Reentry Heating Calculator

Simplified estimate using the Sutton-Graves stagnation-point approximation. Real reentry heating depends on many additional factors.

Why Reentry Vehicles Are Blunt, Not Pointed

Counterintuitively, a blunt reentry capsule survives atmospheric entry better than a sharp, pointed one. A blunt nose pushes the shock wave further away from the vehicle surface, and the Sutton-Graves relationship this calculator implements shows why: stagnation-point heat flux scales inversely with the square root of nose radius, so a larger nose radius meaningfully reduces peak heating even as velocity stays fixed.

The Formula

q = k × √(ρ / Rₘ) × v³

This is the Sutton-Graves approximation for simplified stagnation-point convective heat flux, where k is the Sutton-Graves constant (1.7415 × 10⁻⁴ in SI units), ρ is local atmospheric density, Rₘ is nose radius, and v is velocity.

Note: This is a simplified stagnation-point estimate, not a full reentry heating model. Real reentry heating depends on trajectory shape, vehicle geometry, ablation, radiative heat transfer, and more. It should not be used for actual mission or thermal protection system design.

Where This Calculation Matters

  • Thermal protection system sizing — peak heat flux estimates inform how much ablative or reusable heat shield material a vehicle needs at its stagnation point.
  • Nose radius tradeoffs — the cube relationship with velocity and inverse-square-root relationship with nose radius together explain why reentry capsules (Apollo, Dragon, Orion) use large blunt heat shields rather than aerodynamically sharp shapes.
  • Comparing entry velocities — because heating scales with velocity cubed, a modest increase in entry speed (such as a lunar-return trajectory versus a low-orbit return) produces a dramatic increase in peak heating.
  • Trajectory shaping — entry trajectories are designed to control the velocity-density profile the vehicle experiences, directly trading peak heat flux against total heat load.

Heat Flux Sensitivity to Velocity

Illustrative stagnation-point heat flux at a fixed nose radius (0.3 m) and density (0.001 kg/m³)
VelocityEntry scenarioHeat flux
3,000 m/sSuborbital return0.27 MW/m²
7,800 m/sLow Earth orbit return4.77 MW/m²
11,000 m/sLunar or deep-space return13.38 MW/m²

Roughly a 3.7x increase in velocity from the first to the third row produces close to a 50x increase in heat flux, illustrating the cubic velocity dependence.

How to Use This Calculator

  1. Enter the local atmospheric density in kg/m³.
  2. Enter the vehicle's nose radius in meters.
  3. Enter the velocity in m/s.
  4. Select Calculate to get the estimated stagnation-point heat flux.

Related Calculations

Check the entry velocity itself with the Mach Number Calculator, or trace it back to the deorbit maneuver with the Delta-V Calculator.