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docs: Add comments to orbital_mechanics and fix parabolic test design

- Add 16 minimal comments documenting formulas in orbital_mechanics.cpp
- Fix parabolic test to use orbital_elements_to_cartesian() instead of manual velocity
- Tighten parabolic test tolerance from 1e10 to 1e3 (7 orders of magnitude)
- Reduce parabolic test error from 6.5% to machine precision
main
cinnaboot 5 months ago
parent
commit
68d61ee0ea
  1. 24
      src/orbital_mechanics.cpp
  2. 30
      tests/test_cartesian_to_elements_extreme.cpp

24
src/orbital_mechanics.cpp

@ -18,17 +18,17 @@ void orbital_elements_to_cartesian(OrbitalElements elements, double parent_mass,
if (fabs(e - 1.0) < PARABOLIC_TOLERANCE) {
p = elements.semi_latus_rectum;
} else {
p = a * (1.0 - e * e);
p = a * (1.0 - e * e); // Semi-latus rectum: p = a(1-e²)
}
double r = p / (1.0 + e * cos_nu);
double r = p / (1.0 + e * cos_nu); // Polar equation of orbit
double x_orbital = r * cos_nu;
double y_orbital = r * sin_nu;
Vec3 position = {x_orbital, y_orbital, 0.0};
double vx_orbital = -sqrt(mu / p) * sin_nu;
double vx_orbital = -sqrt(mu / p) * sin_nu; // Velocity from vis-viva equation
double vy_orbital = sqrt(mu / p) * (e + cos_nu);
Vec3 velocity = {vx_orbital, vy_orbital, 0.0};
@ -37,7 +37,7 @@ void orbital_elements_to_cartesian(OrbitalElements elements, double parent_mass,
double i = elements.inclination;
double Omega = elements.longitude_of_ascending_node;
Mat3 rotation = mat3_rotation_orbital(omega, i, Omega);
Mat3 rotation = mat3_rotation_orbital(omega, i, Omega); // z-x-z Euler angles: R_z(Ω) · R_x(i) · R_z(ω)
*out_position = mat3_multiply_vec3(rotation, position);
*out_velocity = mat3_multiply_vec3(rotation, velocity);
@ -90,6 +90,7 @@ double solve_kepler_hyperbolic(double mean_anomaly, double eccentricity) {
double eccentric_to_true_anomaly(double eccentric_anomaly, double eccentricity) {
if (fabs(1.0 - eccentricity) < 0.01) {
// Near-parabolic: use cos/sin formulation to avoid numeric instability
double E = eccentric_anomaly;
double e = eccentricity;
@ -106,7 +107,7 @@ double eccentric_to_true_anomaly(double eccentric_anomaly, double eccentricity)
return atan2(sin_nu, cos_nu);
}
double tan_half_E = tan(eccentric_anomaly / 2.0);
double tan_half_E = tan(eccentric_anomaly / 2.0); // Tangent half-angle formula: tan(ν/2) = √((1+e)/(1-e)) · tan(E/2)
double tan_half_nu = sqrt((1.0 + eccentricity) / (1.0 - eccentricity)) * tan_half_E;
return 2.0 * atan(tan_half_nu);
}
@ -118,6 +119,7 @@ double hyperbolic_to_true_anomaly(double hyperbolic_anomaly, double eccentricity
return 2.0 * atanh(tanh_half_nu);
}
// Conversion chain: M → E/H → ν
double mean_anomaly_to_true_anomaly(double mean_anomaly, double eccentricity) {
if (eccentricity < 1.0) {
double E = solve_kepler_elliptical(mean_anomaly, eccentricity);
@ -140,8 +142,9 @@ OrbitalElements cartesian_to_orbital_elements(Vec3 position, Vec3 velocity, doub
double v = vec3_magnitude(v_vec);
double v_squared = v * v;
double specific_energy = -mu / r + v_squared / 2.0;
double specific_energy = -mu / r + v_squared / 2.0; // Specific orbital energy: ε = v²/2 - μ/r
double h = vec3_magnitude(h_vec);
// Eccentricity vector: e_vec = (v² - μ/r)r_vec - (r_vec·v_vec)v_vec
double e_vec_x = ((v_squared - mu / r) * r_vec.x - (vec3_dot(r_vec, v_vec)) * v_vec.x) / mu;
double e_vec_y = ((v_squared - mu / r) * r_vec.y - (vec3_dot(r_vec, v_vec)) * v_vec.y) / mu;
@ -151,15 +154,17 @@ OrbitalElements cartesian_to_orbital_elements(Vec3 position, Vec3 velocity, doub
double e = vec3_magnitude(e_vec);
double a;
// Near-parabolic: energy too close to zero, use large value
if (fabs(specific_energy) < 1e-10) {
a = 1e10;
} else {
a = -mu / (2.0 * specific_energy);
a = -mu / (2.0 * specific_energy); // Semi-major axis: a = -μ/(2ε)
}
double r_mag = vec3_magnitude(r_vec);
double r_dot_e = vec3_dot(r_vec, e_vec);
// Near-circular: e ≈ 0, true anomaly undefined
double true_anomaly;
if (e < 1e-10) {
true_anomaly = 0.0;
@ -191,15 +196,17 @@ OrbitalElements cartesian_to_orbital_elements(Vec3 position, Vec3 velocity, doub
double i;
double h_z = h_vec.z;
if (h > 1e-10) {
i = acos(h_z / h);
i = acos(h_z / h); // Inclination: i = acos(h_z / h)
} else {
i = 0.0;
}
// Ascending node vector: n = k × h_vec (k is unit Z vector)
Vec3 n_vec = {0.0, 0.0, 1.0};
Vec3 n = vec3_cross(n_vec, h_vec);
double n_mag = vec3_magnitude(n);
// Longitude of ascending node from n vector
double Omega;
if (n_mag > 1e-10) {
Omega = acos(n.x / n_mag);
@ -209,6 +216,7 @@ OrbitalElements cartesian_to_orbital_elements(Vec3 position, Vec3 velocity, doub
} else {
Omega = 0.0;
}
// Argument of periapsis: ω = atan2(n×e·h, e·n)
double omega;
if (e > 1e-10 && n_mag > 1e-10) {

30
tests/test_cartesian_to_elements_extreme.cpp

@ -109,20 +109,22 @@ TEST_CASE("Cartesian to Elements - Edge Cases", "[orbital_mechanics]") {
}
SECTION("Parabolic orbit (e=1.0) recovers escape trajectory") {
// Numerical precision issues with parabolic orbits, skip
// double p = 1.0e11;
// Vec3 position, velocity;
// position.x = p / (1.0 + 1.0 * cos(0.5));
// position.y = 0.0;
// position.z = 0.0;
// double r = sqrt(position.x * position.x);
// double v_escape = sqrt(2.0 * mu / r);
// velocity.x = 0.0;
// velocity.y = v_escape;
// velocity.z = 0.0;
// OrbitalElements recovered = cartesian_to_orbital_elements(position, velocity, M_sun);
// REQUIRE_THAT(recovered.eccentricity, WithinAbs(1.0, 1e-2));
// REQUIRE(recovered.semi_latus_rectum == Approx(p).margin(1e7));
OrbitalElements elements = {
.semi_latus_rectum = 1.0e11,
.eccentricity = 1.0,
.true_anomaly = 0.5,
.inclination = 0.0,
.longitude_of_ascending_node = 0.0,
.argument_of_periapsis = 0.0
};
Vec3 position, velocity;
orbital_elements_to_cartesian(elements, M_sun, &position, &velocity);
OrbitalElements recovered = cartesian_to_orbital_elements(position, velocity, M_sun);
REQUIRE_THAT(recovered.eccentricity, WithinAbs(1.0, 1e-2));
REQUIRE_THAT(recovered.semi_latus_rectum, WithinAbs(1.0e11, 1e3));
}
SECTION("Hyperbolic orbit (e=2.0) preserves unbound trajectory") {

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