import re, numpy as np def read_foam_scalar(path): with open(path) as f: content = f.read() m = re.search(r'List\s+(\d+)', content) if not m: return None, 0 n = int(m.group(1)) start = content.find('(', m.end()) + 1 end = content.find(')', start) vals = np.array([float(x) for x in content[start:end].split()]) return vals, n cases = [ ("rising_bubble", "t00", 128, 256, 1.0, 2.0), ("droplet_impact", "t00", 256, 256, 0.025, 0.025), ("dam_break", "t00", 128, 128, 0.584, 0.584), ] for case, t, nx, ny, Lx, Ly in cases: path = f"/home/alanz/openfoam-workspace/output/data/{case}/{t}/0/alpha.water" vals, n = read_foam_scalar(path) if vals is None: print(f"{case}: FAILED to read") continue # OpenFOAM x-fastest: idx = i + j*nx, so reshape to (ny, nx) # np.where returns (row_idx, col_idx) = (y_idx, x_idx) arr = vals.reshape(ny, nx) if case == "rising_bubble": region = arr < 0.5 # bubble is alpha=0 label = "bubble" elif case == "droplet_impact": region = arr > 0.5 # droplet is alpha=1 label = "droplet" else: region = arr > 0.5 # water column is alpha=1 label = "water" if region.sum() > 0: y_idx, x_idx = np.where(region) r_eq = np.sqrt(region.sum() / np.pi) dx = Lx / nx dy = Ly / ny # Cell center coordinates (0.5 offset for center of cell) cx_phys = (x_idx.mean() + 0.5) * dx cy_phys = (y_idx.mean() + 0.5) * dy r_phys = r_eq * dx # isotropic: dx == dy for these cases print(f"{case}: {label}") print(f" cells={region.sum()}, r_eq={r_eq:.1f} cells ({r_phys*1000:.2f}mm)") print(f" center=({cx_phys*1000:.2f}mm, {cy_phys*1000:.2f}mm)") print(f" domain={Lx*1000:.1f}x{Ly*1000:.1f}mm, dx=dy={dx*1000:.4f}mm") print(f" x_cells=[{x_idx.min()},{x_idx.max()}], y_cells=[{y_idx.min()},{y_idx.max()}]") # Shape aspect ratio span_x = (x_idx.max() - x_idx.min() + 1) span_y = (y_idx.max() - y_idx.min() + 1) print(f" span=({span_x},{span_y}) cells, aspect={span_x/span_y:.2f}") else: print(f"{case}: NO {label} region found")