tracers module¶
Tracer particles in a vector field
Requires scipy.interpolate
Module Summary¶
functions:¶
Return an array of count 3d vertices of random particle positions Minimum and maximum values defined by lowerbound and upperbound |
classes:¶
Interpolator on a regular or rectilinear grid in arbitrary dimensions. |
|
Module Details¶
functions:¶
classes:¶
- class RegularGridInterpolator(points, values, method='linear', bounds_error=True, fill_value=nan, *, solver=None, solver_args=None)[source]¶
Bases:
object
Interpolator on a regular or rectilinear grid in arbitrary dimensions.
The data must be defined on a rectilinear grid; that is, a rectangular grid with even or uneven spacing. Linear, nearest-neighbor, spline interpolations are supported. After setting up the interpolator object, the interpolation method may be chosen at each evaluation.
- Parameters:
points (tuple of ndarray of float, with shapes (m1, ), ..., (mn, )) – The points defining the regular grid in n dimensions. The points in each dimension (i.e. every elements of the points tuple) must be strictly ascending or descending.
values (array_like, shape (m1, ..., mn, ...)) – The data on the regular grid in n dimensions. Complex data is accepted.
method (str, optional) – The method of interpolation to perform. Supported are “linear”, “nearest”, “slinear”, “cubic”, “quintic” and “pchip”. This parameter will become the default for the object’s
__call__
method. Default is “linear”.bounds_error (bool, optional) – If True, when interpolated values are requested outside of the domain of the input data, a ValueError is raised. If False, then fill_value is used. Default is True.
fill_value (float or None, optional) – The value to use for points outside of the interpolation domain. If None, values outside the domain are extrapolated. Default is
np.nan
.solver (callable, optional) –
Only used for methods “slinear”, “cubic” and “quintic”. Sparse linear algebra solver for construction of the NdBSpline instance. Default is the iterative solver scipy.sparse.linalg.gcrotmk.
Added in version 1.13.
solver_args (dict, optional) –
Additional arguments to pass to solver, if any.
Added in version 1.13.
- grid¶
The points defining the regular grid in n dimensions. This tuple defines the full grid via
np.meshgrid(*grid, indexing='ij')
- Type:
tuple of ndarrays
- values¶
Data values at the grid.
- Type:
ndarray
- method¶
Interpolation method.
- Type:
str
- fill_value¶
Use this value for out-of-bounds arguments to __call__.
- Type:
float or
None
- bounds_error¶
If
True
, out-of-bounds argument raise aValueError
.- Type:
bool
Notes
Contrary to LinearNDInterpolator and NearestNDInterpolator, this class avoids expensive triangulation of the input data by taking advantage of the regular grid structure.
In other words, this class assumes that the data is defined on a rectilinear grid.
Added in version 0.14.
The ‘slinear’(k=1), ‘cubic’(k=3), and ‘quintic’(k=5) methods are tensor-product spline interpolators, where k is the spline degree, If any dimension has fewer points than k + 1, an error will be raised.
Added in version 1.9.
If the input data is such that dimensions have incommensurate units and differ by many orders of magnitude, the interpolant may have numerical artifacts. Consider rescaling the data before interpolating.
Choosing a solver for spline methods
Spline methods, “slinear”, “cubic” and “quintic” involve solving a large sparse linear system at instantiation time. Depending on data, the default solver may or may not be adequate. When it is not, you may need to experiment with an optional solver argument, where you may choose between the direct solver (scipy.sparse.linalg.spsolve) or iterative solvers from scipy.sparse.linalg. You may need to supply additional parameters via the optional solver_args parameter (for instance, you may supply the starting value or target tolerance). See the scipy.sparse.linalg documentation for the full list of available options.
Alternatively, you may instead use the legacy methods, “slinear_legacy”, “cubic_legacy” and “quintic_legacy”. These methods allow faster construction but evaluations will be much slower.
Examples
Evaluate a function on the points of a 3-D grid
As a first example, we evaluate a simple example function on the points of a 3-D grid:
>>> from scipy.interpolate import RegularGridInterpolator >>> import numpy as np >>> def f(x, y, z): ... return 2 * x**3 + 3 * y**2 - z >>> x = np.linspace(1, 4, 11) >>> y = np.linspace(4, 7, 22) >>> z = np.linspace(7, 9, 33) >>> xg, yg ,zg = np.meshgrid(x, y, z, indexing='ij', sparse=True) >>> data = f(xg, yg, zg)
data
is now a 3-D array withdata[i, j, k] = f(x[i], y[j], z[k])
. Next, define an interpolating function from this data:>>> interp = RegularGridInterpolator((x, y, z), data)
Evaluate the interpolating function at the two points
(x,y,z) = (2.1, 6.2, 8.3)
and(3.3, 5.2, 7.1)
:>>> pts = np.array([[2.1, 6.2, 8.3], ... [3.3, 5.2, 7.1]]) >>> interp(pts) array([ 125.80469388, 146.30069388])
which is indeed a close approximation to
>>> f(2.1, 6.2, 8.3), f(3.3, 5.2, 7.1) (125.54200000000002, 145.894)
Interpolate and extrapolate a 2D dataset
As a second example, we interpolate and extrapolate a 2D data set:
>>> x, y = np.array([-2, 0, 4]), np.array([-2, 0, 2, 5]) >>> def ff(x, y): ... return x**2 + y**2
>>> xg, yg = np.meshgrid(x, y, indexing='ij') >>> data = ff(xg, yg) >>> interp = RegularGridInterpolator((x, y), data, ... bounds_error=False, fill_value=None)
>>> import matplotlib.pyplot as plt >>> fig = plt.figure() >>> ax = fig.add_subplot(projection='3d') >>> ax.scatter(xg.ravel(), yg.ravel(), data.ravel(), ... s=60, c='k', label='data')
Evaluate and plot the interpolator on a finer grid
>>> xx = np.linspace(-4, 9, 31) >>> yy = np.linspace(-4, 9, 31) >>> X, Y = np.meshgrid(xx, yy, indexing='ij')
>>> # interpolator >>> ax.plot_wireframe(X, Y, interp((X, Y)), rstride=3, cstride=3, ... alpha=0.4, color='m', label='linear interp')
>>> # ground truth >>> ax.plot_wireframe(X, Y, ff(X, Y), rstride=3, cstride=3, ... alpha=0.4, label='ground truth') >>> plt.legend() >>> plt.show()
Other examples are given in the tutorial.
See also
NearestNDInterpolator
Nearest neighbor interpolator on unstructured data in N dimensions
LinearNDInterpolator
Piecewise linear interpolator on unstructured data in N dimensions
interpn
a convenience function which wraps RegularGridInterpolator
scipy.ndimage.map_coordinates
interpolation on grids with equal spacing (suitable for e.g., N-D image resampling)
References
- __call__(xi, method=None, *, nu=None)[source]¶
Interpolation at coordinates.
- Parameters:
xi (ndarray of shape (..., ndim)) – The coordinates to evaluate the interpolator at.
method (str, optional) – The method of interpolation to perform. Supported are “linear”, “nearest”, “slinear”, “cubic”, “quintic” and “pchip”. Default is the method chosen when the interpolator was created.
nu (sequence of ints, length ndim, optional) –
If not None, the orders of the derivatives to evaluate. Each entry must be non-negative. Only allowed for methods “slinear”, “cubic” and “quintic”.
Added in version 1.13.
- Returns:
values_x – Interpolated values at xi. See notes for behaviour when
xi.ndim == 1
.- Return type:
ndarray, shape xi.shape[:-1] + values.shape[ndim:]
Notes
In the case that
xi.ndim == 1
a new axis is inserted into the 0 position of the returned array, values_x, so its shape is instead(1,) + values.shape[ndim:]
.Examples
Here we define a nearest-neighbor interpolator of a simple function
>>> import numpy as np >>> x, y = np.array([0, 1, 2]), np.array([1, 3, 7]) >>> def f(x, y): ... return x**2 + y**2 >>> data = f(*np.meshgrid(x, y, indexing='ij', sparse=True)) >>> from scipy.interpolate import RegularGridInterpolator >>> interp = RegularGridInterpolator((x, y), data, method='nearest')
By construction, the interpolator uses the nearest-neighbor interpolation
>>> interp([[1.5, 1.3], [0.3, 4.5]]) array([2., 9.])
We can however evaluate the linear interpolant by overriding the method parameter
>>> interp([[1.5, 1.3], [0.3, 4.5]], method='linear') array([ 4.7, 24.3])
- class Tracers(grid, count=1000, lowerbound=None, upperbound=None, limit=None, age=4, respawn_chance=0.2, speed_multiply=1.0, height=0.0, viewer=None)[source]¶
Bases:
object
- __init__(grid, count=1000, lowerbound=None, upperbound=None, limit=None, age=4, respawn_chance=0.2, speed_multiply=1.0, height=0.0, viewer=None)[source]¶
Seed random particles into a vector field and trace their positions
- Parameters:
grid (list of coord arrays for each dimension as expected by RegularGridInterpolator,) – or a numpy array of 2d or 3d vertices, which will be converted before being sent to the interpolator Object returned from first call, pass None on first pass
count (int) – Number of particles to seed and track
lowerbound (optional minimum vertex point defining particle bounding box,) – if not provided will be taken from grid lower corner
upperbound (optional maximum vertex point defining particle bounding box,) – if not provided will be taken from grid upper corner
limit (float) – Distance limit over which tracers are not connected, For example if using a periodic boundary, setting limit to half the bounding box size will prevent tracer lines being connected when passing through the boundary
age (int) – Minimum particle age in steps after which particle can be deleted and respawned, defaults to 4
respawn (float) – Probability of respawning, after age reached, default 0.2 ==> 1 in 5 chance of deletion
speed_multiply (float) – Speed multiplier, scaling factor for the velocity taken from the vector values
height (float) – A fixed height value, all positions will be given this height as their Z component
viewer (lavavu.Viewer) – Viewer object for plotting functions