:; cat << 'EOF' > /root/CISA-Vulnerability-Regulatory-Compliance-Tracker/SEC-FTC-FCC/app.py import streamlit as st import numpy as np import plotly.graph_objects as go import plotly.express as px st.set_page_config(page_title="CISA SEC/FTC Quantum & Hydrodynamics Tracker", layout="wide") st.title("CISA Vulnerability & Regulatory Compliance Tracker") st.subheader("Module: FractalPlanckQuantum & Hydrodynamic Deflection") # Sidebar Controls st.sidebar.header("Quantum & Field Parameters") n_scale = st.sidebar.slider("Scale Order (n)", 0.0, 5.0, 1.0, 0.1) d_fractal = st.sidebar.slider("Fractal Dimension (D_f)", 1.0, 3.0, 1.618, 0.05) mass_curvature = st.sidebar.slider("Field Mass Curvature (M)", 0.0, 10.0, 2.5, 0.5) # Invariant Calculation omega_n = np.exp(d_fractal - 1) * ((2 * np.pi) ** (-n_scale)) st.sidebar.metric("Calculated Invariant (Omega_n)", f"{omega_n:.6f}") # Provenance Badge st.sidebar.markdown("---") st.sidebar.markdown("**Provenance Telemetry**") st.sidebar.info("Gemini-Albert Dual Presidential Provenance Active\nNode: CISA-REG-FLUID-01") # Multi-Tab Layout tab_regulatory, tab_geodesic, tab_deflection = st.tabs([ "SEC/FTC Regulatory Risk", "Spacetime Geodesic Vector", "Newtonian Fluid Deflection" ]) with tab_regulatory: st.markdown("### SEC / FTC / FCC Risk Assessment (Quantum Scaled)") st.latex(r"\Omega_n(D_f) = h_0 \left(\frac{l}{l_P}\right)^{D_f - 1} (2\pi)^{-n}") base_cvss = [9.8, 8.5, 7.2, 6.1, 4.3] cve_ids = ["CVE-2026-0012", "CVE-2026-1194", "CVE-2026-3301", "CVE-2026-4410", "CVE-2026-8890"] adjusted_risk = [min(10.0, score * (1 + omega_n)) for score in base_cvss] fig_bar = px.bar( x=cve_ids, y=adjusted_risk, labels={'x': 'Vulnerability ID', 'y': 'Quantum-Adjusted Impact Score'}, title=f"Severity Matrix Scaled by Omega_n = {omega_n:.4f}", color=adjusted_risk, color_continuous_scale="Reds" ) st.plotly_chart(fig_bar, use_container_width=True) with tab_geodesic: st.markdown("### Physical Geodesic vs. Ideal Vector Trajectory") st.write("Visualizing real trajectory curvature under gravitational lensing and scale invariant phase shifts.") t = np.linspace(0, 12, 300) x = t y = mass_curvature * np.sin(t / (1 + omega_n)) * np.exp(-0.08 * t) z = mass_curvature * np.cos(t / (1 + omega_n)) * np.exp(-0.08 * t) fig_geo = go.Figure() fig_geo.add_trace(go.Scatter3d( x=x, y=y, z=z, mode='lines', name='Physical Path (Curved Geodesic)', line=dict(color=t, colorscale='Plasma', width=6) )) fig_geo.add_trace(go.Scatter3d( x=x, y=np.zeros_like(x), z=np.zeros_like(x), mode='lines', name='Ideal Flat Vector (Reference)', line=dict(color='white', width=3, dash='dash') )) fig_geo.update_layout( title="Spacetime Trajectory Perturbation", scene=dict( xaxis_title="Propagation (X)", yaxis_title="Transverse Deflection (Y)", zaxis_title="Orthogonal Shift (Z)" ), margin=dict(l=0, r=0, b=0, t=40) ) st.plotly_chart(fig_geo, use_container_width=True) with tab_deflection: st.markdown("### Newtonian Fluid Projectile Deflection Simulation") st.caption("Gemini-Albert Dual Presidential Provenance Verified Engine") col1, col2, col3 = st.columns(3) with col1: m_ratio = st.slider("Fluid/Mass Ratio (m_f / m_p)", 0.01, 2.0, 0.35, 0.01) with col2: v_impact = st.slider("Impact Velocity (km/s)", 1.0, 30.0, 11.2, 0.5) with col3: viscosity = st.slider("Dynamic Viscosity (Pa·s)", 0.001, 100.0, 12.5, 0.5) # Dynamic Calculations st.latex(r"F_{drag} = \frac{1}{2} \rho v_{rel}^2 C_d A + A_{surf} \mu \frac{\partial u}{\partial y}") st.latex(r"\Delta v_{deflect} = v_{impact} \cdot \left(1 - \frac{1}{1 + (m_f / m_p) \cdot \Omega_n}\right)") v_final = v_impact * (1 / (1 + m_ratio * omega_n)) delta_v = v_impact - v_final deflection_angle = np.degrees(np.arctan2(delta_v * 0.15, v_final)) torque_gen = 0.5 * viscosity * (v_impact * 1e3) * (1 + omega_n) m1, m2, m3 = st.columns(3) m1.metric("Velocity Reduction (\Delta v)", f"{delta_v:.3f} km/s") m2.metric("Angular Trajectory Deflection", f"{deflection_angle:.2f}°") m3.metric("Induced Shear Torque", f"{torque_gen:.1f} N·m") # 3D Hydrodynamic Deflection Path t_sim = np.linspace(0, 10, 200) x_proj = t_sim * v_impact fluid_entry = 3.0 mask = t_sim >= fluid_entry y_proj = np.zeros_like(t_sim) z_proj = np.zeros_like(t_sim) y_proj[mask] = (t_sim[mask] - fluid_entry)**1.5 * (delta_v * 0.2) z_proj[mask] = np.sin((t_sim[mask] - fluid_entry) * 2) * (viscosity * 0.05) fig_deflect = go.Figure() fig_deflect.add_trace(go.Scatter3d( x=x_proj, y=y_proj, z=z_proj, mode='lines', name='Deflected Projectile Trajectory', line=dict(color='cyan', width=6) )) fig_deflect.add_trace(go.Scatter3d( x=[fluid_entry * v_impact] * 20, y=np.linspace(-2, 2, 20), z=np.zeros(20), mode='markers', name='Newtonian Fluid Boundary', marker=dict(size=4, color='rgba(0, 255, 150, 0.5)') )) fig_deflect.update_layout( title="Hypervelocity Projectile Fluid Perimeter Interaction", scene=dict( xaxis_title="Forward Axis (X)", yaxis_title="Transverse Deflection (Y)", zaxis_title="Spin Instability Shift (Z)" ), margin=dict(l=0, r=0, b=0, t=40) ) st.plotly_chart(fig_deflect, use_container_width=True) EOF # Sync module directory cp /root/CISA-Vulnerability-Regulatory-Compliance-Tracker/SEC-FTC-FCC/app.py \ /root/CISA-Vulnerability-Regulatory-Compliance-Tracker/FractalPlanckQuantum/app.py # Relaunch Streamlit kill -9 $(pgrep -f "streamlit") 2>/dev/null PYTHONUNBUFFERED=1 nohup /root/venv/bin/python3 -m streamlit run /root/CISA-Vulnerability-Regulatory-Compliance-Tracker/SEC-FTC-FCC/app.py --server.port 8501 --server.address 0.0.0.0 --server.headless true > streamlit.log 2>&1 & sleep 3 cat streamlit.log