Post-processing: comparing with and without breakwater
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5c05d6ea34
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2 changed files with 59 additions and 12 deletions
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@ -21,6 +21,7 @@ mpi=4
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[post]
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inp=inp_post
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case=sws_spec_buoy.npz
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compare=sws_spec_buoy_nb.npz
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out=out_post
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#nperseg=1024
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dt=0.25
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@ -5,7 +5,6 @@ import pathlib
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import matplotlib.pyplot as plt
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import numpy as np
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import pandas as pd
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import scipy.signal as sgl
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import scipy.fft as fft
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@ -25,7 +24,7 @@ config.read("config.ini")
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inp = pathlib.Path(config.get("post", "inp"))
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root = pathlib.Path(config.get("swash", "out"))
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log.info(f"Reading bathymetry from '{inp}'")
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log.info(f"Reading data from '{inp}'")
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data = np.load(inp.joinpath(config.get("post", "case")))
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x, t = data["x"], data["t"]
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@ -42,15 +41,48 @@ log.info(f"Computing reflection coefficient at x={x0}")
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eta = data["watl"][t > t0, arg_x0]
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u = data["vel"][t > t0, 0, arg_x0]
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phi_eta = np.abs(sgl.welch(eta, f, nperseg=nperseg))
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phi_u = np.abs(sgl.welch(u, f, nperseg=nperseg))
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phi_eta_u = np.abs(sgl.csd(eta, u, f, nperseg=nperseg))
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phi_eta = sgl.welch(eta, f, nperseg=nperseg)
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phi_u = sgl.welch(u, f, nperseg=nperseg)
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phi_eta_u = sgl.csd(eta, u, f, nperseg=nperseg)
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H = np.sqrt(np.abs(phi_eta[1]))
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U = np.sqrt(np.abs(phi_u[1]))
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G = H / U
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th_eta_u = np.angle(phi_eta_u[1])
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# R1 = np.sqrt(
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# (np.abs(phi_eta[1]) + np.abs(phi_u[1]) - 2 * np.abs(phi_eta_u[1]))
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# / (np.abs(phi_eta[1]) + np.abs(phi_u[1]) + 2 * np.abs(phi_eta_u[1]))
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# )
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R = np.sqrt(
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(phi_eta[1] + phi_u[1] - 2 * phi_eta_u[1])
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/ (phi_eta[1] + phi_u[1] + 2 * phi_eta_u[1])
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(1 + G**2 - 2 * G * np.cos(th_eta_u))
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/ (1 + G**2 + 2 * G * np.cos(th_eta_u))
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)
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if config.has_option("post", "compare"):
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data_comp = np.load(inp.joinpath(config.get("post", "compare")))
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x_, t_ = data_comp["x"], data_comp["t"]
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arg_x0_ = np.abs(x_ - x0).argmin()
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arg_t0_ = np.abs(t_ - t0).argmin()
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eta_ = data_comp["watl"][t_ > t0, arg_x0_]
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u_ = data_comp["vel"][t_ > t0, 0, arg_x0_]
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phi_eta_ = sgl.welch(eta_, f, nperseg=nperseg)
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phi_u_ = sgl.welch(u_, f, nperseg=nperseg)
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phi_eta_u_ = sgl.csd(eta_, u_, f, nperseg=nperseg)
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H_ = np.sqrt(np.abs(phi_eta_[1]))
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U_ = np.sqrt(np.abs(phi_u_[1]))
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G_ = H_ / U_
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th_eta_u_ = np.angle(phi_eta_u_[1])
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R_ = np.sqrt(
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(1 + G_**2 - 2 * G_ * np.cos(th_eta_u_))
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/ (1 + G_**2 + 2 * G_ * np.cos(th_eta_u_))
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)
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# Plotting
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log.info("Plotting results")
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fig, (ax_watl, ax_vel) = plt.subplots(2)
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@ -73,13 +105,21 @@ fig_r, ax_r = plt.subplots()
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ax_fft = ax_r.twinx()
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ax_fft.plot(
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*sgl.welch(eta, 1/dt, nperseg=nperseg),
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*sgl.welch(eta, 1 / dt, nperseg=nperseg),
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lw=1,
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c="k",
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alpha=0.2,
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label="PSD ($\\eta$)",
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label="PSD ($\\eta$, cas 1)",
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)
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ax_r.plot(phi_eta[0], R, marker="+", label="R")
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ax_fft.plot(
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*sgl.welch(eta_, 1 / dt, nperseg=nperseg),
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lw=1,
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c="k",
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alpha=0.2,
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label="PSD ($\\eta$, cas 2)",
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)
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ax_r.plot(phi_eta[0], R, marker="+", label="R (cas 1)")
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ax_r.plot(phi_eta[0], R_, marker="+", label="R (cas 2)")
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ax_r.set(xlim=(0, 0.3), ylim=(0, 1), xlabel="f (Hz)", ylabel="R")
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ax_fft.set(ylim=0, ylabel="PSD (m²/Hz)")
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ax_r.grid()
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@ -89,11 +129,16 @@ fig_r.tight_layout()
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fig_x, ax_x = plt.subplots(figsize=(10, 1))
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ax_x.plot(data["x"], -data["botl"], color="k")
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ax_x.fill_between(
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ax_x.plot(data["x"], -data_comp["botl"], color="k", ls="-.")
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ax_x.plot(
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data["x"],
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-data["botl"],
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np.maximum(data["watl"][arg_t0, :], -data["botl"]),
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)
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ax_x.plot(
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data["x"],
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np.maximum(data_comp["watl"][arg_t0, :], -data_comp["botl"]),
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ls="-."
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)
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ax_x.axvline(x0, c="k", alpha=0.2)
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ax_x.set(xlabel="x (m)", ylabel="z (m)")
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ax_x.autoscale(axis="x", tight=True)
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@ -107,5 +152,6 @@ out.mkdir(parents=True, exist_ok=True)
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fig.savefig(out.joinpath("t.png"))
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fig_r.savefig(out.joinpath("R.png"))
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fig_x.savefig(out.joinpath("x.png"))
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plt.show(block=True)
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log.info("Finished post-processing")
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