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1820 1821 1822 1823 1824 1825 1826 1827 1828 1829 1830 1831 1832 1833 1834 1835 1836 1837 1838 1839 1840 1841 1842 1843 1844 1845 1846 1847 1848 1849 1850 1851 1852 1853 1854 1855 1856 1857 1858 1859 1860 1861 1862 1863 1864 1865 1866 1867 1868 1869 1870 1871 1872 1873 1874 1875 1876 1877 1878 1879 1880 1881 1882 1883 1884 1885 1886 1887 1888 1889 1890 1891 1892 1893 1894 1895 1896 1897 1898 1899 1900 1901 1902 1903 1904 1905 1906 1907 1908 1909 1910 1911 1912 1913 1914 1915 1916 1917 1918 1919 1920 1921 1922 1923 1924 1925 1926 1927 1928 1929 1930 1931 1932 1933 1934 1935 1936 1937 1938 1939 1940 1941 1942 1943 1944 1945 1946 1947 1948 1949 1950 1951 1952 1953 1954 1955 1956 1957 1958 1959 1960 1961 1962 1963 1964 1965 1966 1967 1968 1969 1970 1971 1972 1973 1974 1975 1976 1977 1978 1979 1980 1981 1982 1983 1984 1985 1986 1987 1988 1989 1990 1991 1992 1993 1994 1995 1996 1997 | """Interactive Dash front end for the Mountain Waves model.
This UI is the browser-based counterpart to the original MATLAB menu in
Dr. Robert E. (Bob) Hart's 1995 mountain-wave tool (``tlwmenu.m``). Hart's
slider layout, example cases, and readouts (Scorer condition, Rossby
number, dimensionless mountain height) guided the design here. Original
model and documentation: https://moe.met.fsu.edu/~rhart/mtnwave.html.
Two solver modes are exposed:
* **Two-layer** — sliders for the original MATLAB parameters
(surface wind, upper/lower Scorer, interface height, mountain geometry,
domain, spectrum).
* **Profile** — drag control points on an ``u(z)`` graph and a
``theta(z)`` graph to prescribe arbitrary profiles. The app converts
these to a Scorer parameter profile and runs the multi-layer solver.
Both modes render streamline analysis and a vertical-velocity contour
plot side-by-side, along with diagnostic readouts (Scorer condition,
Rossby number, solver backend).
"""
from __future__ import annotations
import math
import os
from pathlib import Path
from typing import Tuple
import numpy as np
import plotly.graph_objects as go
from dash import Dash, Input, Output, State, ctx, dcc, html, no_update
from . import solver
from .profile import (
brunt_vaisala,
default_profile_heights,
default_theta_profile,
default_u_profile,
scorer_from_profile,
)
OMEGA = 7.292e-5
# ---------------------------------------------------------------------------
# README loader (for the Theory & About modal)
# ---------------------------------------------------------------------------
#
# The "Theory & About" link in the header opens a modal that renders the
# project README.md as markdown. The README lives at the project root in the
# dev layout, but in the Docker runtime the installed package is in
# site-packages while README.md is at /app/README.md (copied there by the
# Dockerfile). We probe both and fall back to a short placeholder.
def _load_readme_markdown() -> str:
"""Return README.md with the HF YAML frontmatter stripped.
Candidates are tried in order of specificity: next to the project root
(dev), next to the launcher at /app (Docker), and finally cwd. The HF
Spaces metadata block at the top (between leading ``---`` markers) is
not useful to end users and is stripped before returning.
"""
here = Path(__file__).resolve()
candidates = [
here.parents[2] / "README.md", # <repo>/python/mountain_waves/app.py → <repo>/README.md
Path("/app/README.md"), # Docker runtime
Path.cwd() / "README.md", # last-ditch
]
for p in candidates:
try:
if p.is_file():
text = p.read_text(encoding="utf-8")
break
except OSError:
continue
else:
return (
"# Mountain Waves\n\n"
"*README.md could not be located at runtime — see "
"[the project page](https://huggingface.co/spaces/snesbitt/mountain-waves).*"
)
# Strip leading YAML frontmatter (HF Spaces metadata).
if text.startswith("---\n"):
close = text.find("\n---\n", 4)
if close != -1:
text = text[close + 5:]
return text
_README_MD = _load_readme_markdown()
LATIT_RAD_DEFAULT = math.radians(45.0)
# ---------------------------------------------------------------------------
# Preset scenarios
# ---------------------------------------------------------------------------
# Default two-layer slider values shown when the page first loads. Also
# what the "Reset to defaults" button in the Actions column restores.
# These match the initial slider-default arguments in ``_two_layer_controls``
# and coincide with the "trapped" preset — Hart's Example 2 — which is the
# most instructive starting point.
TWO_LAYER_DEFAULTS = {
"U": 20.0,
"L_upper": 4.0,
"L_lower": 10.0,
"H": 3.5,
"mtn_h": 0.5,
"mtn_a": 2.5,
"xdom": 40.0,
"zdom": 10.0,
"mink_k": 0,
"maxk_k": 30,
}
PRESETS = {
"uniform": {
"label": "Uniform atmosphere (Example 1)",
"U": 20.0,
"L_upper": 4.0,
"L_lower": 4.0,
"H": 3.5,
"mtn_h": 0.5,
"mtn_a": 2.5,
"xdom": 40.0,
"zdom": 10.0,
"mink_k": 0,
"maxk_k": 30,
},
"trapped": {
"label": "Trapped lee waves (Example 2)",
"U": 20.0,
"L_upper": 4.0,
"L_lower": 10.0,
"H": 3.5,
"mtn_h": 0.5,
"mtn_a": 2.5,
"xdom": 40.0,
"zdom": 10.0,
"mink_k": 0,
"maxk_k": 30,
},
"downslope": {
# Not from Hart's MATLAB (he only documented Examples 1 & 2). This is
# a "strong lee wave / near-downslope" case kept inside linear theory.
# Nh/U = L_lower * ho = 10e-4 * 800 = 0.80, just under the
# wave-breaking threshold (~0.85). Scorer condition ≈ 3.0, so a
# robust trapped-wave packet forms downstream — the closest the
# linear Fourier/Scorer model can get to a real downslope windstorm
# without blowing up, which Hart himself flagged in the "Problems"
# section of his documentation.
"label": "Strong lee waves / near-downslope (linear-theory edge)",
"U": 25.0,
"L_upper": 3.0,
"L_lower": 10.0,
"H": 2.5,
"mtn_h": 0.8,
"mtn_a": 2.5,
"xdom": 40.0,
"zdom": 10.0,
"mink_k": 0,
"maxk_k": 30,
},
"critical_caricature": {
# Two-layer caricature of a critical-layer absorber. A real critical
# level requires U(z)=0 somewhere — impossible in two-layer mode —
# so this preset instead stacks a strongly evanescent upper layer
# (L_upper very small) on top of a moderate-Scorer lower layer, with
# the interface at 2 km. For a mountain with a=2500 m the dominant
# forcing wavenumbers are k ~ 4e-4, which satisfies l_upper^2 < k^2
# (evanescent aloft) and l_lower^2 > k^2 (propagating below).
# Most upgoing wave energy is reflected at the interface, so the
# field above 2 km decays rapidly — a linear-theory analog of
# Booker & Bretherton (1967) critical-level absorption. See the
# Profile tab for a physically faithful U(z)=0 setup.
"label": "Near critical-layer caricature (strong absorption at 2 km)",
"U": 20.0,
"L_upper": 1.0,
"L_lower": 10.0,
"H": 2.0,
"mtn_h": 0.5,
"mtn_a": 2.5,
"xdom": 40.0,
"zdom": 10.0,
"mink_k": 0,
"maxk_k": 30,
},
}
def _rossby(u: float, a: float, latit_deg: float) -> float:
"""Return U / (f a) with f evaluated at the given latitude (degrees N)."""
lat = math.radians(max(0.0, min(90.0, latit_deg)))
f = 2.0 * OMEGA * math.sin(lat)
if f == 0.0 or a == 0.0:
return float("inf")
return u / (f * a)
def _two_layer_plots(params, latit_deg: float = 45.0) -> Tuple[go.Figure, go.Figure, go.Figure, float, float]:
"""Run the two-layer solver and build the streamline, w, and u' figures."""
U = params["U"]
L_upper = params["L_upper"] * 1e-4
L_lower = params["L_lower"] * 1e-4
H = params["H"] * 1000.0
a = params["mtn_a"] * 1000.0
ho = params["mtn_h"] * 1000.0
xdom = params["xdom"] * 1000.0
zdom = params["zdom"] * 1000.0
mink = params["mink_k"] / a
maxk = params["maxk_k"] / a
x, z, w, u_prime = solver.compute_two_layer(
L_upper, L_lower, U, H, a, ho, xdom, zdom, mink, maxk, npts=100
)
lines = solver.streamlines(x, z, U, w, num=10)
scorer_cond = 4.0 * H * H * (L_lower ** 2 - L_upper ** 2) / (math.pi ** 2)
rossby = _rossby(U, a, latit_deg)
return (*_make_plots(x, z, w, u_prime, lines, H), scorer_cond, rossby)
def _profile_plots(params, z_prof, u_prof, theta_prof, latit_deg: float = 45.0) -> Tuple[go.Figure, go.Figure, go.Figure, float, float]:
"""Run the multi-layer solver from prescribed profiles."""
U_surface = float(u_prof[0])
a = params["mtn_a"] * 1000.0
ho = params["mtn_h"] * 1000.0
xdom = params["xdom"] * 1000.0
zdom = params["zdom"] * 1000.0
mink = params["mink_k"] / a
maxk = params["maxk_k"] / a
x, z, w, u_prime = solver.compute_from_profile(
z_prof, u_prof, theta_prof, a, ho, xdom, zdom, mink, maxk, npts=100
)
# Pass the full u(z) profile (interpolated onto the render grid) so the
# streamline tracer uses the local mean wind at each streamline's height.
# Using a single U_surface over-amplifies upper streamlines whenever the
# profile has shear, because linear theory gives η(x, z₀) = (1/U(z₀)) ·
# ∫ w dx'.
u_at_z = np.interp(np.asarray(z, dtype=float), np.asarray(z_prof, dtype=float),
np.asarray(u_prof, dtype=float))
lines = solver.streamlines(x, z, u_at_z, w, num=10)
l2 = scorer_from_profile(z_prof, u_prof, theta_prof)
# Effective 2-layer diagnostic: split profile at midpoint of z_prof range.
mid = z_prof[len(z_prof) // 2]
below = l2[z_prof <= mid]
above = l2[z_prof > mid]
l_lower2 = float(np.mean(np.maximum(below, 0.0))) if below.size else 0.0
l_upper2 = float(np.mean(np.maximum(above, 0.0))) if above.size else 0.0
scorer_cond = 4.0 * mid ** 2 * (l_lower2 - l_upper2) / (math.pi ** 2)
rossby = _rossby(U_surface, a, latit_deg)
# Decorate the streamline plot with a dashed line showing the profile's
# dominant interface: the height of maximum |dL^2/dz|.
interface_z = None
if l2.size > 2:
dl = np.abs(np.diff(l2))
interface_z = float(z_prof[1:][np.argmax(dl)])
return (*_make_plots(x, z, w, u_prime, lines, interface_z), scorer_cond, rossby)
def _make_plots(x, z, w, u_prime, lines, interface_z):
"""Build streamline, vertical-velocity, and u' figures from solver output."""
x_km = np.asarray(x) / 1000.0
z_km = np.asarray(z) / 1000.0
# Streamline figure — the first streamline traces the mountain surface;
# fill it to draw the mountain.
stream_fig = go.Figure()
mountain_color = "rgb(50, 196, 50)"
if lines:
xs, ys = lines[0]
xs_km = np.asarray(xs) / 1000.0
ys_km = np.asarray(ys) / 1000.0
stream_fig.add_trace(
go.Scatter(
x=np.concatenate([xs_km, [x_km[-1], x_km[0], x_km[0]]]),
y=np.concatenate([ys_km, [0.0, 0.0, ys_km[0]]]),
fill="toself",
mode="lines",
line=dict(width=1, color=mountain_color),
fillcolor=mountain_color,
name="Mountain",
hoverinfo="skip",
)
)
for xs, ys in lines[1:]:
stream_fig.add_trace(
go.Scatter(
x=np.asarray(xs) / 1000.0,
y=np.asarray(ys) / 1000.0,
mode="lines",
line=dict(width=1.2, color="white"),
hoverinfo="skip",
showlegend=False,
)
)
if interface_z is not None:
stream_fig.add_hline(
y=interface_z / 1000.0,
line=dict(color="magenta", dash="dash", width=1.5),
annotation_text="interface",
annotation_position="top right",
annotation_font_color="magenta",
)
stream_fig.update_layout(
title="Streamline Analysis",
xaxis_title="x (km)",
yaxis_title="height (km)",
template="plotly_dark",
yaxis=dict(range=[0, z_km[-1]]),
xaxis=dict(range=[x_km[0], x_km[-1]]),
margin=dict(l=60, r=20, t=50, b=50),
height=420,
)
# Vertical-velocity contour. Clip at ±10 m/s like the MATLAB caxis.
w_clip = np.clip(w, -10.0, 10.0)
w_fig = go.Figure(
data=go.Heatmap(
x=x_km,
y=z_km,
z=w_clip,
zmin=-10,
zmax=10,
colorscale="RdBu_r",
reversescale=False,
colorbar=dict(title="w (m/s)"),
zsmooth="best",
)
)
if interface_z is not None:
w_fig.add_hline(
y=interface_z / 1000.0,
line=dict(color="magenta", dash="dash", width=1.5),
)
w_fig.update_layout(
title="Vertical Velocity w (m/s)",
xaxis_title="x (km)",
yaxis_title="height (km)",
template="plotly_dark",
margin=dict(l=60, r=20, t=50, b=50),
height=420,
)
# Horizontal-wind perturbation u'. Scale symmetrically around zero using
# the 98th-percentile magnitude so outlier spikes near the mountain don't
# wash out the lee-wave pattern. Use a diverging colormap (PuOr) distinct
# from w's RdBu_r so the two fields stay visually separable at a glance.
up = np.asarray(u_prime)
up_absmax = float(np.nanpercentile(np.abs(up), 98.0))
if not math.isfinite(up_absmax) or up_absmax <= 0.0:
up_absmax = 1.0
up_clip = np.clip(up, -up_absmax, up_absmax)
uprime_fig = go.Figure(
data=go.Heatmap(
x=x_km,
y=z_km,
z=up_clip,
zmin=-up_absmax,
zmax=up_absmax,
colorscale="PuOr",
reversescale=False,
colorbar=dict(title="u' (m/s)"),
zsmooth="best",
)
)
if interface_z is not None:
uprime_fig.add_hline(
y=interface_z / 1000.0,
line=dict(color="magenta", dash="dash", width=1.5),
)
uprime_fig.update_layout(
title="Horizontal-wind perturbation u' (m/s)",
xaxis_title="x (km)",
yaxis_title="height (km)",
template="plotly_dark",
margin=dict(l=60, r=20, t=50, b=50),
height=420,
)
return stream_fig, w_fig, uprime_fig
# ---------------------------------------------------------------------------
# Layout helpers
# ---------------------------------------------------------------------------
def _slider(id_, label, mn, mx, step, value, unit=""):
return html.Div(
className="slider-row",
children=[
html.Div(
[html.Span(label, className="slider-label"), html.Span(f"{value}{unit}", id=f"{id_}-val", className="slider-value")],
className="slider-header",
),
dcc.Slider(
id=id_,
min=mn,
max=mx,
step=step,
value=value,
marks=None,
tooltip={"placement": "bottom", "always_visible": False},
),
],
)
PROFILE_ZDOM_KM = 10.0
PROFILE_N_POINTS = 32
PROFILE_FIG_HEIGHT_PX = 680 # taller graph so 32 layers don't crowd
# Ranges used both for axis limits and drag clamping. Kept as module-level
# constants so the figure builder, the drag handler, and the redraw all agree.
# The U axis allows negative values so HRRR profiles whose mean flow points
# against the user-chosen "flow from" direction read as negative rather than
# getting silently clamped to 0. Theta floor is dropped to 250 K so cold
# continental winter columns stay visible.
U_RANGE = (-40.0, 80.0)
THETA_RANGE = (250.0, 400.0)
UNDO_HISTORY_MAX = 50
def _init_profile_figures():
# Defaults tuned to reproduce MATLAB "Example 2" (trapped lee waves):
# sharp low-level stability, weak stability aloft, light surface shear.
# 32 evenly-spaced levels give finer resolution in both the boundary
# layer and the free troposphere while keeping the column at 10 km.
# At n=32 the transfer-matrix solver converges to within ~1% of the
# two-layer analytic result for the trapped-wave case.
zs = default_profile_heights(PROFILE_ZDOM_KM, PROFILE_N_POINTS)
us = default_u_profile(zs, u_surface=20.0, shear=0.5)
thetas = default_theta_profile(zs, interface_km=3.5, lapse_lower=11.8, lapse_upper=1.9)
return zs, us, thetas
# ---------------------------------------------------------------------------
# App factory
# ---------------------------------------------------------------------------
def create_app() -> Dash:
# suppress_callback_exceptions is required because `controls-block` is
# swapped between two-layer and profile panels at runtime — the IDs
# referenced in the Analyze callback don't all exist in the initial layout.
# Ship static assets (CliMAS logo, favicon) from the package itself
# so the app works regardless of where it's launched from.
_pkg_dir = os.path.dirname(os.path.abspath(__file__))
_assets_dir = os.path.join(_pkg_dir, "assets")
app = Dash(
__name__,
title="Mountain Waves",
update_title=None,
suppress_callback_exceptions=True,
assets_folder=_assets_dir,
)
zs0, us0, thetas0 = _init_profile_figures()
app.layout = html.Div(
className="mw-root",
children=[
html.Header(
className="mw-header",
children=[
html.Img(
src=app.get_asset_url("climas_icon_64.png"),
alt="Climate, Meteorology & Atmospheric Sciences",
className="mw-logo",
),
html.Div(
className="mw-header-text",
children=[
html.H1("Interactive 2-D Linear Mountain Wave Visualizer"),
html.Div(
className="mw-subtitle",
children=[
html.Span("Rust + Python port of "),
html.A("Bob Hart's original MATLAB model", href="https://moe.met.fsu.edu/~rhart/mtnwave.html", target="_blank"),
html.Span(" by "),
html.A("Steve Nesbitt", href="https://publish.illinois.edu/swnesbitt/", target="_blank"),
html.Span(" — CliMAS UIUC"),
html.Span(f" · compute backend: {solver.backend_name()}"),
],
),
# "Theory & About" link sits on its own line directly
# under the subtitle. Clicking it toggles the modal
# defined at the bottom of the layout.
html.Div(
className="mw-readme-link-row",
children=[
html.Button(
"📖 Theory & About",
id="show-readme",
n_clicks=0,
className="mw-readme-link",
),
],
),
],
),
],
),
dcc.Tabs(
id="mode-tabs",
value="two-layer",
children=[
dcc.Tab(label="Two-layer (analytic)", value="two-layer"),
dcc.Tab(label="Profile (multi-layer)", value="profile"),
],
),
html.Div(
className="mw-global",
children=[
html.Div("Latitude (°N)", className="mw-global-label"),
dcc.Slider(
id="latit",
min=0,
max=90,
step=1,
value=45,
marks={0: "0°", 23: "23°", 45: "45°", 66: "66°", 90: "90°"},
tooltip={"placement": "bottom", "always_visible": False},
),
html.Span(id="latit-val", className="mw-global-value"),
html.Span(
"Coriolis f = 2Ω sin(φ) — affects the Rossby-number readout only.",
className="mw-global-note",
),
],
),
# Both control panels live in the DOM simultaneously so every
# callback Input/State ID always resolves; the inactive one is
# hidden via CSS (see the mode-tabs callback below).
html.Div(
id="controls-block",
children=[
html.Div(id="controls-two-layer", children=_two_layer_controls()),
html.Div(
id="controls-profile",
children=_profile_controls(zs0, us0, thetas0),
style={"display": "none"},
),
],
),
html.Div(
className="mw-diagnostics",
children=[
html.Div(id="scorer-readout", className="diag-card"),
html.Div(id="rossby-readout", className="diag-card"),
html.Div(id="nonlin-readout", className="diag-card"),
html.Div(id="critical-readout", className="diag-card"),
],
),
# Top row: w and u' heatmaps side-by-side. Streamline view lives
# below at full width so the trajectory pattern is legible at
# wide aspect ratios (it's the "money plot" of the tool).
html.Div(
className="mw-heatmaps",
children=[
dcc.Graph(id="w-plot", config={"displayModeBar": False}),
dcc.Graph(id="uprime-plot", config={"displayModeBar": False}),
],
),
html.Div(
className="mw-streamline-full",
children=[
dcc.Graph(id="streamline-plot", config={"displayModeBar": False}),
],
),
# Shared state for editable profiles.
dcc.Store(
id="profile-store",
data={
"z": zs0.tolist(),
"u": us0.tolist(),
"theta": thetas0.tolist(),
},
),
# Undo history — a stack of prior profile-store states. Each edit
# pushes the pre-edit state; undo pops the most recent entry.
dcc.Store(id="profile-history", data=[]),
# Raw HRRR column cached after a successful fetch: the east/north
# wind components (u, v), potential temperature, target heights,
# and meta info. Lets the "flow from" slider re-project the wind
# onto a new axis without another AWS round-trip.
dcc.Store(id="hrrr-raw-store", data={}),
html.Footer(
className="mw-footer",
children=[
html.Span("On the Profile tab, drag the gold circles left/right to edit u(z) and θ(z). "),
html.Span("Click 'Analyze flow' to update the fields."),
],
),
# Theory & About modal — hidden by default, shown when the user
# clicks the "📖 Theory & About" link in the header. The outer
# div is the dark backdrop (click-to-dismiss); the inner div is
# the card that actually contains the rendered README.
html.Div(
id="readme-modal",
className="mw-modal",
style={"display": "none"},
n_clicks=0,
children=[
html.Div(
id="readme-modal-card",
className="mw-modal-card",
# Swallow clicks inside the card so clicking text
# doesn't close the modal. Only the backdrop does.
n_clicks=0,
children=[
html.Button(
"×",
id="close-readme",
n_clicks=0,
className="mw-modal-close",
title="Close (Esc)",
),
dcc.Markdown(
_README_MD,
className="mw-readme-content",
link_target="_blank",
),
],
),
],
),
],
)
app.index_string = """
<!doctype html>
<html>
<head>
{%metas%}<title>{%title%}</title>{%favicon%}{%css%}
<style>
body { background: #0b0e14; color: #dfe3ea; font-family: -apple-system, system-ui, sans-serif; }
.mw-root { max-width: 1400px; margin: 0 auto; padding: 20px; }
.mw-header { display: flex; align-items: center; gap: 14px; margin-bottom: 16px; }
.mw-header-text { display: flex; flex-direction: column; }
.mw-logo { width: 56px; height: 56px; border-radius: 6px; flex-shrink: 0; }
.mw-header h1 { margin: 0 0 4px 0; font-size: 24px; }
.mw-subtitle { color: #9aa3ad; font-size: 13px; }
.mw-subtitle a { color: #57b3ff; }
.mw-readme-link-row { margin-top: 6px; }
.mw-readme-link { background: #1e2835; border: 1px solid #2d3a4b; color: #9cd2ff; padding: 3px 12px; border-radius: 4px; font-size: 12px; cursor: pointer; font-family: inherit; }
.mw-readme-link:hover { background: #2a3a4e; color: #c7e4ff; border-color: #3b86e6; }
.mw-modal { position: fixed; top: 0; left: 0; right: 0; bottom: 0; background: rgba(0,0,0,0.72); display: flex; align-items: flex-start; justify-content: center; z-index: 9999; padding: 40px 20px; overflow-y: auto; }
.mw-modal-card { position: relative; background: #0f141c; border: 1px solid #2d3a4b; border-radius: 8px; max-width: 860px; width: 100%; padding: 24px 36px 28px 36px; color: #dfe3ea; box-shadow: 0 16px 40px rgba(0,0,0,0.6); }
.mw-modal-close { position: absolute; top: 8px; right: 12px; background: transparent; border: none; color: #9aa3ad; font-size: 26px; line-height: 1; cursor: pointer; padding: 4px 10px; font-family: inherit; }
.mw-modal-close:hover { color: #ffffff; }
.mw-readme-content h1 { font-size: 24px; color: #6ecbff; margin-top: 0; border-bottom: 1px solid #2d3a4b; padding-bottom: 8px; }
.mw-readme-content h2 { font-size: 18px; color: #6ecbff; margin-top: 22px; }
.mw-readme-content h3 { font-size: 15px; color: #9cd2ff; margin-top: 18px; }
.mw-readme-content p, .mw-readme-content li { color: #cbd3dc; font-size: 13px; line-height: 1.55; }
.mw-readme-content a { color: #57b3ff; }
.mw-readme-content code { background: #131a24; padding: 1px 5px; border-radius: 3px; color: #ffd685; font-family: Monaco, Menlo, "Courier New", monospace; font-size: 12px; }
.mw-readme-content pre { background: #131a24; padding: 10px 14px; border-radius: 4px; overflow-x: auto; border: 1px solid #1f2632; }
.mw-readme-content pre code { background: transparent; padding: 0; color: #dfe3ea; }
.mw-readme-content blockquote { border-left: 3px solid #3b86e6; margin: 12px 0; padding: 2px 14px; color: #c7ced6; background: #131a24; }
.mw-controls { display: grid; grid-template-columns: repeat(2, 1fr); gap: 16px 28px; background: #11161f; padding: 18px; border-radius: 8px; margin: 14px 0; }
.mw-controls.profile { grid-template-columns: 1fr 1fr 1fr; }
/* Two-layer tab mirrors the profile tab's 3-column grid: sliders | sliders | Actions. */
.mw-controls.two-layer { grid-template-columns: 1fr 1fr 1fr; }
.slider-row { display: flex; flex-direction: column; gap: 4px; }
.slider-header { display: flex; justify-content: space-between; font-size: 13px; }
.slider-label { color: #c7ced6; }
.slider-value { color: #6ecbff; font-variant-numeric: tabular-nums; }
.mw-presets { display: flex; gap: 8px; margin: 10px 0 0 0; }
.mw-presets button, .mw-analyze { background: #1e2835; border: 1px solid #2d3a4b; color: #dfe3ea; padding: 6px 12px; border-radius: 6px; cursor: pointer; font-size: 13px; }
.mw-presets button:hover, .mw-analyze:hover { background: #2a3a4e; }
.mw-analyze { background: #2469c6; border-color: #3b86e6; font-weight: 600; padding: 8px 18px; }
.mw-analyze:hover { background: #3079d8; }
.mw-diagnostics { display: grid; grid-template-columns: repeat(2, 1fr); gap: 12px; margin: 10px 0; }
.diag-card { background: #11161f; padding: 10px 16px; border-radius: 6px; font-size: 14px; }
.diag-card .v { color: #ffd685; font-weight: 700; margin-left: 8px; font-variant-numeric: tabular-nums; }
.diag-card .note { color: #9aa3ad; font-size: 12px; margin-left: 10px; }
.mw-plots { display: grid; grid-template-columns: 1fr 1fr; gap: 12px; }
.mw-heatmaps { display: grid; grid-template-columns: 1fr 1fr; gap: 12px; }
.mw-streamline-full { margin-top: 12px; }
.mw-streamline-full > .dash-graph { width: 100%; }
.mw-profile-editors { display: grid; grid-template-columns: 1fr 1fr; gap: 12px; margin-top: 6px; }
.mw-profile-toolbar { display: flex; align-items: center; gap: 10px; margin-top: 10px; }
.mw-undo { background: #1e2835; border: 1px solid #2d3a4b; color: #dfe3ea; padding: 5px 12px; border-radius: 6px; cursor: pointer; font-size: 13px; }
.mw-undo:hover:not(:disabled) { background: #2a3a4e; }
.mw-undo:disabled { opacity: 0.4; cursor: default; }
.mw-undo-status { color: #8d97a2; font-size: 12px; }
/* HRRR card takes the first 2 of 3 columns of .mw-controls.profile (so
its one-line input row has room), and the Actions card sits in the
remaining column to its right. */
.mw-hrrr-section { grid-column: span 2; }
.mw-actions-section { grid-column: span 1; display: flex; flex-direction: column; gap: 10px; }
.mw-action-btn { width: 100%; padding: 10px 14px; font-size: 14px; text-align: center; background: #1e2835; border: 1px solid #2d3a4b; color: #dfe3ea; border-radius: 6px; cursor: pointer; }
.mw-action-btn:hover { background: #2a3a4e; }
.mw-action-btn.mw-analyze { background: #2469c6; border-color: #3b86e6; font-weight: 600; }
.mw-action-btn.mw-analyze:hover { background: #3079d8; }
.mw-hrrr-row { display: flex; align-items: center; gap: 8px; flex-wrap: wrap; margin-top: 6px; }
.mw-hrrr-row-compact { gap: 8px; row-gap: 4px; flex-wrap: nowrap; width: 100%; }
.mw-hrrr-lbl { font-size: 11px; color: #9aa3ad; min-width: 0; white-space: nowrap; flex-shrink: 0; }
.mw-hrrr-input { background: #0f1520; border: 1px solid #2d3a4b; color: #dfe3ea; padding: 2px 6px; border-radius: 4px; font-size: 11px; width: 70px; font-family: inherit; flex-shrink: 0; }
.mw-hrrr-input.wide { flex: 1 1 auto; min-width: 110px; width: auto; }
.mw-hrrr-btn { font-size: 11px; padding: 3px 12px; margin-left: auto; flex-shrink: 0; }
.mw-hrrr-status { color: #9aa3ad; font-size: 11px; margin-top: 4px; min-height: 14px; }
.mw-hrrr-status.error { color: #ff8a8a; }
.mw-hrrr-status.ok { color: #89d185; }
/* Flow-from slider row — label on the left, wide slider stretching to the
edge, current value pinned on the right. */
.mw-hrrr-dir-row { display: flex; align-items: center; gap: 10px; margin-top: 10px; width: 100%; }
.mw-hrrr-dir-row > label { min-width: 60px; flex-shrink: 0; }
.mw-hrrr-dir-slider { flex: 1 1 auto; min-width: 0; padding: 0 8px; }
.mw-hrrr-dir-val { color: #6ecbff; font-variant-numeric: tabular-nums; font-weight: 600; min-width: 56px; text-align: right; flex-shrink: 0; font-size: 12px; }
.mw-profile-diagnostics { display: grid; grid-template-columns: 1fr 1fr; gap: 12px; margin-top: 8px; }
.mw-footer { margin-top: 20px; color: #8f98a3; font-size: 12px; }
.mw-global { display: grid; grid-template-columns: 130px 1fr 80px 1fr; align-items: center; gap: 14px; background: #131a24; padding: 10px 16px; border-radius: 6px; margin-top: 10px; }
.mw-global-label { font-size: 13px; color: #c7ced6; }
.mw-global-value { color: #6ecbff; font-variant-numeric: tabular-nums; font-weight: 600; }
.mw-global-note { font-size: 12px; color: #8f98a3; }
.section-title { font-size: 11px; font-weight: 600; color: #8d97a2; letter-spacing: 0.08em; text-transform: uppercase; margin-bottom: 6px; }
.section { background: #161d29; padding: 12px; border-radius: 6px; }
</style>
</head>
<body>
{%app_entry%}
<footer>{%config%}{%scripts%}{%renderer%}</footer>
</body>
</html>
"""
_register_callbacks(app)
return app
# ---------------------------------------------------------------------------
# Callbacks
# ---------------------------------------------------------------------------
def _two_layer_controls():
d = TWO_LAYER_DEFAULTS
return html.Div(
# Three-column grid to mirror the profile tab: atmospheric sliders |
# terrain+domain+spectrum sliders | Actions column. The Actions
# column holds Reset/Analyze plus the preset buttons so the user's
# eye finds every "do something" control in the same place on both
# tabs.
className="mw-controls two-layer",
children=[
html.Div(
className="section",
children=[
html.Div("Atmospheric profile", className="section-title"),
_slider("U", "Surface wind (m/s)", 0, 100, 1, d["U"]),
_slider("L_upper", "L upper (×10⁻⁴)", 0, 50, 0.1, d["L_upper"]),
_slider("L_lower", "L lower (×10⁻⁴)", 0, 50, 0.1, d["L_lower"]),
_slider("H", "Interface ht. (km)", 0, 20, 0.1, d["H"]),
],
),
html.Div(
className="section",
children=[
html.Div("Terrain profile", className="section-title"),
_slider("mtn_h", "Max height (km)", 0, 3, 0.05, d["mtn_h"]),
_slider("mtn_a", "Half-width (km)", 0.25, 25, 0.25, d["mtn_a"]),
html.Div("Domain profile", className="section-title", style={"marginTop": "12px"}),
_slider("xdom", "Horizontal (km)", 5, 100, 1, d["xdom"]),
_slider("zdom", "Vertical (km)", 1, 20, 0.5, d["zdom"]),
html.Div("Spectral profile", className="section-title", style={"marginTop": "12px"}),
_slider("mink_k", "Min wave# (half-widths)", 0, 50, 0.5, d["mink_k"]),
_slider("maxk_k", "Max wave# (half-widths)", 0, 50, 0.5, d["maxk_k"]),
],
),
# Actions column — Reset / Analyze at the top, presets below.
# Shares the .mw-actions-section layout with the profile tab so
# both tabs look and feel the same.
html.Div(
className="section mw-actions-section",
children=[
html.Div("Actions", className="section-title"),
html.Button(
"Reset to defaults",
id="reset-two",
className="mw-action-btn",
title="Restore every slider on this tab to its initial value.",
),
html.Button(
"Analyze flow",
id="analyze-two",
className="mw-analyze mw-action-btn",
),
html.Div(
"Presets",
className="section-title",
style={"marginTop": "10px"},
),
html.Button(
"Uniform atmosphere",
id="preset-uniform",
className="mw-action-btn",
title="Hart's Example 1 — constant Scorer parameter, no trapping.",
),
html.Button(
"Trapped lee waves",
id="preset-trapped",
className="mw-action-btn",
title="Hart's Example 2 — strong lower-layer Scorer, trapped wave train downstream.",
),
html.Button(
"Near-downslope",
id="preset-downslope",
className="mw-action-btn",
title=(
"Strong lee waves approaching the downslope-windstorm "
"regime. Not from Hart's examples — linear Fourier/Scorer "
"theory cannot fully simulate real downslope windstorms "
"because they are fundamentally nonlinear."
),
),
html.Button(
"Near critical layer at 2 km",
id="preset-critical-2km",
className="mw-action-btn",
title=(
"Two-layer caricature of critical-level absorption. "
"Strong Scorer contrast across an interface at 2 km "
"(l_lower² >> k² >> l_upper²) reflects most wave "
"energy downward, mimicking Booker & Bretherton "
"(1967) absorption. A true critical level requires "
"U(z)=0, which two-layer mode cannot represent — "
"use the Profile tab for the physically faithful "
"wind-reversal setup."
),
),
],
),
],
)
def _profile_controls(zs, us, thetas):
return html.Div(
children=[
html.Div(
className="mw-controls profile",
children=[
html.Div(
className="section",
children=[
html.Div("Terrain", className="section-title"),
_slider("p_mtn_h", "Max height (km)", 0, 3, 0.05, 0.5),
_slider("p_mtn_a", "Half-width (km)", 0.25, 25, 0.25, 2.5),
],
),
html.Div(
className="section",
children=[
html.Div("Domain", className="section-title"),
_slider("p_xdom", "Horizontal (km)", 5, 100, 1, 40),
_slider("p_zdom", "Vertical (km)", 1, 20, 0.5, 10),
],
),
html.Div(
className="section",
children=[
html.Div("Spectrum", className="section-title"),
_slider("p_mink_k", "Min wave# (half-widths)", 0, 50, 0.5, 0),
_slider("p_maxk_k", "Max wave# (half-widths)", 0, 50, 0.5, 30),
],
),
html.Div(
className="section mw-hrrr-section",
children=[
html.Div("Initialize from HRRR (AWS)", className="section-title"),
html.Div(
className="mw-hrrr-row mw-hrrr-row-compact",
children=[
html.Label("Lat °N", className="mw-hrrr-lbl"),
dcc.Input(
id="hrrr-lat",
type="number",
value=40.0,
step=0.01,
className="mw-hrrr-input",
),
html.Label("Lon °E", className="mw-hrrr-lbl"),
dcc.Input(
id="hrrr-lon",
type="number",
value=-105.5,
step=0.01,
className="mw-hrrr-input",
),
html.Label(
"Cycle",
className="mw-hrrr-lbl",
title="UTC init time as YYYYMMDDHH, e.g. 2024060112.",
),
dcc.Input(
id="hrrr-datetime",
type="text",
value="",
placeholder="YYYYMMDDHH",
className="mw-hrrr-input wide",
),
html.Button(
"Fetch",
id="hrrr-fetch",
className="mw-analyze mw-hrrr-btn",
),
],
),
# Flow-from slider lives on its own row so it can
# stretch across the full card. Moving it updates
# the along-flow projection *without* triggering
# another HRRR download — the raw east/north wind
# components are cached in hrrr-raw-store below.
html.Div(
className="mw-hrrr-dir-row",
children=[
html.Label(
"Flow from",
className="mw-hrrr-lbl",
title=(
"Meteorological convention: direction "
"the wind is blowing FROM. 0=N, 90=E, "
"180=S, 270=W. Moving this slider "
"re-projects the cached HRRR wind "
"onto the new axis (no re-download)."
),
),
html.Div(
className="mw-hrrr-dir-slider",
children=dcc.Slider(
id="hrrr-dir",
min=0,
max=360,
step=1,
value=270,
marks={
0: "0° N",
90: "90° E",
180: "180° S",
270: "270° W",
360: "360° N",
},
tooltip={"placement": "bottom", "always_visible": False},
),
),
html.Span(id="hrrr-dir-val", className="mw-hrrr-dir-val"),
],
),
dcc.Loading(
id="hrrr-loading",
type="circle",
children=html.Div(
id="hrrr-status",
className="mw-hrrr-status",
),
),
],
),
# Actions panel — sits in the 3rd grid column beside the
# 2/3-width HRRR card so the Analyze button is always
# visible without scrolling past the fetch controls.
html.Div(
className="section mw-actions-section",
children=[
html.Div("Actions", className="section-title"),
html.Button(
"Reset profile",
id="reset-profile",
className="mw-action-btn",
),
html.Button(
"Analyze flow",
id="analyze-profile",
className="mw-analyze mw-action-btn",
),
],
),
],
),
html.Div(
className="mw-profile-toolbar",
children=[
html.Button(
"↶ Undo",
id="undo-profile",
className="mw-undo",
disabled=True,
title="Revert the last profile edit (up to 50 steps).",
),
html.Span(id="undo-status", className="mw-undo-status"),
],
),
html.Div(
className="mw-profile-editors",
children=[
dcc.Graph(
id="u-profile-graph",
figure=_profile_editor_figure("Zonal wind u(z)", us, zs, xunit="m s⁻¹", xrange=U_RANGE),
config={"edits": {"shapePosition": True}, "displayModeBar": False, "scrollZoom": False},
),
dcc.Graph(
id="theta-profile-graph",
figure=_profile_editor_figure(
"Potential temperature θ(z)", thetas, zs, xunit="K", xrange=THETA_RANGE
),
config={"edits": {"shapePosition": True}, "displayModeBar": False, "scrollZoom": False},
),
],
),
html.Div(
"Drag the gold circles left/right on each profile to change the u or θ "
"value at that height. Heights are fixed at 18 evenly-spaced levels; the "
"blue line shows the current profile and follows the points as you drag. "
"The four diagnostics below update live — Scorer parameter L² (trapped "
"waves need L² to decrease aloft), Richardson number Ri (< 0.25 flags "
"shear instability), Brunt–Väisälä N² (stratification strength), and "
"the potential-temperature lapse rate dθ/dz. Click 'Analyze flow' to "
"update the wave solution.",
style={"color": "#8f98a3", "fontSize": "12px", "marginTop": "6px"},
),
html.Div("Live profile diagnostics", className="section-title",
style={"marginTop": "14px"}),
html.Div(
className="mw-profile-diagnostics",
children=[
dcc.Graph(id="diag-scorer", config={"displayModeBar": False}),
dcc.Graph(id="diag-ri", config={"displayModeBar": False}),
dcc.Graph(id="diag-n2", config={"displayModeBar": False}),
dcc.Graph(id="diag-dthdz", config={"displayModeBar": False}),
],
),
],
)
def _profile_editor_figure(title, values, zs, xunit, xrange):
"""Build an editable profile figure.
Each point is represented as a draggable circle *shape* — Plotly supports
shape dragging via the ``edits.shapePosition`` config flag — and a line
trace connects the current values for visualization. When the user drags
a circle, ``relayoutData`` fires with ``shapes[i].x0``/``x1`` keys, which
the ``_profile_update`` callback parses back into the shared store. The
store-driven ``_redraw_profiles`` callback then regenerates both figures
so the connecting line follows the dragged points.
"""
# Sanitize any NaN/inf so a corrupted store value can't knock a circle
# off screen. We do NOT clip to the nominal xrange here — if HRRR
# delivers a value outside the default axis, extend the axis rather
# than silently mangling the data. The drag callback applies its own
# clamp so user-dragged points still stay on screen.
values = np.asarray(values, dtype=float)
values = np.where(np.isfinite(values), values, 0.5 * (xrange[0] + xrange[1]))
zs_km = np.asarray(zs, dtype=float) / 1000.0
# Data-driven axis: take the wider of the default xrange and the actual
# data span, with a little padding so edge points aren't on the border.
if values.size:
v_min = float(np.min(values))
v_max = float(np.max(values))
span = max(v_max - v_min, 1.0)
pad = 0.05 * span
axis_lo = min(xrange[0], v_min - pad)
axis_hi = max(xrange[1], v_max + pad)
else:
axis_lo, axis_hi = xrange
effective_xrange = (axis_lo, axis_hi)
fig = go.Figure()
fig.add_trace(
go.Scatter(
x=values,
y=zs_km,
mode="lines+markers",
marker=dict(size=8, color="#6ecbff", line=dict(color="white", width=1)),
line=dict(color="#6ecbff", width=2),
name=title,
hoverinfo="skip",
)
)
# One draggable circle per profile point. Pixel sizing makes every
# shape render as a visually round circle regardless of how stretched
# the axes are; dragging updates shapes[i].xanchor in relayoutData.
radius_px = 9
shapes = []
for v, zk in zip(values, zs_km):
shapes.append(
dict(
type="circle",
xref="x",
yref="y",
xsizemode="pixel",
ysizemode="pixel",
xanchor=float(v),
yanchor=float(zk),
x0=-radius_px,
x1=radius_px,
y0=-radius_px,
y1=radius_px,
fillcolor="#ffd685",
line=dict(color="white", width=1.5),
editable=True,
layer="above",
)
)
fig.update_layout(
title=title,
xaxis_title=f"value ({xunit})",
yaxis_title="height (km)",
template="plotly_dark",
margin=dict(l=60, r=20, t=50, b=50),
height=PROFILE_FIG_HEIGHT_PX,
dragmode=False,
xaxis=dict(range=list(effective_xrange), fixedrange=True),
yaxis=dict(range=[0, zs_km[-1]], fixedrange=True),
shapes=shapes,
)
return fig
def _profile_diagnostics(zs, us, thetas):
"""Return (L², Ri, N², dθ/dz) arrays evaluated on the profile grid."""
zs = np.asarray(zs, dtype=float)
us = np.asarray(us, dtype=float)
thetas = np.asarray(thetas, dtype=float)
l2 = scorer_from_profile(zs, us, thetas)
n2 = brunt_vaisala(zs, thetas)
# dU/dz and dθ/dz via the same 3-point finite difference used in
# reference.py / scorer_from_profile so diagnostics stay consistent.
n = zs.size
dudz = np.zeros(n)
dthdz = np.zeros(n)
for i in range(n):
if i == 0:
dudz[i] = (us[1] - us[0]) / (zs[1] - zs[0])
dthdz[i] = (thetas[1] - thetas[0]) / (zs[1] - zs[0])
elif i == n - 1:
dudz[i] = (us[-1] - us[-2]) / (zs[-1] - zs[-2])
dthdz[i] = (thetas[-1] - thetas[-2]) / (zs[-1] - zs[-2])
else:
h1 = zs[i] - zs[i - 1]
h2 = zs[i + 1] - zs[i]
dudz[i] = (
us[i + 1] * h1 ** 2
- us[i - 1] * h2 ** 2
+ us[i] * (h2 ** 2 - h1 ** 2)
) / (h1 * h2 * (h1 + h2))
dthdz[i] = (
thetas[i + 1] * h1 ** 2
- thetas[i - 1] * h2 ** 2
+ thetas[i] * (h2 ** 2 - h1 ** 2)
) / (h1 * h2 * (h1 + h2))
# Ri = N² / (dU/dz)². Guard against vanishing shear.
with np.errstate(divide="ignore", invalid="ignore"):
ri = np.where(np.abs(dudz) > 1e-6, n2 / (dudz ** 2), np.inf)
return l2, ri, n2, dthdz
def _diagnostic_figure(title, values, zs, xunit, color, xrange=None, log_x=False, ref_line=None):
"""Small read-only profile plot of ``values(z)``."""
values = np.asarray(values, dtype=float)
zs_km = np.asarray(zs, dtype=float) / 1000.0
plot_x = values
if log_x:
# Use symmetric log to tolerate negative values without dropping them.
plot_x = values
fig = go.Figure()
fig.add_trace(
go.Scatter(
x=plot_x,
y=zs_km,
mode="lines+markers",
marker=dict(size=6, color=color, line=dict(color="white", width=0.5)),
line=dict(color=color, width=2),
hovertemplate=f"%{{x:.3g}} {xunit}<br>%{{y:.2f}} km<extra></extra>",
showlegend=False,
)
)
if ref_line is not None:
fig.add_vline(x=ref_line, line=dict(color="#ffd685", dash="dot", width=1))
xaxis_kwargs = dict(title=f"{xunit}")
if log_x:
xaxis_kwargs["type"] = "log"
if xrange is not None:
xaxis_kwargs["range"] = list(xrange)
fig.update_layout(
title=title,
yaxis_title="height (km)",
template="plotly_dark",
margin=dict(l=50, r=15, t=40, b=40),
height=340,
xaxis=xaxis_kwargs,
yaxis=dict(range=[0, zs_km[-1]]),
)
return fig
def _diagnostic_figures(store):
"""Build all four diagnostic figures from the current profile store."""
zs = np.asarray(store["z"], dtype=float)
us = np.asarray(store["u"], dtype=float)
thetas = np.asarray(store["theta"], dtype=float)
l2, ri, n2, dthdz = _profile_diagnostics(zs, us, thetas)
# Scorer parameter. Display in units of 10⁻⁸ m⁻² so the magnitudes line
# up with the two-layer L sliders: L_slider = L × 10⁴ m⁻¹ means
# L_slider² = L² × 10⁸, so L²(display) directly equals L_slider².
# E.g. the two-layer defaults of L_lower=10, L_upper=4 correspond to
# L²_lower=100, L²_upper=16 on this plot.
l2_scaled = l2 * 1e8
l_fig = _diagnostic_figure(
"Scorer parameter L²(z)",
l2_scaled,
zs,
xunit="L² (×10⁻⁸ m⁻²) — same units as (two-layer L slider)²",
color="#6ecbff",
ref_line=0.0,
)
# Richardson number. Real-world Ri values span many orders of magnitude
# — a still-stable free-troposphere profile is easily 100s while the
# instability threshold is 0.25. Use a log x-axis so that variation is
# visible; clip negatives (from N² < 0 regions) to a small positive
# floor and mark them with a trailing annotation instead.
neg_mask = ri <= 0
ri_pos = np.where(neg_mask, np.nan, ri)
ri_pos = np.where(np.isfinite(ri_pos), ri_pos, 1e4)
ri_pos = np.clip(ri_pos, 1e-2, 1e4)
ri_fig = _diagnostic_figure(
"Richardson number Ri(z)",
ri_pos,
zs,
xunit="Ri (log scale, clipped 10⁻² – 10⁴)",
color="#ffb86c",
log_x=True,
ref_line=0.25,
)
# N² — units of s⁻², typical tropospheric values ~10⁻⁴; can be negative
# if the user drags θ(z) into a superadiabatic configuration.
n2_scaled = n2 * 1e4
n2_fig = _diagnostic_figure(
"Brunt–Väisälä N²(z)",
n2_scaled,
zs,
xunit="N² (×10⁻⁴ s⁻²)",
color="#a0e878",
ref_line=0.0,
)
# dθ/dz in K/km — the raw stratification before dividing by θ.
dthdz_fig = _diagnostic_figure(
"Lapse rate dθ/dz(z)",
dthdz * 1000.0,
zs,
xunit="dθ/dz (K km⁻¹)",
color="#f57aa5",
ref_line=0.0,
)
return l_fig, ri_fig, n2_fig, dthdz_fig
def _register_callbacks(app: Dash):
# --- latitude readout ------------------------------------------------
app.clientside_callback(
"function(v) { return Math.round(v) + '\u00b0 N'; }",
Output("latit-val", "children"),
Input("latit", "value"),
)
# --- Theory & About modal ----------------------------------------------
# The show button opens the modal, the × button closes it. Returning an
# empty style dict lets the .mw-modal CSS class (display: flex) take
# effect; returning {"display": "none"} hides it.
@app.callback(
Output("readme-modal", "style"),
[
Input("show-readme", "n_clicks"),
Input("close-readme", "n_clicks"),
],
prevent_initial_call=True,
)
def _toggle_readme(_show, _close):
if ctx.triggered_id == "show-readme":
return {}
return {"display": "none"}
# Close the modal on Esc keypress as well. Clientside so it doesn't
# require a round-trip; the keydown listener is attached once on load
# and clicks the × button synthetically when Esc is pressed while the
# modal is visible.
app.clientside_callback(
"""
function() {
if (window.__mw_readme_esc_attached) return window.dash_clientside.no_update;
window.__mw_readme_esc_attached = true;
document.addEventListener('keydown', function(e) {
if (e.key !== 'Escape') return;
var modal = document.getElementById('readme-modal');
if (!modal) return;
if (modal.style.display === 'none') return;
var btn = document.getElementById('close-readme');
if (btn) btn.click();
});
return window.dash_clientside.no_update;
}
""",
Output("close-readme", "title"),
Input("close-readme", "id"),
)
# --- HRRR flow-from slider readout -----------------------------------
# Shows the current azimuth next to the slider with a compass letter
# (N/NE/E/.../NW). Purely a UI hint — the server callback still uses
# the raw degrees when computing the along-flow projection.
app.clientside_callback(
"""
function(v) {
if (v === null || v === undefined) return '';
var deg = Math.round(v);
var dirs = ['N','NE','E','SE','S','SW','W','NW','N'];
var idx = Math.round(deg / 45) % 8;
return deg + '\u00b0 ' + dirs[idx];
}
""",
Output("hrrr-dir-val", "children"),
Input("hrrr-dir", "value"),
)
# --- live slider readouts --------------------------------------------
for sid, unit in [
("U", " m/s"),
("L_upper", ""),
("L_lower", ""),
("H", " km"),
("mtn_h", " km"),
("mtn_a", " km"),
("xdom", " km"),
("zdom", " km"),
("mink_k", ""),
("maxk_k", ""),
("p_mtn_h", " km"),
("p_mtn_a", " km"),
("p_xdom", " km"),
("p_zdom", " km"),
("p_mink_k", ""),
("p_maxk_k", ""),
]:
app.clientside_callback(
f"function(v) {{ return (Math.round(v*100)/100) + '{unit}'; }}",
Output(f"{sid}-val", "children"),
Input(sid, "value"),
)
# --- swap control panel on tab change --------------------------------
# Both control panels are always in the DOM; we just toggle visibility.
@app.callback(
[Output("controls-two-layer", "style"), Output("controls-profile", "style")],
Input("mode-tabs", "value"),
)
def _swap(mode):
if mode == "two-layer":
return {}, {"display": "none"}
return {"display": "none"}, {}
# --- presets and reset apply to sliders ------------------------------
# Both the three preset buttons and the "Reset to defaults" button in
# the Actions column funnel through this callback. Reset is just
# another preset whose values happen to be TWO_LAYER_DEFAULTS.
@app.callback(
[
Output("U", "value"),
Output("L_upper", "value"),
Output("L_lower", "value"),
Output("H", "value"),
Output("mtn_h", "value"),
Output("mtn_a", "value"),
Output("xdom", "value"),
Output("zdom", "value"),
Output("mink_k", "value"),
Output("maxk_k", "value"),
],
[
Input("preset-uniform", "n_clicks"),
Input("preset-trapped", "n_clicks"),
Input("preset-downslope", "n_clicks"),
Input("preset-critical-2km", "n_clicks"),
Input("reset-two", "n_clicks"),
],
prevent_initial_call=True,
)
def _apply_preset(nu, nt, nd, nc, nr):
from dash import ctx
trig = ctx.triggered_id
if trig == "reset-two":
p = TWO_LAYER_DEFAULTS
else:
key = {
"preset-uniform": "uniform",
"preset-trapped": "trapped",
"preset-downslope": "downslope",
"preset-critical-2km": "critical_caricature",
}.get(trig)
if key is None:
return [no_update] * 10
p = PRESETS[key]
return [
p["U"], p["L_upper"], p["L_lower"], p["H"],
p["mtn_h"], p["mtn_a"], p["xdom"], p["zdom"],
p["mink_k"], p["maxk_k"],
]
# --- two-layer analyze ------------------------------------------------
@app.callback(
[
Output("streamline-plot", "figure"),
Output("w-plot", "figure"),
Output("uprime-plot", "figure"),
Output("scorer-readout", "children"),
Output("rossby-readout", "children"),
Output("nonlin-readout", "children"),
Output("critical-readout", "children"),
],
[
Input("analyze-two", "n_clicks"),
Input("analyze-profile", "n_clicks"),
],
[
State("mode-tabs", "value"),
State("U", "value"),
State("L_upper", "value"),
State("L_lower", "value"),
State("H", "value"),
State("mtn_h", "value"),
State("mtn_a", "value"),
State("xdom", "value"),
State("zdom", "value"),
State("mink_k", "value"),
State("maxk_k", "value"),
State("p_mtn_h", "value"),
State("p_mtn_a", "value"),
State("p_xdom", "value"),
State("p_zdom", "value"),
State("p_mink_k", "value"),
State("p_maxk_k", "value"),
State("profile-store", "data"),
State("latit", "value"),
],
prevent_initial_call=False,
)
def _run(
n_two,
n_prof,
mode,
U,
L_upper,
L_lower,
H,
mtn_h,
mtn_a,
xdom,
zdom,
mink_k,
maxk_k,
p_mtn_h,
p_mtn_a,
p_xdom,
p_zdom,
p_mink_k,
p_maxk_k,
store,
latit_deg,
):
from dash import ctx
trig = ctx.triggered_id
print(
f"[mountain-waves] _run fired: trigger={trig!r} mode={mode!r} "
f"n_two={n_two} n_prof={n_prof} lat={latit_deg}",
flush=True,
)
lat = latit_deg if latit_deg is not None else 45.0
try:
if mode == "profile":
params = {
"mtn_h": p_mtn_h if p_mtn_h is not None else 0.5,
"mtn_a": p_mtn_a if p_mtn_a is not None else 2.5,
"xdom": p_xdom if p_xdom is not None else 40,
"zdom": p_zdom if p_zdom is not None else 10,
"mink_k": p_mink_k if p_mink_k is not None else 0,
"maxk_k": p_maxk_k if p_maxk_k is not None else 30,
}
zs = np.asarray(store["z"])
us = np.asarray(store["u"])
thetas = np.asarray(store["theta"])
sfig, wfig, upfig, scorer, rossby = _profile_plots(params, zs, us, thetas, latit_deg=lat)
else:
params = {
"U": U if U is not None else 20.0,
"L_upper": L_upper if L_upper is not None else 4.0,
"L_lower": L_lower if L_lower is not None else 10.0,
"H": H if H is not None else 3.5,
"mtn_h": mtn_h if mtn_h is not None else 0.5,
"mtn_a": mtn_a if mtn_a is not None else 2.5,
"xdom": xdom if xdom is not None else 40,
"zdom": zdom if zdom is not None else 10,
"mink_k": mink_k if mink_k is not None else 0,
"maxk_k": maxk_k if maxk_k is not None else 30,
}
sfig, wfig, upfig, scorer, rossby = _two_layer_plots(params, latit_deg=lat)
print(
f"[mountain-waves] ok: scorer={scorer:.3f} rossby={rossby:.3f}",
flush=True,
)
except Exception as exc:
import traceback
traceback.print_exc()
print(f"[mountain-waves] _run FAILED: {exc!r}", flush=True)
raise
# Nonlinearity indicator Nh/U = L * h (in the layer where the wave
# is forced). Linear Fourier/Scorer theory breaks down around
# Nh/U ≳ 0.85; beyond that, real flow would overturn or transition
# to hydraulic/downslope-windstorm behavior that this model cannot
# represent. See Smith (1985) and Hart's "Problems" note.
if mode == "profile":
zs = np.asarray(store["z"])
thetas = np.asarray(store["theta"])
us = np.asarray(store["u"])
# crude surface N from finite-difference dθ/dz
dth = (thetas[1] - thetas[0]) / (zs[1] - zs[0])
n_sfc = math.sqrt(max(9.80665 / thetas[0] * dth, 0.0))
u_sfc = abs(float(us[0])) or 1e-6
h_m = (p_mtn_h if p_mtn_h is not None else 0.5) * 1000.0
nhu = n_sfc * h_m / u_sfc
else:
# L = N/U for uniform U → N = L·U, and Nh/U = L·h.
L_lower_m = params["L_lower"] * 1e-4
nhu = L_lower_m * params["mtn_h"] * 1000.0
if nhu < 0.5:
flag = "linear regime"
elif nhu < 0.85:
flag = "approaching nonlinear"
elif nhu < 1.2:
flag = "near breaking — results questionable"
else:
flag = "past breaking — model unreliable"
scorer_badge = html.Span(
[
html.B("Scorer condition"),
html.Span(f"{scorer:.3f}", className="v"),
html.Span("(trapped > 1)", className="note"),
]
)
rossby_badge = html.Span(
[
html.B(f"Rossby number ({lat:.0f}°N)"),
html.Span(f"{rossby:.2f}", className="v"),
html.Span("(Coriolis significant if ≲ 1)", className="note"),
]
)
nonlin_badge = html.Span(
[
html.B("Nh/U (nonlinearity)"),
html.Span(f"{nhu:.2f}", className="v"),
html.Span(f"({flag})", className="note"),
]
)
# Critical-level detection — profile mode only. The two-layer mode
# carries a single scalar U, so a "wind reversal" isn't even
# representable there, and the badge just states that.
if mode == "profile":
from .reference import critical_levels as _critical_levels
us_p = np.asarray(store["u"])
zs_p = np.asarray(store["z"])
crits = _critical_levels(zs_p, us_p)
if crits:
heights_km = ", ".join(f"{h/1000.0:.2f}" for h in crits)
critical_badge = html.Span(
[
html.B("⚠️ Critical level(s)"),
html.Span(f"z = {heights_km} km", className="v"),
html.Span(
"(U = 0 → linear theory breaks down; results near "
"these heights are not physical)",
className="note",
),
]
)
else:
critical_badge = html.Span(
[
html.B("Critical levels"),
html.Span("none", className="v"),
html.Span("(U does not cross zero)", className="note"),
]
)
else:
critical_badge = html.Span(
[
html.B("Critical levels"),
html.Span("n/a", className="v"),
html.Span(
"(two-layer mode uses a single U; switch to Profile "
"mode to prescribe wind reversals)",
className="note",
),
]
)
return sfig, wfig, upfig, scorer_badge, rossby_badge, nonlin_badge, critical_badge
# --- profile editing ---------------------------------------------------
# Drag-on-graph → update store. Each profile point is a Plotly "shape",
# and Plotly emits relayoutData entries like {"shapes[3].xanchor": ...}
# when a shape is dragged. We read that, clamp it into the axis range
# (so a stray drag off-screen cannot turn the profile into nonsense),
# and push the previous store onto the undo history before committing.
@app.callback(
[
Output("profile-store", "data", allow_duplicate=True),
Output("profile-history", "data", allow_duplicate=True),
],
[
Input("u-profile-graph", "relayoutData"),
Input("theta-profile-graph", "relayoutData"),
Input("reset-profile", "n_clicks"),
Input("undo-profile", "n_clicks"),
],
[
State("profile-store", "data"),
State("profile-history", "data"),
],
prevent_initial_call=True,
)
def _profile_update(u_relay, th_relay, reset_clicks, undo_clicks, store, history):
from dash import ctx
trig = ctx.triggered_id
history = list(history or [])
def _push(snapshot):
# Deduplicate and cap length.
if history and history[-1] == snapshot:
return
history.append(snapshot)
if len(history) > UNDO_HISTORY_MAX:
del history[: len(history) - UNDO_HISTORY_MAX]
def _snapshot(s):
# Deep-ish copy — plain lists/floats survive JSON round-tripping fine.
return {
"z": list(s["z"]),
"u": list(s["u"]),
"theta": list(s["theta"]),
}
# ---- undo -------------------------------------------------------
if trig == "undo-profile":
if not history:
return no_update, no_update
prev = history.pop()
return prev, history
# ---- reset ------------------------------------------------------
if trig == "reset-profile":
_push(_snapshot(store))
zs, us, thetas = _init_profile_figures()
return (
{"z": zs.tolist(), "u": us.tolist(), "theta": thetas.tolist()},
history,
)
# ---- drag -------------------------------------------------------
lo, hi = (U_RANGE if trig == "u-profile-graph" else THETA_RANGE)
def _has_shape_keys(relay):
return bool(relay) and any(
isinstance(k, str) and k.startswith("shapes[") for k in relay.keys()
)
def _apply(relay, current):
"""Pull new values out of a relayoutData payload and clamp them.
We ONLY honor ``shapes[i].xanchor`` here. Pixel-sized circles
also emit ``shapes[i].x0`` / ``x1`` when the user accidentally
grabs a resize handle — but those are *pixel* offsets, not data
coordinates, so averaging them yields garbage (which was the
bug behind "value shoots off-screen" reports). Rejecting
resize emissions means an edge-grab just does nothing instead
of corrupting the profile.
"""
if not relay:
return current, False
out = list(current)
changed = False
for i in range(len(out)):
kxa = f"shapes[{i}].xanchor"
if kxa not in relay:
continue
try:
v = float(relay[kxa])
except (TypeError, ValueError):
continue
if not math.isfinite(v):
continue
v = max(lo, min(hi, v))
if v != out[i]:
out[i] = v
changed = True
return out, changed
if trig == "u-profile-graph":
relay, field = u_relay, "u"
elif trig == "theta-profile-graph":
relay, field = th_relay, "theta"
else:
return no_update, no_update
new_values, changed = _apply(relay, store[field])
shape_edit = _has_shape_keys(relay)
if changed:
_push(_snapshot(store))
store[field] = new_values
if not changed and not shape_edit:
# Nothing shape-related happened (pan, zoom, autosize) —
# leave the store alone so _redraw_profiles doesn't fire.
return no_update, no_update
# Bump a revision stamp on every shape event so the redraw
# callback fires even if the edit was rejected (e.g. a resize-
# handle grab). This snaps any stretched oval back to its
# canonical round shape.
store["_rev"] = int(store.get("_rev", 0)) + 1
return store, history
# Enable/disable the undo button and show a depth hint.
@app.callback(
[
Output("undo-profile", "disabled"),
Output("undo-status", "children"),
],
Input("profile-history", "data"),
)
def _undo_status(history):
n = len(history or [])
if n == 0:
return True, ""
return False, f"{n} edit{'s' if n != 1 else ''} in history"
# --- HRRR profile fetch ----------------------------------------------
# Pulls U, V, T, HGT from the HRRR 0-h analysis on AWS (byte-range
# subset via the .idx sidecar), computes θ, and caches the raw east/north
# wind components in ``hrrr-raw-store``. The initial along-flow projection
# uses the current ``hrrr-dir`` slider value; further slider moves reuse
# the cached column (see ``_hrrr_redirect``) so no re-download is needed.
@app.callback(
[
Output("profile-store", "data", allow_duplicate=True),
Output("profile-history", "data", allow_duplicate=True),
Output("hrrr-raw-store", "data"),
Output("hrrr-status", "children"),
Output("hrrr-status", "className"),
],
Input("hrrr-fetch", "n_clicks"),
[
State("hrrr-lat", "value"),
State("hrrr-lon", "value"),
State("hrrr-dir", "value"),
State("hrrr-datetime", "value"),
State("profile-store", "data"),
State("profile-history", "data"),
],
prevent_initial_call=True,
)
def _hrrr_fetch(n_clicks, lat, lon, flow_deg, yyyymmddhh, store, history):
if not n_clicks:
return no_update, no_update, no_update, no_update, no_update
# Basic input validation — bail out early with a clear message
# rather than making the user wait on a network round-trip.
try:
lat_f = float(lat)
lon_f = float(lon)
flow_f = float(flow_deg)
except (TypeError, ValueError):
return (
no_update,
no_update,
no_update,
"Lat / Lon / Flow dir must all be numbers.",
"mw-hrrr-status error",
)
if not (-90.0 <= lat_f <= 90.0):
return (
no_update,
no_update,
no_update,
f"Lat {lat_f} outside [-90, 90].",
"mw-hrrr-status error",
)
try:
from .hrrr import along_flow_signed, fetch_profile
except ImportError as exc:
return (
no_update,
no_update,
no_update,
f"HRRR module failed to import: {exc}",
"mw-hrrr-status error",
)
zs_target = np.asarray(store["z"], dtype=float)
try:
z, u_raw, v_raw, theta, meta = fetch_profile(
lat_f, lon_f, yyyymmddhh, z_target_m=zs_target
)
except Exception as exc:
import traceback
traceback.print_exc()
return (
no_update,
no_update,
no_update,
f"Fetch failed: {exc}",
"mw-hrrr-status error",
)
# Don't clip HRRR data — the widened U_RANGE / THETA_RANGE should
# accommodate most real columns, and silently clamping was masking
# real wind and temperature structure (negative along-flow legs,
# cold-air-mass surface θ, etc.). If a sample still falls outside
# the axis, the editor auto-extends at render time.
u_arr = np.asarray(u_raw, dtype=float)
v_arr = np.asarray(v_raw, dtype=float)
th_arr = np.asarray(theta, dtype=float)
# Signed projection — wind reversals (e.g. an easterly jet when the
# user specified flow_from_deg corresponding to westerly) produce
# negative values, which the solver handles via the Scorer critical-
# level clamp and the "⚠️ Critical level" diagnostic badge.
u_along = along_flow_signed(u_arr, v_arr, flow_f)
# Push current state onto history so the fetch is undoable.
history = list(history or [])
snap = {"z": list(store["z"]), "u": list(store["u"]), "theta": list(store["theta"])}
if not history or history[-1] != snap:
history.append(snap)
if len(history) > UNDO_HISTORY_MAX:
del history[: len(history) - UNDO_HISTORY_MAX]
new_store = {
"z": zs_target.tolist(),
"u": u_along.tolist(),
"theta": th_arr.tolist(),
"_rev": int(store.get("_rev", 0)) + 1,
}
# Cache raw east/north wind (and θ / z) so the slider can re-project
# without re-downloading. Meta is kept so the status message can be
# refreshed after a reprojection.
raw_store = {
"z": zs_target.tolist(),
"u": u_arr.tolist(),
"v": v_arr.tolist(),
"theta": th_arr.tolist(),
"meta": {
"s3_key": meta.get("s3_key"),
"grid_lat": float(meta.get("grid_lat", float("nan"))),
"grid_lon": float(meta.get("grid_lon", float("nan"))),
"bytes": int(meta.get("bytes", 0)),
"n_levels": int(meta.get("n_levels", 0)),
"cycle": yyyymmddhh,
},
}
mb = meta["bytes"] / 1e6
msg = (
f"HRRR {yyyymmddhh} at grid point "
f"({meta['grid_lat']:.3f}°N, {meta['grid_lon']:.3f}°E) — "
f"{meta['n_levels']} levels, {mb:.1f} MB fetched. "
f"Flow from {flow_f:.0f}°."
)
return new_store, history, raw_store, msg, "mw-hrrr-status ok"
# --- HRRR reprojection on slider change ------------------------------
# When the flow-from slider moves, reuse the cached raw column (if any)
# and rewrite just the profile-store's u field. No network activity.
@app.callback(
[
Output("profile-store", "data", allow_duplicate=True),
Output("hrrr-status", "children", allow_duplicate=True),
Output("hrrr-status", "className", allow_duplicate=True),
],
Input("hrrr-dir", "value"),
[
State("hrrr-raw-store", "data"),
State("profile-store", "data"),
],
prevent_initial_call=True,
)
def _hrrr_redirect(flow_deg, raw, store):
# No cached column yet — slider moves before any fetch should be
# silent no-ops. (The next Fetch will pick up the current value.)
if not raw or "u" not in raw or "v" not in raw:
return no_update, no_update, no_update
try:
flow_f = float(flow_deg)
except (TypeError, ValueError):
return no_update, no_update, no_update
try:
from .hrrr import along_flow_signed
except ImportError:
return no_update, no_update, no_update
u_raw = np.asarray(raw["u"], dtype=float)
v_raw = np.asarray(raw["v"], dtype=float)
# Signed projection — keep wind reversals instead of clipping to 0.
u_along = along_flow_signed(u_raw, v_raw, flow_f)
new_store = {
"z": list(raw["z"]),
"u": u_along.tolist(),
"theta": list(raw["theta"]),
"_rev": int((store or {}).get("_rev", 0)) + 1,
}
meta = raw.get("meta", {}) or {}
cycle = meta.get("cycle", "")
mb = float(meta.get("bytes", 0)) / 1e6
n_levels = int(meta.get("n_levels", 0))
glat = meta.get("grid_lat")
glon = meta.get("grid_lon")
if glat is not None and glon is not None:
loc = f"({glat:.3f}°N, {glon:.3f}°E)"
else:
loc = ""
msg = (
f"HRRR {cycle} at grid point {loc} — {n_levels} levels, "
f"{mb:.1f} MB cached. Reprojected: flow from {flow_f:.0f}°."
)
return new_store, msg, "mw-hrrr-status ok"
# Store → figures. Whenever the store changes we regenerate both
# editable profile figures (so the line follows the dragged shapes)
# and all four diagnostic profiles (L², Ri, N², dθ/dz).
@app.callback(
[
Output("u-profile-graph", "figure"),
Output("theta-profile-graph", "figure"),
Output("diag-scorer", "figure"),
Output("diag-ri", "figure"),
Output("diag-n2", "figure"),
Output("diag-dthdz", "figure"),
],
Input("profile-store", "data"),
)
def _redraw_profiles(store):
zs = np.asarray(store["z"])
us = np.asarray(store["u"])
thetas = np.asarray(store["theta"])
u_fig = _profile_editor_figure("Zonal wind u(z)", us, zs, xunit="m s⁻¹", xrange=U_RANGE)
th_fig = _profile_editor_figure(
"Potential temperature θ(z)", thetas, zs, xunit="K", xrange=THETA_RANGE
)
l_fig, ri_fig, n2_fig, dthdz_fig = _diagnostic_figures(store)
return u_fig, th_fig, l_fig, ri_fig, n2_fig, dthdz_fig
def main():
app = create_app()
app.run(debug=False, host="127.0.0.1", port=8050)
if __name__ == "__main__":
main()
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