Advanced Topics =============== This section covers advanced usage of MechanicsDSL for expert users and developers looking to extend the framework. .. contents:: Contents :local: :depth: 2 Performance Optimization ------------------------ Symbolic Simplification ~~~~~~~~~~~~~~~~~~~~~~~ Control simplification to balance speed vs. expression size: .. code-block:: python from mechanics_dsl.utils import config # Increase timeout for complex systems config.simplification_timeout = 30.0 # Or disable automatic simplification compiler = PhysicsCompiler() compiler.symbolic.auto_simplify = False # Manually simplify critical expressions simplified = compiler.symbolic.simplify(expr, timeout=60) Numerical Precision ~~~~~~~~~~~~~~~~~~~ Adjust solver tolerances for accuracy vs. speed: .. code-block:: python # High precision (slow) solution = compiler.simulate( (0, 100), rtol=1e-12, atol=1e-14, method='DOP853' ) # Lower precision (fast, for exploration) solution = compiler.simulate( (0, 100), rtol=1e-6, atol=1e-8, method='RK45' ) Caching ~~~~~~~ Leverage the built-in caching system: .. code-block:: python from mechanics_dsl.utils import LRUCache # Create a cache for expensive computations jacobian_cache = LRUCache(maxsize=1000) def cached_jacobian(expr, vars): key = (str(expr), tuple(str(v) for v in vars)) if key in jacobian_cache: return jacobian_cache[key] result = compute_jacobian(expr, vars) jacobian_cache[key] = result return result Stiff Systems ------------- Detecting Stiffness ~~~~~~~~~~~~~~~~~~~ Some mechanical systems are numerically stiff: - Systems with multiple timescales - Near equilibrium points - High spring constants .. code-block:: python # Enable automatic stiffness detection solution = compiler.simulate( (0, 100), detect_stiff=True # Default: True ) # Check what method was selected print(f"Method used: {solution['method']}") Implicit Solvers ~~~~~~~~~~~~~~~~ For stiff systems, use implicit methods: .. code-block:: python # BDF (Backward Differentiation Formula) solution = compiler.simulate((0, 100), method='BDF') # Radau IIA (5th order implicit) solution = compiler.simulate((0, 100), method='Radau') # LSODA (automatic switching) solution = compiler.simulate((0, 100), method='LSODA') Custom Solvers -------------- Implementing Custom Integrators ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Extend the solver framework: .. code-block:: python from mechanics_dsl.core.solver import NumericalSimulator import numpy as np class SymplecticEuler(NumericalSimulator): """Symplectic Euler integrator for Hamiltonian systems.""" def integrate(self, t_span, y0, dt): t = np.arange(t_span[0], t_span[1], dt) n = len(y0) // 2 y = np.zeros((len(y0), len(t))) y[:, 0] = y0 for i in range(len(t) - 1): q = y[:n, i] p = y[n:, i] # Symplectic update p_new = p + dt * self.dp_dt(q, p) q_new = q + dt * self.dq_dt(q, p_new) y[:n, i+1] = q_new y[n:, i+1] = p_new return {'t': t, 'y': y, 'success': True} Extending the Parser -------------------- Adding Custom Commands ~~~~~~~~~~~~~~~~~~~~~~ Extend the parser for domain-specific commands: .. code-block:: python from mechanics_dsl.core.parser import MechanicsParser, ASTNode from dataclasses import dataclass @dataclass class CustomCommandNode(ASTNode): name: str args: list class ExtendedParser(MechanicsParser): def parse_statement(self): token = self.peek() if token.value == '\\mycommand': return self.parse_mycommand() return super().parse_statement() def parse_mycommand(self): self.expect('COMMAND') # \mycommand self.expect('LBRACE') arg = self.parse_expression() self.expect('RBRACE') return CustomCommandNode('mycommand', [arg]) Adding New Physics Domains -------------------------- Create a new physics domain by inheriting from ``PhysicsDomain``: .. code-block:: python from mechanics_dsl.domains.base import PhysicsDomain import sympy as sp class ElectromagneticDomain(PhysicsDomain): """Electromagnetic field dynamics.""" def __init__(self, name='em_system'): super().__init__(name) self._charge = None self._mass = None self._E_field = None self._B_field = None def set_fields(self, E, B): self._E_field = E self._B_field = B def define_lagrangian(self): # L = T - V + (q/c) * v · A q, m, c = sp.symbols('q m c', real=True) # ... implementation pass def define_hamiltonian(self): # H = (p - qA/c)² / 2m + qφ pass def derive_equations_of_motion(self): # Lorentz force: F = q(E + v × B) pass def get_state_variables(self): return ['x', 'y', 'z', 'px', 'py', 'pz'] Code Generation Backends ------------------------ Creating a New Backend ~~~~~~~~~~~~~~~~~~~~~~ Add support for a new target platform: .. code-block:: python from mechanics_dsl.codegen.base import CodeGenerator class JuliaGenerator(CodeGenerator): """Generate Julia simulation code.""" @property def target_name(self): return "julia" @property def file_extension(self): return ".jl" def generate(self, output_file): code = self._generate_julia_code() with open(output_file, 'w') as f: f.write(code) return output_file def generate_equations(self): # Convert SymPy to Julia syntax from sympy.printing.julia import julia_code lines = [] for coord in self.coordinates: expr = self.equations.get(f"{coord}_ddot") julia_expr = julia_code(expr) lines.append(f" dydt[{idx}] = {julia_expr}") return "\n".join(lines) Parallel Execution ------------------ OpenMP Code Generation ~~~~~~~~~~~~~~~~~~~~~~ Generate parallelized C++ code: .. code-block:: python # Generate OpenMP-parallelized code compiler.compile_to_cpp( "simulation_omp.cpp", target="openmp" ) GPU Acceleration ~~~~~~~~~~~~~~~~ For large particle systems (SPH, N-body), use GPU backends: .. code-block:: python # Generate CUDA code (placeholder) compiler.compile_to_cpp( "simulation.cu", target="cuda" ) Testing and Validation ---------------------- Analytical Comparisons ~~~~~~~~~~~~~~~~~~~~~~ Validate against known solutions: .. code-block:: python import numpy as np # Simple pendulum small-angle analytical solution def analytical_pendulum(t, theta0, l, g): omega = np.sqrt(g / l) return theta0 * np.cos(omega * t) # Compare numerical = solution['y'][0] analytical = analytical_pendulum(solution['t'], 0.1, 1.0, 9.81) error = np.max(np.abs(numerical - analytical)) assert error < 1e-6, f"Error too large: {error}" Energy Conservation ~~~~~~~~~~~~~~~~~~~ Validate symplectic behavior: .. code-block:: python from mechanics_dsl.analysis import EnergyAnalyzer analyzer = EnergyAnalyzer() result = analyzer.check_conservation( solution, kinetic, potential, tolerance=1e-6 ) assert result['conserved'], \ f"Energy not conserved: {result['max_relative_error']}" Debugging --------- Verbose Logging ~~~~~~~~~~~~~~~ Enable detailed logs: .. code-block:: python from mechanics_dsl.utils import setup_logging setup_logging(level='DEBUG') Inspecting Symbolic Expressions ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ View derived equations: .. code-block:: python result = compiler.compile_dsl(source) # Print equations of motion for coord, eom in compiler.symbolic.equations.items(): print(f"{coord} = {eom}") # Pretty print with SymPy import sympy as sp sp.pprint(compiler.symbolic.lagrangian) Step-by-Step Execution ~~~~~~~~~~~~~~~~~~~~~~ Debug simulation issues: .. code-block:: python # Use small time steps solution = compiler.simulate( (0, 0.1), num_points=1000 ) # Check for NaN/Inf if not np.all(np.isfinite(solution['y'])): print("Simulation became unstable!") # Find where it failed bad_idx = np.where(~np.isfinite(solution['y']))[1][0] print(f"Failed at t = {solution['t'][bad_idx]}")