Introduction & Context

In process engineering, tethered devices such as aerostats, floating booms, or dust-monitoring balloons must remain on station while exposed to wind. The rope tension that keeps them in place is the vector sum of the buoyant force (lifting the device) and the aerodynamic drag (pushing it downwind). Accurate prediction of this total tension is essential for selecting safe mooring hardware, avoiding line breakage, and ensuring that the device stays within the emission-monitoring zone required by environmental regulations.

Methodology & Formulas

  1. Wind speed conversion
    Convert the reported wind speed from km h−1 to m s−1: \[ v = \frac{v_{\text{wind}} \times 1000}{3600} \]
  2. Projected area of the ellipsoid
    When the wind is aligned with the major axis, the projected area is the area of the corresponding ellipse: \[ A = \pi \left(\frac{L}{2}\right)\left(\frac{d}{2}\right) \]
  3. Drag force
    The aerodynamic drag on the body is: \[ F_{\text{drag}} = \frac{1}{2}\rho v^{2}C_{\text{d}}A \] where
    • \(\rho\) = air density
    • \(C_{\text{d}}\) = drag coefficient (depends on Reynolds number and body shape)
    Aspect ratio \(L/d\) Typical \(C_{\text{d}}\) for prolate spheroid
    1 0.47
    2 0.25
    2.5–3 0.10–0.15
  4. Total rope tension
    The mooring line must withstand the vector resultant of buoyancy and drag: \[ T_{\text{total}} = \sqrt{T_{\text{buoyancy}}^{2} + F_{\text{drag}}^{2}} \]