.. DO NOT EDIT. .. THIS FILE WAS AUTOMATICALLY GENERATED BY SPHINX-GALLERY. .. TO MAKE CHANGES, EDIT THE SOURCE PYTHON FILE: .. "auto_ch3\ch3_4_6.py" .. LINE NUMBERS ARE GIVEN BELOW. .. only:: html .. note:: :class: sphx-glr-download-link-note :ref:`Go to the end ` to download the full example code. .. rst-class:: sphx-glr-example-title .. _sphx_glr_auto_ch3_ch3_4_6.py: 3.4.6 Leray-orthogonal operator =============================== The Leray-orthogonal operator plays a fundamental role in fluid dynamics, particularly in the mathematical formulation and numerical modeling of incompressible flows governed by the Euler or Navier–Stokes equations. Overview -------- The Leray projection is used to decompose a vector field into divergence-free (incompressible) and curl-free components. In CodPy, this is achieved using kernel-based differential operators. We define the **Leray-orthogonal operator** as: $$ L_k(X, Y)^{\perp} = \nabla_k(X, Y) \cdot \Delta_k(X, Y)^{-1} \cdot \nabla_k^T(X, Y) $$ or alternatively: $$ L_k(\cdot)^{\perp} = \nabla_k(\cdot) \cdot \nabla_k^{-1}(\cdot) $$ This operator projects any vector field onto the space orthogonal to the gradient field—i.e., the divergence-free subspace. Action on a Vector Field ------------------------ Given a vector field $f(Z) \in \mathbb{R}^{D \times N_z \times D_f}$, the Leray-orthogonal operator acts as: $$ L_k(Z)^{\perp} f(Z) \in \mathbb{R}^{D \times N_z \times D_f} $$ That is, it returns the projection of $f(Z)$ onto the orthogonal complement of the gradient image in RKHS, which corresponds to the divergence-free component. Use Case in Fluid Dynamics -------------------------- This operator enables **Helmholtz–Hodge decomposition** of a vector field into divergence-free and gradient parts: $$ f(Z) = f^{\perp}(Z) + \nabla_k h(Z) $$ where $f^{\perp} = L_k^{\perp} f$ is divergence-free and $\nabla_k h$ is the gradient component. CodPy Implementation -------------------- To compute the Leray projection operator in CodPy: .. GENERATED FROM PYTHON SOURCE LINES 68-206 .. code-block:: Python # Importing necessary modules import os import sys from matplotlib import pyplot as plt curr_f = os.path.join(os.getcwd(), "codpy-book", "utils") sys.path.insert(0, curr_f) import numpy as np # from codpy.plotting import plot1D # Lets import multi_plot function from codpy utils from codpy.plot_utils import multi_plot # Define the sinusoidal function def periodic_fun(x): """ A sinusoidal function that generates a sum of sines based on the input ``x``. """ from math import pi sinss = np.cos(2 * x * pi) if x.ndim == 1: sinss = np.prod(sinss, axis=0) ress = np.sum(x, axis=0) else: sinss = np.prod(sinss, axis=1) ress = np.sum(x, axis=1) return ress + sinss def nabla_my_fun(x): from math import pi import numpy as np sinss = np.cos(2 * x * pi) if x.ndim == 1: sinss = np.prod(sinss, axis=0) D = len(x) out = np.ones((D)) def helper(d): out[d] += 2.0 * sinss * pi * np.sin(2 * x[d] * pi) / np.cos(2 * x[d] * pi) [helper(d) for d in range(0, D)] else: sinss = np.prod(sinss, axis=1) N = x.shape[0] D = x.shape[1] out = np.ones((N, D)) def helper(d): out[:, d] += ( 2.0 * sinss * pi * np.sin(2 * x[:, d] * pi) / np.cos(2 * x[:, d] * pi) ) [helper(d) for d in range(0, D)] return out # Function to generate periodic data def generate_periodic_data_cartesian(size_x, size_z, fun=None, nabla_fun=None): """ Generates 2D structured Cartesian grid data for x and z domains, and evaluates a given function and optionally its gradient. Parameters: - size_x: number of points per axis for x (grid will be size_x^2) - size_z: number of points per axis for z (grid will be size_z^2) - fun: function to evaluate at each point - nabla_fun: optional gradient function to evaluate Returns: - x, z: 2D Cartesian grids of shape (N, 2) - fx, fz: function values at x and z - nabla_fx, nabla_fz (if nabla_fun is provided) """ def cartesian_grid(size, box): lin = [np.linspace(box[0, d], box[1, d], size) for d in range(2)] X, Y = np.meshgrid(*lin) return np.stack([X.ravel(), Y.ravel()], axis=1) # Define domain boxes X_box = np.array([[-1, -1], [1, 1]]) Z_box = np.array([[-1.5, -1.5], [1.5, 1.5]]) # Generate Cartesian grids x = cartesian_grid(size_x, X_box) z = cartesian_grid(size_z, Z_box) # Function evaluations fx = fun(x).reshape(-1, 1) if fun else None fz = fun(z).reshape(-1, 1) if fun else None if nabla_fun: nabla_fx = nabla_fun(x) nabla_fz = nabla_fun(z) return x, fx, z, fz, nabla_fx, nabla_fz return x, fx, z, fz # Lets define helper function to plot 3D projection of the function def plot_trisurf(xfx, ax, legend="", elev=90, azim=-100, **kwargs): from matplotlib import cm """ Helper function to plot a 3D surface using a trisurf plot. Parameters: - xfx: A tuple containing the x-coordinates (2D points) and their corresponding function values. - ax: The matplotlib axis object for plotting. - legend: The legend/title for the plot. - elev, azim: Elevation and azimuth angles for the 3D view. - kwargs: Additional keyword arguments for further customization. """ xp, fxp = xfx[0], xfx[1] x, fx = xp, fxp X, Y = x[:, 0], x[:, 1] Z = fx.flatten() ax.plot_trisurf(X, Y, Z, antialiased=False, cmap=cm.jet) ax.view_init(azim=azim, elev=elev) ax.title.set_text(legend) # import CodPy's core module and Kernel class from codpy import core from codpy.kernel import Kernel .. GENERATED FROM PYTHON SOURCE LINES 207-210 Leray operator and Helmholtz-Hodge decomposition ######################################################################## .. GENERATED FROM PYTHON SOURCE LINES 210-299 .. code-block:: Python def fun_LerayT(size_x=50, size_y=50): x, fx, z, fz, _, nabla_fz = generate_periodic_data_cartesian( size_x, size_y, periodic_fun, nabla_fun=nabla_my_fun ) nabla_fz = nabla_fz.reshape(-1, 2, 1) kernel_ptr = Kernel( x=x, fx=fx, ).get_kernel() LerayT_fz = core.DiffOps.nabla( x=x, y=x, z=z, fx=core.DiffOps.nabla_inv(x=x, y=x, z=x, fz=nabla_fz, kernel_ptr=kernel_ptr), kernel_ptr=kernel_ptr, order=2, regularization=1e-8, ) multi_plot( [ (z, nabla_fz[:, 0, :]), (z, LerayT_fz[:, 0, :]), (z, nabla_fz[:, 1, :]), (z, LerayT_fz[:, 1, :]), ], plot_trisurf, projection="3d", mp_nrows=1, mp_figsize=(12, 3), mp_title=[ "Comparing f(z) and the transpose of the Leray operator on each direction" ], ) plt.show() fun_LerayT() def fun_LerayT_nabla_nablainv(size_x=50, size_y=50): x, fx, z, fz, _, nabla_fz = generate_periodic_data_cartesian( size_x, size_y, periodic_fun, nabla_fun=nabla_my_fun ) kernel_ptr = Kernel( x=x, fx=fx, set_kernel=core.kernel_setter("tensornorm", "scale_to_unitcube") ).get_kernel() nabla_fx = core.DiffOps.nabla( x=x, y=x, z=z, fx=fx, kernel_ptr=kernel_ptr, order=2, regularization=1e-8, ) nabla_fz = core.DiffOps.leray_t(x=x, y=x, fx=nabla_fx, kernel_ptr=kernel_ptr) LerayT_fz = core.DiffOps.nabla( x=x, y=x, z=z, fx=core.DiffOps.nabla_inv(x=x, y=x, z=z, fz=nabla_fz, kernel_ptr=kernel_ptr), kernel_ptr=kernel_ptr, order=2, regularization=1e-8, ) multi_plot( [ (z, nabla_fz[:, 0, :]), (z, LerayT_fz[:, 0, :]), (z, nabla_fz[:, 1, :]), (z, LerayT_fz[:, 1, :]), ], plot_trisurf, projection="3d", mp_nrows=1, mp_figsize=(12, 3), mp_title=[ "Comparing $\nabla \nabla^{-1}f(z)$ and the transpose of the Leray operator $L_k \nabla f(z)$ on each direction" ], ) plt.show() fun_LerayT_nabla_nablainv() .. rst-class:: sphx-glr-horizontal * .. image-sg:: /auto_ch3/images/sphx_glr_ch3_4_6_001.png :alt: ['Comparing f(z) and the transpose of the Leray operator on each direction'] :srcset: /auto_ch3/images/sphx_glr_ch3_4_6_001.png :class: sphx-glr-multi-img * .. image-sg:: /auto_ch3/images/sphx_glr_ch3_4_6_002.png :alt: ['Comparing $\nabla \nabla^{-1}f(z)$ and the transpose of the Leray operator $L_k \nabla f(z)$ on each direction'] :srcset: /auto_ch3/images/sphx_glr_ch3_4_6_002.png :class: sphx-glr-multi-img .. rst-class:: sphx-glr-timing **Total running time of the script:** (0 minutes 5.676 seconds) .. _sphx_glr_download_auto_ch3_ch3_4_6.py: .. only:: html .. container:: sphx-glr-footer sphx-glr-footer-example .. container:: sphx-glr-download sphx-glr-download-jupyter :download:`Download Jupyter notebook: ch3_4_6.ipynb ` .. container:: sphx-glr-download sphx-glr-download-python :download:`Download Python source code: ch3_4_6.py ` .. container:: sphx-glr-download sphx-glr-download-zip :download:`Download zipped: ch3_4_6.zip ` .. only:: html .. rst-class:: sphx-glr-signature `Gallery generated by Sphinx-Gallery `_