ballistics_engine/

stability_advanced.rs

// Advanced stability calculations using refined Miller formula and modern corrections
// Based on:
// - Don Miller's refined stability formula (2005)
// - Courtney-Miller's plastic-tip stability correction (2012)
// - Bryan Litz's stability refinements
//
// NOTE: Some advanced stability functions are experimental and kept for future use.
#![allow(dead_code)]

/// Advanced stability parameters for different bullet types
#[derive(Debug, Clone)]
pub struct StabilityParameters {
    /// Shape factor for nose profile (1.0 for tangent, 0.9 for secant)
    pub nose_shape_factor: f64,
    /// Boat tail effectiveness factor
    pub boat_tail_factor: f64,
    /// Legacy plastic-tip multiplier, retained at a neutral value for source compatibility.
    /// Use [`apply_courtney_miller_plastic_tip_correction`] with measured tip geometry.
    pub plastic_tip_factor: f64,
    /// Center of pressure adjustment
    pub cop_adjustment: f64,
}

impl StabilityParameters {
    pub fn for_bullet_type(bullet_type: &str, has_boat_tail: bool, _has_plastic_tip: bool) -> Self {
        match bullet_type.to_lowercase().as_str() {
            "match" | "bthp" => Self {
                nose_shape_factor: 0.95,
                boat_tail_factor: if has_boat_tail { 0.94 } else { 1.0 },
                plastic_tip_factor: 1.0,
                cop_adjustment: 0.98,
            },
            "vld" | "very_low_drag" => Self {
                nose_shape_factor: 0.88,
                boat_tail_factor: if has_boat_tail { 0.92 } else { 1.0 },
                plastic_tip_factor: 1.0,
                cop_adjustment: 0.96,
            },
            "hybrid" => Self {
                nose_shape_factor: 0.91,
                boat_tail_factor: if has_boat_tail { 0.93 } else { 1.0 },
                plastic_tip_factor: 1.0,
                cop_adjustment: 0.97,
            },
            "hunting" => Self {
                nose_shape_factor: 0.98,
                boat_tail_factor: if has_boat_tail { 0.95 } else { 1.0 },
                plastic_tip_factor: 1.0,
                cop_adjustment: 0.99,
            },
            _ => Self::default(),
        }
    }

    pub fn default() -> Self {
        Self {
            nose_shape_factor: 1.0,
            boat_tail_factor: 1.0,
            plastic_tip_factor: 1.0,
            cop_adjustment: 1.0,
        }
    }
}

/// Calculate advanced Miller stability with modern corrections.
///
/// `has_plastic_tip` is retained for source compatibility, but a Boolean cannot provide the tip
/// length required by the Courtney-Miller correction. No plastic-tip scalar is applied here; use
/// [`apply_courtney_miller_plastic_tip_correction`] on this result when tip length is known.
///
/// `air_density_kg_m3` is the resolved density for the complete atmospheric state. The
/// `temperature_k` argument is retained for source compatibility but is not applied separately;
/// callers changing temperature must supply the corresponding density.
pub fn calculate_advanced_stability(
    mass_grains: f64,
    velocity_fps: f64,
    twist_rate_inches: f64,
    caliber_inches: f64,
    length_inches: f64,
    air_density_kg_m3: f64,
    temperature_k: f64,
    bullet_type: &str,
    has_boat_tail: bool,
    has_plastic_tip: bool,
) -> f64 {
    if twist_rate_inches == 0.0 || caliber_inches == 0.0 || length_inches == 0.0 {
        return 0.0;
    }

    let params = StabilityParameters::for_bullet_type(bullet_type, has_boat_tail, has_plastic_tip);

    // Calculate base Miller stability
    let sg_base = calculate_miller_refined(
        mass_grains,
        twist_rate_inches,
        caliber_inches,
        length_inches,
        params.nose_shape_factor,
    );

    // Apply velocity correction (Miller's refined formula)
    let sg_velocity_corrected = apply_velocity_correction(sg_base, velocity_fps);

    // Apply atmospheric corrections
    let sg_atmosphere_corrected =
        apply_atmospheric_correction(sg_velocity_corrected, air_density_kg_m3, temperature_k);

    // Apply boat tail correction if applicable
    let sg_boat_tail = sg_atmosphere_corrected * params.boat_tail_factor;

    // Apply center of pressure adjustment
    sg_boat_tail * params.cop_adjustment
}

/// Apply the [Courtney-Miller correction] for a plastic-tipped bullet to a Miller stability value.
///
/// The original Miller denominator uses total length `L` in both `L * (1 + L^2)`. For a
/// plastic-tipped bullet, Courtney and Miller retain total length in the leading aerodynamic term
/// and use metal length only in the inertia term: `L * (1 + L_m^2)`. Therefore this multiplies the
/// uncorrected full-length stability by `(1 + L^2) / (1 + L_m^2)`, where lengths are in calibers and
/// `L_m = (total_length_inches - tip_length_inches) / caliber_inches`.
///
/// Returns `uncorrected_sg` unchanged when the geometry is non-finite or when
/// `0 < tip_length_inches < total_length_inches` is not satisfied.
///
/// [Courtney-Miller correction]: https://arxiv.org/abs/1410.5340
pub fn apply_courtney_miller_plastic_tip_correction(
    uncorrected_sg: f64,
    caliber_inches: f64,
    total_length_inches: f64,
    tip_length_inches: f64,
) -> f64 {
    if !caliber_inches.is_finite()
        || !total_length_inches.is_finite()
        || !tip_length_inches.is_finite()
        || caliber_inches <= 0.0
        || total_length_inches <= 0.0
        || tip_length_inches <= 0.0
        || tip_length_inches >= total_length_inches
    {
        return uncorrected_sg;
    }

    let total_length_calibers = total_length_inches / caliber_inches;
    let metal_length_calibers = (total_length_inches - tip_length_inches) / caliber_inches;
    let correction = (1.0 + total_length_calibers.powi(2)) / (1.0 + metal_length_calibers.powi(2));

    uncorrected_sg * correction
}

/// Miller's refined stability formula (2005 version)
fn calculate_miller_refined(
    mass_grains: f64,
    twist_rate_inches: f64,
    caliber_inches: f64,
    length_inches: f64,
    nose_shape_factor: f64,
) -> f64 {
    // Convert to calibers
    let twist_calibers = twist_rate_inches / caliber_inches;
    let length_calibers = length_inches / caliber_inches;

    // Miller's constant (refined from original 30)
    const MILLER_CONSTANT: f64 = 30.0;

    // Calculate moment of inertia factor
    // For modern bullets: (1 + L²) where L is length in calibers
    let inertia_factor = 1.0 + length_calibers.powi(2);

    // Base Miller formula with nose shape correction
    let numerator = MILLER_CONSTANT * mass_grains * nose_shape_factor;
    let denominator =
        twist_calibers.powi(2) * caliber_inches.powi(3) * length_calibers * inertia_factor;

    if denominator == 0.0 {
        return 0.0;
    }

    numerator / denominator
}

/// Velocity correction using the engine's canonical Miller cube-root approximation.
fn apply_velocity_correction(sg_base: f64, velocity_fps: f64) -> f64 {
    const VELOCITY_REFERENCE: f64 = 2800.0;

    let velocity_factor = (velocity_fps / VELOCITY_REFERENCE).powf(1.0 / 3.0);
    sg_base * velocity_factor
}

/// Atmospheric correction for non-standard conditions
fn apply_atmospheric_correction(sg: f64, air_density_kg_m3: f64, _temperature_k: f64) -> f64 {
    // Standard atmosphere at sea level
    const STD_DENSITY: f64 = 1.225; // kg/m³

    // Density altitude correction (MBA-942): canonical Miller is LINEAR in density ratio
    // (rho0/rho), matching stability.rs and py_ballisticcalc. Density already encodes the
    // temperature/pressure state, so applying `temperature_k` again would double-count it.
    if !air_density_kg_m3.is_finite() || air_density_kg_m3 <= 0.0 {
        return 0.0;
    }

    sg * (STD_DENSITY / air_density_kg_m3)
}

/// Legacy compatibility shim that returns `static_stability` unchanged.
///
/// This signature cannot calculate the aerodynamic dynamic-stability factor from the literature:
/// that requires lift, drag, pitch-moment, pitch-damping, angle-of-attack-rate derivatives, and
/// projectile inertia radii that are not present here. The former yaw and spin multipliers were
/// unsupported and have been removed.
///
/// [`crate::spin_drift::calculate_dynamic_stability`] is a different Miller gyroscopic-stability
/// calculation and is not a replacement for an aerodynamic dynamic-stability model.
#[deprecated(
    since = "0.22.18",
    note = "does not compute aerodynamic dynamic stability; retained as a neutral static-stability pass-through"
)]
pub fn calculate_dynamic_stability(
    static_stability: f64,
    _velocity_mps: f64,
    _spin_rate_rad_s: f64,
    _yaw_angle_rad: f64,
    _caliber_m: f64,
    _mass_kg: f64,
) -> f64 {
    static_stability
}

/// Predict stability over trajectory with velocity and spin decay.
///
/// `spin_decay_factor` is the current spin rate divided by muzzle spin rate, typically 0.95-0.98
/// because axial spin decays much more slowly than forward velocity.
pub fn predict_stability_at_distance(
    initial_stability: f64,
    initial_velocity_fps: f64,
    current_velocity_fps: f64,
    spin_decay_factor: f64,
) -> f64 {
    if initial_velocity_fps == 0.0 || current_velocity_fps == 0.0 {
        return initial_stability;
    }

    // Velocity ratio
    let velocity_ratio = current_velocity_fps / initial_velocity_fps;

    // At otherwise fixed aerodynamic conditions, gyroscopic stability follows
    // Sg ∝ spin_rate² / velocity². `spin_decay_factor` is already the independent spin-rate
    // retention ratio; multiplying it by velocity_ratio would incorrectly force spin to decay in
    // lockstep with forward speed and invert the downrange trend (MBA-1161).
    let stability_ratio = (spin_decay_factor / velocity_ratio).powi(2);

    initial_stability * stability_ratio
}

/// Check if bullet will remain stable throughout trajectory
pub fn check_trajectory_stability(
    muzzle_stability: f64,
    muzzle_velocity_fps: f64,
    terminal_velocity_fps: f64,
    spin_decay_factor: f64,
) -> (bool, f64, String) {
    let terminal_stability = predict_stability_at_distance(
        muzzle_stability,
        muzzle_velocity_fps,
        terminal_velocity_fps,
        spin_decay_factor,
    );

    let is_stable = terminal_stability >= 1.3; // Minimum for adequate stability

    let status = if terminal_stability < 1.0 {
        "UNSTABLE - Bullet will tumble".to_string()
    } else if terminal_stability < 1.3 {
        "MARGINAL - May experience accuracy issues".to_string()
    } else if terminal_stability < 1.5 {
        "ADEQUATE - Acceptable for most conditions".to_string()
    } else if terminal_stability < 2.5 {
        "GOOD - Optimal stability".to_string()
    } else {
        "OVER-STABILIZED - May reduce BC slightly".to_string()
    };

    (is_stable, terminal_stability, status)
}

#[cfg(test)]
mod tests {
    use super::*;

    #[test]
    fn test_advanced_stability() {
        // Test with .308 168gr Match bullet
        let stability = calculate_advanced_stability(
            168.0,   // mass in grains
            2700.0,  // velocity in fps
            10.0,    // twist rate in inches
            0.308,   // caliber in inches
            1.24,    // length in inches
            1.225,   // air density
            288.15,  // temperature in K
            "match", // bullet type
            true,    // has boat tail
            false,   // no plastic tip
        );

        println!("Calculated stability: {}", stability);

        // Should give stability around 1.4-1.8 for typical .308 Match
        assert!(stability > 1.3);
        assert!(
            stability < 2.5,
            "Stability {} exceeds upper bound",
            stability
        );
    }

    #[test]
    fn test_stability_prediction() {
        let (is_stable, terminal_sg, status) = check_trajectory_stability(
            2.2,    // muzzle stability
            2700.0, // muzzle velocity
            1900.0, // terminal velocity
            0.98,   // independent spin retention
        );

        println!(
            "is_stable: {}, terminal_sg: {}, status: {}",
            is_stable, terminal_sg, status
        );

        assert!(
            is_stable,
            "Expected stable trajectory but got: is_stable={}, terminal_sg={}, status={}",
            is_stable, terminal_sg, status
        );
        assert!(
            terminal_sg > 2.2,
            "SG must grow as velocity decays faster than spin: {terminal_sg}"
        );
        assert!(status.contains("OVER-STABILIZED"));
    }

    #[test]
    fn test_stability_parameters_bullet_types() {
        let match_params = StabilityParameters::for_bullet_type("match", true, false);
        let vld_params = StabilityParameters::for_bullet_type("vld", true, false);
        let hunting_params = StabilityParameters::for_bullet_type("hunting", true, true);
        let default_params = StabilityParameters::for_bullet_type("unknown", false, false);

        // VLD should have lower nose_shape_factor (more streamlined)
        assert!(vld_params.nose_shape_factor < match_params.nose_shape_factor);

        // A Boolean cannot determine the metal length needed by Courtney-Miller, so the legacy
        // scalar stays neutral and callers use the geometry-aware correction helper.
        assert_eq!(hunting_params.plastic_tip_factor, 1.0);

        // Default should have all factors at 1.0
        assert_eq!(default_params.nose_shape_factor, 1.0);
        assert_eq!(default_params.boat_tail_factor, 1.0);
    }

    #[test]
    fn plastic_tip_flag_never_reduces_advanced_stability() {
        let calculate = |has_plastic_tip| {
            calculate_advanced_stability(
                178.0,
                2800.0,
                10.0,
                0.308,
                1.420,
                1.225,
                288.15,
                "hunting",
                false,
                has_plastic_tip,
            )
        };

        let untipped = calculate(false);
        let tipped = calculate(true);
        assert_eq!(
            tipped.to_bits(),
            untipped.to_bits(),
            "a Boolean-only plastic-tip flag must not apply an invented correction"
        );
    }

    #[test]
    fn courtney_miller_correction_uses_metal_length_only_in_inertia_term() {
        // Published 60 gr V-MAX measurements: total length 0.868", metal length 0.738".
        let caliber_inches = 0.224_f64;
        let total_length_inches = 0.868_f64;
        let tip_length_inches = total_length_inches - 0.738;
        let uncorrected_sg = 1.0_f64;

        let total_length_calibers = total_length_inches / caliber_inches;
        let metal_length_calibers = (total_length_inches - tip_length_inches) / caliber_inches;
        let expected = uncorrected_sg * (1.0 + total_length_calibers.powi(2))
            / (1.0 + metal_length_calibers.powi(2));
        let corrected = apply_courtney_miller_plastic_tip_correction(
            uncorrected_sg,
            caliber_inches,
            total_length_inches,
            tip_length_inches,
        );

        assert!((corrected - expected).abs() < 1e-12);
        assert!((corrected - 1.351).abs() < 0.001);
        assert!(corrected > uncorrected_sg);
    }

    #[test]
    fn courtney_miller_correction_requires_physical_tip_geometry() {
        let uncorrected_sg = 1.5_f64;
        for (caliber_inches, total_length_inches, tip_length_inches) in [
            (0.0, 0.868, 0.130),
            (-0.224, 0.868, 0.130),
            (f64::NAN, 0.868, 0.130),
            (0.224, 0.0, 0.130),
            (0.224, f64::INFINITY, 0.130),
            (0.224, 0.868, 0.0),
            (0.224, 0.868, -0.130),
            (0.224, 0.868, 0.868),
            (0.224, 0.868, 0.900),
            (0.224, 0.868, f64::NAN),
        ] {
            let corrected = apply_courtney_miller_plastic_tip_correction(
                uncorrected_sg,
                caliber_inches,
                total_length_inches,
                tip_length_inches,
            );
            assert_eq!(corrected.to_bits(), uncorrected_sg.to_bits());
        }
    }

    #[test]
    fn test_stability_edge_cases() {
        // Zero twist rate should return 0
        let zero_twist = calculate_advanced_stability(
            168.0, 2700.0, 0.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );
        assert_eq!(zero_twist, 0.0);

        // Zero caliber should return 0
        let zero_caliber = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.0, 1.24, 1.225, 288.15, "match", true, false,
        );
        assert_eq!(zero_caliber, 0.0);

        // Zero length should return 0
        let zero_length = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 0.0, 1.225, 288.15, "match", true, false,
        );
        assert_eq!(zero_length, 0.0);
    }

    #[test]
    fn test_velocity_correction() {
        // Higher velocity should give higher stability
        let high_vel = calculate_advanced_stability(
            168.0, 3000.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );
        let low_vel = calculate_advanced_stability(
            168.0, 2000.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );

        assert!(
            high_vel > low_vel,
            "Higher velocity ({}) should give higher stability than lower velocity ({})",
            high_vel,
            low_vel
        );
    }

    #[test]
    fn velocity_correction_is_continuous_at_1400_fps() {
        let sg_base = 2.0;
        let epsilon = 1e-6;
        let below = apply_velocity_correction(sg_base, 1400.0 - epsilon);
        let at_boundary = apply_velocity_correction(sg_base, 1400.0);
        let above = apply_velocity_correction(sg_base, 1400.0 + epsilon);

        assert!(
            (below - at_boundary).abs() <= 1e-8,
            "velocity correction jumped from {below} to {at_boundary} at 1400 fps"
        );
        assert!((above - at_boundary).abs() <= 1e-8);
    }

    #[test]
    fn subsonic_velocity_uses_canonical_miller_cube_root() {
        let sg_base = 2.0_f64;
        let velocity_fps = 1050.0_f64;
        let expected = sg_base * (velocity_fps / 2800.0).powf(1.0 / 3.0);
        let actual = apply_velocity_correction(sg_base, velocity_fps);

        assert!(
            (actual - expected).abs() <= expected * 1e-12,
            "subsonic correction was {actual}, expected Miller value {expected}"
        );
    }

    #[test]
    fn advanced_stability_is_continuous_above_3000_fps() {
        let calculate = |velocity_fps| {
            calculate_advanced_stability(
                55.0,
                velocity_fps,
                12.0,
                0.224,
                0.75,
                1.225,
                288.15,
                "unknown",
                false,
                false,
            )
        };

        let at_threshold = calculate(3000.0);
        let just_above = calculate(3000.0 + 1e-6);
        let relative_change = (just_above / at_threshold - 1.0).abs();
        assert!(
            relative_change < 1e-8,
            "Sg jumped by {:.3}% immediately above 3000 fps",
            relative_change * 100.0
        );

        let high_velocity = calculate(4000.0);
        let expected_ratio = (4000.0_f64 / 3000.0).powf(1.0 / 3.0);
        assert!(
            (high_velocity / at_threshold - expected_ratio).abs() < 1e-12,
            "high-velocity Sg did not follow Miller cube-root scaling"
        );
    }

    #[test]
    fn test_atmospheric_correction() {
        // Higher altitude (lower density) should increase stability
        let sea_level = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );
        let high_altitude = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 1.24, 1.0, 288.15, "match", true, false,
        );

        assert!(
            high_altitude > sea_level,
            "High altitude ({}) should have higher stability than sea level ({})",
            high_altitude,
            sea_level
        );
    }

    #[test]
    fn atmospheric_correction_is_only_inverse_density_ratio() {
        let sg = 2.0_f64;
        let temperature_k = 308.15; // Deliberately non-standard to catch a second temperature term.

        for (density, expected) in [(1.225, 2.0), (1.0, 2.45), (0.6125, 4.0)] {
            let actual = apply_atmospheric_correction(sg, density, temperature_k);
            assert!(
                (actual - expected).abs() <= expected * 1e-12,
                "rho {density}: expected {expected}, got {actual}"
            );
        }
    }

    #[test]
    fn advanced_stability_does_not_double_count_temperature_at_fixed_density() {
        let calculate = |temperature_k| {
            calculate_advanced_stability(
                168.0,
                2800.0,
                10.0,
                0.308,
                1.24,
                1.0,
                temperature_k,
                "unknown",
                false,
                false,
            )
        };

        let cold = calculate(253.15);
        let standard = calculate(288.15);
        let hot = calculate(308.15);
        let unknown = calculate(f64::NAN);
        assert_eq!(cold.to_bits(), standard.to_bits());
        assert_eq!(hot.to_bits(), standard.to_bits());
        assert_eq!(unknown.to_bits(), standard.to_bits());
    }

    #[test]
    fn atmospheric_correction_rejects_nonphysical_density() {
        for density in [0.0, -1.0, f64::NAN, f64::INFINITY, f64::NEG_INFINITY] {
            let actual = apply_atmospheric_correction(2.0, density, 288.15);
            assert_eq!(
                actual.to_bits(),
                0.0_f64.to_bits(),
                "density {density} produced {actual}"
            );
        }
    }

    #[test]
    #[allow(deprecated)]
    fn legacy_dynamic_stability_is_neutral_without_aerodynamic_derivatives() {
        let legacy: fn(f64, f64, f64, f64, f64, f64) -> f64 = calculate_dynamic_stability;
        let ancillary_states = [
            (800.0, 1500.0, 0.0, 0.00782, 0.0109),
            (800.0, 1500.0, 0.5, 0.00782, 0.0109),
            (0.0, 0.0, 1.0, 0.00782, 0.0109),
            (f64::NAN, -20_000.0, f64::NAN, -0.009, f64::INFINITY),
        ];

        for static_sg in [
            0.0,
            -0.0,
            1.5,
            -1.0,
            f64::INFINITY,
            f64::NEG_INFINITY,
            f64::NAN,
        ] {
            for (velocity_mps, spin_rate_rad_s, yaw_angle_rad, caliber_m, mass_kg) in
                ancillary_states
            {
                let actual = legacy(
                    static_sg,
                    velocity_mps,
                    spin_rate_rad_s,
                    yaw_angle_rad,
                    caliber_m,
                    mass_kg,
                );
                assert_eq!(
                    actual.to_bits(),
                    static_sg.to_bits(),
                    "legacy API invented a dynamic correction without aerodynamic derivatives"
                );
            }
        }
    }

    #[test]
    fn test_predict_stability_at_distance() {
        let initial_sg = 1.8;
        let initial_vel = 2800.0;
        let current_vel = 2000.0;
        let spin_decay = 0.97;

        let predicted =
            predict_stability_at_distance(initial_sg, initial_vel, current_vel, spin_decay);
        let expected = initial_sg * (spin_decay / (current_vel / initial_vel)).powi(2);

        assert!((predicted - expected).abs() < 1e-12);
        assert!(
            predicted > initial_sg,
            "retaining 97% spin while losing velocity must increase SG: {predicted}"
        );

        let slower = predict_stability_at_distance(initial_sg, initial_vel, 1400.0, spin_decay);
        assert!(
            slower > predicted,
            "SG must increase monotonically as velocity falls at fixed spin retention"
        );
    }

    #[test]
    fn test_predict_stability_edge_cases() {
        // Zero initial velocity should return initial stability
        let zero_initial = predict_stability_at_distance(1.5, 0.0, 2000.0, 0.97);
        assert_eq!(zero_initial, 1.5);

        // Zero current velocity should return initial stability
        let zero_current = predict_stability_at_distance(1.5, 2800.0, 0.0, 0.97);
        assert_eq!(zero_current, 1.5);
    }

    #[test]
    fn test_trajectory_stability_status_messages() {
        // Use identical muzzle/terminal velocity and full spin retention to isolate status
        // thresholds from the downrange stability correction.
        let (is_stable, sg, status) = check_trajectory_stability(0.8, 2700.0, 2700.0, 1.0);
        assert!(!is_stable);
        assert!(sg < 1.0);
        assert!(status.contains("UNSTABLE"));

        // Marginal (1.0 - 1.3)
        let (is_stable, sg, status) = check_trajectory_stability(1.15, 2700.0, 2700.0, 1.0);
        assert!(!is_stable);
        assert!((1.0..1.3).contains(&sg));
        assert!(status.contains("MARGINAL"));

        // Over-stabilized (> 2.5)
        let (_, sg, status) = check_trajectory_stability(4.0, 2700.0, 2700.0, 1.0);
        assert!(sg > 2.5);
        assert!(status.contains("OVER-STABILIZED"));
    }

    #[test]
    fn test_different_calibers_stability() {
        // Smaller caliber with same twist should be less stable
        let large_caliber = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );
        let small_caliber = calculate_advanced_stability(
            90.0, 2700.0, 8.0, 0.264, 1.15, 1.225, 288.15, "match", true, false,
        );

        // Both should produce valid stability values
        assert!(large_caliber > 0.0);
        assert!(small_caliber > 0.0);
    }

    #[test]
    fn test_boat_tail_vs_flat_base() {
        let boat_tail = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", true, false,
        );
        let flat_base = calculate_advanced_stability(
            168.0, 2700.0, 10.0, 0.308, 1.24, 1.225, 288.15, "match", false, false,
        );

        // Flat base should have slightly higher stability factor applied
        // (boat_tail_factor < 1.0 for boat tails)
        assert!(flat_base > boat_tail);
    }
}