Kinematics & Ballistics

Projectile Motion Simulator (Parabolic Trajectory & Air Drag)

Launch projectiles with RK4 precision, compare vacuum parabolas against quadratic air drag, and test 45° maximum range.

Real-Time RK4 Kinematic / Dynamical Waveform Recorder

Physical Principles & Mathematical Derivation

R = (v0² × sin(2θ)) / g, H_max = (v0 × sin θ)² / (2g)

In a uniform gravitational field with zero air resistance, horizontal velocity vx remains constant while vertical velocity vy accelerates downward at −g, tracing a symmetric Galileo parabola maximized at θ = 45°. Enabling quadratic air drag (Fd = kd·v²) breaks symmetry, steepens descent, and shifts optimal range angle below 45°.

Questions & Concepts

What physical equation governs Projectile Motion Simulator (Parabolic Trajectory & Air Drag)?

R = (v0² × sin(2θ)) / g, H_max = (v0 × sin θ)² / (2g) — In a uniform gravitational field with zero air resistance, horizontal velocity vx remains constant while vertical velocity vy accelerates downward at −g, tracing a symmetric Galileo parabola maximized at θ = 45°. Enabling quadratic air drag (Fd = kd·v²) breaks symmetry, steepens descent, and shifts optimal range angle below 45°.

How are the equations of motion integrated in this simulation?

Nonlinear differential equations are integrated at 240–300 Hz substeps using classical 4th-order Runge-Kutta (RK4) to maintain strict Hamiltonian energy accuracy.

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