Max q

The max q , or maximum dynamic pressure, condition is the point when an aerospace vehicle's atmospheric flight reaches the maximum difference between the fluid dynamics total pressure and the ambient static pressure. For an airplane, this occurs at the maximum speed at minimum altitude corner of the flight envelope. For a space vehicle launch, this occurs at the crossover point between dynamic pressure increasing with speed and static pressure decreasing with increasing altitude. This is an important design factor of aerospace vehicles, since the aerodynamic structural load on the vehicle is proportional to dynamic pressure.

Dynamic pressure
Dynamic pressure q is defined in incompressible fluid dynamics as $$q = \tfrac{1}{2} \rho v^2,$$ where ρ is the local air density, and v is the vehicle's velocity. The dynamic pressure can be thought of as the kinetic energy density of the air with respect to the vehicle, and for incompressible flow equals the difference between total pressure and static pressure. This quantity appears notably in the lift and drag equations.

For a car traveling at 56 mph at sea level (where the air density is about 0.0765 lb/ft3, ) the dynamic pressure on the front of the car is 0.0555 psi, about 0.38% of the static pressure (14.696 psi at sea level).

For an airliner cruising at 755 ft/s at an altitude of 33000 ft (where the air density is about 0.0258 lb/ft3), the dynamic pressure on the front of the plane is 1.586 psi, about 41% of the static pressure (3.84 psi).

In rocket launches
For a launch of a space vehicle from the ground, dynamic pressure is:
 * zero at lift-off, when the air density ρ is high but the vehicle's speed v = 0;
 * zero outside the atmosphere, where the speed v is high, but the air density ρ = 0;
 * always non-negative, given the quantities involved.

During the launch, the vehicle speed increases but the air density decreases as the vehicle rises. Therefore, by Rolle's theorem, there is a point where the dynamic pressure is maximal.

In other words, before reaching max q, the dynamic pressure increase due to increasing velocity is greater than the dynamic pressure decrease due to decreasing air density such that the net dynamic pressure (opposing kinetic energy) acting on the craft continues to increase. After passing max q, the opposite is true. The net dynamic pressure acting against the craft decreases faster as the air density decreases with altitude than it increases from increasing velocity, ultimately reaching 0 when the air density becomes zero.

This value is significant, since it is one of the constraints that determines the structural load that the vehicle must bear. For many vehicles, if launched at full throttle, the aerodynamic forces would be higher than what they can withstand. For this reason, they are often throttled down before approaching max q and back up afterwards, so as to reduce the speed and hence the maximum dynamic pressure encountered along the flight.

Examples
During a normal Space Shuttle launch, for example, max q value of 0.32 atmospheres occurred at an altitude of approximately 11 km, about one minute after launch. The three Space Shuttle Main Engines were throttled back to about 65–72% of their rated thrust (depending on payload) as the dynamic pressure approached max q. Combined with the propellant grain design of the solid rocket boosters, which reduced the thrust at max q by one third after 50 seconds of burn, the total stresses on the vehicle were kept to a safe level.

During a typical Apollo mission, the max q (also just over 0.3 atmospheres) occurred between 13 and(-) of altitude; approximately the same values occur for the SpaceX Falcon 9.

The point of max q is a key milestone during a space vehicle launch, as it is the point at which the airframe undergoes maximum mechanical stress.