tutorial. The OTA Android security update for the Essential Phone has just started rolling out.
Note: There are 3 different build numbers for the Pixel 4:
- US (AT&T & Verizon): QD1A.190821.014.C2
- US (T-Mobile, Sprint, Google Fi) & UK carriers: QD1A.190821.014
- All other carriers (AU/JP/CA/TW/US): QD1A.190821.007.A3


Closes the client and removes all listeners.
Connects to the client.
ClientConnectOptions
Promise
Checks if appId is available on the receiver.
TODO:
Queries for currently running applications.
Array with the currently running application ids.
Queries for current ReceiverStatus.
The current ReceiverStatus.
Gets the device volume.
volume - the current volume
Joins the currently running Application.
Launches specified application.
application
Sets the device volume.
volume - the new volume
Stops the specified application.
ReceiverStatusApplication[] - list of sessions
Generated using TypeDoc
This represents a Google Cast Client (a Chromecast).


the furthest distance in the world,is not between love and death
the furthest distance in the world,is not between love and death


Library Informative
Scale
Explore
Download
Read
Practice
Perfection
Stacks you would get to Work on
python
DBMS
JAVA
PHP
artificial Intelligence
JAVASCRIPT
python
DBMS
JAVA
PHP
artificial Intelligence
JAVASCRIPT
INTERVIEW PREPARATION
PERSONALITY DEVELOPMENT
PUBLIC SPEAKING
LEADERSHIP
PRODUCT MANAGEMENT
RESUME WRITING
INTERVIEW PREPARATION
PERSONALITY DEVELOPMENT
PUBLIC SPEAKING
LEADERSHIP
PRODUCT MANAGEMENT
RESUME WRITING
What others say for us
Bulbul Gupta Student,
“This website is very useful for me because I'm from technical background and in this website all the technical books are available. Best part is, all books are freely available.”
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“This platfrom is informative and useful for students those are not like to sign in before downloading books."


de.uni.bamberg.wiai.minf.forflow.datagenerator.controller.datageneration.filltype
Class Editor
java.lang.Object
de.uni.bamberg.wiai.minf.forflow.datagenerator.controller.datageneration.filltype.Editor
- All Implemented Interfaces:
- FillBehaviour, ObservableFillBehaviour
public class Editor
- extends java.lang.Object
- implements FillBehaviour
The editor filling type is a fast and handy option
when no flat file exits, no interval can be defined
and no pre-defined generator fits.
The editor offers the option to create a list of values
in the system itself, rather to switch the application
an create one.
It's more of convenience. It's also possible to save the
entered text and link it with the external file option.
Example
Here is an example how to enter the values for an attribute
(facet). Each line holds one value, it doesn't matter how
long the line is or how it is written.
Notice, the class implements FillBehaviour
interface.
It makes this kind of strategy observable.
Observable
Observable means in this context, whenever an observer
registers to or un-registers from this class, the subject
itself notifies the UI to register this class in a specific
list of generators.
- Since:
- Apr/29/09
- Version:
- 0.1
- Author:
- Michael Munz
|
Constructor Summary |
Editor()
sole default constructor |
|
Method Summary |
int |
calculateN(java.net.URI file)
this method is not used here and
therefore throws an UnsupportedOperationException . |
int |
getLowerBound()
gets the lower bound |
int |
getN()
each filling behaviour whether it is via a
value file, an interval or by editor each
of them has a range of values. |
java.lang.String |
getName()
gets the name of this filling. |
int |
getUpperBound()
gets the upper endpoint |
java.lang.String |
getValueAt(int n)
this method has the job of retrieving the value at
the specified index. |
java.util.List<java.lang.String> |
getValues()
gets the list of values at once. |
boolean |
isValueIncremented()
sometimes it is useful to increment one
value rather than typing in a whole bunch
of different ones. |
void |
isValueIncremented(boolean increment)
sometimes it is useful to increment one
value rather than typing in a whole bunch
of different ones. |
java.util.Iterator<java.lang.String> |
iterator()
Returns an iterator over the elements
in this list in proper sequence. |
void |
notifyOberverFillBehaviour()
Here's the fun part; this is where we tell
all observers about the state. |
void |
registerObserverFillBehaviour(ObserverFillBehaviour observer)
When an observer registers, it's just added to the
end of an observer list. |
void |
removeObserverFillBehaviour(ObserverFillBehaviour observer)
Likewise, when an observer wants to un-register
we just take it off the list. |
void |
setValues(java.util.List<java.lang.String> values)
sets the values which has been typed
in by the editor. |
| Methods inherited from class java.lang.Object |
clone, equals, finalize, getClass, hashCode, notify, notifyAll, toString, wait, wait, wait |
Editor
public Editor()
- sole default constructor
setValues
public void setValues(java.util.List<java.lang.String> values)
- sets the values which has been typed
in by the editor.
Notice, this method awaits the complete list
at once. Calls calulateN() to get the latest
update on it.
- Parameters:
values
- the list of possible values
isValueIncremented
public void isValueIncremented(boolean increment)
- sometimes it is useful to increment one
value rather than typing in a whole bunch
of different ones.
When to use?
This is especially true, when file names are generated.
In the file system are usually files containing the same file
name but have different version numbers, as
an example. This is simulated with the increment option.
Example
Here is a quick example on how the values in the editor
are used. Suppose you've typed in something like this:
Presentation_
Order
Contract with Certkiller.com
Furthermore, we assume the increment function has been enabled.
The generated values for the 1st increment and the last will be:
Presentation_0
Order0
Contract with Certkiller.com 0
...
Presentation_n
Ordern
Contract with Certkiller.com n
There is still one thing to mention. Only those values will be
incremented which are actually taken for generation.
When available?
The option is only available when the editor
is used as the fill behaviour. If you save the
typed in values as an value file and
then link it with external file the
option will not be available anymore.
- Parameters:
increment
- enable function incrementing values?
isValueIncremented
public final boolean isValueIncremented()
- sometimes it is useful to increment one
value rather than typing in a whole bunch
of different ones.
When to use?
This is especially true, when file names are generated.
In the file system are usually files containing the same file
name but have different version numbers, as
an example. This is simulated with the increment option.
Example
Here is a quick example on how the values in the editor
are used. Suppose you've typed in something like this:
Presentation_
Order
Contract with Certkiller.com
Furthermore, we assume the increment function has been enabled.
The generated values for the 1st increment and the last will be:
Presentation_0
Order0
Contract with Certkiller.com 0
...
Presentation_n
Ordern
Contract with Certkiller.com n
There is still one thing to mention. Only those values will be
incremented which are actually taken for generation.
When available?
The option is only available when the editor
is used as the fill behaviour. If you save the
typed in values as an value file and
then link it with external file the
option will not be available anymore.
- Returns:
- true when function is enabled otherwise false
getValueAt
public final java.lang.String getValueAt(int n)
- Description copied from interface:
FillBehaviour
- this method has the job of retrieving the value at
the specified index. Most fill behaviour strategies are based on
value files. These files have a specific amount of possible
values from i = 1, ..., n where i is the index.
When the process of generating test data is activated, to each
facet values of the fill behaviour are used. To get
values in the range of the value file, this method is needed.
By the way, only the strategies itselves have access to
value files.
- Specified by:
getValueAt
in interface FillBehaviour
- Parameters:
n
- the index specifies the value at position n to retrieve.
- Returns:
- the value at position n or null
getValues
public final java.util.List<java.lang.String> getValues()
- gets the list of values at once.
Notice, if the list hasn't been initialized, yet,
then null will be returned.
- Returns:
- list of typed in values
calculateN
public final int calculateN(java.net.URI file)
- this method is not used here and
therefore throws an
UnsupportedOperationException
.
There exits an alternative method doing the job for editors.
- Specified by:
calculateN
in interface FillBehaviour
- Parameters:
file
- the path to the file to calc the values
- Returns:
- N = Σn_i
- See Also:
calculateN()
getN
public final int getN()
- Description copied from interface:
FillBehaviour
- each filling behaviour whether it is via a
value file, an interval or by editor each
of them has a range of values. This range
is referred to as N. N is
the total number of possible or available values
to use for generation.
Example
Imagine having a value file called names.txt.
The file has in total about 300 names, so as a
result N = 300;
Each of those values n = 1, ..., N gets a probability
value later when it comes to probability distributions.
A particular probability density function is laid over
the values.
Probability density function
As an example we assume the Uniform probability distribution
is used. The probability density function is for all values
constant. In other words, each values is equal likely.
P(X=x) = 1/N.
f(x)
|
|
|------------ (1/N)
|
|
|___________|______
N values
- Specified by:
getN
in interface FillBehaviour
- Returns:
- number of values N = Σn_i for this filling behaviour.
getLowerBound
public final int getLowerBound()
- gets the lower bound
- Returns:
- lower endpoint
getUpperBound
public final int getUpperBound()
- gets the upper endpoint
- Returns:
- upper bound
iterator
public java.util.Iterator<java.lang.String> iterator()
- Returns an iterator over the elements
in this list in proper sequence.
- Returns:
- iterator for values
getName
public final java.lang.String getName()
- Description copied from interface:
FillBehaviour
- gets the name of this filling.
It is for displaying purposes.
- Specified by:
getName
in interface FillBehaviour
- Returns:
- a meaningful name
registerObserverFillBehaviour
public void registerObserverFillBehaviour(ObserverFillBehaviour observer)
- Description copied from interface:
ObservableFillBehaviour
- When an observer registers, it's just added to the
end of an observer list.
- Specified by:
registerObserverFillBehaviour
in interface ObservableFillBehaviour
- Parameters:
observer
- an object to notify about changes
removeObserverFillBehaviour
public void removeObserverFillBehaviour(ObserverFillBehaviour observer)
- Description copied from interface:
ObservableFillBehaviour
- Likewise, when an observer wants to un-register
we just take it off the list.
- Specified by:
removeObserverFillBehaviour
in interface ObservableFillBehaviour
- Parameters:
observer
- an object which doesn't want any notifications anymore.
notifyOberverFillBehaviour
public void notifyOberverFillBehaviour()
- Description copied from interface:
ObservableFillBehaviour
- Here's the fun part; this is where we tell
all observers about the state.
Because they're all Observers, we
know how to notify them.
- Specified by:
notifyOberverFillBehaviour
in interface ObservableFillBehaviour


Math Editor V0.1
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Unilateral Failure Universal Soldier: The Return
By Ross Anthony
"We'll have to blow them up and hope the pieces don't fight us."
Hi-tech military department resurrects soldiers killed in battle and monitors them with brain implanted micro-chips. The soldiers are fierce, hard to kill, and relatively emotionless. Nonetheless, the program's budget gets cut which prompts the main computer to take over the Universal Soldier squad and threaten anything biological that gets in its way. Jean Claude plays an earlier model minus the chip. He's the only one who has the code the computer needs to stay alive.
Like a theme park action show in which stunt-people run through a set of pops and propane blasts into safety nets barely hidden behind facade walls, "Universal Soldier: The Return" is mildly flashy to look at, but there is no sense of real danger. The Soldiers themselves are like the little green plastic guys I used to play with at age five. We expect a bit more from a Hollywood action movie. In one scene four U-soldiers are shot up by what seemed like a hundred SWAT guys. Somehow, not one of the four was hit in the face. That's way too hokey for a Van Damme movie.
The script fails to take any real risks as well. Formula action flick, with standard dialogue: "What's going on?" "They'll stop at nothing!" ... add gratuitous expletives. The acting is right on par with my plastic green army guys. Even Jean (whom I normally enjoy) was plastic.
I'm sorry to say, "Universal Soldier" seems to be a quickly made film, with uninspired direction, no unique purpose, populated with safe stunts and lots of shooting.
Starring Jean-Claude Van Damme, Michael Jai White, Kiana Tom, Bill Goldberg. Directed by Mic Rogers. Written by William Malone, John Fasano. Produced by Craig Baumgarten, Allen Shaprio and Van Damme at Tri-Star/Baumgarten-Prophet/Indi-Prod/Long Road. Rated R.
Grade..........................C
-- Copyright © 1999 Ross Anthony, currently based in Los Angeles, has scripted and shot documentaries, music videos, and shorts in 35 countries across North America, Europe, Africa and Asia. For more reviews visit: http://RossAnthony.com
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
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Please direct comments/criticisms of the review to relevant newsgroups.
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Related links: index of all rec.arts.movies.reviews reviews


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"DIAL "for the measurement of time, only once mentioned in the Bible, erected by Ahaz (2 Kings 20:11; Isaiah 38:8). The Hebrew word(ma’aloth) is rendered “steps” in Exodus 20:26, 1 Kings 10:19, and“degrees” in 2 Kings 20:9, 10, 11. The ma’aloth was probably stairs on which the shadow of a column or obelisk placed on the top fell. The shadow would cover a greater or smaller number of steps, according as the sun was low or high. Probably the sun-dial was a Babylonian invention. Daniel at Babylon(Daniel 3:6) is the first to make mention of the “hour.”
"DIAL "for the measurement of time, only once mentioned in the Bible, erected by Ahaz (2 Kings 20:11; Isaiah 38:8). The Hebrew word(ma’aloth) is rendered “steps” in Exodus 20:26, 1 Kings 10:19, and“degrees” in 2 Kings 20:9, 10, 11. The ma’aloth was probably stairs on which the shadow of a column or obelisk placed on the top fell. The shadow would cover a greater or smaller number of steps, according as the sun was low or high.
Probably the sun-dial was a Babylonian invention. Daniel at Babylon(Daniel 3:6) is the first to make mention of the “hour.”


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{% from 'attachments/_attachments.html' import render_attachments as _render_attachments %} {% macro render_attachments(category) %} {%- set can_manage = category.can_manage(session.user) -%} {%- if category.attachment_count or can_manage %}


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{% if not kiosk %}
Remote control active
Remote control
Search
Edit
{% include 'includes/manage.html' %} {% include 'includes/servers.html' %}
{% endif %}
{% block content %}{% endblock %}


cursejs
A nodeJS based implementation of the CurseAPI for bot and third party apps developers. The library is not considered yet to be stable.
If you want to join the project, or just discuss about Curse implementations you can join us in the Curse unofficial API dev server.
Documentation
Installing
Branch master:
(Take this one if you don't know which one to take.)
npm install git://github.com/njibhu/cursejs.git
With branch dev:
npm install git://github.com/njibhu/cursejs.git#dev
Updating
npm update cursejs
Use of library
var cursejs = require('cursejs');
var client = new cursejs.Client;
//This is a very basic command handling
client.on('message_received', function(message){
if(message.content === "!ping"){
message.reply("pong!");
}
});
client.run("LOGIN", "PASSWORD");
Requirements
- NodeJS 4+
ws
librarywinston
library
Usually npm
will handle these for you.


Model¶
High Level Design¶
As for a high level idea, we start off by preprocessing our data, which includes sampling, labelling, cleaning and splitting it into train and test data. We the use a linear regression approach to model our dataset and get the output. This is further evaluated by metrics such as Mean Absolute Error as explained below.
Linear Regression¶
Linear regression is a linear approach to modelling the relationship between a scalar response and one or more explanatory variables. The case of one explanatory variable is called simple linear regression.
Linear regression is the next step up after correlation. It is used when we want to predict the value of a variable based on the value of another variable. The variable we want to predict is called the dependent variable (or sometimes, the outcome variable). Linear regression consists of finding the best-fitting straight line through the points. The best-fitting line is called a regression line.
Evaluation¶
Since we are attempting to perform regression which outputs continuous value within a given range. Our main goal is to minimize the error which is defined by the Loss Function.
We have chosen average lifespan as our baseline. We compare our other features with this baseline by plotting graphs and using Mean Absolute Error (MAE) as a metric to evaluate the results of the prediction. MAE is the sum of absolute distances between our target variable and predicted values.
Mathematically, it can be expressed as follows:
where \(y_i\) is the predicted value from the regression model, \(x_i\) is the true value of the datapoint and N is the number of datapoints.


{% extends "issues/base.html" %}
{% block content %}
{% include "issues/contract/partials/table_header.html" %}
{% for contract in contracts %}
{% include "issues/contract/partials/row.html" %}
{% endfor %}
{% endblock %}
{% block tablesorter %}
, sortList: [[0,0]]
{% endblock %}


To change the content of this section, you will make edits to the incidents.html file located in the /js/views folder.


Web Maps 101
By Will (@skorasaurus) based on presentations from
Alan
Beth (@maptimesf), lyzi, Andy W,
Housekeeping!
Links are in blue boxes,
green is just emphasis. You can comment and edit on
github!
Today we will be talking about the very most basic principles of web mapping.
We're including a little history, so you can get an idea of how web maps have come to be.
How is a web map different than a digital map?
Digital: involves a computer, but might not be accessible by the internet.
A web map is a kind of digital map. And both are obviously quite different from analog maps, such as paper maps and atlases!
web map (aka: slippy map) require internet * [usually] interactive, * multiple zoom levels!
OpenStreetMap.org
maps.stamen.com
but how about a little history:
How did web maps come to be?
First, there were digital maps like
ArcGIS.
In 1996, Mapquest launched its web service.
Directions! Online! Revolutionary!
The problem: it was slow to load :(
Google Maps really paved the way for online mapping, beginning in 2005.
But what was the revolution?
Was it the interface?
The red marker?
The weather widget?
Because it was google?
No!
It was the
tile!
tiles
=
256x256 pixel image
same boundaries
~20 zoom levels
not interactive
Each zoom level has its own set of tiles!
Zoom level 0: one tile for the world.
With each additional zoom level, the number of tiles increases exponentially.
Zoom level 1: 4 tiles for the world.
Number of tiles at zoom level z:
2z x 2z = 4z
Tiles are rendered in advance (usually) then stored in a cache
Map tiles are just images on the web, so you can link to them individually.
In order to understand how this works, let's break down the URL.
http://tile.openstreetmap.org/4/2/6.png -- this is the name of the tile server.
http://tile.openstreetmap.org/4/2/6.png -- this is the z value, or the zoom level.
http://tile.openstreetmap.org/4/2/6.png -- This is the x/y value, or the place in the grid where the tile lives.
Web maps use Mercator projection, which is designed for sailors BUT....
it's equidistant at local, small levels
by: Stefan Kühn
ZOOM LEVEL ≠ SCALE
a web map
is (usually) not just tiles!
When we add points or lines on top of the base layer, we call those feature layers
Sometimes you can interact with them (clicking to produce a popup, for example).
Here's the breakdown of how these pieces fit together:
a peek at javascript
What javascript does: Grabs the tiles, adds the base layer (already styled), handles interaction, customizes look of feature layer
Filetypes: GIS uses
shapefiles, but web maps prefer
KML, or more recently,
GeoJSON
standardized
Organized
what format do you want your data in?
what layer(s) should have interaction?
We mentioned tiles...
Do you want a custom basemap?
Or can you use an existing one?
How much money do you have?
<
learn JS.
Mozilla CDN
Codecademy
CodeSchool
JavaScript.is(Sexy)
Now, it's time to make your own web map (Base map and layers!)
No CODING required
mapbox.com
3 exceptions to the simplified story!
Exception #1: Tiles are always rasters EXCEPT when they're not!
vector tiles: they are an alternative to a database that makes raster tiles. They still render to rasters for display
So someone has to go through and chop up that data, like
MapBox
Exception #2: Can’t interact with features on a raster. BUT
UTFGrid (Mapbox invention) makes it possible.
UTFGrid is an invisble tile layer made up of arbitrary letters which are indexes into the clickable data
Exception #3:
D3 exists outside the world of tiles
you can’t easily make road map in D3 BUT can do things that are clumsy in slippy maps like...
different map projections (in the browser!)
sta.mn/jfs
IS
IN
SANE
Very powerful, but steep learning curve
So.
Where do I start?
Do I need to make my own custom tiles?
Yes? Use
TileMill to design your own tiles.
Pretty!
Style your map with
CartoCSS (or just carto)
You can host these files on
MapBox, or...
Do I need a content layer?
No? Put all your data into the tiles, possibly using UTFGrid for interactivity
Yes? Convert a Shapefile to GeoJSON with
OGRE or write your own GeoJSON with
geojson.io
Finally,
CartoDB takes care of almost all of this for you!
Thanks to:
You!
Presentation made with
big


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Ronny Jackson, Trump’s Old VA Nominee Who Went Down In Flames, May Run For Office
Navy Rear Adm. Ronny Jackson, President Donald Trump’s onetime VA nominee who was sunk amid allegations of workplace drunkenness and overprescription, is considering a run for Texas Congress.
According to Roll Call, he’s considering a run in Texas’ 13th district, a safe Republican seat, after the incumbent retired.
Jackson, who won Trump’s adoration after he gave a dubiously glowing public report of the President’s health when he was his chief physician, still works at the White House.
Jackson also served as a physician to Presidents Barack Obama and George W. Bush.


Psalm 9
For the chief musician; set to Muth Labben style.
All remembrance of them has perished.
7 But Yahweh remains forever;
he establishes his throne for justice.
8 He judges the world fairly.
He makes just decisions for the nations.
9 Yahweh also will be a stronghold for the oppressed,
a stronghold in times of trouble.
10 Those who know your name trust in you,
for you, Yahweh, do not abandon those who seek you.
11 Sing praises to Yahweh, who rules in Zion;
tell the nations what he has done.
12 For the God who avenges bloodshed remembers;
he does not forget the cry of the oppressed.
13 Have mercy on me, Yahweh; see how I am oppressed by those who hate me,
you who can snatch me from the gates of death.
14 Oh, that I might proclaim all your praise.
In the gates of the daughter of Zion
I will rejoice in your salvation!
15 The nations have sunk down into the pit that they made;
their feet are caught in the net that they hid.
16 Yahweh has made himself known; he has executed judgment;
the wicked is ensnared by his own actions.
Selah
17 The wicked are turned back and sent to sheol,
the destiny of all the nations that forget God.
18 For the needy will not always be forgotten,
nor will the hopes of the oppressed be forever dashed.
19 Arise, Yahweh; do not let man conquer us;
may the nations be judged in your sight.
20 Terrify them, Yahweh;
may the nations know that they are mere men.
Selah


LOADING
Group14: O2CO2 exchange in erythrocytes
Score:
Score:
Score:
You are finished this group, please go to next group
Next


Links open in a new window.
Advisory Committee on the Safety of Blood, Tissues and Organs (SaBTO)
(2012) Position statement on cytomegalovirus tested blood components.
Open
Advisory Committee on the Safety of Blood, Tissues and Organs (SaBTO)
(2012) Report of the Cytomegalovirus Steering Group
Open
Bolton-Maggs, P (Ed) and Cohen, H (2012) on behalf of the Serious Hazards
of Transfusion (SHOT) Steering Group. The 2011 Annual SHOT Report.
Open
Bolton-Maggs P (Ed), Poles D, Watt A, Thomas D and Cohen H (2013) on behalf
of the Serious Hazards of Transfusion (SHOT) Steering Group. The 2012
Annual SHOT Report.Open
Joint UKBTS / HPA Professional Advisory Committee (2012) Position Statement
on Granulocyte Therapy. Revised by Edwin Massey, Simon Stanworth and
Rebecca Cardigan at the request of the Standing Advisory Committee on Blood
Components. Open
McClelland DBL (ed) (2007) Handbook of Transfusion Medicine, 4th Ed.
Published in the UK by The Stationary Office. Open
McClelland DBL, Pirie E, Franklin IM (2010) for the EU Optimal Use of Blood
Project Partners. The Optimal Blood Use Manual. Published by Scottish
National Blood Transfusion Service.
Open
Medical Subject Headings (2013) published by the U.S. National Library of
Medicine, National Institutes of Health.
Open
NHS National Genetics and Genomics Education Centre,
glossary item "First-degree relative".
Open
Public Health Image Library (PHIL), 1986, Centres for Disease Control and Prevention.
Open
Taylor C, Cohen H, Jones H, et al (2008), on behalf of the Serious Hazards
of Transfusion (SHOT) Steering Group. The 2007 Annual SHOT Report.
Open
Taylor C (Ed.), Cohen H, Mold D, Jones H, et al (2009), on behalf of the
Serious Hazards of Transfusion (SHOT) Steering Group. The 2008 Annual SHOT
Report. Open
Taylor C (Ed.), Cohen H, Mold D, Jones H, et al (2010), on behalf of the
Serious Hazards of Transfusion (SHOT) Steering Group. The 2009 Annual SHOT
Report. Open
Treleaven, J., Gennery, A., Marsh, J., Norfolk, D., Page, L., Parker, A.,
Saran, F., Thurston, J. and Webb, D. (2011), Guidelines on the use of
irradiated blood components prepared by the British Committee for Standards
in Haematology blood transfusion task force. British Journal of
Haematology, 152: 35-51. doi: 10.1111/j.1365-2141.2010.08444.x
Open
Press 'Home' to return to the front screen or select a topic in from the list above.


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| Package | Description |
|---|---|
| gui | |
| gui.tab | |
| gui.tab.insertTab | |
| gui.tab.selectTab | |
| gui.tab.updateTab | |
| persistence | |
| persistence.bin | |
| persistence.database |
| Class and Description |
|---|
| IAbstractPersistenceFactory
Interface IAbstractPersistenceFactory
|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IAbstractPersistenceFactory
Interface IAbstractPersistenceFactory
|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|
| Class and Description |
|---|
| IFacadeCallPersistence
Interface IFacadeCallPersistence
|
| IFacadeContactPersistence
Interface IFacadeContactPersistence
|
| IFacadeContactTypePersistence
Interface IFacadeContactTypePersistence
|
| IFactoryPersistence
Interface IFactoryPersistence
|


Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb
Flat, responsive, lightweight, fast, easy customizable modal window plugin with declarative state notation and hash tracking.
Minified version size: ~4kb


Jinia:
Alright, we'll depart now. Keep those nerves of steel!
Enter the Ice Queen's Castle.
"Wait a moment, I'm not ready."


Genres : {{genres}}
Rated {{rating}} by {{users}} users!
Movie Description : {{des}}
Tagline : {{tag}}
Release Year : {{rel}}
Website : {{website}}
Length : {{run}}
Production house : {{production}}
Budget : {{budget}}$


public class CustomerMainScreenController
extends java.lang.Object
implements javafx.fxml.Initializable
| Constructor and Description |
|---|
CustomerMainScreenController() |
| Modifier and Type | Method and Description |
|---|---|
void |
addAppointment(javafx.event.ActionEvent event) |
void |
addRecord(javafx.event.ActionEvent event) |
static int |
appointmentToModifyIndex()
producttoModifyIndex , same deal as partToModifyIndex, created to get
around the error of moving parts from place to place detailed description
of a logical or runtime error that you corrected in the code and a
detailed description of how you corrected it above the line of code you
are referring to
• a compatible feature suitable to your application that would extend
functionality to the next version if you were to update the application :
Java SE should work
|
void |
deleteAppointment(javafx.event.ActionEvent event) |
void |
Exit(javafx.event.ActionEvent event) |
static Customer |
getModifyRecordrecord() |
void |
initialize(java.net.URL url,
java.util.ResourceBundle rb)
Initializes the controller class.
|
void |
OnMonth(javafx.event.ActionEvent event)
OnMonth, this Action required interaction with the Database, specifically
the "DBAppointment" file I added a lambda here because it's the most
effective way to find which month an appointment lands in should work
fine with Java SE
|
void |
OnWeek(javafx.event.ActionEvent event)
OnWeek this Action required interaction with the Database, specifically
the "DBAppointment" file.
|
static int |
recordToModifyIndex() |
void |
setModifyAppointment(Appointment modifyAppointmentappointment) |
void |
setModifyRecord(Customer modifyRecordrecord) |
void |
updateAppointment(javafx.event.ActionEvent event) |
void |
updateRecord(javafx.event.ActionEvent event) |
public void initialize(java.net.URL url, java.util.ResourceBundle rb)
initialize
in interface javafx.fxml.Initializable
public void addAppointment(javafx.event.ActionEvent event) throws java.io.IOException
java.io.IOException
public void updateAppointment(javafx.event.ActionEvent event) throws java.io.IOException
java.io.IOException
public void deleteAppointment(javafx.event.ActionEvent event) throws java.io.IOException
java.io.IOException
public void addRecord(javafx.event.ActionEvent event) throws java.io.IOException
java.io.IOException
public void Exit(javafx.event.ActionEvent event)
public void updateRecord(javafx.event.ActionEvent event) throws java.io.IOException
java.io.IOException
public static Customer getModifyRecordrecord()
public void setModifyRecord(Customer modifyRecordrecord)
public void setModifyAppointment(Appointment modifyAppointmentappointment)
public static int recordToModifyIndex()
public static int appointmentToModifyIndex()
public void OnWeek(javafx.event.ActionEvent event)
public void OnMonth(javafx.event.ActionEvent event)


| Figure 1 |
Distribution and images of the studied species. Limits of th ... |
| Figure 2 |
Haplotype diversity of the studied species. Landscape distri ... |
| Figure 3 |
Ecological niche models for every studied species. Geographi ... |
| Figure 4 |
Environmental resistances for every species studied. Environ ... |
| Figure 5 |
Reserves and haplotype diversity. Haplotype diversity of the ... |


Before Change
max_mean = np.max(self.tree.instances.Y)
instances = self.tree.get_instances_in_nodes(self.label)
mean = np.mean(instances.Y)
return self.color_palette[(mean - min_mean) / (max_mean - min_mean)]
def _color_var(self):
Color the nodes with respect to the variance of instances inside.
min_std, max_std = 0, np.std(self.tree.instances.Y)
After Change
def _color_mean(self):
Color the nodes with respect to the mean of instances inside.
min_mean = np.min(self.tree.instances.Y)
max_mean = np.max(self.tree.instances.Y)
instances = self.tree.get_instances_in_nodes(self.label)
mean = np.mean(instances.Y)
return self.color_palette.value_to_qcolor(
mean, low=min_mean, high=max_mean)
def _color_var(self):
Color the nodes with respect to the variance of instances inside.
min_std, max_std = 0, np.std(self.tree.instances.Y)


three musketeers
"All for one. One for all."
This module serves as an intuitive tool to introspect, debug and test any THREE.js application.
GitHub — Documentation — Examples — Demo
Demo
Usage
Download the minified library and include it in your HTML, or install and import it as a npm module.
$ npm i three-musketeers
The code below creates a scene, a camera, and a geometric cube, and it adds the cube to the scene. It then creates a WebGL
renderer for the scene and camera, and it adds that viewport to the document.body element. Finally, it animates the cube within the scene for the camera.
Lastly, we simply pass the necessary resources to the musketeers instance and attach it to our window
via the alias $$$
for experimentation:
// sample application
import * as THREE from 'three';
import musketeers from 'three-musketeers';
init();
function init() {
const { innerWidth, innerHeight } = window;
const scene = new THREE.Scene();
const renderer = new THREE.WebGLRenderer({ antialias: true });
renderer.setSize(innerWidth, innerHeight);
document.body.appendChild(renderer.domElement);
const camera = new THREE.PerspectiveCamera(70, innerWidth / innerHeight, 0.01, 10);
camera.position.z = 1;
scene.add(camera);
const mesh = new THREE.Mesh(
new THREE.BoxGeometry(0.2, 0.2, 0.2),
new THREE.MeshBasicMaterial({ color: 0xFF0000 })
);
// assign a unique name to our mesh to be able to query it later
mesh.name = 'CUBE_1';
scene.add(mesh);
renderer.render(scene, camera);
// attach $$$ to the window for browser debugging
window.$$$ = musketeers({ renderer, scene, camera });
}
Now, you can inspect the scene through the window
object:
// javascript console in the browser
$$$
.debug() // enable visual debug mode
.isValid(); // true
$$$
.find('Cube_1') // the unique identifier we assigned to our mesh
.exists(); // true
$$$
.findAll((node) => node.geometry.type === 'BoxGeometry') // returns an array of items of this type
$$$
.find('Cube_1')
.click(); // locates the item in the 3D scene and clicks the item
window.addEventListener('click', (event) => {
// find all intersected items on 'click'
const intersectedItems = $$$.pickFromEvent(event);
console.log(intersectedItems); // useful for debugging
});
Check out the documentation for more details. You can also check out the example testing a 3D application with selenium.
# running and testing the example 3d application
$ npm run selenium
$ npm run start
$ npm run test:e2e
Contribute
I welcome contributors. Please contribute if you have ideas to improve this library. Please use GitHub's pull request and issues features. You can also help implement upcoming features from the TODO page. Feel free to reach out if you'd like more context or info for implementation details.
Here are a few scripts to help you get started:
| NPM Commands | Description |
|---|---|
start |
Runs the examples for development |
test |
Runs unit tests for the module |
build |
Builds the module |
docs |
Updates the documentation |
components |
Updates the component entry points |
selenium |
Runs selenium |
test:e2e |
Runs e2e automated testing for the examples as an example |
Other Resources
Three.js Questions — Three.js Forum — Three.js Gitter — Three.js Slack


Download Library
Download Options
Minimally Formatted Text Output
Text
Saves stories as an offline HTML page that contains the fimifction.net styling
Html
Kindle/E-Reader Format
Epub


This test passes if the iframe lays out and paints (meaning it is purple) after the test naviagtes back.


Although Seattle's existing approach to homelessness has had some successes, it is ineffective in meeting the current greatest needs of our homeless population: shelter and security.
Since 1980, Seattle has organized an annual One Night Count to get a snapshot of how many people are living without shelter. The count has grown from 2,759 in 2010 to 5,485 in 2017. However, this count doesn’t cover all areas of the city nor count the population in shelters and transitional housing.
There is estimated to be a total of around 10,000 homeless people in Seattle.
Every year, the city of Seattle spends $40 million on the homelessness issue, and there are a number of nonprofits who operate on donations. A state of emergency has been declared, there are clearly funds available, yet the number of homeless individuals continues to grow. What barriers are keeping services from being used effectively?
Shelters
Most of Seattle’s housing programs are centered around short-term housing, between 30 days and 180 days. However, just 8% of adults who stay in emergency shelters find permanent housing, and long-term housing is afflicted with long, long waiting lists.
This is an expensive but still ineffective approach.
Counseling
There are a number of shelters in Seattle with counselors available: the Union Gospel Mission, Mary’s Place, and Millionair Club are just a few.
Counselors are resources to set plans, identify relevant services, and help navigate the maze of paperwork associated with many homelessness programs. Housing, job trainings, and addiction recovery are just some examples.
Developing this relationship can provide great guidance, but requires a degree of trust which is sometimes difficult to accomplish. Furthermore, shelters are often crowded, have long lines, and don’t have the capacity to support individuals with mental illnesses, disabilities, pets, or addictions.
The Good News: There’s Food
I’ve had the opportunity to work with the homeless in a number of circumstances, from Outdoor Meal Site by First Hill to Search & Rescue in SoDo. At all of these events, there was always food available to give out.
Although the homeless people of Seattle won’t starve, limited access to vital services such as housing is detrimental.


Here you will need to provide details of your mail server.
The SMTP Server text box requires the Internet address of your service provider's SMTP server machine.
The POP3 Server text box requires the Internet address of your service provider's POP3 Mail server machine.
If you are unsure about any of these details, then contact your service provider for details. When you have entered the relevant information in all the text boxes, click the Next button to continue.


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