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Add bioheatExact solver #788
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| Original file line number | Diff line number | Diff line change |
|---|---|---|
| @@ -0,0 +1,155 @@ | ||
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| import numpy as np | ||
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| def bioheat_exact( | ||
| T0, | ||
| S, | ||
| material, | ||
| dx, | ||
| t, | ||
| device="cpu", | ||
| return_numpy=False, | ||
| ): | ||
| """ | ||
| Fourier solution of Pennes' bioheat equation for a constant source. | ||
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| Assumes periodic boundary conditions: opposite edges of each axis | ||
| are connected by the Fourier representation. | ||
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| Uses NumPy on the CPU or CuPy on the GPU. Does not require PyTorch. | ||
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| Equation | ||
| -------- | ||
| dT/dt = D * Laplacian(T) - P * (T - Ta) + S | ||
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| Parameters | ||
| ---------- | ||
| T0 : array-like | ||
| Initial temperature field, 1D, 2D, or 3D. | ||
| S : array-like or scalar | ||
| Constant heat source [K/s], or scalar zero. | ||
| material : array-like | ||
| [D, P, Ta], where D is thermal diffusivity [m²/s], | ||
| P is the perfusion coefficient [1/s], and Ta is | ||
| the reference temperature [K]. | ||
| dx : float or sequence | ||
| Grid spacing in metres. | ||
| t : float | ||
| Evaluation time in seconds. | ||
| device : {"cpu", "gpu"} | ||
| NumPy CPU execution or CuPy GPU execution. | ||
| return_numpy : bool | ||
| Return a NumPy array, including when device="gpu". | ||
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| Returns | ||
| ------- | ||
| numpy.ndarray or cupy.ndarray | ||
| Temperature field at time t. By default, the returned array | ||
| uses the selected backend. | ||
| """ | ||
| if device not in ("cpu", "gpu"): | ||
| raise ValueError("device must be 'cpu' or 'gpu'.") | ||
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| # Select the array backend. | ||
| if device == "gpu": | ||
| try: | ||
| import cupy as cp | ||
| except ImportError as exc: | ||
| raise ImportError( | ||
| "GPU execution requires CuPy and a compatible CUDA runtime." | ||
| ) from exc | ||
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| try: | ||
| if cp.cuda.runtime.getDeviceCount() < 1: | ||
| raise RuntimeError("No usable CUDA GPU was found for CuPy.") | ||
| except cp.cuda.runtime.CUDARuntimeError as exc: | ||
| raise RuntimeError( | ||
| "No usable CUDA GPU was found for CuPy." | ||
| ) from exc | ||
|
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| xp = cp | ||
| else: | ||
| xp = np | ||
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| # Convert fields using the selected backend. In GPU mode, existing | ||
| # CuPy arrays stay on the GPU and can be reused as inputs. | ||
| T0_arr = xp.asarray(T0, dtype=xp.float64) | ||
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| if T0_arr.ndim not in (1, 2, 3) or T0_arr.size <= 1: | ||
| raise ValueError("T0 must be a non-scalar 1D, 2D, or 3D array.") | ||
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| S_arr = xp.asarray(S, dtype=xp.float64) | ||
| source_is_zero = S_arr.ndim == 0 and S_arr.item() == 0 | ||
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| if source_is_zero: | ||
| S_arr = None | ||
| elif S_arr.ndim == 0 or S_arr.shape != T0_arr.shape: | ||
| raise ValueError("S must be zero or have the same shape as T0.") | ||
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| # Material parameters and grid spacing are small CPU-side metadata. | ||
| material_arr = np.asarray(material, dtype=float).ravel() | ||
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| if material_arr.size != 3: | ||
| raise ValueError("material must contain [D, P, Ta].") | ||
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| D, P, Ta = map(float, material_arr) | ||
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| if not np.all(np.isfinite(material_arr)) or D < 0 or P < 0: | ||
| raise ValueError( | ||
| "Material parameters must be finite; D and P must be non-negative." | ||
| ) | ||
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| t = float(t) | ||
| if not np.isfinite(t) or t < 0: | ||
| raise ValueError("t must be finite and non-negative.") | ||
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| if np.isscalar(dx): | ||
| spacing = [float(dx)] * T0_arr.ndim | ||
| else: | ||
| spacing = np.asarray(dx, dtype=float).ravel().tolist() | ||
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| if len(spacing) != T0_arr.ndim: | ||
| raise ValueError( | ||
| f"dx must be a scalar or contain {T0_arr.ndim} values." | ||
| ) | ||
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| if not np.all(np.isfinite(spacing)) or any(d <= 0 for d in spacing): | ||
| raise ValueError("Grid spacing must be finite and positive.") | ||
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| # Build squared angular wavenumber magnitude in FFT ordering. | ||
| # No fftshift/ifftshift is required with fftfreq. | ||
| k_axes = [ | ||
| 2.0 * np.pi * xp.fft.fftfreq(n, d=d) | ||
| for n, d in zip(T0_arr.shape, spacing) | ||
| ] | ||
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| k_mesh = xp.meshgrid(*k_axes, indexing="ij") | ||
| k_squared = sum(ki**2 for ki in k_mesh) | ||
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| denominator = D * k_squared + P | ||
| decay = xp.exp(-denominator * t) | ||
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| # Stable evaluation of (1 - exp(-a*t)) / a, including a == 0. | ||
| nonzero = denominator != 0 | ||
| safe_denominator = xp.where(nonzero, denominator, 1.0) | ||
| Q = xp.where( | ||
| nonzero, | ||
| -xp.expm1(-denominator * t) / safe_denominator, | ||
| t, | ||
| ) | ||
|
rhh006 marked this conversation as resolved.
Resolved
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| # Fourier solution for T - Ta. | ||
| T0_fft = xp.fft.fftn(T0_arr - Ta) | ||
|
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| if S_arr is None: | ||
| T_fft = decay * T0_fft | ||
| else: | ||
| T_fft = decay * T0_fft + Q * xp.fft.fftn(S_arr) | ||
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| T = xp.fft.ifftn(T_fft).real + Ta | ||
|
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| if return_numpy: | ||
| return xp.asnumpy(T) if device == "gpu" else T | ||
|
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| return T | ||
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| Original file line number | Diff line number | Diff line change |
|---|---|---|
| @@ -0,0 +1,99 @@ | ||
|
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| import numpy as np | ||
| import pytest | ||
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| from kwave.bioheatExact import bioheat_exact | ||
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| def test_zero_time_preserves_initial_temperature(): | ||
| T0 = np.arange(12, dtype=float).reshape(3, 4) + 20.0 | ||
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| result = bioheat_exact( | ||
| T0=T0, | ||
| S=0, | ||
| material=[1.2e-7, 0.02, 37.0], | ||
| dx=(1e-3, 2e-3), | ||
| t=0, | ||
| ) | ||
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| np.testing.assert_allclose(result, T0, rtol=1e-12, atol=1e-12) | ||
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| def test_zero_diffusion_and_perfusion(): | ||
| T0 = np.arange(12, dtype=float).reshape(3, 4) | ||
| S = np.full_like(T0, 2.5) | ||
| t = 3.0 | ||
|
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| result = bioheat_exact( | ||
| T0=T0, | ||
| S=S, | ||
| material=[0.0, 0.0, 37.0], | ||
| dx=(1e-3, 2e-3), | ||
| t=t, | ||
| ) | ||
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| np.testing.assert_allclose(result, T0 + t * S, rtol=1e-12, atol=1e-12) | ||
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| def test_single_fourier_mode_on_uneven_grid(): | ||
| nx, ny = 16, 12 | ||
| dx = (0.2, 0.07) | ||
| D = 0.3 | ||
| P = 0.15 | ||
| Ta = 37.0 | ||
| t = 0.4 | ||
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| x = np.arange(nx)[:, None] | ||
| y = np.arange(ny)[None, :] | ||
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| # A single periodic Fourier mode with nonzero wavenumbers | ||
| # along both axes. | ||
| mode = np.cos(2 * np.pi * x / nx + 2 * np.pi * y / ny) | ||
| T0 = Ta + mode | ||
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| kx = 2 * np.pi / (nx * dx[0]) | ||
| ky = 2 * np.pi / (ny * dx[1]) | ||
| decay = np.exp(-(D * (kx**2 + ky**2) + P) * t) | ||
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| expected = Ta + decay * mode | ||
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| result = bioheat_exact( | ||
| T0=T0, | ||
| S=0, | ||
| material=[D, P, Ta], | ||
| dx=dx, | ||
| t=t, | ||
| ) | ||
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| np.testing.assert_allclose(result, expected, rtol=1e-11, atol=1e-11) | ||
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| def test_gpu_result_can_be_reused(): | ||
| cp = pytest.importorskip("cupy") | ||
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| try: | ||
| if cp.cuda.runtime.getDeviceCount() < 1: | ||
| pytest.skip("No CUDA GPU available") | ||
| cp.zeros(1).sum().item() # Check that GPU execution works. | ||
| except cp.cuda.runtime.CUDARuntimeError: | ||
| pytest.skip("No usable CUDA GPU available") | ||
|
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| T0 = cp.full((8, 8), 37.0) | ||
| S = cp.ones((8, 8), dtype=cp.float64) | ||
|
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| kwargs = { | ||
| "S": S, | ||
| "material": [0.0, 0.0, 37.0], | ||
| "dx": 1e-3, | ||
| "t": 0.1, | ||
| "device": "gpu", | ||
| } | ||
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| T1 = bioheat_exact(T0=T0, **kwargs) | ||
| T2 = bioheat_exact(T0=T1, **kwargs) | ||
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| assert isinstance(T1, cp.ndarray) | ||
| assert isinstance(T2, cp.ndarray) | ||
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| cp.testing.assert_allclose(T1, 37.1) | ||
| cp.testing.assert_allclose(T2, 37.2) |
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