CIDM-Foundation-A1-R1-R2-FIX1-Results / sources /neuraloperator /examples /layers /plot_fourier_diff.py
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| """ | |
| .. _fourier_diff : | |
| Fourier Differentiation | |
| ====================== | |
| This tutorial demonstrates Fourier-based differentiation methods for computing | |
| derivatives of periodic functions. Fourier differentiation is crucial for: | |
| - Computing derivatives of functions with spectral accuracy | |
| - Implementing physics-informed loss functions | |
| The `FourierDiff` class provides efficient implementations of spectral | |
| differentiation for periodic functions in 1D, 2D, and 3D domains. | |
| """ | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Import the library | |
| # ------------------ | |
| # We first import our `neuralop` library and required dependencies. | |
| import torch | |
| import numpy as np | |
| import matplotlib.pyplot as plt | |
| from neuralop.losses.differentiation import FourierDiff | |
| device = torch.device("cuda" if torch.cuda.is_available() else "cpu") | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Creating an example of periodic 1D curve | |
| # ---------------------------------------- | |
| # Here we consider sin(x) and cos(x), which are periodic on the interval [0, 2π] | |
| L = 2 * torch.pi | |
| x = torch.linspace(0, L, 101)[:-1] | |
| f = torch.stack([torch.sin(x), torch.cos(x)], dim=0) | |
| x_np = x.cpu().numpy() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Differentiate the signal | |
| # ----------------------------------------- | |
| # We use the FourierDiff class to differentiate the signal | |
| fd1d = FourierDiff(dim=1, L=L, use_fc=False) | |
| derivatives = fd1d.compute_multiple_derivatives(f, [1, 2, 3]) | |
| dfdx, df2dx2, df3dx3 = derivatives | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot the results for sin(x) | |
| # --------------------------- | |
| plt.figure() | |
| plt.plot(x_np, dfdx[0].squeeze().cpu().numpy(), label="Fourier dfdx") | |
| plt.plot(x_np, np.cos(x_np), "--", label="dfdx") | |
| plt.plot(x_np, df2dx2[0].squeeze().cpu().numpy(), label="Fourier df2dx2") | |
| plt.plot(x_np, -np.sin(x_np), "--", label="df2dx2") | |
| plt.plot(x_np, df3dx3[0].squeeze().cpu().numpy(), label="Fourier df3dx3") | |
| plt.plot(x_np, -np.cos(x_np), "--", label="df3dx3") | |
| plt.xlabel("x") | |
| plt.legend() | |
| plt.show() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot the results for cos(x) | |
| # --------------------------- | |
| plt.figure() | |
| plt.plot(x_np, dfdx[1].squeeze().cpu().numpy(), label="Fourier dfdx") | |
| plt.plot(x_np, -np.sin(x_np), "--", label="dfdx") | |
| plt.plot(x_np, df2dx2[1].squeeze().cpu().numpy(), label="Fourier df2dx2") | |
| plt.plot(x_np, -np.cos(x_np), "--", label="df2dx2") | |
| plt.plot(x_np, df3dx3[1].squeeze().cpu().numpy(), label="Fourier df3dx3") | |
| plt.plot(x_np, np.sin(x_np), "--", label="df3dx3") | |
| plt.xlabel("x") | |
| plt.legend() | |
| plt.show() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Creating an example of non-periodic 1D curve | |
| # ------------------------------------------- | |
| # Here we consider sin(3x)-cos(x) and exp(-0.8x)+sin(x) | |
| L = 2 * torch.pi | |
| x = torch.linspace(0, L, 101)[:-1] | |
| f = torch.stack( | |
| [torch.sin(3 * x) - torch.cos(x), torch.exp(-0.8 * x) + torch.sin(x)], dim=0 | |
| ) | |
| x_np = x.cpu().numpy() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Differentiate the signal | |
| # ----------------------------------------- | |
| # We use the FourierDiff class with Fourier continuation to differentiate the signal | |
| fd1d = FourierDiff(dim=1, L=L, use_fc="Legendre", fc_degree=4, fc_n_additional_pts=50) | |
| derivatives = fd1d.compute_multiple_derivatives(f, [1, 2]) | |
| dfdx, df2dx2 = derivatives | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot the results for sin(3x)-cos(x) | |
| # -------------------------------------- | |
| plt.figure() | |
| plt.plot(x_np, dfdx[0].squeeze().cpu().numpy(), label="Fourier dfdx") | |
| plt.plot(x_np, 3 * torch.cos(3 * x) + torch.sin(x), "--", label="dfdx") | |
| plt.plot(x_np, df2dx2[0].squeeze().cpu().numpy(), label="Fourier df2dx2") | |
| plt.plot(x_np, -9 * torch.sin(3 * x) + torch.cos(x), "--", label="df2dx2") | |
| plt.xlabel("x") | |
| plt.legend() | |
| plt.show() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot the results for exp(-0.8x)+sin(x) | |
| # --------------------------------------- | |
| plt.figure() | |
| plt.plot(x_np, dfdx[1].squeeze().cpu().numpy(), label="Fourier dfdx") | |
| plt.plot(x_np, -0.8 * torch.exp(-0.8 * x) + torch.cos(x), "--", label="dfdx") | |
| plt.plot(x_np, df2dx2[1].squeeze().cpu().numpy(), label="Fourier df2dx2") | |
| plt.plot(x_np, 0.64 * torch.exp(-0.8 * x) - torch.sin(x), "--", label="df2dx2") | |
| plt.xlabel("x") | |
| plt.legend() | |
| plt.show() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # 2D Fourier Differentiation Examples | |
| # =================================== | |
| # Here we demonstrate the FourierDiff class for 2D functions | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Creating an example of periodic 2D function | |
| # ----------------------------------------- | |
| # Here we consider f(x,y) = sin(x) * cos(y), which is periodic on the interval [0, 2π] × [0, 2π] | |
| L_x, L_y = 2 * torch.pi, 2 * torch.pi | |
| nx, ny = 180, 186 | |
| x = torch.linspace(0, L_x, nx, dtype=torch.float64) | |
| y = torch.linspace(0, L_y, ny, dtype=torch.float64) | |
| X, Y = torch.meshgrid(x, y, indexing="ij") | |
| # Test function: f(x,y) = sin(x) * cos(y) | |
| f_2d = torch.sin(X) * torch.cos(Y) | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Differentiate the 2D signal | |
| # ----------------------------------------- | |
| # We use the FourierDiff class to compute derivatives | |
| fd2d = FourierDiff(dim=2, L=(L_x, L_y)) | |
| # Compute derivatives | |
| df_dx = fd2d.dx(f_2d) | |
| df_dy = fd2d.dy(f_2d) | |
| laplacian = fd2d.laplacian(f_2d) | |
| # Expected analytical results for f(x,y) = sin(x) * cos(y) | |
| df_dx_expected = torch.cos(X) * torch.cos(Y) | |
| df_dy_expected = -torch.sin(X) * torch.sin(Y) | |
| laplacian_expected = -2 * torch.sin(X) * torch.cos(Y) | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot the 2D results | |
| # ---------------------- | |
| fig, axes = plt.subplots(2, 3, figsize=(15, 10)) | |
| fig.suptitle("2D Fourier Differentiation Results: f(x,y) = sin(x) * cos(y)") | |
| # Compute consistent colorbar limits for each derivative pair | |
| df_dx_min = min(df_dx.min().item(), df_dx_expected.min().item()) | |
| df_dx_max = max(df_dx.max().item(), df_dx_expected.max().item()) | |
| df_dy_min = min(df_dy.min().item(), df_dy_expected.min().item()) | |
| df_dy_max = max(df_dy.max().item(), df_dy_expected.max().item()) | |
| # Original function | |
| im0 = axes[0, 0].imshow(f_2d.cpu().numpy()) | |
| axes[0, 0].set_title("Original: sin(x) * cos(y)") | |
| plt.colorbar(im0, ax=axes[0, 0], shrink=0.57) | |
| # ∂f/∂x computed | |
| im1 = axes[0, 1].imshow(df_dx.cpu().numpy(), vmin=df_dx_min, vmax=df_dx_max) | |
| axes[0, 1].set_title("∂f/∂x (computed)") | |
| plt.colorbar(im1, ax=axes[0, 1], shrink=0.57) | |
| # ∂f/∂x expected | |
| im2 = axes[0, 2].imshow(df_dx_expected.cpu().numpy(), vmin=df_dx_min, vmax=df_dx_max) | |
| axes[0, 2].set_title("∂f/∂x (expected: cos(x) * cos(y))") | |
| plt.colorbar(im2, ax=axes[0, 2], shrink=0.57) | |
| # ∂f/∂y computed | |
| im3 = axes[1, 0].imshow(df_dy.cpu().numpy(), vmin=df_dy_min, vmax=df_dy_max) | |
| axes[1, 0].set_title("∂f/∂y (computed)") | |
| plt.colorbar(im3, ax=axes[1, 0], shrink=0.57) | |
| # ∂f/∂y expected | |
| im4 = axes[1, 1].imshow(df_dy_expected.cpu().numpy(), vmin=df_dy_min, vmax=df_dy_max) | |
| axes[1, 1].set_title("∂f/∂y (expected: -sin(x) * sin(y))") | |
| plt.colorbar(im4, ax=axes[1, 1], shrink=0.57) | |
| # Laplacian | |
| im5 = axes[1, 2].imshow(laplacian.cpu().numpy()) | |
| axes[1, 2].set_title("∇²f (computed)") | |
| plt.colorbar(im5, ax=axes[1, 2], shrink=0.57) | |
| plt.tight_layout() | |
| plt.show() | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # 3D Fourier Differentiation Examples | |
| # =================================== | |
| # Here we demonstrate the FourierDiff class for 3D functions | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Creating an example of periodic 3D function | |
| # ----------------------------------------- | |
| # Here we consider f(x,y,z) = sin(x) * cos(y) * sin(z), which is periodic on [0, 2π]³ | |
| L_x, L_y, L_z = 2 * torch.pi, 2 * torch.pi, 2 * torch.pi | |
| nx, ny, nz = 176, 180, 192 | |
| x = torch.linspace(0, L_x, nx, dtype=torch.float64) | |
| y = torch.linspace(0, L_y, ny, dtype=torch.float64) | |
| z = torch.linspace(0, L_z, nz, dtype=torch.float64) | |
| X, Y, Z = torch.meshgrid(x, y, z, indexing="ij") | |
| # Test function: f(x,y,z) = sin(x) * cos(y) * sin(z) | |
| f_3d = torch.sin(X) * torch.cos(Y) * torch.sin(Z) | |
| # Alternative: create tensor directly like in the test | |
| f_3d_alt = torch.randn(nx, ny, nz, dtype=torch.float64) | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Differentiate the 3D signal | |
| # ----------------------------------------- | |
| # We use the FourierDiff class to compute derivatives | |
| fd3d = FourierDiff(dim=3, L=(L_x, L_y, L_z)) | |
| # Compute derivatives | |
| df_dx_3d = fd3d.dx(f_3d) | |
| df_dy_3d = fd3d.dy(f_3d) | |
| df_dz_3d = fd3d.dz(f_3d) | |
| laplacian_3d = fd3d.laplacian(f_3d) | |
| # Expected analytical results for f(x,y,z) = sin(x) * cos(y) * sin(z) | |
| df_dx_expected_3d = torch.cos(X) * torch.cos(Y) * torch.sin(Z) | |
| df_dy_expected_3d = -torch.sin(X) * torch.sin(Y) * torch.sin(Z) | |
| df_dz_expected_3d = torch.sin(X) * torch.cos(Y) * torch.cos(Z) | |
| laplacian_expected_3d = -3 * torch.sin(X) * torch.cos(Y) * torch.sin(Z) | |
| # %% | |
| # .. raw:: html | |
| # | |
| # <div style="margin-top: 3em;"></div> | |
| # | |
| # Plot a slice of the 3D results (z=0 plane) | |
| # ------------------------------------------ | |
| z_slice_idx = nz // 2 | |
| fig, axes = plt.subplots(2, 3, figsize=(18, 12)) | |
| fig.suptitle("3D Fourier Differentiation Results (z=0 slice): f(x,y,z) = sin(x) * cos(y) * sin(z)") | |
| # Compute consistent colorbar limits for each derivative pair at the z-slice | |
| df_dx_3d_slice = df_dx_3d[:, :, z_slice_idx] | |
| df_dx_expected_3d_slice = df_dx_expected_3d[:, :, z_slice_idx] | |
| df_dy_3d_slice = df_dy_3d[:, :, z_slice_idx] | |
| df_dy_expected_3d_slice = df_dy_expected_3d[:, :, z_slice_idx] | |
| df_dx_3d_min = min(df_dx_3d_slice.min().item(), df_dx_expected_3d_slice.min().item()) | |
| df_dx_3d_max = max(df_dx_3d_slice.max().item(), df_dx_expected_3d_slice.max().item()) | |
| df_dy_3d_min = min(df_dy_3d_slice.min().item(), df_dy_expected_3d_slice.min().item()) | |
| df_dy_3d_max = max(df_dy_3d_slice.max().item(), df_dy_expected_3d_slice.max().item()) | |
| # Original function slice | |
| im0 = axes[0, 0].imshow(f_3d[:, :, z_slice_idx].cpu().numpy()) | |
| axes[0, 0].set_title("Original: sin(x) * cos(y) * sin(z)") | |
| plt.colorbar(im0, ax=axes[0, 0], shrink=0.57) | |
| # ∂f/∂x slice | |
| im1 = axes[0, 1].imshow(df_dx_3d_slice.cpu().numpy(), vmin=df_dx_3d_min, vmax=df_dx_3d_max) | |
| axes[0, 1].set_title("∂f/∂x (computed)") | |
| plt.colorbar(im1, ax=axes[0, 1], shrink=0.57) | |
| # ∂f/∂x expected slice | |
| im2 = axes[0, 2].imshow(df_dx_expected_3d_slice.cpu().numpy(), vmin=df_dx_3d_min, vmax=df_dx_3d_max) | |
| axes[0, 2].set_title("∂f/∂x (expected: cos(x) * cos(y) * sin(z))") | |
| plt.colorbar(im2, ax=axes[0, 2], shrink=0.57) | |
| # ∂f/∂y slice | |
| im3 = axes[1, 0].imshow(df_dy_3d_slice.cpu().numpy(), vmin=df_dy_3d_min, vmax=df_dy_3d_max) | |
| axes[1, 0].set_title("∂f/∂y (computed)") | |
| plt.colorbar(im3, ax=axes[1, 0], shrink=0.57) | |
| # ∂f/∂y expected slice | |
| im4 = axes[1, 1].imshow(df_dy_expected_3d_slice.cpu().numpy(), vmin=df_dy_3d_min, vmax=df_dy_3d_max) | |
| axes[1, 1].set_title("∂f/∂y (expected: -sin(x) * sin(y) * sin(z))") | |
| plt.colorbar(im4, ax=axes[1, 1], shrink=0.57) | |
| # ∂f/∂z slice | |
| im5 = axes[1, 2].imshow(df_dz_3d[:, :, z_slice_idx].cpu().numpy()) | |
| axes[1, 2].set_title("∂f/∂z (computed)") | |
| plt.colorbar(im5, ax=axes[1, 2], shrink=0.57) | |
| plt.tight_layout() | |
| plt.show() | |