Spaces:
Running
Running
Update app.py
Browse filesseparate logic (orbmol and visualization )
app.py
CHANGED
|
@@ -10,12 +10,12 @@ from ase.md.verlet import VelocityVerlet
|
|
| 10 |
from ase.md.velocitydistribution import MaxwellBoltzmannDistribution
|
| 11 |
from ase.io.trajectory import Trajectory
|
| 12 |
|
| 13 |
-
#
|
| 14 |
try:
|
| 15 |
-
|
| 16 |
-
|
| 17 |
except Exception:
|
| 18 |
-
|
| 19 |
|
| 20 |
from orb_models.forcefield import pretrained
|
| 21 |
from orb_models.forcefield.calculator import ORBCalculator
|
|
@@ -67,16 +67,13 @@ def predict_molecule(xyz_content, charge=0, spin_multiplicity=1):
|
|
| 67 |
forces = atoms.get_forces() # eV/Å
|
| 68 |
|
| 69 |
lines = []
|
| 70 |
-
lines.append(f"Total Energy: {energy:.6f} eV")
|
| 71 |
-
lines.append("")
|
| 72 |
lines.append("Atomic Forces:")
|
| 73 |
for i, f in enumerate(forces):
|
| 74 |
-
lines.append(
|
| 75 |
-
|
| 76 |
-
)
|
| 77 |
max_force = float(np.max(np.linalg.norm(forces, axis=1)))
|
| 78 |
-
lines.append("")
|
| 79 |
-
lines.append(f"Max Force: {max_force:.4f} eV/Å")
|
| 80 |
|
| 81 |
os.unlink(xyz_file)
|
| 82 |
return "\n".join(lines), "Calculation completed with OrbMol"
|
|
@@ -86,17 +83,11 @@ def predict_molecule(xyz_content, charge=0, spin_multiplicity=1):
|
|
| 86 |
|
| 87 |
|
| 88 |
# =========================
|
| 89 |
-
# Trajectory → HTML 3D
|
| 90 |
-
# (funciona con o sin py3Dmol)
|
| 91 |
# =========================
|
| 92 |
def traj_to_html(traj_path, width=520, height=520, interval_ms=200):
|
| 93 |
-
"""
|
| 94 |
-
Genera un bloque HTML con 3Dmol para animar una lista de frames en XYZ.
|
| 95 |
-
Sin dependencias de JupyterLab.
|
| 96 |
-
"""
|
| 97 |
traj = Trajectory(traj_path)
|
| 98 |
xyz_frames = []
|
| 99 |
-
|
| 100 |
for atoms in traj:
|
| 101 |
symbols = atoms.get_chemical_symbols()
|
| 102 |
coords = atoms.get_positions()
|
|
@@ -105,37 +96,25 @@ def traj_to_html(traj_path, width=520, height=520, interval_ms=200):
|
|
| 105 |
parts.append(f"{s} {x:.6f} {y:.6f} {z:.6f}")
|
| 106 |
xyz_frames.append("\n".join(parts))
|
| 107 |
|
| 108 |
-
# HTML+JS autopackage
|
| 109 |
html = f"""
|
| 110 |
-
<div id="viewer_md" style="width:{width}px; height:{height}px;
|
| 111 |
<script src="https://3dmol.org/build/3Dmol-min.js"></script>
|
| 112 |
<script>
|
| 113 |
(function() {{
|
| 114 |
-
var
|
| 115 |
-
if (!element) return;
|
| 116 |
-
var viewer = $3Dmol.createViewer(element, {{backgroundColor: 'white'}});
|
| 117 |
var frames = {xyz_frames!r};
|
| 118 |
var i = 0;
|
| 119 |
-
|
| 120 |
function show(i) {{
|
| 121 |
viewer.clear();
|
| 122 |
-
viewer.addModel(frames[i],
|
| 123 |
-
viewer.setStyle({{}}, {{stick: {{}}
|
| 124 |
viewer.zoomTo();
|
| 125 |
viewer.render();
|
| 126 |
}}
|
| 127 |
-
|
| 128 |
-
if
|
| 129 |
-
|
| 130 |
-
}}
|
| 131 |
-
show(0);
|
| 132 |
-
}} else {{
|
| 133 |
-
show(0);
|
| 134 |
-
setInterval(function() {{
|
| 135 |
-
i = (i + 1) % frames.length;
|
| 136 |
-
show(i);
|
| 137 |
-
}}, {int(interval_ms)});
|
| 138 |
-
}}
|
| 139 |
}})();
|
| 140 |
</script>
|
| 141 |
"""
|
|
@@ -168,38 +147,39 @@ def run_md(xyz_content, charge=0, spin_multiplicity=1,
|
|
| 168 |
opt = LBFGS(atoms, logfile=None)
|
| 169 |
opt.run(fmax=0.05, steps=20)
|
| 170 |
|
| 171 |
-
# Velocidades (2*T por partición de energía)
|
| 172 |
MaxwellBoltzmannDistribution(atoms, temperature_K=2*float(temperature))
|
| 173 |
|
| 174 |
-
# Integrador NVE
|
| 175 |
dyn = VelocityVerlet(atoms, timestep=float(timestep) * units.fs)
|
| 176 |
|
| 177 |
-
# Trayectoria temporal
|
| 178 |
tf = tempfile.NamedTemporaryFile(suffix=".traj", delete=False)
|
| 179 |
tf.close()
|
| 180 |
traj = Trajectory(tf.name, "w", atoms)
|
| 181 |
dyn.attach(traj.write, interval=1)
|
| 182 |
-
|
| 183 |
-
# Ejecutar MD
|
| 184 |
dyn.run(int(steps))
|
| 185 |
|
| 186 |
-
|
| 187 |
-
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 188 |
|
| 189 |
-
# Limpieza archivo xyz temporal
|
| 190 |
try:
|
| 191 |
os.unlink(xyz_file)
|
| 192 |
except Exception:
|
| 193 |
pass
|
| 194 |
|
| 195 |
-
return f"MD completed: {int(steps)} steps at {int(temperature)} K",
|
| 196 |
|
| 197 |
except Exception as e:
|
| 198 |
return f"Error during MD simulation: {str(e)}", ""
|
| 199 |
|
| 200 |
|
| 201 |
# =========================
|
| 202 |
-
# Ejemplos
|
| 203 |
# =========================
|
| 204 |
examples = [
|
| 205 |
["""2
|
|
@@ -228,67 +208,31 @@ H -0.3630 -0.5133 -0.8887""", 0, 1],
|
|
| 228 |
# =========================
|
| 229 |
with gr.Blocks(theme=gr.themes.Ocean(), title="OrbMol Demo") as demo:
|
| 230 |
with gr.Tabs():
|
| 231 |
-
# -------- Tab 1:
|
| 232 |
with gr.Tab("Single Point Energy"):
|
| 233 |
with gr.Row():
|
| 234 |
with gr.Column(scale=2):
|
| 235 |
with gr.Column(variant="panel"):
|
| 236 |
-
gr.Markdown("# OrbMol Demo - Quantum-Accurate
|
|
|
|
| 237 |
|
| 238 |
-
gr.
|
| 239 |
-
"
|
| 240 |
-
"
|
|
|
|
| 241 |
)
|
| 242 |
|
| 243 |
-
gr.
|
| 244 |
-
|
| 245 |
-
gr.
|
| 246 |
-
|
| 247 |
-
|
| 248 |
-
|
| 249 |
-
|
| 250 |
-
|
| 251 |
-
|
| 252 |
-
|
| 253 |
-
|
| 254 |
-
),
|
| 255 |
-
lines=12,
|
| 256 |
-
info="Paste XYZ coordinates of your molecule here",
|
| 257 |
-
)
|
| 258 |
-
|
| 259 |
-
gr.Markdown("OMol-specific settings for total charge and spin multiplicity")
|
| 260 |
-
with gr.Row():
|
| 261 |
-
charge_input = gr.Slider(
|
| 262 |
-
value=0, label="Total Charge", minimum=-10, maximum=10, step=1
|
| 263 |
-
)
|
| 264 |
-
spin_input = gr.Slider(
|
| 265 |
-
value=1, maximum=11, minimum=1, step=1, label="Spin Multiplicity"
|
| 266 |
-
)
|
| 267 |
-
|
| 268 |
-
predict_btn = gr.Button("Run OrbMol Prediction", variant="primary", size="lg")
|
| 269 |
-
|
| 270 |
-
with gr.Column(variant="panel", elem_id="results", min_width=500):
|
| 271 |
-
gr.Markdown("## OrbMol Prediction Results")
|
| 272 |
-
|
| 273 |
-
results_output = gr.Textbox(
|
| 274 |
-
label="Energy & Forces",
|
| 275 |
-
lines=15,
|
| 276 |
-
interactive=False,
|
| 277 |
-
info="OrbMol energy and force predictions",
|
| 278 |
-
)
|
| 279 |
-
|
| 280 |
-
status_output = gr.Textbox(
|
| 281 |
-
label="Status",
|
| 282 |
-
interactive=False,
|
| 283 |
-
max_lines=1,
|
| 284 |
-
)
|
| 285 |
-
|
| 286 |
-
gr.Markdown("### Examples")
|
| 287 |
-
gr.Examples(
|
| 288 |
-
examples=examples,
|
| 289 |
-
inputs=[xyz_input, charge_input, spin_input],
|
| 290 |
-
label="Click any example to load it",
|
| 291 |
-
)
|
| 292 |
|
| 293 |
predict_btn.click(
|
| 294 |
predict_molecule,
|
|
@@ -299,43 +243,27 @@ with gr.Blocks(theme=gr.themes.Ocean(), title="OrbMol Demo") as demo:
|
|
| 299 |
with gr.Sidebar(open=True):
|
| 300 |
gr.Markdown("## Learn more about OrbMol")
|
| 301 |
with gr.Accordion("What is OrbMol?", open=False):
|
| 302 |
-
gr.Markdown(
|
| 303 |
-
|
| 304 |
-
|
| 305 |
-
|
| 306 |
-
)
|
| 307 |
-
|
| 308 |
-
|
| 309 |
-
"* Validate results for your use case\n"
|
| 310 |
-
"* Consider limitations of the training level of theory"
|
| 311 |
-
)
|
| 312 |
-
with gr.Accordion("Open source packages", open=False):
|
| 313 |
-
gr.Markdown(
|
| 314 |
-
"* Model code: orbital-materials/orb-models\n"
|
| 315 |
-
"* This demo uses ASE and Gradio"
|
| 316 |
-
)
|
| 317 |
-
|
| 318 |
-
# -------- Tab 2: MD + Visualización 3D --------
|
| 319 |
with gr.Tab("Molecular Dynamics"):
|
| 320 |
with gr.Row():
|
| 321 |
with gr.Column(scale=2):
|
| 322 |
-
|
| 323 |
-
|
| 324 |
-
|
| 325 |
-
|
| 326 |
-
|
| 327 |
-
|
| 328 |
-
|
| 329 |
-
spin_input_md = gr.Slider(value=1, minimum=1, maximum=11, step=1, label="Spin Multiplicity")
|
| 330 |
-
steps_input = gr.Slider(value=100, minimum=10, maximum=1000, step=10, label="Steps")
|
| 331 |
-
temp_input = gr.Slider(value=300, minimum=10, maximum=1000, step=10, label="Temperature (K)")
|
| 332 |
-
timestep_input = gr.Slider(value=1.0, minimum=0.1, maximum=5.0, step=0.1, label="Timestep (fs)")
|
| 333 |
-
run_md_btn = gr.Button("Run MD Simulation", variant="primary")
|
| 334 |
|
| 335 |
with gr.Column(variant="panel", min_width=520):
|
| 336 |
-
gr.Markdown("## MD Visualization")
|
| 337 |
md_status = gr.Textbox(label="MD Status", lines=2, interactive=False)
|
| 338 |
-
md_view = gr.HTML()
|
| 339 |
|
| 340 |
run_md_btn.click(
|
| 341 |
run_md,
|
|
|
|
| 10 |
from ase.md.velocitydistribution import MaxwellBoltzmannDistribution
|
| 11 |
from ase.io.trajectory import Trajectory
|
| 12 |
|
| 13 |
+
# Intentar importar Molecule3D para vista 3D nativa
|
| 14 |
try:
|
| 15 |
+
from gradio_molecule3d import Molecule3D
|
| 16 |
+
HAVE_MOL3D = True
|
| 17 |
except Exception:
|
| 18 |
+
HAVE_MOL3D = False
|
| 19 |
|
| 20 |
from orb_models.forcefield import pretrained
|
| 21 |
from orb_models.forcefield.calculator import ORBCalculator
|
|
|
|
| 67 |
forces = atoms.get_forces() # eV/Å
|
| 68 |
|
| 69 |
lines = []
|
| 70 |
+
lines.append(f"Total Energy: {energy:.6f} eV\n")
|
|
|
|
| 71 |
lines.append("Atomic Forces:")
|
| 72 |
for i, f in enumerate(forces):
|
| 73 |
+
lines.append(f"Atom {i+1}: [{f[0]:.4f}, {f[1]:.4f}, {f[2]:.4f}] eV/Å")
|
| 74 |
+
|
|
|
|
| 75 |
max_force = float(np.max(np.linalg.norm(forces, axis=1)))
|
| 76 |
+
lines.append(f"\nMax Force: {max_force:.4f} eV/Å")
|
|
|
|
| 77 |
|
| 78 |
os.unlink(xyz_file)
|
| 79 |
return "\n".join(lines), "Calculation completed with OrbMol"
|
|
|
|
| 83 |
|
| 84 |
|
| 85 |
# =========================
|
| 86 |
+
# Trajectory → HTML 3D fallback
|
|
|
|
| 87 |
# =========================
|
| 88 |
def traj_to_html(traj_path, width=520, height=520, interval_ms=200):
|
|
|
|
|
|
|
|
|
|
|
|
|
| 89 |
traj = Trajectory(traj_path)
|
| 90 |
xyz_frames = []
|
|
|
|
| 91 |
for atoms in traj:
|
| 92 |
symbols = atoms.get_chemical_symbols()
|
| 93 |
coords = atoms.get_positions()
|
|
|
|
| 96 |
parts.append(f"{s} {x:.6f} {y:.6f} {z:.6f}")
|
| 97 |
xyz_frames.append("\n".join(parts))
|
| 98 |
|
|
|
|
| 99 |
html = f"""
|
| 100 |
+
<div id="viewer_md" style="width:{width}px; height:{height}px;"></div>
|
| 101 |
<script src="https://3dmol.org/build/3Dmol-min.js"></script>
|
| 102 |
<script>
|
| 103 |
(function() {{
|
| 104 |
+
var viewer = $3Dmol.createViewer("viewer_md", {{backgroundColor: 'white'}});
|
|
|
|
|
|
|
| 105 |
var frames = {xyz_frames!r};
|
| 106 |
var i = 0;
|
|
|
|
| 107 |
function show(i) {{
|
| 108 |
viewer.clear();
|
| 109 |
+
viewer.addModel(frames[i], "xyz");
|
| 110 |
+
viewer.setStyle({{}}, {{stick: {{}}}});
|
| 111 |
viewer.zoomTo();
|
| 112 |
viewer.render();
|
| 113 |
}}
|
| 114 |
+
if(frames.length>0) show(0);
|
| 115 |
+
if(frames.length>1) setInterval(function(){{
|
| 116 |
+
i=(i+1)%frames.length; show(i);
|
| 117 |
+
}}, {int(interval_ms)});
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 118 |
}})();
|
| 119 |
</script>
|
| 120 |
"""
|
|
|
|
| 147 |
opt = LBFGS(atoms, logfile=None)
|
| 148 |
opt.run(fmax=0.05, steps=20)
|
| 149 |
|
|
|
|
| 150 |
MaxwellBoltzmannDistribution(atoms, temperature_K=2*float(temperature))
|
| 151 |
|
|
|
|
| 152 |
dyn = VelocityVerlet(atoms, timestep=float(timestep) * units.fs)
|
| 153 |
|
|
|
|
| 154 |
tf = tempfile.NamedTemporaryFile(suffix=".traj", delete=False)
|
| 155 |
tf.close()
|
| 156 |
traj = Trajectory(tf.name, "w", atoms)
|
| 157 |
dyn.attach(traj.write, interval=1)
|
|
|
|
|
|
|
| 158 |
dyn.run(int(steps))
|
| 159 |
|
| 160 |
+
if HAVE_MOL3D:
|
| 161 |
+
# Mostrar último frame en Molecule3D
|
| 162 |
+
last = traj[-1]
|
| 163 |
+
mol_xyz = f"{len(last)}\nFinal frame\n"
|
| 164 |
+
for s, (x, y, z) in zip(last.get_chemical_symbols(), last.get_positions()):
|
| 165 |
+
mol_xyz += f"{s} {x:.6f} {y:.6f} {z:.6f}\n"
|
| 166 |
+
view = Molecule3D(value=mol_xyz, label="Final Frame (XYZ)")
|
| 167 |
+
else:
|
| 168 |
+
view = traj_to_html(tf.name)
|
| 169 |
|
|
|
|
| 170 |
try:
|
| 171 |
os.unlink(xyz_file)
|
| 172 |
except Exception:
|
| 173 |
pass
|
| 174 |
|
| 175 |
+
return f"MD completed: {int(steps)} steps at {int(temperature)} K", view
|
| 176 |
|
| 177 |
except Exception as e:
|
| 178 |
return f"Error during MD simulation: {str(e)}", ""
|
| 179 |
|
| 180 |
|
| 181 |
# =========================
|
| 182 |
+
# Ejemplos
|
| 183 |
# =========================
|
| 184 |
examples = [
|
| 185 |
["""2
|
|
|
|
| 208 |
# =========================
|
| 209 |
with gr.Blocks(theme=gr.themes.Ocean(), title="OrbMol Demo") as demo:
|
| 210 |
with gr.Tabs():
|
| 211 |
+
# -------- Tab 1: Single Point --------
|
| 212 |
with gr.Tab("Single Point Energy"):
|
| 213 |
with gr.Row():
|
| 214 |
with gr.Column(scale=2):
|
| 215 |
with gr.Column(variant="panel"):
|
| 216 |
+
gr.Markdown("# OrbMol Demo - Quantum-Accurate Predictions")
|
| 217 |
+
gr.Markdown("OrbMol is a neural network potential trained on the OMol25 dataset.")
|
| 218 |
|
| 219 |
+
xyz_input = gr.Textbox(
|
| 220 |
+
label="XYZ Coordinates",
|
| 221 |
+
placeholder="Paste XYZ here...",
|
| 222 |
+
lines=12,
|
| 223 |
)
|
| 224 |
|
| 225 |
+
with gr.Row():
|
| 226 |
+
charge_input = gr.Slider(value=0, minimum=-10, maximum=10, step=1, label="Charge")
|
| 227 |
+
spin_input = gr.Slider(value=1, minimum=1, maximum=11, step=1, label="Spin Multiplicity")
|
| 228 |
+
|
| 229 |
+
predict_btn = gr.Button("Run OrbMol Prediction", variant="primary")
|
| 230 |
+
|
| 231 |
+
with gr.Column(variant="panel", min_width=500):
|
| 232 |
+
results_output = gr.Textbox(label="Energy & Forces", lines=15, interactive=False)
|
| 233 |
+
status_output = gr.Textbox(label="Status", interactive=False, max_lines=1)
|
| 234 |
+
|
| 235 |
+
gr.Examples(examples=examples, inputs=[xyz_input, charge_input, spin_input])
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 236 |
|
| 237 |
predict_btn.click(
|
| 238 |
predict_molecule,
|
|
|
|
| 243 |
with gr.Sidebar(open=True):
|
| 244 |
gr.Markdown("## Learn more about OrbMol")
|
| 245 |
with gr.Accordion("What is OrbMol?", open=False):
|
| 246 |
+
gr.Markdown("* Neural network potential for molecules\n* Built on Orb-v3, trained on OMol25\n* Supports charge and spin")
|
| 247 |
+
with gr.Accordion("Benchmarks", open=False):
|
| 248 |
+
gr.Markdown("* <1 kcal/mol error on Wiggle150\n* Accurate protein–ligand binding energies\n* Stable MD on biomolecules >20k atoms")
|
| 249 |
+
with gr.Accordion("Disclaimers", open=False):
|
| 250 |
+
gr.Markdown("* Validate results for your use case\n* Training level of theory may limit accuracy")
|
| 251 |
+
|
| 252 |
+
# -------- Tab 2: MD --------
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 253 |
with gr.Tab("Molecular Dynamics"):
|
| 254 |
with gr.Row():
|
| 255 |
with gr.Column(scale=2):
|
| 256 |
+
xyz_input_md = gr.Textbox(label="XYZ Coordinates", lines=12)
|
| 257 |
+
charge_input_md = gr.Slider(value=0, minimum=-10, maximum=10, step=1, label="Charge")
|
| 258 |
+
spin_input_md = gr.Slider(value=1, minimum=1, maximum=11, step=1, label="Spin Multiplicity")
|
| 259 |
+
steps_input = gr.Slider(value=100, minimum=10, maximum=1000, step=10, label="Steps")
|
| 260 |
+
temp_input = gr.Slider(value=300, minimum=10, maximum=1000, step=10, label="Temperature (K)")
|
| 261 |
+
timestep_input = gr.Slider(value=1.0, minimum=0.1, maximum=5.0, step=0.1, label="Timestep (fs)")
|
| 262 |
+
run_md_btn = gr.Button("Run MD Simulation", variant="primary")
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 263 |
|
| 264 |
with gr.Column(variant="panel", min_width=520):
|
|
|
|
| 265 |
md_status = gr.Textbox(label="MD Status", lines=2, interactive=False)
|
| 266 |
+
md_view = gr.HTML() if not HAVE_MOL3D else Molecule3D(label="Trajectory Viewer")
|
| 267 |
|
| 268 |
run_md_btn.click(
|
| 269 |
run_md,
|