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Operation 31<br />

a) Horizontal velocity Vh or vertical rate of climb Vz (times an input factor).<br />

b) Aircraft altitude.<br />

c) Aircraft angular rate, ˙ θ (pull-up) or ˙ ψ (turn).<br />

d) Aircraft linear acceleration (airframe, inertial, or ground axes).<br />

If the variable is velocity, first the velocity is found for the specified maximum effort; then the performance<br />

is evaluated at that velocity times an input factor. For endurance, range, or climb, the slope of the quantity<br />

to be maximized must be zero; hence in all cases the target is zero. The slope of the quantity is evaluated<br />

by first-order backward difference. For the range, first the variable is found such that V/ ˙w is maximized<br />

(slope zero); then the variable is found such that V/ ˙w equals 99% of that maximum. Two maximum<br />

effort quantity/variable pairs can be specified, and solved in nested iterations. The secant method or<br />

the method of false position is used to solve for the maximum effort. The task of finding maximum<br />

endurance, range, or climb is usually solved using the golden-section method. A tolerance ɛ and a<br />

perturbation Δ are specified.<br />

Given the gross weight and useful load (from the flight condition or mission specification), the<br />

performance is calculated for this flight state. The calculated state information includes weight, speed<br />

and velocity orientation (climb and sideslip), aircraft Euler angles, rotor tip speeds, and aircraft controls.<br />

The aircraft weight statement defines the fixed useful load and operating weight for the design<br />

configuration. For each flight state, the fixed useful load may be different from the design configuration,<br />

because of changes in auxiliary-fuel-tank weight or kit weights or increments in crew or furnishings<br />

weights. Thus the fixed useful-load weight is calculated for the flight state; and from it the useful-load<br />

weight and operating weight. The gross weight, payload weight, and usable-fuel weight (in standard<br />

and auxiliary tanks) completes the weight information for the flight state.<br />

4–5 Environment and Atmosphere<br />

The aerodynamic environment is defined by the speed of sound cs, density ρ, and kinematic viscosity<br />

ν = μ/ρ of the air (or other fluid). These quantities can be obtained from the standard day (International<br />

Standard Atmosphere), or input directly. The following options are implemented:<br />

a) Input the altitude hgeom and a temperature increment ΔT . Calculate the temperature<br />

and pressure for the standard day, add ΔT , and then calculate the density from<br />

the equation of state for a perfect gas. Calculate the speed of sound and viscosity<br />

from the temperature.<br />

b) Input the pressure altitude hgeom and the temperature τ ( ◦ For ◦ C). Calculate the<br />

pressure for the standard day, and then the density from the equation of state for a<br />

perfect gas. Calculate the speed of sound and viscosity from the temperature.<br />

c) Input the density ρ and the temperature τ ( ◦ For ◦ C). Calculate the speed of sound<br />

and viscosity from the temperature.<br />

d) Input the density ρ, sound speed cs, and viscosity μ. Calculate the temperature<br />

from the sound speed.<br />

Here hgeom is the geometric altitude above mean sea level.<br />

The International Standard Atmosphere (ISA) is a model for the variation with altitude of pressure,

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