Gravity's Influence
The primary force acting on a projectile in external ballistics is gravitational acceleration (g), typically taken as 9.81 m/s². This constant downward acceleration causes the projectile to decelerate as it moves towards Earth, resulting in its characteristic parabolic trajectory.
The vertical component of gravity directly impacts the projectile’s height and time of flight. The equation governing this motion is: Δy = v₀t + (1/2)gt² , where Δy is the change in vertical position, v₀ is the initial vertical velocity component, t is time, and g is the acceleration due to gravity.
Δy = v₀t + (1/2)gt²
Drag Force – Air Resistance
As a projectile travels through air, it experiences drag force, which opposes its motion. Drag is proportional to the square of the projectile’s velocity and depends on factors like air density and the projectile's cross-sectional area.
The drag force can be approximated by: F_drag = (1/2)ρC_dAV², where ρ is the air density, C_d is the drag coefficient (dependent on shape), A is the reference area, and V is the velocity.
F_drag = (1/2)ρC_dAV²
The Coriolis Effect
For projectiles traveling over significant distances, the Coriolis effect introduces a deflection perpendicular to both the projectile’s velocity and the Earth's axis of rotation. This force is not constant but varies with speed and latitude.
The Coriolis acceleration is given by: a_coriolis = -2Ω×v , where Ω is the angular velocity vector of the Earth (approximately 7.29 x 10⁻⁵ rad/s) and v is the projectile’s velocity vector.
a_coriolis = -2Ω×v
Wind Effects
Wind introduces a horizontal force component that significantly alters the trajectory, particularly at longer ranges. The wind’s effect is typically modeled as a constant or variable velocity vector acting on the projectile.
The resultant horizontal velocity due to wind is: V_wind = V_wind_component * cos(θ), where V_wind_component is the component of the wind speed and θ is the angle between the wind direction and the projectile's path.
V_wind = V_wind_component * cos(θ)
Trajectory Types & Calculations
Different firing angles result in distinct trajectories. A direct fire trajectory (0-5° angle) is most accurate for short ranges, while a half-circle trajectory (5-45° angle) is employed for engaging targets behind cover.
Calculating range (R) involves integrating the projectile’s acceleration over time, accounting for gravity, drag, and wind. A simplified approximation can be found using ballistic equations, but these are significantly impacted by environmental factors.
R ≈ ∫₀ᵀ v(t) dt (integration subject to initial conditions)
Key Considerations
Temperature and humidity affect air density, directly influencing drag. Higher temperatures generally lead to lower air densities and reduced drag.
Altitude also impacts air density; higher altitudes have lower air densities due to decreased atmospheric pressure.
Frequently asked questions
What is the significance of the drag coefficient (C_d)?
The drag coefficient quantifies a projectile’s aerodynamic properties. A streamlined shape will have a lower C_d than a blunt one, resulting in less drag at the same velocity.
How does wind speed affect range?
Increasing wind speed generally decreases range due to the increased drag force acting against the projectile’s motion. The effect is non-linear; small changes in wind can have disproportionately large impacts on trajectory.
Why is Coriolis deflection important for long-range fire?
The Coriolis effect becomes increasingly significant over longer distances due to the projectile’s higher velocity and its movement relative to the Earth's rotating frame of reference. It can cause a substantial deviation from the intended trajectory.
Try it live
Everything above runs in your browser — open External Ballistics Simulator and change the parameters while it is running. Nothing is installed, nothing is uploaded, the whole model lives in one tab.
▶ Open External Ballistics Simulator simulation