Introduction & Context

A gravity settling tank is the simplest device for separating dispersed phases (drops, bubbles, or solid particles) from a continuous fluid. Its capacity design answers the question: “What volumetric throughput \(Q\) can a tank of given plan area \(A\) handle while guaranteeing that all particles larger than a specified cut-off diameter \(d_{min}\) are removed?” The answer is governed by two independent velocities:

  1. The terminal settling velocity \(v_t\) of the particle in the continuous phase.
  2. The superficial velocity \(v_s\) of the continuous phase, defined as the volumetric flow rate divided by the tank’s horizontal cross-section, \(v_s = Q/A\).

Because these velocities are independent, the design criterion is purely kinematic: the settling velocity must exceed the superficial velocity. No further numerical calculation is required once \(v_t\) is known from Stokes’ or Newton’s laws. The method is ubiquitous in water treatment, oil–water separation, decanter design, and dust chambers.

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Methodology & Formulas

  1. Step 1 – Identify the flow regime
    The drag coefficient \(C_D\) depends on the particle Reynolds number \(Re_p = \dfrac{\rho_f v_t d}{\mu}\). Select the appropriate correlation:
    Regime Reynolds Range Drag Law Terminal Velocity Formula
    Stokes (laminar) \(Re_p \le 1\) \(C_D = \dfrac{24}{Re_p}\) \(v_t = \dfrac{g(\rho_p - \rho_f)d^2}{18\mu}\)
    Intermediate \(1 \lt Re_p \le 1000\) \(C_D = \dfrac{18.5}{Re_p^{0.6}}\) \(v_t = \sqrt{\dfrac{4g(\rho_p - \rho_f)d}{3\rho_f C_D}}\)
    Newton (turbulent) \(Re_p \gt 1000\) \(C_D \approx 0.44\) \(v_t = \sqrt{\dfrac{4g(\rho_p - \rho_f)d}{3\rho_f C_D}}\)
  2. Step 2 – Apply the capacity criterion
    For complete removal of particles of diameter \(d\), the superficial velocity must satisfy: \[ v_s \le v_t \quad \Rightarrow \quad \dfrac{Q}{A} \le v_t \] Hence, the minimum plan area required for a given flow rate is: \[ A_{min} = \dfrac{Q}{v_t} \] and the corresponding nominal residence time is: \[ \tau = \dfrac{H}{v_t} \] where \(H\) is the vertical height of the dispersion band.
  3. Step 3 – Check for hindered settling (optional)
    If the dispersed-phase volume fraction \(\phi\) exceeds 1%, correct the terminal velocity using the Richardson–Zaki relation: \[ v_t(\phi) = v_t(0)(1 - \phi)^n \] with exponent \(n\) between 2.4 (Stokes) and 4.8 (Newton).