Angles

atack angle
α\alpha

trajectory angle
γ\gamma

roll angle
ϕ\phi

pitch angle
θ\theta

yaw angle
ψ\psi

slid angle
β\beta

Rates

roll rate
pp

pitch rate
qq

yaw rate
rr

Speed

Speed vector
V=u2+v2+w2V = \sqrt{u^2 + v^2 + w^2}

longitudinal speed vector
u=Vcosβcosαu = V \cos{\beta} \cos{\alpha}

lateral speed vector
v=Vsin(β)v = V \sin(\beta)

vertical speed vector
w=Vcosβsinαw = V \cos{\beta} \sin{\alpha}

Quaternions

η0=cos(ϕ2)cos(θ2)cos(ψ2)+sin(ϕ2)sin(θ2)sin(ψ2)\eta_0 = \cos(\frac{\phi}{2}) \cos(\frac{\theta}{2}) \cos(\frac{\psi}{2}) + \sin(\frac{\phi}{2}) \sin(\frac{\theta}{2}) \sin(\frac{\psi}{2})

η1=sin(ϕ2)cos(θ2)cos(ψ2)+cos(ϕ2)sin(θ2)sin(ψ2)\eta_1 = \sin(\frac{\phi}{2}) \cos(\frac{\theta}{2}) \cos(\frac{\psi}{2}) + \cos(\frac{\phi}{2}) \sin(\frac{\theta}{2}) \sin(\frac{\psi}{2})

η2=cos(ϕ2)sin(θ2)cos(ψ2)+sin(ϕ2)cos(θ2)sin(ψ2)\eta_2 = \cos(\frac{\phi}{2}) \sin(\frac{\theta}{2}) \cos(\frac{\psi}{2}) + \sin(\frac{\phi}{2}) \cos(\frac{\theta}{2}) \sin(\frac{\psi}{2})

η3=cos(ϕ2)cos(θ2)sin(ψ2)+sin(ϕ2)sin(θ2)cos(ψ2)\eta_3 = \cos(\frac{\phi}{2}) \cos(\frac{\theta}{2}) \sin(\frac{\psi}{2}) + \sin(\frac{\phi}{2}) \sin(\frac{\theta}{2}) \cos(\frac{\psi}{2})

[η0˙η1˙η2˙η3˙]=12[η1η2η3η0η3η2η3η0η1η2η1η0][pqr]=12[0pqrp0rqqr0prqp0][η0η1η2η3]\begin{bmatrix} \dot{\eta_0} \\ \dot{\eta_1} \\ \dot{\eta_2} \\ \dot{\eta_3} \\ \end{bmatrix} = \frac{1}{2} \begin{bmatrix} -\eta_1 & -\eta_2 & -\eta_3 \\ \eta_0 & -\eta_3 & \eta_2 \\ \eta_3 & \eta_0 & -\eta_1 \\ -\eta_2 & \eta_1 & \eta_0 \\ \end{bmatrix} \begin{bmatrix} p \\ q \\ r \\ \end{bmatrix} = \frac{1}{2} \begin{bmatrix} 0 & -p & -q & -r \\ p & 0 & r & -q \\ q & -r & 0 & p \\ r & q & -p & 0 \\ \end{bmatrix} \begin{bmatrix} \eta_0 \\ \eta_1 \\ \eta_2 \\ \eta_3 \\ \end{bmatrix}

Stabiliy Derivatives
CL0C_{L_0}

CLαC_{L_\alpha}

CLα˙C_{L_{\dot{\alpha}}}

CLqC_{L_q}

CD0C_{D_0}

CDαC_{D_\alpha}

CDα˙C_{D_{\dot{\alpha}}}

CDqC_{D_q}

Cm0C_{m_0}

CmαC_{m_\alpha}

Cmα˙C_{m_{\dot{\alpha}}}

CmqC_{m_q}

CyβC_{y_\beta}

ClβC_{l_\beta}

ClpC_{l_p}

ClrC_{l_r}

CnβC_{n_\beta}

CnpC_{n_p}

CnrC_{n_r}

Control Derivatives
CLδeC_{L_{\delta_{e}}}

CDδeC_{D_{\delta_{e}}}

CyδαC_{y_{\delta_{\alpha}}}

CyδrC_{y_{\delta_{r}}}

ClδaC_{l_{\delta_{a}}}

ClδrC_{l_{\delta_{r}}}

CyδaC_{y_{\delta_{a}}}

CmδeC_{m_{\delta_{e}}}

CnδaC_{n_{\delta_{a}}}

CnδrC_{n_{\delta_{r}}}

General equations

CL=LρVSC_L = \frac{L}{\rho V S}

CD=DρVSC_D = \frac{D}{\rho V S}

E=LD=CLCDE = \frac{L}{D} = \frac{C_L}{C_D}

F=maF = m a

P=FVP = F V

P=JtP = J t

Forces Coeficients

Lift

CL=CL0+CLαα+cˉ2V(CLα˙α˙+CLqq)+CLδeδeC_L = C_{L_0} + C_{L_\alpha} \alpha + \frac{\bar{c}}{2V} (C_{L_{\dot{\alpha}}} \dot{\alpha} + C_{L_q} q) + C_{L_{\delta_{e}}} \delta_{e}

Drag

CD=CD0+CDαα+cˉ2V(CDα˙α˙+CDqq)+CDδeδeC_D = C_{D_0} + C_{D_\alpha} \alpha + \frac{\bar{c}}{2V} (C_{D_{\dot{\alpha}}} \dot{\alpha} + C_{D_q} q) + C_{D_{\delta_{e}}} \delta_{e}

Lateral Force

Cy=Cyββ+Cyδαδα+CyδrδrC_y = C_{y_\beta} \beta + C_{y_{\delta_{\alpha}}} \delta_{\alpha} + C_{y_{\delta_{r}}} \delta{r}

Moments Coeficients

Roll

Cl=Clββ+b2V(Clpp+Clrr)+Clδaδa+ClδrδrC_l = C_{l_\beta} \beta + \frac{b}{2V} (C_{l_p} p + C_{l_r} r) + C_{l_{\delta_{a}}} \delta_{a} + C_{l_{\delta_{r}}} \delta_{r}

Pitch
Cm=Cm0+Cmαα+α+cˉ2V(Cmα˙α˙+Cmqq)+CmδeδeC_m = C_{m_0} + C_{m_\alpha} \alpha + \alpha + \frac{\bar{c}}{2V} (C_{m_{\dot{\alpha}}} \dot{\alpha} + C_{m_q} q) + C_{m_{\delta_{e}}} \delta_{e}

Yaw
Cn=Cnββ+b2V(Cnpp+Cnrr)+Cnδaδa+CnδrδrC_n = C_{n_\beta} \beta + \frac{b}{2V} (C_{n_p} p + C_{n_r} r) + C_{n_{\delta_{a}}} \delta_{a} + C_{n_{\delta_{r}}} \delta_{r}