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Propulsion System Mathematical Model

This document defines the core mathematical model for the electric propulsion system (propeller + brushless motor + battery/ESC).

1) Symbols and Units

Symbol Description SI Unit
\(V\) Flight airspeed \(\text{m/s}\)
\(D\) Propeller diameter \(\text{m}\)
\(n\) Propeller shaft speed \(\text{1/s}\) (with \(n = \text{RPM}/60\))
\(\rho\) Air density \(\text{kg/m}^3\)
\(J\) Advance ratio Dimensionless
\(C_t, C_p\) Thrust and power coefficients Dimensionless
\(T\) Thrust force \(\text{N}\)
\(Q\) Propeller torque \(\text{N}\cdot\text{m}\)
\(P_{\text{shaft}}\) Shaft mechanical power \(\text{W}\)
\(K_v\) Motor speed constant \(\text{RPM/V}\)
\(K_t\) Motor torque constant \(\text{N}\cdot\text{m/A}\)
\(I\) Motor winding current \(\text{A}\)
\(I_0\) Motor no-load current \(\text{A}\)
\(R\) Motor internal winding resistance \(\Omega\)
\(R_{\text{system}}\) Lumped transmission system resistance \(\Omega\)
\(V_m\) Motor terminal voltage \(\text{V}\)
\(V_{\text{back}}\) Back-EMF voltage \(\text{V}\)

2) Propeller Aerodynamics

Propeller coefficients \(C_t(J, \text{RPM})\) and \(C_p(J, \text{RPM})\) are loaded from an empirical database and evaluated using bilinear interpolation.

Aerodynamic Equations

\[ J = \frac{V}{n D}, \quad n = \frac{\text{RPM}}{60} \]
\[ T = C_t \rho n^2 D^4 \]
\[ Q = \frac{C_p \rho n^2 D^5}{2\pi} \]
\[ P_{\text{shaft}} = 2\pi n Q = C_p \rho n^3 D^5 \]

3) Brushless DC Motor Model

The relationship between torque, back-EMF, and speed is defined below:

\[ K_t = \frac{30}{\pi K_v} \]
\[ I = \frac{Q}{K_t} + I_0 \]
\[ V_{\text{back}} = \frac{\text{RPM}}{K_v} (1 + \tau \omega) \]
\[ V_m = V_{\text{back}} + I R \]

where \(\tau\) is the magnetic lag time constant (set to \(0\) for first-order models), and \(\omega = n \cdot 2\pi\).


4) System Electrical Resistance & Power Chain

The voltage drops across ESC MOSFETs, battery internal resistance, cables, and connectors are modeled as a lumped transmission system resistance (\(R_{\text{system}}\)):

\[ V_m = \text{throttle} \times V_{\text{pack}} - I R_{\text{system}} \]

The overall electrical power drawn from the battery pack is:

\[ P_{\text{battery}} = \frac{V_m I + I^2 R_{\text{system}}}{\eta_{\text{discharge}}} \]

5) Coupled Equilibrium Condition

For a given throttle setting and airspeed, the equilibrium shaft speed (RPM) is the solution of the coupled electrical and aerodynamic torque equilibrium equation:

\[ F(\text{RPM}) = \text{throttle} \times V_{\text{pack}} - \Big( V_{\text{back}}(\text{RPM}) + I(\text{RPM}) (R + R_{\text{system}}) \Big) = 0 \]

A root-finding method (e.g., Brent's method) solves \(F(\text{RPM}) = 0\) for RPM. Once the equilibrium RPM is determined, \(T, Q, P_{\text{shaft}}, I\), and efficiency parameters are calculated.


References

  1. First-Order DC Electric Motor Model
    Mark Drela, MIT Aero & Astro, February 2007
    PDF Link

  2. Second-Order DC Electric Motor Model
    Mark Drela, MIT Aero & Astro, March 2006
    PDF Link